,language,creator,title,subject,keyword,identifier,description,date
0,['eng'],"['Mans, J']",['Search for a Higgs boson decaying to massive vector boson pairs at LEP'],['Particle Physics - Experimental Results'],"['Thesis', 'Thesis']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0204029'],"[""This dissertation presents a search for a Higgs boson decaying to massive vector boson pairs. The search is based on data collected by the L3 experiment at CERN during the 1999-2000 period. We present the details and results of analyses for six of the physical channels of hZ->WWff. The combined analyses exclude a fermiophobic Higgs decaying to massive vector boson pairs for 83.8 GeV < m_h < 104.2 GeV at a 95% confidence level with an unexcluded region between 88.8 GeV < m_h < 89.6 GeV. Monte Carlo predictions of the analyses' performance predict an exclusion range of 86.8 GeV < m_h <107.5 GeV. We also present model-independent branching ratio limits for the massive vector boson search, as well as a scan of the fermiophobic plane combining with the results of the LEP h->gamma gamma search.""]",['2002-04-23']
1,['eng'],"['Eigen, G']",['Detectors as a Function of Luminosity at e+ e- Machines'],['Particle Physics - Experimental Results'],"['talk, Ise-Shima 2001/02/19']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0112043'],['The performance of present multipurpose detectors at high luminosities is discussed.'],['2002-01-11']
2,['eng'],"['Biryukov, V M', 'Chepegin, V N', 'Chesnokov, Yu A', 'Kotov, V I', 'Lyudmirskiy, E A', 'Maisheev, V A', 'Troyanov, E F', 'Vishnevskiy, N K', 'Zarucheisky, V G']",['Development of crystal extraction studies at the IHEP accelerator'],['Particle Physics - Experimental Results'],"['string model', 'gauge field theory, Yang-Mills', 'phase space', 'sigma model', 'instanton', 'Higgs model, abelian', 'dimension, 2-4', 'vortex']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0111071'],['The crystal extraction of 10^7 proton/s on BEC experiment facility is described. Detailed computer analysis is made to explain the basic experimental results. Future high-intensity efficient extraction using a short crystal is announced.'],['2001-11-23']
3,['eng'],"['Boyarski, A M']",['Additives That Prevent Or Reverse Cathode Aging In Drift Chambers With Helium-Isobutane Gas'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2001/10/02', 'drift chamber, gas', 'drift chamber, damage', 'helium, organic compounds', 'gas, admixture', 'oxygen', 'water', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0111090'],"['Noise and Malter breakdown have been studied at high rates in a test chamber having the same cell structure and gas as in the BaBar drift chamber. The chamber was first damaged by exposing it to a high source level at an elevated high voltage, until its operating current at normal voltages was below 0.5nA/cm. Additives such as water or alcohol allowed the damaged chamber to operate at 25 nA/cm, but when the additive was removed the operating point reverted to the original low value. However with 0.2% to 0.5% oxygen or 5% carbon dioxide the chamber could operate at more than 25 nA/cm, and continued to operate at this level even after the additive was removed. This shows for the first time that running with an O2 or CO2 additive at high ionisation levels can cure a damaged chamber from breakdown problems.']",['2001-11-29']
4,['eng'],"['Abe, K']",['Improved Direct Measurement of $A_{b}$ and $A_{c}$ at the $Z^{0}$ Pole Using a Lepton Tag'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, hadronic decay', 'quark, charm', 'quark, beauty', 'quark, pair production', 'coupling, (Z0 quark antiquark)', 'parity, violation', 'cross section, angular dependence', 'quark, semileptonic decay', 'lepton, particle identification', 'analyzing power', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0111035'],"['The parity violation parameters $A_b$ and $A_c$ of the $Zb{\\bar b}$ and $Zc\\bar{c}$ couplings have been measured directly, using the polar angle dependence of the polarized cross sections at the $Z^0$ pole. Bottom and charmed hadrons were tagged via their semileptonic decays. Both the electron and muon analyses take advantage of new multivariate techniques to increase the analyzing power. Based on the 1993-98 SLD sample of 550,000 $Z^0$ decays produced with highly polarized electron beams we measure $ A_b = 0.919 \\pm 0.030_{stat} \\pm 0.024_{syst} $, and $ A_c = 0.583 \\pm 0.055_{stat} \\pm 0.055_{syst} $.']",['2001-11-12']
5,['eng'],"['Mangeol, D J']",['Correlations in the Charged-Particle Multiplicity Distribution'],['Particle Physics - Experimental Results'],"['Thesis', 'Thesis']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0110029'],"['In this thesis, we perform an analysis on e+e- hadronic Z decays recorded in 1994 and 1995 by the L3 detector of LEP at center-of-mass energy corresponding to the Z mass. The analysis is performed in parallel for all hadronic events and for selected b-quark and light-quark events. The distribution of two variables, the charged-particle multiplicity and the inclusive charged-particle momentum are measured, from which all the analysis is carried out. From the measurement of the charged-particle multiplicity distribution, it is possible to extract information concerning the dynamics of the interaction. Using moments, one can obtain informations on particle correlation. We measure the Hq moments of the charged-particle multiplicity distribution which give the relative amount of genuine q-particle correlation order q. An oscillatory pattern is observed when the H_q moments are plotted versus the order q. Comparisons with different theoretical approaches are discussed.']",['2001-10-17']
6,['eng'],"['Jones, L T']",['A search for GMSB sleptons with lifetime at ALEPH'],['Particle Physics - Experimental Results'],['Thesis'],['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0110022'],"['A search for slepton production via the decay of pair-produced neutralinos has been performed under the assumption that the sleptons have observable lifetime in the detector before each decaying to a lepton and a gravitino. Sleptons, neutralinos and gravitinos are particles predicted by the theory of supersymmetry, and are the supersymmetric partners of the Standard Model leptons, neutral bosons and of the graviton respectively. The search was performed in 628 inverse picobarns of data taken by the ALEPH detector at LEP centre-of-mass energies from 189 to 208 GeV. It was motivated by general predictions of Gauge-Mediated Supersymmetry Breaking (GMSB) models in which the lightest supersymmetric particle is always the gravitino. No evidence of the process was found. Model-independent cross-section limits are quoted as a function of neutralino mass, slepton mass and slepton lifetime in the case that the neutralino branching ratios to each slepton are equal at one third (the so-called slepton co-NLSP scenario) and in the case that the neutralino decays exclusively to the stau (the stau-NLSP scenario). Excluded regions in the neutralino-stau mass plane are shown for four gravitino masses under model-specific assumptions.']",['2001-10-15']
7,['eng'],[],['Dijet production in neutral current deep inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'neutral current', 'jet, pair production', 'kinematics, Breit frame', 'channel cross section, transverse energy', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'tables', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109029'],"['Dijet cross sections in neutral current deep inelastic ep scattering have been measured in the range $10 < \\Q2 < 10^4$ GeV$^2$ with the ZEUS detector at HERA using an integrated luminosity of 38.4 pb$^{-1}$. The cross sections, measured in the Breit frame using the $\\kt$ jet algorithm, are compared with next-to-leading-order perturbative QCD calculations using proton parton distribution functions. The uncertainties of the QCD calculations have been studied. The predictions are in reasonable agreement with the measured cross sections over the entire kinematic range.']",['2001-09-24']
8,['eng'],[],"[""Reconstruction of Vees, Kinks, $\\Xi^-$'s, and $\\Omega^-$'s in the Focus Spectrometer""]",['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium', 'charmed particle, photoproduction', 'hyperon, photoproduction', 'charmed particle, hadronic decay', 'hyperon, hadronic decay', 'particle identification', 'track data analysis, vertex', 'track data analysis, kink', 'mass spectrum', 'semiconductor detector, microstrip', 'proportional chamber', 'magnetic spectrometer', 'Batavia TEVATRON PS', 'Xi/c+ --> Xi- pi+ pi-', 'Xi- --> Lambda pi-', 'Omega- --> Lambda K-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109028'],"['We describe the various techniques developed in the Fermilab Wideband Experiments, E687 and FOCUS, to reconstruct long-lived states. The techniques all involve modifications to standard tracking techniques and are useful to report for future experiments.']",['2001-09-28']
9,['eng'],"['Garrow, K']","[""Nuclear transparency from quasielastic A(e,e'p) reactions uo to Q^2=8.1 (GeV/c)^2""]",['Particle Physics - Experimental Results'],"['electron nucleus, inelastic scattering', 'deuterium', 'carbon', 'iron', 'p, emission', 'nucleus, transparency', 'color, transparency', 'impulse approximation', 'dependence, mass number', 'momentum transfer, dependence', 'magnetic spectrometer, experimental results', 'Newport News CEBAF Linac', 'electron nucleus --> nucleus p electron', '3.06-5.56 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109027'],"[""The quasielastic (e,e$^\\prime$p) reaction was studied on targets of deuterium, carbon, and iron up to a value of momentum transfer $Q^2$ of 8.1 (GeV/c)$^2$. A nuclear transparency was determined by comparing the data to calculations in the Plane-Wave Impulse Approximation. The dependence of the nuclear transparency on $Q^2$ and the mass number $A$ was investigated in a search for the onset of the Color Transparency phenomenon. We find no evidence for the onset of Color Transparency within our range of $Q^2$. A fit to the world's nuclear transparency data reflects the energy dependence of the free proton-nucleon cross section.""]",['2001-09-28']
10,['eng'],"['Abe, K']",['Observation of the Decay $B \\to K \\mu^{+} \\mu^{-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'lepton, pair production', 'strange meson', 'neutral current, flavor changing', 'B, branching ratio', 'mass spectrum', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> K lepton+ lepton-', 'B --> K*(892) lepton+ lepton-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109026'],"['We report a search for the flavor-changing neutral current decay $B \\to K^{(*)} \\ell^{+} \\ell^{-}$ using a 29.1 fb${}^{-1}$ data sample accumulated at the $\\Upsilon(4S)$ resonance with the Belle detector at the KEKB $e^{+}e^{-}$ storage ring. The decay process $B\\to K\\mu^+\\mu^-$ is observed, for the first time, with a branching fraction of ${\\cal B}(B \\to K \\mu^{+} \\mu^{-}) = (0.99^{+0.40}_{-0.32}{}^{+0.13}_{-0.14}) \\times 10^{-6}$. In addition, we set 90% confidence level upper limits ${\\cal B}(B \\to K e^{+} e^{-}) < 1.3 \\times 10^{-6}$, ${\\cal B}(B \\to K^* e^{+} e^{-}) < 5.6 \\times 10^{-6}$ and ${\\cal B}(B \\to K^* \\mu^{+} \\mu^{-}) < 3.1 \\times 10^{-6}$.']",['2001-09-28']
11,['eng'],"['Affolder, T']",['Diffractive Dijet Production at sqrt(s)=630 and 1800 GeV at the Fermilab Tevatron'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, pair production', 'anti-p, structure function', 'diffraction, structure function', 'energy dependence', 'quantum chromodynamics, factorization', 'momentum spectrum, pomeron', 'pomeron, structure function', 'momentum spectrum, parton', 'transverse energy, energy spectrum', 'rapidity spectrum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet p anything', '630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109025'],"['We report a measurement of the diffractive structure function $F_{jj}^D$ of the antiproton obtained from a study of dijet events produced in association with a leading antiproton in $\\bar pp$ collisions at $\\sqrt s=630$ GeV at the Fermilab Tevatron. The ratio of $F_{jj}^D$ at $\\sqrt s=630$ GeV to $F_{jj}^D$ obtained from a similar measurement at $\\sqrt s=1800$ GeV is compared with expectations from QCD factorization and with theoretical predictions. We also report a measurement of the $\\xi$ ($x$-Pomeron) and $\\beta$ ($x$ of parton in Pomeron) dependence of $F_{jj}^D$ at $\\sqrt s=1800$ GeV. In the region $0.035<\\xi<0.095$, $|t|<1$ GeV$^2$ and $\\beta<0.5$, $F_{jj}^D(\\beta,\\xi)$ is found to be of the form $\\beta^{-1.0\\pm 0.1} \\xi^{-0.9\\pm 0.1}$, which obeys $\\beta$-$\\xi$ factorization.']",['2001-09-28']
12,['eng'],"['Goulianos, K']",['CDF results on diffraction from Run I and plans for Run II'],['Particle Physics - Experimental Results'],"['talk, Pruhonice 2001/06/09', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'diffraction, multiple', 'jet, pair production', 'rapidity, gap', 'cross section, energy dependence', 'anti-p, leading particle', 'momentum transfer, dependence', 'transverse energy, energy spectrum', 'diffraction, structure function', 'pomeron, exchange', 'exchange, (2pomeron)', 'factorization, violation', 'magnetic detector, CDF', 'experimental results', 'proposed experiment', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109024'],"['Results on soft and hard diffraction obtained by the CDF Collaboration in Run I of the Fermilab Tevatron pbar-p collider are reviewed and compared with results from the DESY e-p collider HERA and with theoretical expectations. In addition, the CDF program for diffractive studies in Run II is briefly reviewed with emphasis on the relevant detector upgrades and physics goals.']",['2001-09-28']
13,['eng'],"['Abe, K']","['Observation of Color-suppressed $\\bar{B}^0 \\to D^{0}\\pi^0$, $D^{*0}\\pi^0$, $D^0\\eta$, and $D^0\\omega$ Decays']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'anti-B0, hadronic decay', 'anti-B0, branching ratio', 'meson, pair production', 'D', 'D*(2010)', 'pi0', 'omega(783)', 'eta', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'anti-B0 --> charmed meson pi0', 'anti-B0 --> charmed meson eta', 'anti-B0 --> charmed meson omega(783)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109021'],"['We report the first observation of color-suppressed $\\bar{B}{}^0 \\to D^0 \\pi^0$, $D^{*0} \\pi^0$, $D^{0} \\eta$, and $D^{0}\\omega$ decays and evidence for $\\bar{B}{}^0 \\to D^{*0} \\eta$ and $D^{*0}\\omega$. The branching fractions are found to be ${\\cal B} (\\bar{B}{}^0 \\to D^0 \\pi^0) = (3.1 \\pm 0.4 \\pm 0.5) \\times 10^{-4}$, ${\\cal B} (\\bar{B}{}^0 \\to D^{*0} \\pi^0) = (2.7 ^{+0.8}_{-0.7} ^{+0.5}_{-0.6})\\times 10^{-4}$, ${\\cal B} (\\bar{B}{}^0 \\to D^0 \\eta) = (1.4 ^{+0.5}_{-0.4}\\pm 0.3) \\times 10^{-4}$, ${\\cal B} (\\bar{B}{}^0 \\to D^0 \\omega) = (1.8 \\pm 0.5 ^{+0.4}_{-0.3}) \\times 10^{-4}$, and we set 90% confidence level upper limits of ${\\cal B} (\\bar{B}{}^0 \\to D^{*0} \\eta) < 4.6\\times 10^{-4}$ and ${\\cal B} (\\bar{B}{}^0 \\to D^{*0} \\omega) < 7.9 \\times 10^{-4}$. The analysis is based on a data sample of 21.3 fb$^{-1}$ collected at the $\\Upsilon(4S)$ resonance by the Belle detector at the KEKB $e^{+} e^{-}$ collider.']",['2001-09-28']
14,['eng'],"['Apollinari, G']","['Additional studies of the anomalous $l+MET+2,3$ jet events observed by CDF']",['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'jet, multiple production', 'transverse energy, high', 'lepton, associated production', 'transverse momentum, high', 'transverse energy, missing-energy', 'kinematics', 'quark, heavy', 'electroweak interaction, validity test', 'new particle, search for', 'squark, scalar', 'squark, beauty', 'track data analysis, vertex', 'effective Lagrangian', 'Higgs particle, decay', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W (n)jet anything', 'anti-p p --> 2jet lepton missing-energy', 'anti-p p --> 3jet lepton missing-energy', 'quark antiquark --> W Higgs particle', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109020'],"['We present additional studies of the kinematics of the anomalous events observed by the CDF experiment. These events contain a high-$p_T$ lepton, large transverse missing energy ($\\MET$), and 2 or 3 high-$E_T$ jets, one of which contains both a displaced secondary vertex and a soft lepton. Previous articles detailed the selection and the kinematic properties of these events. In the present paper, we use several phenomenological approaches to model these data and to estimate their production cross section.']",['2001-09-26']
15,['eng'],"['Apollinari, G']",['Additional studies of the probability that the events with a superjet observed by CDF are consistent with the SM prediction'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'jet, multiple production', 'W, associated production', 'event shape analysis', 'kinematics, correlation', 'statistical analysis', 'quark, heavy', 'lepton', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W 2jet anything', 'anti-p p --> 3jet anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109019'],"['In the $\\W+$ 2,3 jet data collected by CDF during the 1992-1995 Fermilab collider run, 13 events were observed to contain a superjet when $4.4 \\pm 0.6$ events are expected. A previous article detailed the selection and the kinematical properties of these events. The present paper provides estimates of the probability that the kinematics of these 13 events is statistically consistent with the standard model prediction.']",['2001-09-26']
16,['eng'],"['Chekanov, S']",['Searches for excited fermions in ep collisions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'electron p, colliding beams', 'positron p, inclusive reaction', 'new particle, search for', 'quark, excited state', 'electron, excited state', 'neutrino, excited state', 'excited state, mass', 'excited state, decay', 'coupling, upper limit', 'mass, dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'electron* --> electron photon', 'electron* --> Z0 electron', 'electron* --> W neutrino', 'quark* --> quark photon', 'quark* --> W quark', 'neutrino* --> neutrino photon', 'neutrino* --> Z0 neutrino', 'neutrino* --> W electron', '300, 318 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109018'],"['Searches in ep collisions for heavy excited fermions have been performed with the ZEUS detector at HERA. Excited states of electrons and quarks have been searched for in e^+p collisions at a centre-of-mass energy of 300 GeV using an integrated luminosity of 47.7 pb^-1. Excited electrons have been sought via the decays e*->egamma, e*->eZ and e*->nuW. Excited quarks have been sought via the decays q*->qgamma and q*->qW. A search for excited neutrinos decaying via nu*->nugamma, nu*->nuZ and nu*->eW is presented using e^-p collisions at 318 GeV centre-of-mass energy, corresponding to an integrated luminosity of 16.7 pb^-1. No evidence for any excited fermion is found, and limits on the characteristic couplings are derived for masses below 250 GeV.']",['2001-09-26']
17,['eng'],"['García, F G']","['Hadronic Production of Lambda_c from 600 GeV/c pion, sigma and proton beams']",['Particle Physics - Experimental Results'],"['hadron nucleus, inclusive reaction', 'pi-', 'p', 'Sigma-', 'carbon', 'copper', 'Lambda/c+, hadroproduction', 'Antilambda/c+, hadroproduction', 'Lambda/c+, hadronic decay', 'production, asymmetry', 'mass spectrum', 'spectra, x-dependence', 'transverse momentum, spectra', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'hadron nucleus --> Lambda/c+ anything', 'Lambda/c+ --> p K pi', '540, 600 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109017'],"['We present data from Fermilab experiment E781 (SELEX) on the hadroproduction asymmetry for anti-Lambda_c compared to Lambda_c+ as a function of xF and pt2 distributions for Lambda_c+. These data were measured in the same apparatus using incident pi-, sigma- beams at 600 GeV/c and proton beam at 540 GeV/c. The asymmetry is studied as a function of xF. In the forward hemisphere with xF >= 0.2 both baryon beams exhibit very strong preference for producing charm baryons rather than charm antibaryons, while the pion beam asymmetry is much smaller. In this energy regime the results show that beam fragments play a major role in the kinematics of Lambda_c formation, as suggested by the leading quark picture.']",['2001-09-26']
18,['eng'],"['Moss, J M', 'Garvey, G T', 'Johnson, M B', 'Leitch, M J', 'McGaughey, P L', 'Kopeliovich, B Z', 'Potashnikova, I K', 'Peng, J C']",['Energy loss of fast quarks in nuclei'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'deuteron', 'carbon', 'calcium', 'iron', 'tungsten', 'muon, pair production', 'Drell-Yan process', 'quark, energy loss', 'shadowing', 'dependence, mass number', 'numerical calculations, interpretation of experiments', '800 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109014'],"['We report an analysis of the nuclear dependence of the yield of Drell-Yan (DY) dimuons from the 800 GeV/c proton bombardment of $^2H$, C, Ca, Fe, and W targets. A light-cone formulation of the DY process is employed in the rest frame of the nucleus. In this frame, for $x_2\\ll x_1$, DY production appears as bremsstrahlung of a virtual photon followed by decay into dileptons. We treat the two sources of nuclear suppression, energy loss and shadowing, in a consistent formulation. Shadowing, involving no free parameters, is calculated within the light-cone dipole formalism. Initial-state energy loss, the only unknown in the problem, is determined from a fit to the nuclear-dependence ratio versus $x_1$. With the assumption of constant energy loss per unit path length, we find $-dE/dz = 2.32 \\pm 0.52\\pm 0.5$ GeV/fm. This is the first observation of a nonzero energy loss of partons traveling in nuclear environment.']",['2001-09-13']
19,['eng'],"['Kudryavtsev, V A', 'Spooner, N J C', 'Lightfoot, P K', 'Roberts, J W', 'Lehner, M J', 'Gamble, T', 'Carson, M J', 'Lawson, T B', 'Lüscher, R', 'McMillan, J E', 'Morgan, B', 'Paling, S M', 'Robinson, M', 'Tovey, D R', 'Smith, N J T', 'Smith, P F', 'Alner, G J', 'Hart, S P', 'Lewin, J D', 'Preece, R M', 'Sumner, T J', 'Jones, W G', 'Quenby, J J', 'Ahmed, B', 'Bewick, A', 'Davidge, D', 'Dawson, J V', 'Howard, A S', 'Ivaniouchenkov, Yu', 'Joshi, M K', 'Lebedenko, V', 'Liubarsky, I', 'Barton, J C', 'Gerbier, G', 'Mallet, J', 'Mosca, L', 'Tao, Charling']",['Study and suppression of anomalous fast events in inorganic scintillators for dark matter searches'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'scintillation counter, crystal', 'cesium, iodine', 'deep underground detector']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109013'],"['The status of dark matter searches with inorganic scintillator detectors at Boulby mine is reviewed and the results of tests with a CsI(Tl) crystal are presented. The objectives of the latter experiment were to study anomalous fast events previously observed and to identify ways to remove this background. Clear indications were found that these events were due to surface contamination of crystals by alphas, probably from radon decay. A new array of unencapsulated NaI(Tl) crystals immersed either in liquid paraffin or pure nitrogen atmosphere is under construction at Boulby. Such an approach allows complete control of the surface of the crystals and the ability to remove any surface contamination. First data from the unencapsulated NaI(Tl) do not show the presence of anomalous fast events.']",['2001-09-13']
20,['eng'],"['Acosta, D']",['Study of the heavy flavor content of jets produced in association with W bosons in $p\\bar{p}$ collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'jet, associated production', 'jet, multiplicity', 'W, leptonic decay', 'quark, truth', 'quark, charm', 'quark, beauty', 'quark, decay', 'particle identification, flavor', 'track data analysis, vertex', 'transverse energy, missing-energy', 'lepton, momentum spectrum', 'lepton, rapidity spectrum', 'energy spectrum, transverse energy', 'transverse momentum, spectra', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W jet anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109012'],"['We present a detailed examination of the heavy flavor content of the $W $ + jet data sample collected with the CDF detector during the 1992-1995 collider run at the Fermilab Tevatron. Jets containing heavy flavor quarks are selected via the identification of secondary vertices or semileptonic decays of $b$ and $c$ quarks. There is generally good agreement between the rates of secondary vertices and soft leptons in the data and in the standard model simulation including single and pair production of top quarks. An exception is the number of events in which a single jet has both a soft lepton and a secondary vertex tag. In $W +$ 2,3 jet data, we find 13 such events where we expected 4.4 $\\pm$ 0.6 events. The kinematic properties of this small sample of events are statistically difficult to reconcile with the simulation of standard model processes.']",['2001-09-11']
21,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D', 'Azuelos, G', 'Bailey, I', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bell, P J', 'Bella, G', 'Bellerive, A', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Etzion, E', 'Fabbri, F', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hamann, M', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hauschildt, J', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kramer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lillich, J', 'Littlewood, C', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Masetti, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Moed, S', 'Mohr, W', 'Mori, T', 'Mutter, A', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oh, A', 'Okpara, A', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rozen, Y', 'Runge, K', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Toya, D', 'Trefzger, T M', 'Tricoli, A', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Ujvári, B', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for Lepton Flavour Violation in $e^+e^-$ Collisions at $\\sqrt{s}$ = 189 - 209 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'flavor, violation', 'channel cross section, energy dependence', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> muon electron', 'electron positron --> tau electron', 'electron positron --> tau muon', '189-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109011'],"['We search for lepton flavour violating events (e mu, e tau and mu tau) that could be directly produced in e+e- annihilations, using the full available data sample collected with the OPAL detector at centre-of-mass energies between 189 GeV and 209 GeV. In general, the Standard Model expectations describe the data well for all the channels and at each sqrt(s). A single e mu event is observed where according to our Monte Carlo simulations only 0.019 events are expected from Standard Model processes. We obtain the first limits on the cross-sections sigma(e+e- -> e mu, e tau and mu tau) as a function of sqrt(s) at LEP2 energies.']",['2001-09-11']
22,['eng'],"['Moinester, M A', 'Grajek, O A', 'Piasetzky, E', 'Sandacz, A']",['Color Transparency via Coherent Exclusive rho Production'],['Particle Physics - Experimental Results'],"['talk, Trento 2001/07/23', 'muon nucleus, exclusive reaction', 'carbon', 'lead', 'rho(770)0, electroproduction', 'rho(770)0, hadronic decay', 'coherence, length', 'color, transparency', 'dependence, mass number', 'momentum transfer, high', 'rho(770), angular distribution', 'numerical calculations, Monte Carlo', 'CERN SPS', 'muon nucleus --> nucleus rho(770)0 muon', '190 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109010'],['We examine the potential of the COMPASS experiment at CERN to study color transparency via exclusive coherent vector meson production in hard muon-nucleus scattering. It is demonstrated that COMPASS has high sensitivity to test this important prediction of perturbative QCD.'],['2001-09-11']
23,['eng'],"['Aubert, Bernard']",['Study of B-->D(*)anti-D(*) decays with the BABAR detector'],['Particle Physics - Experimental Results'],"['talk, Pasadena 2001/09/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'charmed meson, pair production', 'D', 'D*(2010)', 'Kobayashi-Maskawa angle, unitarity', 'B0, branching ratio', 'angular distribution', 'asymmetry, CP', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> 2D*(2010)', 'B0 --> D*(2010) D', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109009'],"['Decays of the type B-->D(*)anti-D(*) can be used to provide a measurement of the parameter sin2beta of the Unitarity Triangle that is complementary to that derived from the mode \\bpsiks. Here we report a measurement of the branching fraction and a study of the CP parity content for the decay B^0 --> D^{*+}D^{*-} with the BABAR detector. With data corresponding to an integrated luminosity of 20.7 fb^{-1} collected at the Upsilon(4S) resonance during 1999-2000, we determine the branching fraction to be BF(B^0-->D^{*+}D^{*-})=(8.0 +/- 1.6 (stat) +/- 1.2 (syst)) x 10^{-4}. The measured fraction of the component with odd CP parity is 0.22 +/- 0.18(stat) +/- 0.03(syst). Observation of a significant number of candidates in the decay modes B^0-->D^{*+}D^- and B^+ --> D^{*+}D^{*0} is reported. All results presented in this note are preliminary.']",['2001-09-11']
24,['eng'],"['Aubert, Bernard']",['Search for a Lifetime Difference in D^0 Decays'],['Particle Physics - Experimental Results'],"['talk, Pasadena 2001/09/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'mass spectrum, (K- pi+)', 'mass spectrum, (K+ K-)', 'D0, lifetime', 'lifetime, difference', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K+ K-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109008'],['The D^0 mixing parameter y = Delta Gamma/2 Gamma was determined by measuring the D^0 lifetime separately for the K^-pi^+ decay mode and the K^-K^+ decay mode with 12.4 fb^{-1} of data collected by the BABAR experiment in 2001. Backgrounds were suppressed with the D^* --> D^0pi^+ decay and particle identification. The following preliminary result was obtained: y = (-1.0 +/- 2.2 (stat) +/- 1.7 (syst))%.'],['2001-12-10']
25,['eng'],"['Aubert, Bernard']",['Measurement of the Branching Fraction for B^+ --> K^{*0} pi^+'],['Particle Physics - Experimental Results'],"['talk, Pasadena 2001/09/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B+, hadronic decay', 'B+, branching ratio', 'K*(892), intermediate state', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B+ --> K*(892) pi+', 'K*(892) --> K+ pi-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109007'],['We present a preliminary result of the branching fraction for the B meson decay to the final state K^+pi^-pi^+ via an intermediate K^{*0} resonance using the sample of approximately 23 million B-anti-B mesons produced at the Upsilon(4S) resonance with the BABAR detector at the PEP II e+e- collider. The K^{*0} was detected through the decay to the final state K^+pi^-. The result of this analysis is BF(B^+ --> K^{*0} pi^+) = (15.5 +/- 3.4 +/- 1.8) x 10^{-6} where the first error is statistical and the second is systematic.'],['2001-09-10']
26,['eng'],"['Aubert, Bernard']",['Search for B Decays into K0-anti-K0'],['Particle Physics - Experimental Results'],"['talk, Pasadena 2001/09/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'K0, pair production', 'final state, (2K0(S))', 'B0, branching ratio', 'upper limit', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> K0 anti-K0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109005'],['We present preliminary results of a search for B0-->K0-anti-K0 decays in the K0SK0S final state using a sample of approximately 23 million B-anti-B pairs collected by the BABAR detector at the PEP-II asymmetric B Factory at SLAC. We find no evidence for a signal and set an upper limit on the branching fraction of 7.3 x 10^{-6} at the 90% confidence level.'],['2001-09-10']
27,['eng'],[],['First Measurement of pi e -> pi e gamma Pion Virtual Compton Scattering'],['Particle Physics - Experimental Results'],"['electron p, interaction', 'Compton scattering, off-shell', 'electron, bound state', 'perturbation theory, chiral', 'channel cross section', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- electron --> pi- electron photon', '600 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109003'],"['Pion Virtual Compton Scattering (VCS) via the reaction pi e ---> pi e gamma was observed in the Fermilab E781 SELEX experiment. SELEX used a 600 GeV/c pi- beam incident on target atomic electrons, detecting the incident pi- and the final state pi-, electron and gamma. Theoretical predictions based on chiral perturbation theory are incorporated into a Monte Carlo simulation of the experiment and are compared to the data. The number of reconstructed events (9) and their distribution with respect to the kinematic variables (for the kinematic region studied) are in reasonable accord with the predictions. The corresponding pi- VCS experimental cross section is sigma=38.8+-13 nb, in agreement with the theoretical expectation sigma=34.7 nb.']",['2001-09-10']
28,['eng'],"['Bosi, F', 'Burdin, S V', 'Cavasinni, V', 'Costanzo, D', 'Del Prete, T', 'Flaminio, Vincenzo', 'Mazzoni, E', 'Roda, C', 'Usai, G L', 'Vasilev, A V']",['A device to characterize optical fibres'],['Detectors and Experimental Techniques'],"['calorimeter, hadronic', 'iron', 'scintillation counter, sandwich', 'optics, transformation', 'optics, fibre', 'radiation, yield', 'optics, absorption', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0109002'],"['ATLAS is a general purpose experiment approved for the LHC collider at CERN. An important component of the detector is the central hadronic calorimeter; for its construction more than 600,000 Wave Length Shifting (WLS) fibres (corresponding to a total length of 1,120 Km) have been used. We have built and put into operation a dedicated instrument for the measurement of light yield and attenuation length over groups of 20 fibres at a time. The overall accuracy achieved in the measurement of light yield (attenuation length) is 1.5% (3%). We also report the results obtained using this method in the quality control of a large sample of fibres.']",['2001-12-10']
29,['eng'],"['Abazov, V M']",['Subjet Multiplicity of Gluon and Quark Jets Reconstructed with the $k_{\\perp}$ Algorithm in $p\\bar{p}$ Collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'jet, multiplicity', 'quark, jet', 'gluon, jet', 'jet, particle identification', 'track data analysis, cluster', 'jet, transverse momentum', 'color', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108054'],"['The D0 Collaboration has studied for the first time the properties of hadron-collider jets reconstructed with a successive-combination algorithm based on relative transverse momenta ($k_{\\perp}$) of energy clusters. Using the standard value D = 1.0 of the jet-separation parameter in the $k_{\\perp}$ algorithm, we find that the $p_T$ of such jets is higher than the $E_T$ of matched jets reconstructed with cones of radius R = 0.7, by about 5 (8) GeV at $p_T \\approx 90$ (240) GeV. To examine internal jet structure, the $k_{\\perp}$ algorithm is applied within D = 0.5 jets to resolve any subjets. The multiplicity of subjets in jet samples at $\\sqrt{s} = 1800$ GeV and 630 GeV is extracted separately for gluons ($M_g$) and quarks ($M_q$), and the ratio of average subjet multiplicities in gluon and quark jets is measured as $(M_{g} - 1) / (M_{q} - 1) = 1.84 \\pm 0.15 (stat.) \\pm ^{0.22}_{0.18} (sys.)$. This ratio is in agreement with the expectations from the HERWIG Monte Carlo event generator and a resummation calculation, and with observations in $e^+e^-$ annihilations, and is close to the naive prediction for the ratio of color charges of $C_A/C_F = 9/4 = 2.25$.']",['2001-09-03']
30,['eng'],"['Smy, M B']",['Implications for Solar Neutrino Oscillations from Super-Kamiokande and SNO Data'],['Particle Physics - Experimental Results'],"['talk, Venice 2001/07/24', 'neutrino, solar', 'neutrino, oscillation', 'neutrino electron, elastic scattering', 'electron, energy spectrum', 'neutrino deuteron, interaction', 'charged current', 'neutrino, mixing angle', 'neutrino, mass difference', 'deep underground detector, Sudbury', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108053'],"['Super-Kamiokande uses neutrino-electron elastic scattering to measure the recoil electron spectrum and zenith-angle dependence of solar $^8$B neutrinos. SNO has measured the $^8$B neutrino--deuteron charged-current reaction rate. The elastic scattering rate, spectrum and zenith-angle dependence in conjunction with the charged-current reaction rate favors active neutrino oscillations at large mixing angles by about 3$\\sigma$ over the no-oscillation hypothesis and small mixing angles. The analysis is independent of the absolute $^8$B and {\\it hep} flux and assumes two-flavor oscillations described by mixing angle and mass$^2$ difference. Two allowed regions at large mixing are found.']",['2001-09-03']
31,['eng'],"['Kroseberg, J']",['Open Beauty Production at HERA'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'positron p, colliding beams', 'positron p, inclusive reaction', 'quark, beauty', 'quark, photoproduction', 'quark, semileptonic decay', 'lepton, transverse momentum', 'differential cross section, transverse momentum', 'channel cross section', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108052'],"['Recent results on open beauty production in positron-proton collisions at a centre-of-mass energy of 300 GeV are presented. The beauty photoproduction cross section is measured by ZEUS and H1 via the semileptonic decay. Both experiments use the transverse lepton momentum with respect to a jet as an observable. The H1 central silicon vertex detector makes it possible to analyse, in addition, the lepton impact parameter spectrum, thus exploiting lifetime information for the first time at HERA. The combined lifetime and transverse momentum signature is further used to observe beauty production for the first time in deep inelastic scattering. All results are compared with NLO QCD calculations.']",['2001-09-03']
32,['eng'],"['Bandourin, D V', 'Skachkov, N B']","['Separation of a single photon $\\gamma$ and products of the $\\pi^0,\\eta, K^0_s$ meson neutral decay channels using the CMS electromagnetic calorimeter']",['Particle Physics - Experimental Results'],"['particle identification, (eta K0(S) pi0 photon)', 'neutral particle, decay modes', 'neural network', 'calorimeter, electromagnetic', 'transverse energy, dependence', 'numerical calculations', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108051'],"['The artificial neural network approach is used here for a separation of signals from a single photon and products of pi0, eta, K^0_s meson neutral decay channels basing on the data from CMS electromagnetic calorimeter only. Rejection values for three considered types of mesons as a function of a single photon selection efficiencies are obtained for two Barrel and one Endcap pseudorapidity regions and initial Et values equal to 20, 40, 60 and 100 GeV.']",['2001-09-03']
33,['eng'],"['Bandourin, D V', 'Konoplyanikov, V F', 'Skachkov, N B']","['$\\pi^0, \\eta, \\omega, K^0_s$ mesons and a photon discrimination based on the calorimeter information in the CMS detector']",['Particle Physics - Experimental Results'],"['neutral particle, particle identification', 'neutral particle, decay modes', 'particle identification, (omega(783) eta K0(S) pi0 photon)', 'calorimeter, electromagnetic', 'rapidity dependence', 'transverse energy, dependence', 'angular distribution', 'numerical calculations, Monte Carlo', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108050'],"['The analysis of discrimination possibilities of pi0, eta, omega, K^0_s mesons and a photon was done. Basing on the calorimeter information only the rejection factors for two pseudorapidity regions 0.4<\\eta<1.0 and 1.6<\\eta<2.0 and six $\\Et$ values, equal to 20, 40, 60, 80, 100, 200 GeV, were obtained. The cases of eta, omega and K^0_s mesons decaying through neutral and charged channels were considered separately.']",['2001-09-03']
34,['eng'],[],['Centrality dependence of the expansion dynamics in Pb-Pb collisions at 158 A GeV/c'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'lead', 'charged particle, multiple production', 'correlation function, (2negative particle)', 'correction, Coulomb', 'hadron, formation', 'dependence, impact parameter', 'particle flow', 'velocity, expansion', 'nuclear reaction, temperature', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', '158 GeV/c/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108049'],"['Two-particle correlation functions of negatively charged hadrons from Pb-Pb collisions at 158 GeV/c per nucleon have been measured by the WA97 experiment at the CERN SPS. A Coulomb correction procedure that assumes an expanding source has been implemented. Within the framework of an expanding thermalized source model the size and dynamical state of the collision fireball at freeze-out have been reconstructed as a function of the centrality of the collision. Less central collisions exhibit a different dynamics than central ones: both transverse and longitudinal expansion velocities are slower, the expansion duration is shorter and the system freezes out showing smaller dimensions and higher temperature.']",['2001-09-03']
35,['eng'],"['Korzhavina, I A']",['Study of $D^{*+/-}$ Meson Production in Diffractive $ep$ Scattering at HERA'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'D*(2010), photoproduction', 'diffraction', 'rapidity, gap', 'D*(2010), hadronic decay', 'channel cross section', 'differential cross section, transverse momentum', 'rapidity dependence', 'mass, dependence', 'pomeron, resolved', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108048'],['$D^{*+/-}$ production in the diffractive interactions was measured with the ZEUS detector at HERA using integrated luminosities of 44 pb$^{-1}$ in deep inelastic scattering and 38 pb$^{-1}$ in photoproduction processes. Diffractive interactions were identified by a large gap in the rapidity distribution of final states. $D^{*+/-}$ mesons were reconstructed from the decay $D^{*+} -> D^0\\pi_s^+$ with {$D^0 -> K^-\\pi^+$} (+c.c.). Integrated and differential cross sections were compared to theoretical expectations.'],['2001-09-14']
36,['eng'],"['Adloff, C']",['D* Meson Production in Deep-Inelastic Diffractive Interactions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'diffraction', 'D*(2010), photoproduction', 'rapidity, gap', 'D*(2010), hadronic decay', 'differential cross section, momentum transfer', 'transverse momentum, dependence', 'rapidity dependence', 'fusion, photon gluon', 'quantum chromodynamics', 'pomeron, resolved', 'exchange, two-gluon', 'color, dipole', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108047'],"['A measurement is presented of the cross section for D* meson production in diffractive deep-inelastic scattering for the first time at HERA. The cross section is given for the process ep -> eXY, where the system X contains at least one D* meson and is separated by a large rapidity gap from a low mass proton remnant system Y. The cross section is presented in the diffractive deep-inelastic region defined by 2< Q^2 < 100 GeV^2, 0.05 < y < 0.7, x_pom < 0.04, M_Y < 1.6 GeV and |t| < 1 GeV^2. The D* mesons are restricted to the range ptD* > 2 GeV and |\\eta_D* | < 1.5. The cross section is found to be 246+-54+-56 pb and forms about 6% of the corresponding inclusive D* cross section. The cross section is presented as a function of various kinematic variables, including z_pom^obs which is an estimate of the fraction of the momentum of the diffractive exchange carried by the parton entering the hard-subprocess. The data show a large component of the cross section at low z_pom^obs where the contribution of the Boson-Gluon-Fusion process is expected to dominate. The data are compared with several QCD--based calculations.']",['2001-08-31']
37,['eng'],"['Battaglia, M']",['The CLIC Study'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/04/18', 'electron positron, linear collider', 'linear collider, proposed', 'accelerator, two-beam', 'new particle, search for', 'Higgs particle', 'supersymmetry', ""Z'"", 'CERN Lab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108045'],['The CLIC Study that aims at a linear collider able to deliver e+e- collisions at centre-of-mass energies up to 5 TeV with luminosity of 10^35 cm^-2 s^-1 is presented. Its physics potential is outlined with special emphasis to the relationships to the experience gained in a decade of e+e- experimentation at LEP.'],['2001-09-14']
38,['eng'],"['Hanagaki, K', 'Kakuno, H', 'Ikeda, H', 'Iijima, T', 'Tsukamoto, T']",['Electron Identification in Belle'],['Particle Physics - Experimental Results'],"['electron, particle identification', 'efficiency', 'Cherenkov counter, aerogel', 'calorimeter, electromagnetic', 'drift chamber', 'helium, organic compounds', 'ionization, energy loss', 'J/psi(3100), leptonic decay', 'magnetic detector, BELLE', 'KEK TRISTAN Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108044'],"['We report on electron identification methods and their performance in the Belle experiment at the KEK-B asymmetric B-Factory $e^{+} e^{-}$ storage ring. Electrons are selected using a likelihood approach that takes information from the electromagnetic calorimeter, the central drift chamber, and the silica aerogel Cherenkov counters as input. We achieve an electron identification efficiency of $(92.4 \\pm 0.4)%$ with a $\\pi^{\\pm}$ fake rate of $(0.25 \\pm 0.02)%$ for the momentum range between 1.0 GeV/$c$ and 3.0 GeV/$c$ in laboratory frame.']",['2001-08-29']
39,['eng'],"['Anastassov, A']",['First Measurement of $\\Gamma(D^{*+})$ and Precision Measurement of $ m_{D^{*+}}-m_{D^{0}}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), width', 'D*(2010), hadronic decay', 'mass difference, (D*(2010) D0)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D*(2010) --> D0 pi', 'D0 --> K- pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108043'],['We present the first measurement of the D*+ width using 9/fb of e+ e- data collected near the Upsilon(4S) resonance by the CLEO II.V detector. Our method uses advanced tracking techniques and a reconstruction method that takes advantage of the small vertical size of the CESR beam spot to measure the energy release distribution from the D*+ -> D0 pi+ decay. We find Gamma(D*+) = 96 +- 4 (Statistical) +- 22 (Systematic) keV. We also measure the energy release in the decay and compute Delta m = m(D*+) - m(D0) = 145.412 +- 0.002 (Statistical) +- 0.012 (Systematic) MeV/c^2'],['2001-09-14']
40,['eng'],"['Baldini, L', 'Brocco, L', 'Casadei, D', 'Castellini, G', 'Cindolo, F', 'Contin, A', 'Laurenti, G', 'Levi, G', 'Palmonari, F', 'Zichichi, Antonino']",['The AMS Time of Flight System'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2001/08/07', 'p, cosmic radiation', 'nucleus, cosmic radiation', 'magnetic spectrometer, satellite', 'fast logic, time-of-flight', 'time resolution', 'scintillation counter', 'Cherenkov counter, aerogel', 'photoelectron, amplifier', 'trigger']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108042'],"['The Time of Flight (TOF) system of the AMS experiment provides the fast trigger to the detector and measures the crossing particle direction, velocity and charge. AMS was operated aboard of the shuttle Discovery on June 1998 (NASA STS-91 mission) and will be upgraded and installed on the International Space Station at the end of 2003, for 3 years of data taking. The performances of the TOF during the precursor flight and modifications needed in the final version of the detector are presented.']",['2001-08-28']
41,['eng'],"['Raja, R', 'Cline, D', 'Gallardo, J', 'Geer, S', 'Kaplan, D', 'McDonald, K F', 'Palmer, R', 'Sessler, A', 'Skrinsky, A N', 'Summers, D', 'Tigner, Maury', 'Tollestrup, A V', 'Wurtele, J S', 'Zisman, M']",['The Program in Muon and Neutrino Physics'],['Particle Physics - Experimental Results'],"['talk, Snowmass 2001/06/30', 'neutrino, oscillation', 'neutrino, particle source', 'proton synchrotron', 'target', 'muon, secondary beam', 'beam cooling, ionization', 'hydrogen, liquid', 'muon, storage ring', 'muon+ muon-, storage ring', 'neutrino, counters and detectors', 'deep underground detector', 'costs', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108041'],"['We outline in detail a staging scenario for realizing the Neutrino Factory and the Muon Collider. As a first stage we envisage building an intense proton source that can be used to perform high intensity conventional neutrino beam experiments (""Superbeams""). While this is in progress, we perform R&D in collecting, cooling and accelerating muons which leads to the next two stages of ""Cold Muon Beams"" and the Neutrino Factory. Further progress in Muon Cooling especially in the area of emittance exchange will lead us to the Muon Collider. A staged scenario such as this opens up new physics avenues at each step and will provide a long range base program for particle physics.']",['2001-09-14']
42,['eng'],"['Fleming, B T', 'Krane, J', 'Zeller, G P', 'Canelli, F', 'Connolly, B', 'Erbacher, R D', 'Fleming, G T', 'Harris, D A', 'Hawker, E A', 'Hildreth, M', 'Kilminster, B', 'Lammers, S', 'Medoff, D', 'Monroe, J', 'Toback, D', 'Sorel, M', 'Turcot, A S', 'Velasco, M', 'Wascko, M O', 'Watts, G', 'Zimmerman, E D']",['Results of the Survey on the Future of HEP'],['Particle Physics - Experimental Results'],"['review', 'particle physics', 'sociology']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108040'],"[""The Young Physicists Panel (YPP) summarizes results from their Survey on the Future of High Energy Physics, which was conducted from July 2 to July 15, 2001. Over 1500 physicists from around the world, both young and tenured, responded to the survey. We first describe the origin, design, and advertisement of the survey, and then present the demographics of the respondents. Following sections analyze the collected opinions on the desire for balance in the field, the impact of globalization, the necessity of outreach, how to build the field, the physics that drives the field, and the selection of the next big machine. Respondents' comments follow the survey analysis in an appendix.""]",['2001-08-24']
43,['eng'],"['Badelek, A', 'Blöchinger, C', 'Blümlein, Johannes', 'Boos, E', 'Brinkmann, R', 'Burkhardt, H', 'Bussey, Peter J', 'Carimalo, C', 'Chyla, J', 'Çiftçi, A K', 'Decking, W', 'de Roeck, A', 'Fadin, V S', 'Ferrario, M', 'Finch, A', 'Fraas, H', 'Franke, F', 'Galynsky, M V', 'Gamp, A', 'Ginzburg, I F', 'Godbole, R M', 'Gorbunov, D S', 'Gounaris, G', 'Hagiwara, K', 'Han, L', 'Heuer, R D', 'Heusch, C A', 'Illana, J I', 'Ilyin, V A', 'Jankowski, P', 'Jiang, Y', 'Jikia, G', 'Jönsson, L', 'Kalachnikow, M', 'Kapusta, F', 'Klanner, R', 'Klasen, M', 'Kobayashi, K', 'Kon, T', 'Kotkin, G L', 'Krämer, M', 'Krawczyk, M', 'Kuang Yu Ping', 'Kuraev, E A', 'Kwiecinski, J', 'Leenen, M', 'Levchuk, M I', 'Ma, W F', 'Martyn, H U', 'Mayer, T', 'Melles, M', 'Miller, D J', 'Mtingwa, S K', 'Mühlleitner, M M', 'Muryn, B', 'Nickles, P V', 'Orava, Risto', 'Pancheri, G', 'Penin, A', 'Potylitsin, A P', 'Poulose, P', 'Quast, T', 'Raimondi, P', 'Redlin, H', 'Richard, F', 'Rindani, S D', 'Rizzo, T', 'Saldin, E L', 'Sandner, W', 'Schonnagel, H', 'Schneidmiller, E A', 'Schreiber, H J', 'Schreiber, S', 'Schüler, K P', 'Serbo, V', 'Seryi, A', 'Shanidze, R', 'Silva, W D', 'Söldner-Rembold, S', 'Spira, Michael', 'Stasto, A M', 'Sultansoy, S F', 'Takahashi, T', 'Telnov, V I', 'Tkabladze, A V', 'Trines, D', 'Undrus, A', 'Wagner, A', 'Walker, N', 'Watanabe, I', 'Wengler, T', 'Will, I', 'Wipf, S', 'Yavas, O', 'Yokoya, K', 'Yurkov, M', 'Zarnecki, A F', 'Zerwas, Peter M', 'Zomer, F']","['TESLA Technical Design Report, 6.1']",['Particle Physics - Experimental Results'],"['electron positron, linear collider', 'linear collider, proposed', 'photon photon, colliding beams', 'photon electron, colliding beams', 'luminosity, beam monitoring', 'Compton scattering', 'radiation, laser', 'photon, polarization', 'electron, pair production', 'beam, radiation', 'scattering, beam-beam', 'background', 'Higgs particle', 'supersymmetry', 'quantum chromodynamics', 'numerical calculations', 'DESY TESLA Linac', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108012'],"['TESLA Technical Design Report, Part VI, Chapter 1: The Photon Collider at TESLA']",['2001-08-08']
44,['eng'],"['Affolder, T']",['Observation of Diffractive $J/\\psi$ Production at the Fermilab Tevatron'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'J/psi(3100), hadroproduction', 'diffraction, production', 'J/psi(3100), leptonic decay', 'cross section, ratio', 'x-dependence', 'p, structure function', 'diffraction, structure function', 'gluon', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> J/psi(3100) p anything', 'anti-p p --> J/psi(3100) anti-p anything', 'anti-p p --> J/psi(3100) anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107071'],"['We report the first observation of diffractive $J/\\psi(\\to \\mu^+\\mu^-)$ production in $\\bar pp$ collisions at $\\sqrt{s}$=1.8 TeV. Diffractive events are identified by their rapidity gap signature. In a sample of events with two muons of transverse momentum $p_T^{\\mu}>2$ GeV/$c$ within the pseudorapidity region $|\\eta|<$1.0, the ratio of diffractive to total $J/\\psi$ production rates is found to be $R_{J/\\psi}= [1.45\\pm 0.25]%$. The ratio $R_{J/\\psi}(x)$ is presented as a function of $x$-Bjorken. By combining it with our previously measured corresponding ratio $R_{jj}(x)$ for diffractive dijet production, we extract a value of $0.59\\pm 0.15$ for the gluon fraction of the diffractive structure function of the proton.']",['2001-09-14']
45,['eng'],"['Affolder, T']",['Double Diffraction Dissociation at the Fermilab Tevatron Collider'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'diffraction, dissociation', 'p, dissociation', 'anti-p, dissociation', 'hadron, multiple production', 'rapidity, gap', 'central region', 'pomeron, exchange', 'Regge poles', 'cross section, factorization', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107070', 'http://fnalpubs.fnal.gov/archive/2001/pub/Pub-01-063-E.html']",['We present results from a measurement of double diffraction dissociation in $\\bar pp$ collisions at the Fermilab Tevatron collider. The production cross section for events with a central pseudorapidity gap of width $\\Delta\\eta^0>3$ (overlapping $\\eta=0$) is found to be $4.43\\pm 0.02{(stat)}{\\pm 1.18}{(syst) mb}$ [$3.42\\pm 0.01{(stat)}{\\pm 1.09}{(syst) mb}$] at $\\sqrt{s}=1800$ [630] GeV. Our results are compared with previous measurements and with predictions based on Regge theory and factorization.'],['2001-07-26']
46,['eng'],"['Goulianos, K']",['Diffraction in CDF'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'diffraction', 'W, hadroproduction', 'J/psi(3100), hadroproduction', 'quark, beauty', 'jet, pair production', 'rapidity, gap', 'anti-p, leading particle', 'pomeron, exchange', 'exchange, (2pomeron)', 'Regge poles', 'quantum chromodynamics', 'factorization', 'magnetic detector, CDF', 'experimental results', 'proposed experiment', 'Batavia TEVATRON Coll', '546, 630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107069'],['Results on diffraction obtained by the CDF Collaboration in Run I of the Fermilab Tevatron $\\bar pp$ collider are reviewed. New results are reported on soft double diffraction and diffractive $J/\\psi$ production. The CDF program for diffractive studies in Run II is briefly discussed.'],['2001-09-14']
47,['eng'],"['Foster, B']",['Zeus at HERA II'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'semiconductor detector, microstrip', 'drift chamber, drift tube', 'luminosity, monitoring', 'electron, polarized beam', 'magnetic detector, ZEUS', 'upgrade', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107066'],"['The ZEUS detector has been upgraded in a number of areas to prepare for the physics opportunities of HERA II. These upgrades, and their physics rationale and promise, are briefly outlined. The measurement of polarisation at HERA II, and its importance for the HERA II physics programme, is also discussed.']",['2001-07-25']
48,['eng'],"['Abe, K']",['Observation of Radiative B Meson Decays into Higher Kaonic Resonances'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, radiative decay', 'mass spectrum, (K 2pi)', 'K*2(1430)', 'K*(892)', 'K1(1270)', 'B, branching ratio', 'upper limit', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> K*2(1430) photon', 'B --> K1(1270) photon', 'B --> K rho(770) photon', 'B --> K*(892) pi photon', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107065'],"['We have studied radiative B meson decays into higher kaonic resonances decaying into a two-body or three-body final state, using a data sample of 21.3 fb$^{-1}$ recorded at the $\\Upsilon(4S)$ resonance with the Belle detector at KEKB. For the two-body final state, we extract the $B \\to K_2^{*}(1430)^0 \\gamma$ component from an analysis of the helicity angle distribution, and obtain ${\\cal B}(B^0 \\to K_2^{*}(1430)^0 \\gamma) = (1.26\\pm 0.66\\pm 0.10)\\times 10^{-5}$. For the three-body final state, we observe a $B \\to K\\pi\\pi\\gamma$ signal that is consistent with a mixture of $B \\to K^* \\pi \\gamma$ and $B \\to K \\rho \\gamma$. This is the first time that $B \\to K^* \\pi \\gamma$ and $B \\to K \\rho \\gamma$ have been observed separately. We find their branching fractions to be ${\\cal B}(B \\to K^* \\pi \\gamma; M_{K^*\\pi}<2.0 GeV/c^2) = (5.6\\pm 1.1\\pm 0.9)\\times 10^{-5}$ and ${\\cal B}(B \\to K \\rho \\gamma; M_{K\\rho} < 2.0 GeV/c^2) = (6.5\\pm 1.7^{+1.1}_{1.2})\\times 10^{-5}$, respectively.']",['2001-07-25']
49,['eng'],"['Lüders, S']",['Compact Frontend-Electronics and Bidirectional 3.3 Gbps Optical Datalink for Fast Proportional Chamber Readout'],['Particle Physics - Experimental Results'],"['proportional chamber, wire', 'proportional chamber, readout', 'optics, communications', 'optics, fibre', 'trigger', 'magnetic detector, H1', 'DESY HERA Stor', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107064'],"['The 9600 channels of the multi-wire proportional chamber of the H1 experiment at HERA have to be read out within 96 ns and made available to the trigger system. The tight spatial conditions at the rear end flange require a compact bidirectional readout electronics with minimal power consumption and dead material. A solution using 40 identical optical link modules, each transferring the trigger information with a physical rate of 4 x 832 Mbps via optical fibers, has been developed and commisioned. The analog pulses from the chamber can be monitored and the synchronization to the global HERA clock signal is ensured.']",['2001-09-14']
50,['eng'],"['Bussey, Peter J']",['Prompt Photons in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'positron p, colliding beams', 'positron p, inclusive reaction', 'photon, direct production', 'jet, associated production', 'jet, energy flow', 'p, structure function', 'quark, transverse momentum', 'differential cross section, transverse momentum', 'angular distribution', 'energy dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> photon anything', 'positron p --> (n)jet photon anything', '300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107063'],"['The production of prompt photons in photoproduction reactions in the ZEUS experiment is discussed. Cross sections for inclusive prompt photons and for prompt photons accompanied by jets are compared with theory, and the latter are used to determine the effective transverse momentum of the quarks in the proton.']",['2001-07-24']
51,['eng'],"['Dauncey, P D']",['Design and Performance of the Level 1 Calorimeter Trigger for the BABAR Detector'],['Particle Physics - Experimental Results'],"['calorimeter, trigger', 'electronics', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107062'],"['Since May 1999 the BABAR detector has been taking data at the PEP-II asymmetric electron-positron collider at the Stanford Linear Accelerator Center, California. This experiment requires a very large data sample and the PEP-II accelerator uses intense beams to deliver the high collision rates needed. This poses a severe challenge to the BaBar trigger system, which must reject the large rate of background signals resulting from the high beam currents whilst accepting the collisions of interest with very high efficiency. One of the systems that performs this task is the Level 1 Calorimeter Trigger, which identifies energy deposits left by particles in the BABAR calorimeter. It is a digital, custom, fixed latency system which makes heavy use of high-speed FPGA devices to allow flexibility in the choice of data filtering algorithms. Results from several intermediate processing stages are read out, allowing the selection algorithm to be fully analysed and optimized offline. In addition, the trigger is monitored in real time by sampling these data and cross-checking each stage of the trigger calculation against a software model. The design, implementation, construction and performance of the Level 1 Calorimeter Trigger during the first year of BABAR operation are presented.']",['2001-07-24']
52,['eng'],"['Aubert, Bernard']",['Investigation of B --> D^{(*)}anti-D^{(*)}K decays with the BABAR detector'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'charmed meson, pair production', 'D', 'D*(2010)', 'K, associated production', 'B, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> 2charmed meson K', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107056'],"['Using about 23M $B \\overline B$ events collected in 1999-2000 with the BABAR detector, we report the observation of several hundred $B \\to D^{(*)}\\overline D^{(*)}K$ decays with two completely reconstructed D mesons. The preliminary branching fractions of the low background decay modes $B^0\\to D^{*-}D^{(*)0}K^+$ are determined to be ${\\cal B}(B^0 \\to D^{*-}D^{0}K^+) = (2.8 \\pm 0.7 \\pm 0.5)\\times 10^{-3}$ and ${\\cal B}(B^0 \\to D^{*-}D^{*0}K^+) = (6.8 \\pm 1.7 \\pm 1.7)\\times 10^{-3}$. Observation of a significant number of candidates in the color-suppressed decay mode $B^+\\to D^{*+}D^{*-}K^+$ is reported with a preliminary branching fraction ${\\cal B}(B^+\\to D^{*+}D^{*-}K^+)= (3.4\\pm 1.6\\pm 0.9)\\times 10^{-3}.$']",['2001-07-24']
53,['eng'],"['Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D', 'Magill, S', 'Musgrave, B', 'Pellegrino, A', 'Repond, J', 'Yoshida, R', 'Mattingly, M C K', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Sar--, G', 'Zichichi, Antonino', 'Aghuzumtsyan, G', 'Brock, I', 'Goers, S', 'Hartmann, H', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Kind, O', 'Paul, E', 'Rautenberg, J', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Brook, N H', 'Cole, J E', 'Heath, B', 'Foster G P', 'Heath, H F', 'Robins, S', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Wing, M', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Helbich, M', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K', 'Olkiewicz, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Grabowska-Bold, I', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowal, M', 'Kowalski, T', 'Mindur, B', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Szuba, J', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Borras, K', 'Chiochia, V', 'Crittenden, J A', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Geiser, A', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hebbel, K', 'Hillert, S', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Labes, H', 'Löhr, B', 'Mankel, R', 'Martens, J', 'Martínez, M', 'Milite, M', 'Moritz, M', 'Notz, D', 'Petrucci, M C', 'Polini, A', 'Schneekloth, U', 'Selonke, F', 'Stonjek, S', 'Wolf, G', 'Wollmer, U', 'Whitmore, J J', 'Wichmann, R', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Bamberger, Andreas', 'Benen, A', 'Coppola, N', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bell, M', 'Bussey, Peter J', 'Doyle, A T', 'Glasman, C', 'Lee, S W', 'Lupi, A', 'McCance, G J', 'Saxon, D H', 'Skillicorn, Ian O', 'Bodmann, B', 'Gendner, N', 'Holm, U', 'Salehi, H', 'Wick, K', 'Yildirim, A', 'Ziegler, A', 'Carli, T', 'Garfagnini, A', 'Gialas, I', 'Lohrmann, E', 'Foudas, C', 'Goncalo, R', 'Long, K R', 'Metlica, F', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Cloth, P', 'Filges, D', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Barakbaev, A N', 'Boos, E G', 'Pokrovskiy, N S', 'Zhautykov, B O', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Son, D', 'Barreiro, F', 'García, G', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Vázquez, M', 'Barbi, M', 'Bertolin, A', 'Corriveau, F', 'Ochs, A', 'Padhi, S', 'Stairs, D G', 'Tsurugai, T', 'Antonov, A', 'Bashkirov, V', 'Danilov, P', 'Dolgoshein, B A', 'Gladkov, D', 'Sosnovtsev, V', 'Suchkov, S', 'Dementiev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Levchenko, B B', 'Lukina, O Yu', 'Proskuryakov, A S', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Engelen, J', 'Grijpink, S', 'Maddox, E', 'Koffeman, E', 'Kooijman, P', 'Schagen, S', 'Tassi, E', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Wiggers, L', 'De Wolf, E', 'Brümmer, N', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Ferrando, J', 'Grosse-Knetter, J', 'Matsushita, T', 'Rigby, M', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dusini, S', 'Limentani, S', 'Longhin, A', 'Parenti, A', 'Posocco, M', 'Stanco, L', 'Turcato, M', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Saull, P R B', 'Toothacker, W S', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Heusch, C A', 'Park, I H', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Gabareen, A', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Kohno, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Matsuzawa, K', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Mirea, A', 'Sabetfakhri, A', 'Butterworth, J M', 'Gwenlan, C', 'Hall-Wilton, R', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'Lightwood, M S', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Smalska, B', 'Tymieniecka, T', 'Ukleja, J', 'Zakrzewski, J A', 'Adamus, M', 'Plucinsky, P P', 'Sztuk, J', 'Eisenberg, Y', 'Gladilin, L K', 'Hochman, D', 'Karshon, U', 'Breitweg, J', 'Chapin, D', 'Cross, R', 'Kcira, D', 'Lammers, S', 'Reeder, D D', 'Savin, A A', 'Smith, W H', 'Deshpande, A A', 'Dhawan, S', 'Straub, V W', 'Hughes P B', 'Bhadra, S', 'Catterall, C D', 'Frisken, W R', 'Khakzad, M', 'Menary, S']",['Properties of hadronic final states in diffractive deep inelastic ep scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'electron p, deep inelastic scattering', 'diffraction', 'photon, dissociation', 'hadron, multiple production', 'p, leading particle', 'event shape analysis', 'energy flow', 'effect, seagull', 'pomeron, resolved', 'quark, pair production', 'gluon, radiation', 'final state, (quark antiquark gluon)', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'electron p --> p electron (n)hadron']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107052', 'http://www-zeus.desy.de/~schlenst/conf/osaka_paper.html']","[""Characteristics of the hadronic final state of diffractive deep inelastic scattering events, ep -> eXp, were studied in the kinematic range 4 < M_X < 35 GeV, 4 < Q^2 < 150 GeV^2, 70 < W < 250 GeV and 0.0003 < x_pom < 0.03 with the ZEUS detector at HERA using an integrated luminosity of 13.8 pb^{-1}. The events were tagged by identifying the diffractively scattered proton using the leading proton spectrometer. The properties of the hadronic final state, X, were studied in its center-of-mass frame using thrust, thrust angle, sphericity, energy flow, transverse energy flow and ``seagull'' distributions. As the invariant mass of the system increases, the final state becomes more collimated, more aligned and more asymmetric in the average transverse momentum with respect to the direction of the virtual photon. Comparisons of the properties of the hadronic final state with predictions from various Monte Carlo model generators suggest that the final state is dominated by qqg states at the parton level.""]",['2001-07-23']
54,['eng'],"['Abe, K']",['Study of three-body charmless B decays at Belle'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B+, hadronic decay', 'final state, (0charm)', 'mass spectrum, (pi+ pi-)', 'mass spectrum, (K+ K-)', 'mass spectrum, (K+ pi-)', 'K*(892)', 'f0(975\\)', 'magnetic detector, BELLE', 'experimental results', 'SLAC PEP Stor', 'B+ --> K+ pi+ pi-', 'B+ --> 2K+ K-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107051'],"['Using a data sample of 21.3 fb$^{-1}$ collected by the Belle detector, three body charmless decays $B^+\\to K^+ h^+ h^-$ have been studied. With no assumptions on the intermediate mechanisms, the following branching fractions have been measured for the first time $ {\\cal{B}}(B^+\\to K^+ \\pi^- \\pi^+) = (58.5\\pm 7.1\\pm 8.8)\\times 10^{-6}$ and $ {\\cal{B}}(B^+\\to K^+ K^- K^+) = (37.0\\pm 3.9\\pm 4.4)\\times 10^{-6}$. We also present the first observations of the decay mode $B^+\\to K^{*0}(892)\\pi^+$ with a branching fraction of ${\\cal{B}}(B^+\\to K^{*0}(892) \\pi^+) = (16.7^{+3.7+2.1+3.0}_{-3.4-2.1-5.9})\\times 10^{-6}$ and the decay mode $B^+\\to f_0(980)K^+$ with a product branching fraction of ${\\cal{B}}(B^+\\to f_0(980) K^+)\\times{\\cal{B}}(f_0(980)\\to \\pi^+\\pi^-) = (11.7^{+2.5+1.5+4.1}_{-2.7-1.5-1.0})\\times 10^{-6}$.']",['2001-07-23']
55,['eng'],"['Abe, K']",['Observation of $B^+ \\to \\chi_{c0} K^+ $'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B+, hadronic decay', 'B+, branching ratio', 'chi/c0(3415), hadronic decay', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B+ --> chi/c0(3415) K+', 'chi/c0(3415) --> K*(892) K+ pi', 'chi/c0(3415) --> pi+ pi-', 'chi/c0(3415) --> K+ K-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107050'],"['We report the first observation of the decay $B^+ \\to \\chi_{c0} K^+$ using 21.3 fb$^{-1}$ of data collected by the Belle detector at the $\\Upsilon$(4S) resonance. The preliminary result for the branching fraction is ${\\cal{B}}(B^+\\to \\chi_{c0}K^+)=(8.0^{+2.7}_{-2.4}\\pm 1.0\\pm 1.1)\\times 10^{-4}$ where the first error is statistical, the second is systematic, and the third comes from the uncertainty in the $\\chi_{c0}\\to\\pi^+\\pi^-$ branching fraction.']",['2001-07-23']
56,['eng'],"['Abe, K']",['Observation of Color-Suppressed $\\overline{B}^0 \\to D^{(*)0}X^0$ Decays'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'anti-B0, hadronic decay', 'anti-B0, branching ratio', 'D0', 'D*(2010)', 'omega(783)', 'eta', 'pi0', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'anti-B0 --> charmed meson meson', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107048'],"['We report the first observation of color-suppressed $\\overline{B}^0\\to D^0 \\pi^0$ and $D^{(*)0} \\omega$ decays and evidence of $\\overline{B}^0 \\to D^{*0} \\pi^0$ and $D^{(*)0} \\eta$. The branching fractions are found to be ${\\cal B} (\\overline{B}^0\\to D^0 \\pi^0) = (2.9 ^{+0.4}_{-0.3} \\pm 0.6) \\times 10^{-4}$, ${\\cal B} (\\overline{B}^0 \\to D^0 \\omega) = (1.7 ^{+0.5 +0.3}_{-0.4 -0.4}) \\times 10^{-4}$, and ${\\cal B} (\\overline{B}^0 \\to D^{*0} \\omega) = (3.4 ^{+1.3}_{-1.1}\\pm 0.8) \\times 10^{-4}$. The analysis is based on a data sample of 21.3 fb$^{-1}$ collected at the $\\Upsilon(4S)$ resonance by the Belle detector at the KEKB $e^{+} e^{-}$ collider.']",['2001-07-23']
57,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D', 'Azuelos, G', 'Bailey, I', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bell, P J', 'Bella, G', 'Bellerive, A', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Etzion, E', 'Fabbri, F', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hamann, M', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hauschildt, J', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kramer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lillich, J', 'Littlewood, C', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Masetti, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Moed, S', 'Mohr, W', 'Mori, T', 'Mutter, A', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oh, A', 'Okpara, A', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rozen, Y', 'Ruken, H', 'Runge, K', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spielmann, P', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Toya, D', 'Trefzger, T M', 'Tricoli, A', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Ujvári, B', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of $Z/\\gamma^{*}$ production in Compton scattering of quasi-real photons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, inelastic scattering', 'photon electron, Compton scattering', 'hadron, multiple production', 'Z0, intermediate boson', 'photon, intermediate state', 'channel cross section, energy dependence', 'channel cross section, branching ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> (n)hadron positron electron', '189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107047'],"['The process e+ e- -> e+ e- Z/gamma* is studied with the OPAL detector at LEP at a centre of mass energy of sqrt(s) = 189 GeV. The cross-section times the branching ratio of the Z/gamma* decaying into hadrons is measured within Lorentz invariant kinematic limits to be (1.2 +/- 0.3 +/- 0.1) pb for invariant masses of the hadronic system between 5 GeV and 60 GeV and (0.7 +/- 0.2 +/- 0.1) pb for hadronic masses above 60 GeV. The differential cross-sections of the Mandelstam variables s-hat, t-hat, and u-hat are measured and compared with the predictions from the Monte Carlo generators grc4f and PYTHIA. From this, based on a factorisation ansatz, the total and differential cross-sections for the subprocess e gamma -> e Z/gamma* are derived.']",['2001-09-14']
58,['eng'],"['Bellantoni, L']",['KTeVrare decay results'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'K0(L), secondary beam', 'K0(L), semileptonic decay', 'K0(L), leptonic decay', 'angular distribution, asymmetry', 'K0(L), form factor', 'form factor, electric', 'Kobayashi-Maskawa angle', 'flavor, violation', 'K0(L), branching ratio', 'upper limit', 'experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi electron neutrino', 'K0(L) --> 2pi positron electron', 'K0(L) --> pi0 muon electron', 'K0(L) --> lepton+ lepton- photon', 'K0(L) --> lepton+ lepton- positron electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107045'],['Recent results are presented for (1) the charge asymmetry in semielectronic kaon decay; (2) the charge radius of the neutral kaon; (3) the decay Klong -> pi0 pi0 e+e-; (4) constraints on rho(CKM) from kaon decays; (5) lepton flavor violation. A few words about future kaon physics work at Fermilab are included.'],['2001-07-20']
59,['eng'],[],['Measuring the Hadronic Cross Section at KLOE using the Radiative Return'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'cross section, hadronic', 'pi, pair production', 'photon, associated production', 'radiation, initial-state interaction', 'differential cross section, mass', 'threshold', 'pi, form factor', 'energy dependence', 'luminosity', 'magnetic detector, KLOE', 'experimental results', 'Frascati Stor', '< 1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107023'],"['We present a study of the reaction e+e- \\to pi+pi-gamma at the phi peak with the KLOE detector at the phi-factory DAPHNE. This reaction allows us to obtain the cross section for \\e+e- \\to pi+pi- from the e+e- center-of-mass energy W = m_\\phi = 1019 MeV down to threshold, i.e. 2m_pi < M_(pipi) < m_phi. This is called radiative return. The status of the analysis and preliminary results on the invariant mass spectrum of the two-pion-state are presented.']",['2001-07-12']
60,['eng'],"['Meer, D', 'Müller, D', 'Müller, J', 'Schöning, A', 'Wissing, C']",['A Multifunctional Processing Board for the Fast Track Trigger of the H1 Experiment'],['Particle Physics - Experimental Results'],"['luminosity, upgrade', 'trigger', 'track data analysis', 'microprocessor', 'communications', 'programming', 'technology', 'magnetic detector, H1', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107010'],"['The electron-proton collider HERA is being upgraded to provide higher luminosity from the end of the year 2001. In order to enhance the selectivity on exclusive processes a Fast Track Trigger (FTT) with high momentum resolution is being built for the H1 Collaboration. The FTT will perform a 3-dimensional reconstruction of curved tracks in a magnetic field of 1.1 Tesla down to 100 MeV in transverse momentum. It is able to reconstruct up to 48 tracks within 23 mus in a high track multiplicity environment. The FTT consists of two hardware levels L1, L2 and a third software level. Analog signals of 450 wires are digitized at the first level stage followed by a quick lookup of valid track segment patterns. For the main processing tasks at the second level such as linking, fitting and deciding, a multifunctional processing board has been developed by the ETH Zurich in collaboration with Supercomputing Systems (Zurich). It integrates a high-density FPGA (Altera APEX 20K600E) and four floating point DSPs (Texas Instruments TMS320C6701). This presentation will mainly concentrate on second trigger level hardware aspects and on the implementation of the algorithms used for linking and fitting. Emphasis is especially put on the integrated CAM (content addressable memory) functionality of the FPGA, which is ideally suited for implementing fast search tasks like track segment linking.']",['2001-09-14']
61,['eng'],"['Barnes, P D', 'Bunker, B D', 'Dennert, H', 'Eisenstein, R A', 'Eyrich, W', 'Fischer, H', 'Franklin, G', 'Franz, J', 'Geyer, R', 'Harris, P', 'Hauffe, J', 'Hertzog, D W', 'Johansson, T', 'Jones, T', 'Kilian, K', 'Oelert, Walter', 'Pomp, S', 'Quinn, B', 'Röhrich, K', 'Rössle, E', 'Sachs, K', 'Schmitt, H', 'Sefzick, T', 'Seydoux, J', 'Stinzing, F', 'Tayloe, R', 'Todenhagen, R', 'Traneus, E', 'Wirth, S']",['Measurement of the $\\overline{p}p \\to K_S K_S \\eta$ cross section at beam momenta in the regions of 1.45 and 1.7 GeV/c'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'K0(S), pair production', 'eta, associated production', 'channel cross section, momentum dependence', 'mass spectrum, missing-mass', 'magnetic spectrometer, experimental results', 'CERN LEAR', 'anti-p p --> 2K0(S) eta', '1.45-1.70 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107007'],"['The PS185 experiment at LEAR/CERN has investigated strangeness production in antiproton-proton collisions with final states such as $\\overline{\\Lambda} \\Lambda$, $\\overline{\\Sigma}^0 \\Lambda + c.c$, $\\overline{\\Sigma^+} \\Sigma^+$, $\\overline{\\Sigma^-} \\Sigma^-$ and $K_S K_S$. Results are presented from a study of about 32,000 {$K_S K_S X$} events obtained at several antiproton momenta in the regions of 1.45 and 1.7 GeV/c. The $\\overline{p} p \\to K_S K_S \\eta$ cross sections extracted at these momenta constitute the first measurement of this reaction in flight and are broadly consistent with expectations of a phase-space extrapolation of branching ratios from annihilation at rest.']",['2001-07-04']
62,['eng'],"['De Min, A']","['Other Susy searches (RPV, GMSB...) and exotics at LEP']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'new interaction, search for', 'electroweak interaction, validity test', 'supersymmetry, symmetry breaking', 'fermion, composite', ""Z'"", 'space-time, higher-dimensional', 'Goldstino', 'lepton, multiple production', 'jet, multiple production', 'radiation, initial-state interaction', 'neutrino, pair production', 'photon, associated production', 'photon, multiple production', 'mass spectrum, missing-mass', 'event shape analysis', 'planarity', 'experimental results', 'CERN LEP Stor', '130-208 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106097'],"['In the last five years, the operation of the LEP accelerator has provided the HEP community with a unique opportunity to search for physics beyond the standard model at the typical energy scale of $~200$ GeV. Although most of the data analysis has been focused on the traditional sectors of Higgs and gravity-mediated SUSY physics, a considerable effort has been dedicated by ALEPH, DELPHI L3 and OPAL to the search for more exotic physics scenarios, which go from gauge-mediated supersymmetry breaking, to compositeness, to gravitational extra-dimensions. This talk reviews the latest experimental results on a selection of final states which are believed to be of particular interest for exotic physics or which present some anomaly in the data with respect to standard model expectations.']",['2001-06-29']
63,['eng'],"['Bhat, P C']",['New Directions in Data Analysis'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'data analysis method', 'statistical analysis', 'neural network', 'trigger', 'anti-p p, colliding beams', 'mass, truth', 'particle identification, flavor', 'new particle, search for', 'leptoquark', 'Higgs particle', 'interpretation of experiments, Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106096'],"['In the next decade, high energy physicists will use very sophisticated equipment to record unprecedented amounts of data in the hope of making major advances in our understanding of particle phenomena. Some of the signals of new physics will be small, and the use of advanced analysis techniques will be crucial for optimizing signal to noise ratio. I will discuss new directions in data analysis and some novel methods that could prove to be particularly valuable for finding evidence of any new physics, for improving precision measurements and for exploring parameter spaces of theoretical models.']",['2001-06-29']
64,['eng'],[],['Searches for New Physics in Events with a Photon and b-quark Jet at CDF'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'quark, beauty', 'photon, associated production', 'transverse energy, missing-energy', 'supersymmetry, search for', 'sparticle, pair production', 'sparticle, decay modes', 'chargino', 'neutralino', 'squark, truth', 'gravitino, LSP', 'technicolor', 'electroweak interaction, validity test', 'cross section, upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'anti-p p --> beauty photon anything', 'anti-p p --> chargino neutralino anything', 'chargino --> squark beauty', 'neutralino --> gravitino photon', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106012'],"['We have searched for evidence of physics beyond the standard model in events that include an energetic photon and an energetic b-quark jet, produced in 85pb of ppbar collisions at 1.8 TeV at the Tevatron Collider at Fermilab. This signature, containing at least one gauge boson and a third-generation quark, could arise in the production and decay of a pair of new particles, such as those predicted by Supersymmetry, leading to a production rate exceeding standard model predictions. We also search these events for anomalous production of missing transverse energy, additional jets and leptons (e, mu and tau), and additional b quarks. We find no evidence for any anomalous production of gamma-b or gamma-b+X events. We present limits on two supersymmetric models: a model where the photon is produced in the decay chi2->gamma chi1, and a model where the photon is produced in the neutralino decay into the Gravitino LSP, chi1 -> gamma G. We also present our limits in a model-independent form and test methods of applying model-independent limits.']",['2001-06-05']
65,['eng'],"['Arnaldi, R']",['The onset of the anomalous J/psi suppression in Pb-Pb collisions at the CERN SPS'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'scattering, heavy ion', 'lead', 'hadron, multiple production', 'J/psi(3100), yield', 'J/psi(3100), leptonic decay', 'quark gluon, plasma', 'dependence, impact parameter', 'model, nuclear reaction', 'energy loss, small-angle', 'magnetic spectrometer, experimental results', 'CERN SPS', 'lead lead --> J/psi(3100) anything', 'J/psi(3100) --> muon+ muon-', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106079'],"['The J/psi suppression observed by the NA50 experiment is one of the most striking signatures for quark gluon plasma formation in Pb-Pb collisions at 158 AGeV. The J/psi production has been studied as a function of the centrality of the collision estimated via the forward energy EZDC released in a zero degree calorimeter (ZDC). The study of the correlation between the number of participant nucleons in the collisions, Npart, and EZDC allows to check whether the J/psi suppression pattern vs. EZDC is compatible with a sudden J/psi suppression mechanism expressed as a function of Npart.']",['2001-09-14']
66,['eng'],"['Adloff, C']",['Three-Jet Production in Deep-Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'mass spectrum, (3jet)', 'angular distribution, (3jet)', 'kinematics, Breit frame', 'differential cross section, x-dependence', 'momentum transfer, dependence', 'final state, (2jet)', 'channel cross section, ratio', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'electron p --> 3jet anything', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106078'],['Three-jet production is studied for the first time in deep-inelastic positron-proton scattering. The measurement carried out with the H1 detector at HERA covers a large range of four-momentum transfer squared 5 < Q^2 < 5000 GeV^2 and invariant three-jet masses 25 < M_(3jet) < 140 GeV. Jets are defined by the inclusive k_T algorithm in the Breit frame. The size of the three-jet cross section and the ratio of the three-jet to the dijet cross section R_(3/2) are described over the whole phase space by the predictions of perturbative QCD in next-to-leading order. The shapes of angular jet distributions deviate significantly from a uniform population of the available phase space but are well described by the QCD calculation.'],['2001-06-21']
67,['eng'],"['Van Beveren, E', 'Rupp, G']",['Modified Breit-Wigner formula for mesonic resonances describing OZI decays of confined $q\\bar{q}$ states and the light scalar mesons'],['Particle Physics - Experimental Results'],"['meson meson, interaction', 'meson resonance, hadroproduction', 'model, Breit-Wigner', 'expansion, mass', 'scattering amplitude, partial wave', 'coupled channel', 'S-matrix, formula', 'meson resonance, decay', 'Iizuka-Okubo-Zweig rule', 'quark, pair production', 'quark, valence', 'quark, confinement', 'quantum chromodynamics', 'lattice field theory', 'approximation, quenching', 'pi K, interaction', 'mass spectrum, (K pi)', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106077'],"[""A model-independent expression resembling Breit-Wigner formulae is derived for the description of resonances which appear in meson-meson scattering. Starting point is a unitarised meson model, but reduced to a simpler form and freed from the specific assumption about the confining force. The parameters of the resulting ``Resonance-Spectrum Expansion'' are directly related to the confinement spectrum and the mechanism of $^3P_0$ valence-quark-pair creation for OZI-allowed hadronic decay, and not to the central positions and widths of resonances. The method also provides a straightforward explanation for the origin of the light scalar mesons without requiring extra degrees of freedom.""]",['2001-06-21']
68,['eng'],"['Sandacz, A', 'Grajek, O A', 'Moinester, M A', 'Piasetzky, E']",['Color Transparency at COMPASS - Feasibility Study'],['Particle Physics - Experimental Results'],"['talk, Dubna 2000/10/09', 'muon p, exclusive reaction', 'muon nucleus, exclusive reaction', 'carbon', 'lead', 'vector meson, electroproduction', 'vector meson, hadronic decay', 'J/psi(3100), leptonic decay', 'rho(770)0, polarization', 'Phi(1020)', 'color, transparency', 'quantum chromodynamics, perturbation theory', 'coherent interaction', 'incoherent interaction', 'dependence, mass number', 'momentum transfer, dependence', 'polarized target', 'background', 'transverse momentum, dependence', 'decay, angular distribution', 'photon, longitudinal', 'photon, transverse', 'trigger, acceptance', 'counters and detectors, efficiency', 'numerical calculations, Monte Carlo', 'proposed experiment, CERN SPS', 'muon nucleon --> nucleon rho(770) 0muon', 'muon nucleus --> nucleus nucleon rho(770) muon', '190 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106076'],['We examine the potential of the COMPASS experiment at CERN to study color transparency via exclusive vector meson production in hard muon-nucleus scattering. It is demonstrated that COMPASS has high sensitivity to test this important prediction of perturbative QCD.'],['2001-06-21']
69,['eng'],"['Chiarelli, G']",['Higgs Discovery before LHC?'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/04/18', 'anti-p p, colliding beams', 'Higgs particle, search for', 'Higgs particle, mass', 'Higgs particle, hadroproduction', 'intermediate boson, associated production', 'background', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'proposed experiment', 'Batavia TEVATRON Coll', '1800, 2000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106074'],['The proposed Run IIb of the Tevatron Collider will provide 15 fb-1 worth of ppbar data at c.o.m energy of 2 TeV per experiment by year 2007. We review the plans of the Tevatron accelerator complex upgrade and the plans for the upgrades of the experiments to match this challenge. Perspectives for the discovery of an Higgs particle are reviewed and the concrete possibility of a 5 sigmas discovery for a low mass Higgs are discussed.'],['2001-06-21']
70,['eng'],"['Valassi, A']",['Measurements of single W production at LEP2'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/04/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, electroproduction', 'W, hadronic decay', 'W, leptonic decay', 'channel cross section, energy dependence', 'coupling, (3gauge boson)', 'electroweak interaction, validity test', 'experimental results', 'CERN LEP Stor', 'electron positron --> W electron neutrino', '130-207 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106073'],"['In the energy region of LEP2 and above, four fermion final states in e+e- collisions can be produced by Feynman diagrams involving two, one or zero resonant bosons...']",['2001-06-21']
71,['eng'],"['Pislak, S', 'Appel, R', 'Atoyan, G S', 'Bassalleck, B', 'Bergman, D R', 'Cheung, N', 'Dhawan, S K', 'Do, H', 'Egger, J', 'Eilerts, S W', 'Herold, W D', 'Issakov, V V', 'Kaspar, H', 'Kraus, D E', 'Lazarus, D M', 'Lichard, P', 'Lowe, J', 'Lozano, J', 'Ma, H', 'Majid, W A', 'Poblaguev, A A', 'Rehak, P', 'Sher, A E', 'Thompson, J A', 'Truöl, P', 'Zeller, M E']",['A new measurement of K+(e4) decay and the s-wave pi-pi-scattering length a00'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'K+, branching ratio', 'pi, pair production', 'mass spectrum, two-pion', 'pi pi, scattering length', 'current, hadronic', 'form factor', 'partial wave', 'mass, dependence', 'momentum dependence', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ pi- positron neutrino/e']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106071'],"['A sample of 400000 events from the decay K+->pi+pi-e+nu(e)(K(e4)) has been collected in experiment E865 at the Brookhaven AGS. The analysis of these data yields new measurements of the K(e4) branching ratio (4.11+-0.01+-0.11)*10**(-5)), the s-wave pi-pi scattering length a00=0.228+-0.012+-0.003, and the form factors F, G, and H of the hadronic current and their dependence on the invariant pi-pi mass.']",['2001-09-14']
72,['eng'],"['Adloff, C']",['Photoproduction with a Leading Proton at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'positron p, inclusive reaction', 'photon, dissociation', 'hadron, photoproduction', 'p, leading particle', 'p, energy', 'exchange, Regge', 'differential cross section, energy dependence', 'Regge poles, triple-Regge limit', 'momentum transfer, dependence', 'magnetic detector, H1', 'forward spectrometer, experimental results', 'DESY HERA Stor', 'positron p --> p positron anything', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106070'],"[""The total cross section for the photoproduction process with a leading proton in the final state has been measured at gamma p centre-of-mass energies W of 91, 181 and 231 GeV. The measured cross sections apply to the kinematic range with the transverse momentum of the scattered proton restricted to p_Tproton <= 0.2 GeV and 0.68 <= z <= 0.88, where z = E_p'/E_p is the scattered proton energy normalised to the beam energy. The cross section dsigma_{gamma p -> Xp'}(W,z)/dz is observed to be independent of W and z within the measurement errors and amounts to (8.05 +- 0.06 stat +- 0.89 syst) mub on average. The data are well described by a Triple Regge model in which the process is mediated by a mixture of exchanges with an effective Regge trajectory of intercept alpha_i(0)=0.33 +- 0.04 stat +- 0.04 syst. The total cross section for the interaction of the photon with this mixture (gamma alpha_i -> X) can be described by an effective trajectory of intercept alpha_k(0)=0.99 +- 0.01 stat +- 0.05 syst. The measured cross sections are compared with deep inelastic scattering leading proton data in the same region of z and p_Tproton for photon virtuality Q^2 > 2.5 GeV^2. The ratio of the cross section for leading proton production to the total cross section is found to rise with Q^2.""]",['2001-06-20']
73,['eng'],"['Airapetian, A']",['Measurement of the Beam-Spin Azimuthal Asymmetry Associated with Deeply-Virtual Compton Scattering'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron, polarized beam', 'polarization, longitudinal', 'Compton scattering, off-shell', 'photon, electroproduction', 'angular distribution, asymmetry', 'helicity, dependence', 'analyzing power', 'approximation, Bethe-Heitler', 'interference', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', '26.7 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106068'],['The beam-spin asymmetry in hard electroproduction of photons has been measured for the first time. The data have been accumulated by the HERMES experiment at DESY using the HERA 27.6 GeV longitudinally polarized positron beam and an unpolarized hydrogen gas target. The asymmetry in the azimuthal distribution of the produced photons in the angle phi relative to the lepton scattering plane was determined with respect to the helicity state of the incoming positron beam. The beam-spin analyzing power in the sin(phi) moment was measured to be -0.23 +/- 0.04(stat) +/- 0.03(syst) in the missing-mass range below 1.7 GeV. The observed asymmetry is attributed to the interference of the Bethe-Heitler and deeply-virtual Compton scattering processes.'],['2001-09-14']
74,['eng'],"['Favart, L']",['Deeply Virtual Compton Scattering at H1 and ZEUS'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'positron p, colliding beams', 'photon, electroproduction', 'Compton scattering, off-shell', 'approximation, Bethe-Heitler', 'differential cross section, energy dependence', 'momentum transfer, dependence', 'photon, angular distribution', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> p positron photon', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106067'],"['Results on Deeply Virtual Compton Scattering at HERA measured by the H1 and ZEUS Collaborations are presented. The cross section, measured for the first time, is reported for $Q^2 > 2 GeV^2$, $30 < W < 120 GeV$ and $|t| < 1 GeV^2$.']",['2001-06-19']
75,['eng'],"['Blumenstengel, M', 'Biebel, O', 'Fernández, P A M', 'Pfeifenschnedier, P', 'Bethke, Siegfried', 'Kluth, S']",['Measurement of the longitudinal and transverse cross-section in e^+e^- annihilation at sqrt(s)=35-44 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'angular distribution', 'total cross section', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'quantum chromodynamics, perturbation theory', 'correction, nonperturbative', 'strong interaction, coupling constant', 'magnetic detector, JADE', 'experimental results', 'DESY PETRA Stor', '35-44 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106066'],"['An investigation of the polar angle distribution of charged hadrons is presented using data taken by the JADE experiment at the PETRA e^+e^- collider at centre-of-mass energies of 35 and 44 GeV. From fits to the polar angle distribution the longitudinal, sigma_L, and transverse, sigma_T, cross-section relative to the total hadronic are determined at an average energy scale of 36.6 GeV. The results are sigma_L/sigma_tot = 0.067 +/- 0.013, sigma_T/sigma_tot = 0.933 -/+ 0.013 where total errors are given and the results are exactly anti-correlated. Using the next-to-leading order QCD prediction for the longitudinal cross-section, the value alpha_S(36.6 GeV) = 0.150 +/- 0.025 of the strong coupling constant is obtained in agreement with the world average value of alpha_S evolved to an energy scale of 36.6 GeV.']",['2001-06-19']
76,['eng'],"['Smy, M B']",['Super-K solar neutrino results'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'neutrino, solar', 'neutrino, flux', 'neutrino electron, elastic scattering', 'electron, energy spectrum', 'time dependence', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'Cherenkov counter, water', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106064'],"['Super-Kamiokande has measured the solar neutrino flux using elastic neutrino-electron scattering in water. The measured flux is $2.32\\pm0.03$(stat)$^{+0.08}_{-0.07}$(syst)$\\times10^6$/(cm$^2$s) based on the energy range of 5 to 20 MeV for the recoiling electron. The time-dependence and energy spectrum of the recoiling electrons were studied to search for two-neutrino oscillation signatures. The absence of either significant zenith angle flux variation or distortions of the recoil electron spectrum places strong constraints on neutrino mass difference and mixing. In combination with the flux measurement, two allowed regions at large mixing are found.']",['2001-06-18']
77,['eng'],"['Affolder, T']",['Search for Gluinos and Squarks Using Like-Sign Dileptons in p-pbar Collisions at sqrt(s)=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'sparticle, search for', 'sparticle, pair production', 'sparticle, decay modes', 'gluino', 'final state, ((n)jet dilepton)', 'charge, dilepton', 'transverse energy, missing-energy', 'supersymmetry', 'sparticle, mass', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> (n)jet 2lepton+ missing-energy anything', 'anti-p p --> (n)jet 2lepton- missing-energy anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106061'],"['We present results of the first search for like-sign dilepton ($e^{\\pm}e^{\\pm}$, $e^{\\pm}\\mu^{\\pm}$, $\\mu^{\\pm}\\mu^{\\pm}$) events associated with multijets and large missing energy using 106 \\ipb\\ of data in \\ppbar\\ collisions at $\\sqrt{s} = 1.8$ TeV collected during 1992-95 by the CDF experiment. Finding no events that pass our selection, we examine pair-production of gluinos ($\\gluino$) and squarks ($\\squark$) in a constrained framework of the Minimal Supersymmetric Standard Model. At $\\tan\\beta = 2$ and $\\mu=-800$ \\gevcc, we set 95\\% confidence level limits of $\\mgluino > 221$ \\gevcc\\ for $\\mgluino \\simeq \\msquark$, and $\\mgluino > 168$ \\gevcc for $\\msquark \\gg \\mgluino$, both with small variation as a function of $\\mu$.']",['2001-06-15']
78,['eng'],"['Anderson, S']",['Improved Upper Limits on the FCNC Decays $B\\to K\\ell^{+}\\ell^{-}$ and $B\\to K^{*}(892)\\ell^{+}\\ell^{-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'K*(892)', 'B, branching ratio', 'upper limit', 'neutral current, flavor changing', 'mass, dilepton', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> K*(892) lepton+ lepton-', 'B --> K lepton+ lepton-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106060'],['We have searched a sample of 9.6 million BBbar events for the flavor-changing neutral current decays B -> K l^+ l^- and B -> K^*(892) l^+ l^-. We subject the latter decay to the requirement that the dilepton mass exceed 0.5 GeV. There is no indication of a signal. We obtain the 90% confidence level upper limits on the branching fractions Br(B -> K l^+ l^-) < 1.7 \\times 10^{-6} and Br(B -> K^*(892) l^+ l^-) < 3.3 \\times 10^{-6}. We also obtain an upper limit on the weighted average 0.65 Br(B -> K l^+ l^-) + 0.35 Br(B -> K^*(892) l^+ l^-) < 1.5 \\times 10^{-6}. The weighted-average limit is only 50% above the Standard Model prediction.'],['2001-06-15']
79,['eng'],"['Abazov, V M']",['Search for Single Top Quark Production at DZero Using Neural Networks'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, hadroproduction', 'quark, decay', 'channel cross section, upper limit', 'track data analysis, neural network', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> truth beauty anything', 'anti-p p --> truth beauty quark anything', 'truth --> W beauty', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106059'],"['We present a search for electroweak production of single top quarks in ~90 pb^-1 of data collected with the DZero detector at the Fermilab Tevatron collider. Using arrays of neural networks to separate signals from backgrounds, we set upper limits on the cross sections of 17 pb for the s-channel process ppbar->tb+X, and 22 pb for the t-channel process ppbar->tqb+X, both at the 95% confidence level.']",['2001-06-15']
80,['eng'],"['Abe, T']","['Linear Collider Physics Resource Book for Snowmass 2001, 4']",['Particle Physics - Experimental Results'],"['talk, Snowmass 2001/06/30', 'electron positron, linear collider', 'linear collider, proposed', 'electron positron, colliding beams', 'photon photon, colliding beams', 'photon electron, colliding beams', 'electron electron, colliding beams', 'supersymmetry', 'new interaction, search for', 'new particle, search for', 'Higgs particle, composite', 'technicolor', 'space-time, higher-dimensional', 'positron, polarized beam', 'Compton scattering, backscatter', 'laser', 'beam transport', 'scattering, beam-beam', 'colliding beam detector, proposed', 'costs', 'numerical calculations', 'tables', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106058'],"['This Resource Book reviews the physics opportunities of a next-generation e+e- linear collider and discusses options for the experimental program. Part 4 discusses options for the linear collider program, at a number of levels. First, it presents a broad review of physics beyond the Standard Model, indicating how the linear collider is relevant to each possible pathway. Next, it surveys options for the accelerator and experimental plan, including the questions of the running scenario, the issue of one or two interaction regions, and the options for positron polarization, photon-photon collisions, and e-e- collisions. Finally, it reviews the detector design issues for the linear collider and presents three possible detector designs.']",['2001-06-15']
81,['eng'],"['Abe, T']","['Linear Collider Physics Resource Book for Snowmass 2001, 3']",['Particle Physics - Experimental Results'],"['talk, Snowmass 2001/06/30', 'electron positron, linear collider', 'linear collider, proposed', 'electron positron, annihilation', 'photon photon, interaction', 'electroweak interaction, validity test', 'electroweak interaction, symmetry breaking', 'W, pair production', 'coupling, (3gauge boson)', 'coupling, (4gauge boson)', 'new particle, search for', 'space-time, higher-dimensional', 'quark, truth', 'quark, beauty', 'quark, pair production', 'quantum chromodynamics', 'strong interaction, coupling constant', 'W, mass', 'numerical calculations', 'proposed experiment', 'bibliography', '500, 800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106057'],"['This Resource Book reviews the physics opportunities of a next-generation e+e- linear collider and discusses options for the experimental program. Part 3 reviews the possible experiments on that can be done at a linear collider on strongly coupled electroweak symmetry breaking, exotic particles, and extra dimensions, and on the top quark, QCD, and two-photon physics. It also discusses the improved precision electroweak measurements that this collider will make available.']",['2001-06-15']
82,['eng'],"['Abe, T']","['Linear Collider Physics Resource Book for Snowmass 2001, 2']",['Particle Physics - Experimental Results'],"['talk, Snowmass 2001/06/30', 'electron positron, linear collider', 'linear collider, proposed', 'electron electron, interaction', 'photon electron, interaction', 'photon photon, interaction', 'Higgs particle, search for', 'electroweak interaction, symmetry breaking', 'Higgs particle, decay modes', 'Higgs particle, coupling', 'supersymmetry', 'sparticle, mass', 'sparticle, coupling', 'R parity, violation', 'numerical calculations', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106056'],['This Resource Book reviews the physics opportunities of a next-generation e+e- linear collider and discusses options for the experimental program. Part 2 reviews the possible experiments on Higgs bosons and supersymmetric particles that can be done at a linear collider.'],['2001-06-15']
83,['eng'],"['Abe, T']","['Linear Collider Physics Resource Book for Snowmass 2001, 1']",['Particle Physics - Experimental Results'],"['talk, Snowmass 2001/06/30', 'electron positron, linear collider', 'linear collider, proposed', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, composite', 'Higgs particle, multiplet', 'Higgs particle, mass', 'supersymmetry', 'sparticle, mass', 'electroweak interaction, validity test', 'quark, truth', 'quark, pair production', 'new particle, search for', ""Z'"", 'space-time, higher-dimensional', 'numerical calculations', 'proposed experiment', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106055'],['This Resource Book reviews the physics opportunities of a next-generation e+e- linear collider and discusses options for the experimental program. Part 1 contains the table of contents and introduction and gives a summary of the case for a 500 GeV linear collider.'],['2001-06-15']
84,['eng'],"['Raghavan, R S']",['pp-Solar Neutrino Spectroscopy'],['Particle Physics - Experimental Results'],"['neutrino, solar', 'neutrino/e', 'scintillation counter, liquid', 'organic compounds, liquid', 'indium', 'ytterbium', 'deep underground detector, Gran Sasso']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106054'],"['A new indium-loaded liquid scintillator (LS) with up to 15wt% In and high light output promises a breakthrough in the 25y old proposal for observing pp solar neutrinos (nue) by tagged nue capture in 115In. Intense background from the natural beta-decay of In, the single obstacle blocking this project till now, can be reduced by more than x100 with the new In-LS. Only non-In background remains, dramatically relaxing design criteria. Eight tons of In yields ~400 pp nue/y after analysis cuts. With the lowest threshold yet, Q=118 keV, In is the most sensitive detector of the pp nue spectrum, the long sought touchstone for nue conversion.']",['2001-09-14']
85,['eng'],"['Eschrich, I']",['Measurement of the Sigma^- Charge Radius by Sigma^- Electron Elastic Scattering'],['Particle Physics - Experimental Results'],"['elastic scattering, electron Sigma-', 'electron, bound state', 'Sigma-, form factor', 'form factor, electric', 'momentum transfer, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106053'],['The Sigma^- mean squared charge radius has been measured in the space-like Q^2 range 0.035-0.105 GeV^2/c^2 by elastic scattering of a Sigma^- beam off atomic electrons. The measurement was performed with the SELEX (E781) spectrometer using the Fermilab hyperon beam at a mean energy of 610 GeV/c. We obtain <r^2> = (0.61 +/- 0.12 (stat.) +/- 0.09 (syst.)) fm^2. The proton and pi^- charge radii were measured as well and are consistent with results of other experiments. Our result agrees with the recently measured strong interaction radius of the Sigma^-.'],['2001-06-14']
86,['eng'],"['Venanzoni, G']",['$\\sigma(e^+ e^- \\to hadrons)$ at low energy'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/04/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'cross section, hadronic', 'quantum electrodynamics, coupling constant', 'muon, magnetic moment', 'experimental results', 'proposed experiment', '< 10 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106052'],['In this talk I will review the recent experimental status of $\\sigma(e^+ e^- \\to hadrons)$ at $\\sqrt{s}<10 GeV$ and the prospects for the future. The influence on $\\alpha_{QED}(M^2_{Z})$ and $(g-2)_{\\mu}$ is also discussed.'],['2001-06-14']
87,['eng'],"['Moneta, L']",['Higgs Searches at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'anti-p p, colliding beams', 'Higgs particle, search for', 'supersymmetry', 'intermediate boson, hadroproduction', 'intermediate boson, decay modes', 'Higgs particle, associated production', 'Higgs particle, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, truth', 'quark, decay', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> Higgs particle W anything', 'anti-p p --> Higgs particle Z0 anything', 'Higgs particle --> 2beauty', 'truth --> Higgs particle beauty', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106050'],['This paper describes the searches for the Higgs boson performed by the CDF and D0 collaborations at the Tevatron ppbar Collider using the data collected in the 1992-95 run. Searches for standard model Higgs and as well for neutral and charged minimal SUSY Higgs bosons are also presented. No signal has been observed and limits are set for production cross sections.'],['2001-06-14']
88,['eng'],[],['Matter Effects in Upward-Going Muons and Sterile Neutrino Oscillations'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'neutrino nucleus, interaction', 'charged current', 'muon, angular distribution', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, sterile', 'matter, effect', 'deep underground detector, MACRO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106049'],"['The angular distribution of upward-going muons produced by atmospheric neutrinos in the rock below the MACRO detector show anomalies in good agreement with two flavor neutrino-mu ==> neutrino-tau oscillations with maximum mixing and Delta m**2 around 0.0024 eV**2. Exploiting the dependence of magnitude of the matter effect on oscillation channel, and using a set of 809 upward-going muons observed in MACRO, we show that the two flavor neutrino-mu ==> neutrino-tau oscillation is disfavored with 99% C.L. with respect to neutrino-mu ==> neutrino-tau.']",['2001-06-14']
89,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Beloborodov, K I', 'Berdyugin, A V', 'Bogdanchikov, A G', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Druzhinin, V P', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Otboev, A V', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Vasilev, A V', 'Velikzhanin, Yu S']",['Study of the $\\pi\\pi$ mass spectra in the process $e^+e^- \\to \\pi^+\\pi^-\\pi^0$ at $\\sqrt[]{s} \\simeq 1020$ MeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'pi, multiple production', 'mass spectrum, two-pion', 'vector dominance', 'rho(770), intermediate state', 'rho(770), mass', 'rho(770), width', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'interference, (omega(783) rho(770))', 'magnetic detector, SND', 'experimental results', 'Novosibirsk Stor2', 'tables', 'electron positron --> pi+ pi- pi0', '1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106048'],"['The invariant mass spectra of the $\\pi^+\\pi^-$ and $\\pi^\\pm\\pi^0$ pairs in the process $e^+e^- \\to \\pi^+\\pi^-\\pi^0$ were studied in the SND experiment at the VEPP-2M collider in the energy region $\\sqrt[]{s} \\simeq 1020$ MeV. These studies were based on about $0.5 \\times 10^6$ experimental events. The spectra were analyzed in the framework of the vector meson dominance model. It was found that the experimental data can be described with $e^+e^- \\to \\rho\\pi \\to \\pi^+\\pi^-\\pi^0$ transition only. Upper limit on the branching ratio of the $\\phi(1020)\\to\\pi^+\\pi^-\\pi^0$ decay through intermediate states different from $\\rho\\pi$ was obtained at the 90 % confidence level: $B(\\phi\\to\\pi^+\\pi^-\\pi^0)<6 \\cdot 10^{-4}$. The $\\rho$-meson mass and width which follow from the spectra analysis are $m_\\rho=775.0\\pm 1.3$ MeV, $\\Gamma_\\rho=150.4 \\pm 3.0$ MeV. Neutral and charged $\\rho$-mesons mass difference was found to equal $m_{\\rho^\\pm}-m_{\\rho^0}=-1.3\\pm2.3$ MeV. In the $\\pi^+\\pi^-$ mass spectrum the $\\rho-\\omega$ interference was seen at two standard deviations level.']",['2001-09-14']
90,['eng'],"['Affolder, T']",['Measurement of dsigma/DM Forward-Backward Charge Asymmetry for High Mass Drell-Yan e+e- Pairs from p-pbar Collisions at sqrt(s)=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electron, pair production', 'Drell-Yan process', 'differential cross section, mass', 'angular distribution, asymmetry', 'charge, asymmetry', 'electroweak interaction, validity test', ""Z'"", 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> positron electron anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106047'],"[""We report on a measurement of the mass dependence of the forward-backward charge asymmetry, A_FB, and production cross section dsigma/dM for e+e- pairs with mass M_ee>40 GeV/c2. The data sample consists of 108 pb-1 of p-pbar collisions at sqrt(s)=1.8 TeV taken by the Collider Detector at Fermilab during 1992-1995. The measured asymmetry and dsigma/dM are compared with the predictions of the Standard Model and a model with an extra Z' gauge boson.""]",['2001-06-13']
91,['eng'],"['Zallo, A']",['New results in diffractive production from E687 at FNAL'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'photon nucleus, inclusive reaction', 'beryllium', 'pi, multiple production', 'mass spectrum, (3pi+ 3pi-)', 'mass spectrum, (2pi+ 2pi-)', 'transverse momentum, spectra', 'diffraction, production', 'resonance, mass', 'resonance, width', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'photon beryllium --> 3pi+ 3pi- anything']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106046'],['A narrow dip structure has been observed at 1.9 GeV/c$^2$ in a study of diffractive photoproduction of the $~3\\pi^+3\\pi^-$ final state performed by the Fermilab experiment E687. Preliminary results on new structures in $~2\\pi^+2\\pi^-$ final states are also given.'],['2001-09-14']
92,['eng'],"['Spiropulu, M']",['SUSY Searches at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'anti-p p, colliding beams', 'supersymmetry', 'sparticle, search for', 'squark, truth', 'squark, pair production', 'squark, semileptonic decay', 'gluino', 'R parity, violation', 'LSP, decay', 'final state, (4jet dimuon)', 'final state, (2jet tau+ tau-)', 'final state, (positron electron 2photon missing-energy)', 'final state, ((n)jet missing-energy)', 'sparticle, mass', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106045'],['We discuss some of the latest results from supersymmetry searches at the Tevatron'],['2001-06-12']
93,['eng'],"['Convery, M']","['Charmless B decays from BABAR $(B^{0} \\to K^{+0}\\gamma and \\to \\pi^{+}\\pi^{-},K^{+}\\pi^{-},K^{+}K^{-})$']",['Particle Physics - Experimental Results'],"['talk, La Thuile 2001/03/04', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'B0, radiative decay', 'final state, (0charm)', 'final state, (meson+ meson-)', 'K*(892)', 'Feynman graph, penguin', 'B0, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> K*(892) photon', 'B0 --> pi+ pi-', 'B0 --> K+ pi-', 'B0 --> K+ K-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106043'],"[""The BABAR experiment has completed its first year of data-taking during which 21 $fb^{-1}$ of data were accumulated. We present preliminary results on two types of charmless B decays based on this data sample. The first, $B^0 \\to K^{*0}\\gamma$, is a so-called electromagnetic penguin. And the second, $B^0 \\to h^+h^{'-}$, where $h^{(')}$ can be either a pion or kaon, can come from either penguin diagrams or Cabibbo suppressed tree diagrams.""]",['2001-06-11']
94,['eng'],"['Akimov, D Y', 'Bewick, A', 'Davidge, D', 'Dawson, J', 'Howard, A S', 'Ivaniouchenkov, Yu', 'Jones, W G', 'Joshi, M', 'Kudryavtsev, V A', 'Lawson, T B', 'Lebedenko, V', 'Lehner, M J', 'Lightfoot, P K', 'Liubarsky, I', 'Lüscher, R', 'McMillan, J E', 'Peak, C D', 'Quenby, J J', 'Spooner, N J C', 'Sumner, T J', 'Tovey, D R', 'Ward, C K']",['Measurements of Scintillation Efficiency and Pulse-Shape for Low Energy Recoils in Liquid Xenon'],['Particle Physics - Experimental Results'],"['scintillation counter, liquid', 'xenon, liquid', 'nucleus, recoil', 'electron, recoil', 'efficiency', 'astrophysics, missing-mass', 'search for, WIMP']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106042'],"['Results of observations of low energy nuclear and electron recoil events in liquid xenon scintillator detectors are given. The relative scintillation efficiency for nuclear recoils is 0.22 +/- 0.01 in the recoil energy range 40 keV - 70 keV. Under the assumption of a single dominant decay component to the scintillation pulse-shape the log-normal mean parameter T0 of the maximum likelihood estimator of the decay time constant for 6 keV < Eee < 30 keV nuclear recoil events is equal to 21.0 ns +/- 0.5 ns. It is observed that for electron recoils T0 rises slowly with energy, having a value ~ 30 ns at Eee ~ 15 keV. Electron and nuclear recoil pulse-shapes are found to be well fitted by single exponential functions although some evidence is found for a double exponential form for the nuclear recoil pulse-shape.']",['2001-06-11']
95,['eng'],"['Messchendorp, J G', 'Sibirtsev, A A', 'Cassing, W', 'Metag, V', 'Schadmand, S']",['Studying the $\\omega$-mass in-medium in $\\gamma + A\\to \\pi^0\\gamma +X$ reactions'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'carbon', 'calcium', 'niobium', 'pi0, photoproduction', 'mass spectrum, (pi0 photon)', 'omega(783), intermediate state', 'omega(783), mass', 'nuclear matter, density', 'spectral representation', 'transport theory', 'pi0, final-state interaction', 'dependence, mass number', 'photon, energy spectrum', 'numerical calculations', 'proposed experiment', 'photon nucleus --> pi0 photon anything']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106041'],"['Simulations based on a coupled-channel transport model have been performed to analyze the feasibility to study the in-medium $\\omega$ mass e xploiting the process $\\gamma+A\\to\\pi^0\\gamma+X$ for $C$, $Ca$ and $Nb$ nuclei. The distortions due to final-state interactions of the $\\pi^0$ and background contributions from the reaction $\\gamma+A\\to\\pi^0\\pi^0+X$ are found to be small in the mass range of interest ($0.6<M_{\\pi^0\\gamma}<0.8$ GeV). Furthermore, the effect of the detector resolution on the $\\pi^0\\gamma$-mass determination is discussed.']",['2001-06-11']
96,['eng'],[],['Subjet Multiplicity in Quark and Gluon Jets at Dzero'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'talk, Budapest 2001/07/12', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'particle identification, jet', 'quark, jet', 'gluon, jet', 'jet, multiplicity', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> (n)jet anything', '630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106040'],"['We measure the subjet multiplicity M in jets reconstructed with a successive combination type of jet algorithm (kT). We select jets with 55<pT<100 GeV and |eta|<0.5. We compare similar samples of jets at sqrt(s)=1800 and 630 GeV. The HERWIG Monte Carlo simulation predicts that 59% of the jets are gluon jets at sqrt(s)=1800 GeV, and 33% at sqrt(s)=630 GeV. Using this information, we extract the subjet multiplicity in quark (Mq) and gluon (Mg) jets. We also measure the ratio R= (<Mg> -1)/(<Mq>-1)= 1.84 +- 0.15(stat) +0.22-0.18(sys).']",['2001-06-11']
97,['eng'],"['Abazov, V M']",['Search for New Physics Using Quaero'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'new interaction, search for', 'intermediate boson, pair production', 'quark, truth', 'quark, pair production', 'Higgs particle, associated production', 'leptoquark, pair production', 'data analysis method', 'channel cross section, branching ratio', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106039'],"['We describe Quaero, a method that i) enables the automatic optimization of searches for physics beyond the standard model, and ii) provides a mechanism for making high energy collider data generally available. We apply Quaero to searches for standard model WW, ZZ, and ttbar production, and to searches for these objects produced through a new heavy resonance. Through this interface, we make three data sets collected by the D0 experiment at sqrt(s)=1.8 TeV publicly available.']",['2001-06-11']
98,['eng'],"['Ammar, R']","['Search for the Familon via $B^{\\pm}\\to \\pi^{\\pm}X^{0}$, $B^{\\pm}\\to K^{\\pm}X^{0}$, and $B^{0}\\to K_{S}^{0} X^{0}$ Decays']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'familon, search for', 'symmetry, family', 'symmetry, spontaneously broken', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> pseudoscalar meson familon', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106038'],"['We have searched for the two-body decay of the B meson to a light pseudoscalar meson $h = \\pi^+, K^+, K^0_S$ and a massless neutral weakly-interacting particle $X^0$ such as the familon, the Nambu-Goldstone boson associated with a spontaneously broken global family symmetry. We find no significant signal by analyzing a data sample containing 9.7 million $B\\bar{B}$ mesons collected with the CLEO detector at the Cornell Electron Storage Ring, and set a 90% C.L. upper limit of $4.9 \\times 10^{-5}$ and $5.3 \\times 10^{-5}$ on the branching fraction for the decays $B^+ \\to h^+ X^0$ and $B^0 \\to K^0_S X^0$, respectively. These upper limits correspond to a lower bound of about $10^{8}$ GeV on the family symmetry breaking scale involving the third generation of quarks.']",['2001-09-14']
99,['eng'],"['Achenbach, C P', 'Cobb, J H']",['A new airborne detector for atmospheric muons'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2001/08/07', 'muon, cosmic radiation', 'neutrino, cosmic radiation', 'showers, air', 'scintillation counter, hodoscope', 'scintillation counter, plastics', 'lead']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106037'],['The University of Oxford has started the design and development of the new experiment ADLER (Airborne Detector for Low Energy Rays). This apparatus will measure the cosmic-ray muon flux at an altitude of 10 - 13km. The detector should be flown by aircrafts on transatlantic routes crossing the magnetic equator to investigate the flux at different geomagnetic latitudes. The goal of the experiment is to obtain better constraints on the low energy atmospheric neutrino flux and the results will be of importance to the atmospheric neutrino anomaly.'],['2001-06-08']
100,['eng'],"['Pöschl, R']",['Jets and Event Shape Studies in ep-collisions at HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'electron p, colliding beams', 'electron p, deep inelastic scattering', 'jet, electroproduction', 'hadron, multiple production', 'event shape analysis', 'quantum chromodynamics, perturbation theory', 'correction, nonperturbative', 'final state, (2jet)', 'strong interaction, coupling constant', 'p, structure function', 'gluon, momentum spectrum', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106036'],"['The results of complementary tests of perturbative QCD in DIS at large centre-of-mass energies at HERA are presented. The analysis of event shape variables allows for the investigation of approaches to understand aspects of non-perturbative QCD such as the formation of the hadronic final state. The strong coupling constant, $\\alpha_s$, is extracted from both inclusive jet cross sections and dijet rates and is found to be competitive with the world average.']",['2001-06-08']
101,['eng'],"['Kirsanov, M M']",['Calculations of neutrino spectra with a program based on the GEANT library'],['Particle Physics - Experimental Results'],"['neutrino, secondary beam', 'beam, energy', 'p nucleus, interaction', 'hadron, multiple production', 'hadron, decay', 'pi', 'K', 'beam dump', 'programming, Monte Carlo', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106035'],['The methods of neutrino spectra calculations with GEANT library and the peculiarities of such calculations for different neutrino beams are summarized. The formula expressing $K^0$ yields from a neutrino target through the $K^+$ and $K^-$ yields from the same target is proposed'],['2001-06-08']
102,['eng'],"['Martínez, G']","['ALICE, the heavy ion experiment at LHC']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'scattering, heavy ion', 'lead', 'quark gluon, plasma', 'critical phenomena', 'luminosity', 'particle identification', 'magnetic detector, ALICE', 'proposed experiment, CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106034'],"['ALICE, A Large Ion Collider Experiment, is the future Large Hadron Collider (LHC) experiment at CERN devoted to the physics of Quantum Chromo-thermo-dynamics. Relativistic Heavy-Ion Collisions (HIC) at LHC aim at the production of a plasma of quarks and gluons (QGP). This plasma is expected to be much hotter, bigger and longer than in previous HIC experiments at lower center-of-mass energies. In the ALICE experiment, the ephemeral QGP created during the first stages of the HIC will be studied by the concomitant detection of most of the probes of high temperature strongly interacting matter.']",['2001-06-08']
103,['eng'],"['Fusayasu, T']",['EW tests at High Q2'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron p, colliding beams', 'positron p, colliding beams', 'electron p, deep inelastic scattering', 'momentum transfer, high', 'neutral current', 'charged current', 'channel cross section, momentum transfer', 'x-dependence', 'structure function', 'W, propagator', 'quark, valence', 'quark, momentum spectrum', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300, 318 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106033'],['High-Q^2 NC and CC DIS cross sections have been measured by H1 and ZEUS at HERA. Both NC and CC results based on data taken during the year 1994-2000 are in good agreement with Standard Model expectations. The structure function xF_3 is extracted from the NC cross sections and the mass of the W propagator is extracted from the CC cross sections. Valence quark distributions are derived by means of an NLO QCD fit.'],['2001-06-08']
104,['eng'],"['Abazov, V M']",['Measurement of the ratio of the differential cross sections for W and Z boson production as a function of transverse momentum in pbarp collisions at sqrt(s)=1.8TeV'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'talk, Budapest 2001/07/12', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'differential cross section, ratio', 'transverse momentum, dependence', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106027'],"['We report on a preliminary measurement of the ratio of the differential cross sections for W and Z boson production as a function of transverse momentum in proton-antiproton collisions at $\\sqrt{s}$ = 1.8 TeV. It has been shown that the ratio between W and Z observables can be reliably calculated using perturbative QCD, even when the individual observables are not. We present the first comparison between the measurement of a W and Z observable ratio and a purely perturbative calculation. The use of the ratio reduces both experimental and theoretical uncertainites and might result in smaller overall uncertainties on the measured W mass and width, compared to currently used methods at hadron colliders.']",['2001-09-14']
105,['eng'],"['Habig, A']",['Discriminating between nu_mu <-> nu_tau and nu_mu <-> nu_sterile in atmospheric nu_mu oscillations with the Super-Kamiokande detector'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2001/08/07', 'neutrino, oscillation', 'neutrino/mu, cosmic radiation', 'neutrino/tau', 'neutrino, sterile', 'matter, effect', 'neutrino nucleus, interaction', 'neutral current', 'charged current', 'tau, particle identification', 'angular distribution', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106025'],"[""A strong body of evidence now exists for atmospheric nu_mu disappearance oscillations. Such disappearance could be explained by oscillations to either nu_tau or a ``sterile'' neutrino (nu_s). Super-Kamiokande uses three different methods to distinguish between these two scenarios. First, matter effects would suppress the nu_mu <-> nu_s oscillation amplitude at high energy. Second, oscillation to nu_s would reduce the overall neutral-current neutrino interaction rate. Third, the smoking gun of nu_mu <-> nu_tau oscillations would be the observation of tau appearance resulting from charged-current nu_tau interactions. The results of these three techniques are presented, which strongly favor nu_mu <-> nu_tau oscillations over nu_mu <-> nu_s.""]",['2001-06-06']
106,['eng'],"['Habig, A']",['An Indirect Search for WIMPs with Super-Kamiokande'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2001/08/07', 'astrophysics, missing-mass', 'WIMP, annihilation', 'scattering, WIMP nucleus', 'neutrino/mu, production', 'neutrino nucleus, interaction', 'charged current', 'muon, angular distribution', 'muon, flux', 'neutrino, flux', 'upper limit', 'mass, dependence', 'WIMP, mass', 'Cherenkov counter, water', 'experimental results', 'deep underground detector, KAMIOKANDE']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106024'],"['A potential source of high energy neutrinos is the annihilation of Weakly Interacting Massive Particles (WIMPs) collecting in gravitational potential wells such as the centers of the Earth, the Sun, or the Galaxy. A search for such a WIMP annihilation signal using the Super-Kamiokande (Super-K) detector is presented. Super-K observes 1.1 upward through-going muons per day. These events are caused by high energy (typical E_nu ~ 100 GeV) nu_mu interactions in the rock under the detector, and are generally consistent with the expected flux from atmospheric neutrinos. No enhancement of the neutrino signal due to WIMP annihilation is seen, so upper limits on the possible flux of WIMPS are set. These limits are compared to those from other such indirect searches, and a model-independent method is used to compare the Super-K results with direct-detection WIMP experiments.']",['2001-06-06']
107,['eng'],"['Zech, G']",['Frequentist and Bayesian Confidence Limits'],['Particle Physics - Experimental Results'],"['statistical analysis', 'performance', 'numerical calculations, Monte Carlo', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106023'],"['Frequentist (classical) and the Bayesian approaches to the construction of confidence limits are compared. Various examples which illustrate specific problems are presented. The Likelihood Principle and the Stopping Rule Paradox are discussed. The performance of the different methods is investigated relative to the properties coherence, precision, bias, universality, simplicity. A proposal on how to define error limits in various cases are derived from the comparison. They are based on the likelihood function only and follow in most cases the general practice in high energy physics. Classical methods are not recommended because they violate the Likelihood Principle, they can produce physically inconsistent results, suffer from lack of precision and generality. Also the extreme Bayesian approach with arbitrary choice of the prior probability density or priors deduced from scaling laws is rejected.']",['2001-06-06']
108,['eng'],"['Heinsius, F H']",['Structure Functions and the Spin of the Nucleon'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'positron p, deep inelastic scattering', 'lepton nucleus, deep inelastic scattering', 'lepton, polarized beam', 'nucleus, polarized target', 'hadron, multiple production', 'nucleon, structure function', 'nucleon, spin', 'quark, polarization', 'dependence, flavor', 'gluon, polarization', 'Compton scattering, off-shell', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'proposed experiment, CERN SPS', '27.5, 100-200 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106021'],['The HERMES and SMC experiments have determined the contribution of different quark flavors to the nucleon spin in a large range of Bjorken-x via semi-inclusive deep inelastic scattering. The main goal of the COMPASS experiment is to measure the gluon polarization in the nucleon. In all experiments a polarized lepton is scattered off a polarized nucleon. Latest results from HERMES and perspectives for COMPASS running in 2001 and beyond are presented.'],['2001-06-06']
109,['eng'],"['Böhrer, A']",['Bottom Production in Two-Photon Collisions at LEP'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'electron, transverse momentum', 'channel cross section, energy dependence', 'eta/b, search for', 'width, branching ratio', 'upper limit', 'magnetic detector, ALEPH', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106020'],"['Results on inclusive and exclusive bottom production in gammagamma collisions are presented. The total cross section of inclusive bottom production is investigated through its leptonic decays at LEP II energies by the experiments L3 and OPAL. The average cross section, after correction for acceptances and efficiencies, is sigma_tot = 13.3 +- 1.5 +- 2.3 pb. The next-to-leading order calculations are lower than the data by a factor three, which corresponds to a difference of more than three standard deviations. ALEPH studied the exclusive bottom production. Searching for the eta_b one candidate is found. Limits on Gamma_gammagamma(eta_b)*BR for 4 and 6 charged particles are extracted. The candidate has a mass of 9.30 +- 0.04 GeV.']",['2001-06-06']
110,['eng'],"['Abazov, V M']",['The Inclusive Jet Cross Section in ppbar Collisions at sqrt{s}=1.8 TeV using the kT Algorithm'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/07/23', 'talk, Budapest 2001/07/12', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'jet, particle identification', 'track data analysis, cluster', 'differential cross section, transverse momentum', 'rapidity, central region', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> jet anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106032'],"['We present a preliminary measurement of the central inclusive jet cross section using a successive combination algorithm based on relative transverse momenta (kT) for jet reconstruction. We analyze a 87.3 pb-1 data sample collected by the D0 detector at the Fermilab Tevatron ppbar Collider during 1994-1995. The cross section, reported as a function of transverse momentum (pT > 60 GeV) in the central region of pseudo-rapidity (|eta| < 0.5), is in reasonable agreement with next-to-leading order QCD predictions. This is the first jet production measurement in a hadron collider using a successive combination type of jet algorithm.']",['2001-09-14']
111,['eng'],"['Abbiendi, G', 'Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Etzion, E', 'Fabbri, F L', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kramer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Moed, S', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rozen, Y', 'Runge, K', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Ujvári, B', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for Single Leptoquark and Squark Production in Electron-Photon Scattering at $\\sqrt{s_{ee}}$ = 189 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'photon electron, interaction', 'new particle, search for', 'leptoquark, scalar', 'leptoquark, vector', 'squark', 'supersymmetry', 'R parity, violation', 'photon, resolved', 'electroweak interaction, validity test', 'leptoquark, decay', 'leptoquark, mass', 'lower limit', 'coupling, Yukawa', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> leptoquark anything', 'leptoquark --> quark electron', 'leptoquark --> quark neutrino', '189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106031'],"[""A search for first generation scalar and vector leptoquarks (LQ) as well as for squarks in R-parity violating SUSY models has been performed using e+e- collisions collected with the OPAL detector at LEP at an e+e- centre-of-mass energy sqrt(s_ee) of 189 GeV. The data correspond to an integrated luminosity of about 160 pb-1. The dominant process for this search is e q -> LQ/squark -> e q, nu q, where a photon, which has been radiated by one of the beam electrons, serves as a source of quarks. The numbers of selected events found in the two decay channels are in agreement with the expectations from Standard Model processes. This result allows to set lower limits at the 95% confidence level on the mass of first generation scalar and vector leptoquarks, and of squarks in R-parity violating SUSY models. For Yukawa couplings lambda to fermions larger than sqrt{4 pi alpha_em}, the mass limits range from 121 GeV/c^2 to 175 GeV/c^2 (149 GeV/c^2 to 188 GeV/c^2) depending on the branching ratio beta of the scalar (vector) leptoquark state. Furthermore, limits are set on the Yukawa couplings lambda for leptoquarks and lambda'_1jk for squarks, and on beta as a function of the scalar leptoquark/squark mass.""]",['2001-06-07']
112,['eng'],"['Kuze, M']",['Searches for New Physics at HERA'],['Particle Physics - Experimental Results'],"['talk, La Thuile 2001/03/04', 'electron p, colliding beams', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'new particle, search for', 'new interaction, search for', 'four-fermion interaction', 'leptoquark', 'coupling, Yukawa', 'supersymmetry', 'supergravity', 'R parity, violation', 'flavor, violation', 'fermion, excited state', 'lepton, final state', 'transverse momentum, high', 'mass spectrum, transverse', 'space-time, higher-dimensional', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300, 318 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106030'],"['Recent results from searches for new physics at HERA are reviewed. Exploiting the uniqueness of lepton-hadron collisions at high energy, searches are performed for electron-quark resonant states (leptoquarks or squarks in R-parity-violating supersymmetry) or excited states of fermions. New phenomena at a very high energy scale, manifested at present energies as effective four-fermion contact interaction, are also investigated, including cases with lepton-flavor violation. Finally, the status of events with a high-energy lepton and missing transverse momentum is presented, resulting in the most stringent constraint on the flavor-changing neutral current t-u-\\gamma coupling which could yield single-top production.']",['2001-06-07']
113,['eng'],"['Frabetti, P L']",['Evidence for a narrow dip structure at 1.9 GeV/c$^2$ in $3\\pi^+ 3\\pi^- $ diffractive photoproduction'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium', 'meson resonance, photoproduction', 'pi, multiple production', 'mass spectrum, (3pi+ 3pi-)', 'mass spectrum, dip', 'diffraction', 'meson resonance, (1900)', 'meson resonance, mass', 'meson resonance, width', 'spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106029'],['A narrow dip structure has been observed at 1.9 GeV/c$^2$ in a study of diffractive photoproduction of the $~3\\pi^+3\\pi^-$ final state performed by the Fermilab experiment E687.'],['2001-06-07']
114,['eng'],"['Zhao, Z']",['Results and Future Plans from Bes'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'electron positron, colliding beams', 'electron positron, annihilation', 'cross section, hadronic', 'energy dependence', 'psi mesons, electroproduction', 'psi mesons, hadronic decay', 'muon, pair production', 'J/psi(3100), radiative decay', 'mass spectrum', 'partial wave analysis', 'f0(1710)', 'f2(1525)', 'magnetic spectrometer, BES', 'experimental results', 'proposed experiment', 'Beijing Stor', '2-5 GeV']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106028', 'http://www.slac.stanford.edu/econf/C010430/m10.html']","['The values of $R = \\sigma(e^+e^-\\to{hadrons})/ \\sigma(e^+e^-\\to\\mu^+\\mu^-)$ for 85 center-of-mass energies between 2 and 5 GeV are reported. Preliminary results using partial wave analysis for $J/\\psi$ decays to $\\gamma \\pi^+ \\pi^-$, $\\gamma K^+K^-$, $\\phi \\pi^+\\pi^-$ and $\\phi K^+K^-$ are presented. The BESIII/BEPCII, a project for the future of BES, is introduced.']",['2001-06-07']
115,['eng'],"['Schöning, A']",['Searches for deviations from SM at HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'positron p, colliding beams', 'electron p, colliding beams', 'positron p, deep inelastic scattering', 'new interaction, search for', 'four-fermion interaction', 'new particle, search for', 'space-time, higher-dimensional', 'graviton, exchange', 'quantum gravity', 'leptoquark, mass', 'fermion, excited state', 'supersymmetry', 'supergravity', 'sparticle, mass', 'R parity, violation', 'electroweak interaction, validity test', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300-318 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106022'],"['At HERA, new physics processes beyond the SM are probed in e^+/- proton collisions at a center of mass energy of 300-318 GeV. Recent results on searches obtained by the H1 and ZEUS experiments are presented with an emphasis on data taken in e^-p collisions in the years 1998/99 and in e^+p collisions in the years 1999 and 2000.']",['2001-06-06']
116,['eng'],"['Hu, H', 'Tai, A']",['Production at Intermediate Energies and Lund Area Law'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'electron positron, annihilation', 'hadron, multiple production', 'model, hadronization', 'string model, fragmentation', 'multiplicity, spectra', 'transverse momentum, spectra', 'programming, Monte Carlo', 'numerical calculations, Monte Carlo', 'interpretation of experiments, Beijing Stor']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106017', 'http://www.slac.stanford.edu/econf/C010430/T24.html']",['The Lund area law was developed into a Monte Carlo program LUARLW. The important ingredients of this generator was described. It was found that the LUARLW simulations are in good agreement with the BEPC/BES R scan data between 2--5 GeV.'],['2001-06-05']
117,['eng'],"['Barnyakov, M Y', 'Bobrovnikov, V S', 'Buzykaev, A R', 'Kolachev, G M', 'Kononov, S A', 'Kravchenko, E A', 'Minakov, G D', 'Onuchin, A P', 'Danilyuk, A F', 'Guber, F F', 'Kurepin, A B', 'Krasnov, V A']",['Proposal for the aerogel Cherenkov counters for the PEP-N detector'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'particle identification, (K pi)', 'Cherenkov counter, aerogel', 'optics, transformation', 'photoelectron, amplifier', 'magnetic detector, PEP-N', 'magnetic detector, KEDR', 'SLAC PEP Stor', 'Novosibirsk Stor4']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106016', 'http://www.slac.stanford.edu/econf/C010430/t15.html']","['The work is devoted to the development of the aerogel Cherenkov counters with the light collection on wavelength shifters and PMTs (ASHIPH). The ASHIPH system has been developed for the KEDR detector. Tests of the counters have been carried out on the Dubna accelerator, the pi/K separation obtained is about 4 sigma. The ASHIPH system is suggested for the PEP-N detector.']",['2001-06-05']
118,['eng'],"['Ganis, G']",['Supersymmetric dark matter in the light of LEP'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/04/18', 'astrophysics, missing-mass', 'supersymmetry', 'sparticle, search for', 'sneutrino, LSP', 'neutralino, LSP', 'Higgsino', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, width', 'sparticle, mass', 'lower limit', 'interpretation of experiments, CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106015'],['The negative outcome of searches for supersymmetry performed at LEP have been used to derive indirect constraints on the parameters of the most plausible models for cold dark matter based on supersymmetric extensions of the Standard Model. The main results are summarized.'],['2001-06-05']
119,['eng'],"['Levonian, S']",['F2p at low Q^2 and the total gamma-p cross section at HERA'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'positron p, colliding beams', 'neutral current', 'photon p, interaction', 'total cross section, energy dependence', 'momentum transfer, low', 'p, structure function', 'momentum transfer, dependence', 'structure function, longitudinal', 'quantum chromodynamics, perturbation theory', 'gluon, momentum spectrum', 'scaling, violation', 'pomeron', 'Regge poles', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106014'],['New precise measurements of the neutral current cross section at HERA are presented in different Q^2 regimes. In the photoproduction limit the total gamma-p cross section is found to be in agreement with the universal soft Pomeron prediction. At medium scales 1.5 < Q^2 < 150 GeV^2 both the F_2 and the F_L structure functions are determined. These data are well described by NLO pQCD. The gluon density in the proton has been extracted from the scaling violation of F_2 at low x. The transition between the two regimes occurs at around Q^2=1 GeV^2.'],['2001-06-05']
120,['eng'],"['Savinov, V']",['QCD Studies in Two-Photon Collisions at CLEO'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'quarkonium, charm', 'quarkonium, photoproduction', 'quarkonium, width', 'J/psi(3100), radiative decay', 'chi mesons, charm', 'eta/c(2980)', 'hadron, pair production', 'glueball', 'f4(2220), width', 'pseudoscalar meson', 'form factor, transition', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106013', 'http://www.slac.stanford.edu/econf/C010430/w03.html']","['We review QCD results of CLEO two-photon analyses and discuss the measurements of two-photon partial widths of charmonium and cross sections for hadron pairs production, antisearch for glueballs and the measurements of $\\gamma^*\\gamma \\to$ pseudoscalar meson transition form factors. We emphasize the importance of other possible analyses, favorable trigger conditions and selection criteria of the presently running experiment and the advantages of CLEOc - the future $\\tau$-charm factory at Cornell with the existing CLEO III detector.']",['2001-06-05']
121,['eng'],"['Menke, S']",['$\\alpha_{s}$ as at Low Q$^{2}$ from $e^{+}e^{-}$ and $\\tau$ Data'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'electron positron, annihilation', 'tau, semileptonic decay', 'hadron, multiple production', 'momentum transfer, low', 'strong interaction, coupling constant', 'spectral representation, moment', 'energy dependence', 'current, vector', 'current, axial-vector', 'quantum chromodynamics, perturbation theory', 'correction, nonperturbative', 'numerical calculations, Monte Carlo', 'interpretation of experiments']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106011', 'http://www.slac.stanford.edu/econf/C010430/M09.html']",['It has been shown in recent analyses by ALEPH [1] and OPAL [2] that precision QCD tests are possible with hadronic tau decays by comparing spectral moments of the hadronic decay ratio of the tau with QCD calculations. In principle e+e- data can be used in a similar manner by evaluating spectral moments of R. The current e+e- data is compared with the OPAL tau data and a prediction is made on the achievable accuracy of QCD tests with the projected precision of PEP-N [3].'],['2001-06-05']
122,['eng'],"['Grigoriev, D']",['CMD-2 Detector Upgrade'],['Particle Physics - Experimental Results'],"['talk, Stanford 01/04/30', 'electron positron, colliding beam detector', 'upgrade', 'superconducting, solenoid', 'drift chamber, gas', 'argon, organic compounds', 'carbon, fluorine', 'calorimeter', 'scintillation counter, crystal', 'scintillation counter, bismuth-germanate', 'cesium, iodine', 'xenon, liquid', 'Novosibirsk Stor2']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106009', 'http://www.slac.stanford.edu/econf/C010430/t09.html']","['The project of upgrading the detector CMD-2 is presented. The upgraded detector is called CMD-2M and is going to take data with new collider VEPP-2000 at BINP. The general structure of the detector CMD-2 will remain as is but major parameters of the detector, such as momentum and angular resolution for charged particle and energy and spatial resolution for photons, will be substantially improved.']",['2001-09-14']
123,['eng'],"['Ishii, T']",['K2K results'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'neutrino, oscillation', 'neutrino/mu, beam', 'neutrino/mu, flux', 'neutrino/e, search for', 'neutrino nucleon, interaction', 'iron', 'charged current', 'muon, energy spectrum', 'muon, angular distribution', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, KAMIOKANDE', 'experimental results', 'KEK PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106008'],"['The KEK-to-Kamioka long-baseline neutrino experiment (K2K) has begun its investigation of neutrino oscillation, and has established the method of a long-baseline neutrino experiment. From the first 100 days of data-taking, a deficit of muon neutrino in the 1-GeV energy region after 250-km flight was observed at the 90% significance level.']",['2001-06-04']
124,['eng'],"['Monaco, V']",['Diffractive structure functions from HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'diffraction, structure function', 'photon, dissociation', 'rapidity, gap', 'jet, multiple production', 'differential cross section', 'pomeron, exchange', 'pomeron, structure function', 'momentum spectrum, parton', 'momentum transfer, dependence', 'model, interaction', 'Altarelli-Parisi equation', 'color, dipole', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet positron anything', 'positron p --> 3jet positron anything', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106007'],"['Recent results on diffraction at HERA are presented, focusing on the measurement of the inclusive diffractive cross section and on the study of two and three jets in diffractive ep scattering.']",['2001-06-04']
125,['eng'],"['Horie, K']",['Measurement of $\\Gamma(K_{\\mu 3})/\\Gamma(K_{e3})$ ratio using stopped positive kaons'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'at rest', 'K+, branching ratio', 'decay, form factor', 'momentum transfer, dependence', 'universality, (muon electron)', 'Dalitz plot', 'magnetic spectrometer, experimental results', 'KEK PS', 'K+ --> pi0 muon+ neutrino/mu', 'K+ --> pi0 positron neutrino/mu', '0 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106006'],"['The ratio of the $K^{+}\\to \\pi^{0} \\mu^{+} \\nu$ ($K_{\\mu3}^+$) and $K^{+}\\to \\pi^{0} e^{+} \\nu$ ($K_{e3}^+$) decay widths, $\\Gamma(K_{\\mu 3})/\\Gamma(K_{e3})$, has been measured with stopped positive kaons. $K_{\\mu3}^+$ and $K_{e3}^+$ samples containing 2.4$\\times 10^4$ and 4.0$\\times 10^4$ events, respectively, were analyzed. The $\\Gamma(K_{\\mu3})/\\Gamma(K_{e3})$ ratio was obtained to be 0.671$\\pm$0.007(stat.)$\\pm$0.008(syst.) calculating the detector acceptance by a Monte Carlo simulation with the assumption of $\\mu$-$e$ universality in $K_{l3}^+$ decay. The coefficient of the $q^2$ dependent term of the $f_0$ form factor was also determined to be $\\lambda_0$=0.022$\\pm$0.005(stat.)$\\pm$0.004(syst.).']",['2001-06-04']
126,['eng'],"['Iori, M']",['Measurement of the Ds lifetime'],['Particle Physics - Experimental Results'],"['hadron nucleus, inclusive reaction', 'Sigma-', 'pi-', 'p', 'carbon', 'copper', 'D/s, hadroproduction', 'D/s, hadronic decay', 'D/s, lifetime', 'K*(892)', 'Phi(1020)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'hadron nucleus --> D/s anything', 'D/s --> K*(892) K', 'D/s --> Phi(1020) pi', '600 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106005'],"['We report a precise measurement of the Ds meson lifetime. The data were taken by the SELEX experiment (E781) spectrometer using 600 GeV/c Sigma-, pi- and p beams. The measurement has been done using 918 reconstructed Ds. The lifetime of the Ds is measured to be 472.5 +- 17.2 +- 6.6 fs, using K*(892)0K and phi pi decay modes. The lifetime ratio of Ds to D0 is 1.145 +- 0.049.']",['2001-06-04']
127,['eng'],"['Affolder, T']",['Cross Section and Heavy Quark Composition of Photon+Muon Events Produced in ppbar Collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'photon, direct production', 'quark, associated production', 'quark, charm', 'quark, beauty', 'quark, semileptonic decay', 'quark gluon, Compton scattering', 'photon, transverse momentum', 'yield, (beauty charm)', 'differential cross section, transverse momentum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> muon photon anything', 'charm gluon --> charm photon', 'charm gluon --> muon anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106004'],"['We present a measurement of the cross section and the first measurement of the heavy flavor content of associated direct photon + muon events produced in hadronic collisions. These measurements come from a sample of 1.8 TeV ppbar collisions recorded with the Collider Detector at Fermilab. Quantum chromodynamics (QCD) predicts that these events are primarily due to Compton scattering process charm+gluon -> charm+photon, with the final state charm quark producing a muon. The cross section for events with a photon transverse momentum between 12 and 40 GeV/c is measured to be 46.8+-6.3+-7.5 pb, which is two standard deviations below the most recent theoretical prediction. A significant fraction of the events in the sample contain a final-state bottom quark. The ratio of charm to bottom production is measured to be 2.4+-1.2, in good agreement with QCD models.']",['2001-06-04']
128,['eng'],"['Harris, F A']",['R Measurements at High $Q^{2}$'],['Particle Physics - Experimental Results'],"['review, Stanford 2001/04/30', 'electron positron, colliding beams', 'electron positron, annihilation', 'cross section, hadronic', 'energy dependence', 'momentum transfer, high', 'experimental results', 'magnetic spectrometer, BES', 'Beijing Stor', 'magnetic detector, CLEO', 'Cornell CESR Stor']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106003', 'http://www.slac.stanford.edu/econf/C010430/m12.html']","['Previous Measurements of R at high Q^2 are reviewed. Recent R measurement results, including those from the Beijing Spectrometer Experiment, are described. The present status of R measurements and future measurement possiblities are summarized.']",['2001-06-04']
129,['eng'],"['Anchordoqui, L A', 'Cook, J', 'Gabour, M', 'Kirsch, N', 'MacLeod, J', 'McCauley, T P', 'Musienko, Yu V', 'Paul, T C', 'Reucroft, S', 'Swain, J D', 'Terry, R']",['School Cosmic Ray Outreach Detector (SCROD)'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2001/08/07', 'ion, cosmic radiation', 'showers, air', 'scintillation counter, plastics', 'optics, transformation', 'semiconductor, optical', 'photoelectron, avalanche', 'data acquisition']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0106002'],"['We report on our studies of applying novel detector technologies developed for LHC-era experiments to cosmic ray detection. In particular, we are investigating usage of scintillating tiles with embedded wavelength-shifting fibers and avalanche photodiode readout as part of a robust, inexpensive cosmic air shower detector. In the near future, we are planning to deploy detector stations based on this technology at area high schools and colleges as part of an outreach and education effort, known as SCROD.']",['2001-06-04']
130,['eng'],"['Abramov, G N', 'Achasov, M N', 'Aulchenko, V M', 'Beloborodov, K I', 'Berdyugin, A V', 'Bogdanchikov, A G', 'Bozhenok, A V', 'Bukin, D A', 'Bukin, M A', 'Burdin, S V', 'Danilyuk, A F', 'Dimova, T V', 'Drozdetsky, A A', 'Druzhinin, V P', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Korol, A A', 'Koshuba, S V', 'Kravchenko, E A', 'Maksimov, L V', 'Obrazovsky, A E', 'Onuchin, A P', 'Ovchar, A V', 'Pakhtusova, E V', 'Peshkov, M A', 'Popov, V M', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Silagadze, Z K', 'Sirotkin, A A', 'Skripkin, A G', 'Usov, Yu V', 'Vasilev, A V', 'Velikzhanin, Yu S']",['SND Upgade'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'electron positron, colliding beam detector', 'upgrade', 'calorimeter, electromagnetic', 'energy resolution', 'scintillation counter, sodium-iodide', 'scintillation counter, crystal', 'drift chamber, gas', 'argon, organic compounds', 'particle identification, (K pi)', 'Cherenkov counter, threshold', 'Cherenkov counter, aerogel', 'data acquisition', 'programming', 'four-pi-detector, SND', 'Novosibirsk Stor2']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105093', 'http://www.slac.stanford.edu/econf/C010430/T10.html']","['The program of upgrade of the Spherical Neutral Detector for future experiments at a new VEPP-2000 $e^+e^-$ collider is presented. Modernization includes upgrades of electromagnetic calorimeter, tracking system, detector electronics, data acquisition system, and offline software. It is also planned to equip the detector with two new subsystems: particle identification system based on aerogel Cherenkov counters and external electron tagging system for $\\gamma\\gamma$ physics.']",['2001-09-14']
131,['eng'],"['Tournefier, E']",['Electroweak fits and the Higgs likelihood'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'electroweak interaction, validity test', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'angular distribution, asymmetry', 'W, pair production', 'W, mass', 'Higgs particle, mass', 'mass, truth', 'Weinberg angle', 'CERN LEP Stor', 'SLAC SLC Linac', '91, 161-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105091'],['An update of the electroweak measurements at LEP and SLC is presented. These measurements are used to perform precise tests of the Standard Model. A constraint on the Standard Model Higgs mass is obtained when the direct measurements of $m_{top}$ and $M_W$ are included in the fit. A combination with the direct Higgs search is also shown.'],['2001-06-01']
132,['eng'],[],['Measurement of the neutral current cross section and F2 structure function for deep inelastic e+p scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'neutral current', 'channel cross section', 'p, structure function', 'momentum transfer, dependence', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'Altarelli-Parisi equation', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'tables', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105090'],['The cross section and the proton structure function F2 for neutral current deep inelastic e+p scattering have been measured with the ZEUS detector at HERA using an integrated luminosity of 30 pb-1. The data were collected in 1996 and 1997 at a centre-of-mass energy of 300 GeV. They cover the kinematic range 2.7 < Q^2 < 30000 GeV2 and 6.10^-5 < x < 0.65. The variation of F2 with x and Q2 is well described by next-to-leading-order perturbative QCD as implemented in the DGLAP evolution equations.'],['2001-06-01']
133,['eng'],"['Ahrens, J']",['First measurement of the Gerasimov-Drell-Hearn integral for Hydrogen from 200 to 800 MeV'],['Particle Physics - Experimental Results'],"['photon p, interaction', 'photon, polarized beam', 'photon, tagged beam', 'polarized target', 'photon, absorption', 'pi, photoproduction', 'cross section, helicity', 'sum rule, Drell-Hearn-Gerasimov', 'p, polarizability', 'four-pi-detector, experimental results', 'Mainz Linac', 'photon p --> p pi0', 'photon p --> n pi+', '0.2-0.8 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105089'],"['A direct measurement of the helicity dependence of the total photoabsorption cross section on the proton was carried out at MAMI (Mainz) in the energy range 200 < E_gamma < 800 MeV. The experiment used a 4$\\pi$ detection system, a circularly polarized tagged photon beam and a frozen spin target. The contributions to the Gerasimov-Drell-Hearn sum rule and to the forward spin polarizability $\\gamma_0$ determined from the data are 226 \\pm 5 (stat)\\pm 12(sys) \\mu b and -187 \\pm 8 (stat)\\pm 10(sys)10^{-6} fm^4, respectively, for 200 < E_\\gamma < 800 MeV.']",['2001-06-01']
134,['eng'],"['Davies, G J']",['Standard Model Higgs Search in the Four Jet Channel at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, hadronic decay', 'Z0, hadronic decay', 'final state, (4jet)', 'particle identification, beauty', 'Higgs particle, mass', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'Higgs particle --> 2beauty', 'Z0 --> quark antiquark', '200-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105088'],"['The Standard Model Higgs boson was searched for at LEP, by the four collaborations in the year 2000, at centre-of-mass energies from 200-209GeV. An excess of events, potentially compatible with the production of a Higgs boson of mass ~115GeV was observed, largely in the four-jet channel. The search in this channel is discussed in this letter.']",['2001-06-01']
135,['eng'],"['Bakari, D', 'Becherini, Y', 'Spurio, M']",['Estimate of the Energy of Upgoing Muons with Multiple Coulomb Scattering'],['Particle Physics - Experimental Results'],"['talk, Oujda 2001/03/21', 'neutrino/mu, cosmic radiation', 'neutrino nucleus, interaction', 'charged current', 'muon, angular distribution', 'muon, energy spectrum', 'multiple scattering, Coulomb', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, MACRO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105087'],"['Upward throughgoing muons in underground detectors are induced by atmospheric $\\nu_\\mu$ with energies in the $1-10^4 GeV$ range. The oscillations of atmospheric muon neutrinos should affect mainly those with energy smaller than $E_\\nu \\sim 50 GeV$, or $E_\\mu \\le 10 GeV$ . We analyzed the MACRO upward throughgoing muons data set, using the Multiple Coulomb Scattering to estimate the energy $E_\\mu$ of muons crossing the detector. We analyzed the event distribution for six event subsamples with different values of $<\\ell_\\nu / E_\\nu>$. The event distribution is in agreement with the hypothesis of neutrino oscillations with $\\Delta m^2$ few times $10^{-3} eV^2$ and maximum mixing.']",['2001-05-31']
136,['eng'],"['Gritsan, A']",['Search for the Decay B+ -> D*+ K0_S'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B+, hadronic decay', 'B+, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B+ --> D*(2010) K0(S)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105086'],['We report on a search for the decay B+ -> D*+ K0_S and its charge conjugate with the CLEO detector at the Cornell Electron Storage Ring (CESR). No candidates are found in 9.10/fb of data. The background is estimated to be 0.29 +- 0.05 leading to an upper limit BF(B+ -> D*+ K0_S) = 9.5 x 10^{-5} (90% C.L.).'],['2001-05-31']
137,['eng'],"['Neganov, B S', 'Trofimov, V N', 'Yukhimchuk, A A', 'Bogdanova, L N', 'Beda, A G', 'Starostin, A S']",['Status of the Experiment on the Laboratory Search for the Electron Antineutrino Magnetic Moment at the Level mu_nu < 3 s 10^{-12}mu_B'],['Particle Physics - Experimental Results'],"['antineutrino/e, magnetic moment', 'tritium, semileptonic decay', 'antineutrino electron, elastic scattering', 'weak interaction', 'electromagnetic interaction', 'spectrometer, proposed', 'semiconductor detector', 'silicon', 'germanium', 'threshold', 'deep underground detector', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105083'],"['The experiment on the direct detection of antineutrino-electron scattering with an artificial tritium source allows to lower the present-day laboratory limit for the neutrino magnetic moment by two orders of magnitude. The experiment brings together novel unique technologies in studies of rare processes of neutrino-electron scattering: an artificial source of antineutrinos from tritium decay of 40 MCi activity with the antineutrino flux density ~6 10^{14}cm^{-2} s^{-1}; new types of detectors capable of detecting electrons with energy down to ~10 eV, namely, a silicon cryogenic detector based on the ionization-into-heat conversion effect, a high purity germanium detector with the internal amplification of a signal in the electric field. A compact installation located in a specially equipped laboratory underground <100 m w.e.) will provide favorable background conditions for running the experiment. With the background level about 0.1 events/kg keV day and detector assembly masses 3kg and 5kg for the silicon and germanium ones, respectively, the limit for the electron antineutrino magnetic moment mu_nu < 3 10^{-12}mu_B will be obtained during 1-2 years of data acquisition. Status of the experiment and state-of-the-art are presented.']",['2001-05-29']
138,['eng'],"['Miyake, S']",['Discussion on the nucleon decay experiments'],['Particle Physics - Experimental Results'],"['p, decay', 'p, lifetime', 'lower limit', 'background', 'Cherenkov counter, water', 'deep underground detector, experimental results', 'p --> K0(S) positron', 'p --> pi+ antineutrino', 'p --> K+ antineutrino', 'p --> meson lepton+']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105081'],"['The results of KGF experiments are compared with the results of Soudan 2 and Frejus experiments and reasonable agreements are obtained. Nevertheless, the results of Super-Kamiokande (SK) are somewhat different from the other experiments and some points in SK are discussed.']",['2001-05-29']
139,['eng'],"['Riemann, S']",['Search for exotic physics with four-fermion coupling at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'quark, pair production', 'new particle, search for', 'new interaction, search for', ""Z', exchange"", 'leptoquark, exchange', 'four-fermion interaction', 'channel cross section', 'angular distribution, asymmetry', 'space-time, higher-dimensional', 'experimental results', 'CERN LEP Stor', 'electron positron --> fermion antifermion', '130-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105079'],"[""Preliminary results of measurements of fermion-pair production at LEP2 are used to derive limits on new physics phenomena. Combinations of the cross sections and asymmetrie of the 4 LEP collaborations are interpreted in terms four-fermion contact interactions, exchange of Z' and leptoquarks. Results on the search for extra dimensions are also presented.""]",['2001-05-28']
140,['eng'],"['Kcira, D']",['Real and Virtual Photon Structure at HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon, structure function', 'photon, on-shell', 'photon, off-shell', 'jet, pair production', 'differential cross section, momentum dependence', 'transverse energy, dependence', 'momentum transfer, dependence', 'quark, momentum spectrum', 'gluon, momentum spectrum', 'parametrization', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105078'],"[""The structure of real and virtual photons has been studied in ep collisions at HERA using dijet production. Measurements of differential dijet cross sections as function of the fraction of photon's momentum invested in the dijet system are presented. The dependence of the cross sections on the virtuality of the photon and mean transverse energy squared of the two leading jets has been investigated. QCD calculations based on current parametrizations of the real and virtual photon parton distribution functions have been compared to the data.""]",['2001-05-28']
141,['eng'],"['Strom, D']",['Electroweak Measurements on the Z Resonance'],['Particle Physics - Experimental Results'],"['review, Carmel 2000/09/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, width', 'Z0, mass', 'electroweak interaction, validity test', 'cross section, hadronic', 'angular distribution, asymmetry', 'strong interaction, coupling constant', 'quantum electrodynamics, coupling constant', 'quantum chromodynamics, correction', 'Weinberg angle', 'vacuum polarization, hadronic', 'polarization, asymmetry', 'Higgs particle, mass', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'bibliography', 'approx. 91 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105076', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']","['Almost all precision electroweak measurements from the Z resonance made at the LEP storage ring by the ALEPH, DELPHI, L3 and OPAL experiments and those made using a polarized electron beam at the SLC by the SLD experiment are now final and have been published. Changes in the measurements since the last RADCOR meeting are discussed. The internal consistency of the measurements is considered. The impact of remaining theoretical uncertainties in the QCD sector are examined as well as the impact of experimental and theoretical uncertainties on the value of $\\alpha_{\\mathrm{QED}}(m_{\\mathrm{Z}})$.']",['2001-09-14']
142,['eng'],"['Huang, G S']",['R Measurement at BES'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'cross section, hadronic', 'energy dependence', 'vacuum polarization, hadronic', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', '2-5 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105074'],"['The values of $R = \\sigma(e^+e^-\\to {hadrons})/\\sigma(e^+e^-\\to\\mu^+\\mu^-)$ for 85 center-of-mass energies between 2 and 5 GeV were measured with the upgraded Beijing Spectrometer at the Beijing Electron-Positron Collider, with an average uncertainty of $\\sim7%$.']",['2001-05-25']
143,['eng'],"['Abazov, V M']",['Search for First-Generation Scalar and Vector Leptoquarks'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'leptoquark, search for', 'leptoquark, scalar', 'leptoquark, vector', 'leptoquark, pair production', 'leptoquark, decay modes', 'leptoquark, mass', 'lower limit', 'channel cross section, mass', 'upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', 'anti-p p --> 2leptoquark anything', 'leptoquark --> quark electron', 'leptoquark --> quark neutrino', 'anti-p p --> 2jet positron electron anything', 'anti-p p --> 2jet electron neutrino anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105072'],"['We describe a search for the pair production of first-generation scalar and vector leptoquarks in the eejj and enujj channels by the D0 Collaboration. The data are from the 1992--1996 ppbar run at sqrt{s} = 1.8 TeV at the Fermilab Tevatron collider. We find no evidence for leptoquark production; in addition, no kinematically interesting events are observed using relaxed selection criteria. The results from the eejj and enujj channels are combined with those from a previous D0 analysis of the nunujj channel to obtain 95% confidence level (C.L.) upper limits on the leptoquark pair-production cross section as a function of mass and of beta, the branching fraction to a charged lepton. These limits are compared to next-to-leading-order theory to set 95% C.L. lower limits on the mass of a first-generation scalar leptoquark of 225, 204, and 79 GeV/c^2 for beta=1, 1/2, and 0, respectively. For vector leptoquarks with gauge (Yang-Mills) couplings, 95% C.L. lower limits of 345, 337, and 206 GeV/c^2 are set on the mass for beta=1, 1/2, and 0, respectively. Mass limits for vector leptoquarks are also set for anomalous vector couplings.']",['2001-09-14']
144,['eng'],"['Edwards, K W']",['First Observation of B0bar -> D*0 pi+ pi+ pi- pi- Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'anti-B0, hadronic decay', 'anti-B0, branching ratio', 'D*(2010)', 'factorization, validity test', 'mass spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'anti-B0 --> D*(2010) 2pi+ 2pi-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105071'],"['We report on the observation of B0bar -> D*0 pi+ pi+ pi- pi- decays. The branching ratio is (0.30 +/- 0.07 +/- 0.06)%. Interest in this particular mode was sparked by Ligeti, Luke and Wise who propose it as a way to check the validity of factorization tests in B0bar -> D*+ pi+ pi- pi- pi0 decays.']",['2001-05-24']
145,['eng'],"['Dissertori, G']",['Experimental status of measurements of $\\alpha_s$ at LEP'],['Particle Physics - Experimental Results'],"['review, Rome 2001/04/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, decay modes', 'Z0, branching ratio', 'tau, pair production', 'tau, decay modes', 'tau, branching ratio', 'strong interaction, coupling constant', 'energy dependence', 'jet, electroproduction', 'event shape analysis', 'quantum chromodynamics, perturbation theory', 'correction, nonperturbative', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105070'],['A summary is given of the current status of measurements of the strong coupling constant $\\alpha_s$ performed at LEP. These include measurements from inclusive observables as well as from event shape variables. Recent results based on power law corrections are discussed.'],['2001-05-24']
146,['eng'],"['Krane, J']","['Latest Jet Results from the Tevatron or, QCD']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'anti-p p, colliding beams', 'jet, hadroproduction', 'jet, multiplicity', 'event shape analysis', 'quantum chromodynamics', 'momentum spectrum, parton', 'cross section', 'transverse energy, dependence', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105069'],"['This article summarizes several analyses I discussed at Moriond and I attempt to maintain my speaking voice throughout. I extract several broad themes in the recent development of QCD,and emphasize how the latest results on jet physics reinforce these themes: that QCD is in a transitional stage from providing qualitative descriptions to providing true quantitative descriptions of the results. Certain figures presented in the talk are not reproduced here in the interest of space, but can be found directly in the transparencies available online, or in the references to the refereed journals.']",['2001-05-24']
147,['eng'],"['Auerbach, L B', 'Burman, R L', 'Caldwell, D O', 'Church, E D', 'Donahue, J B', 'Fazely, A', 'Garvey, G T', 'Gunasingha, R M', 'Imlay, R', 'Louis, W C', 'Majkic, R', 'Malik, A', 'Metcalf, W', 'Mills, G B', 'Sandberg, V D', 'Smith, D', 'Stancu, I', 'Sung, M', 'Tayloe, R', 'VanDalen, G J', 'Vernon, W', 'Wadia, N', 'White, D H', 'Yellin, S']",['Measurements of Charged Current Reactions of $\\nu_e$ on $^{12}C$'],['Particle Physics - Experimental Results'],"['neutrino nucleus, nuclear reaction', 'neutrino/e', 'carbon', 'nitrogen, energy levels', 'charged current', 'channel cross section', 'electron, energy spectrum', 'angular distribution', 'scintillation counter, liquid', 'experimental results', 'LAMPF Linac', 'neutrino/e carbon-12 --> nitrogen-12 electro']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105068'],"['Charged Current reactions of $\\nu_e$ on $^{12}C$ have been studied using a $\\mu^+$ decay-at-rest $\\nu_e$ beam at the Los Alamos Neutron Science Center. The cross section for the exclusive reaction $^{12}C(\\nu_e,e^-)^{12}N_{g.s.}$ was measured to be $(8.9\\pm0.3\\pm0.9)\\times10^{-42}$ cm$^2$. The observed energy dependence of the cross section and angular distribution of the outgoing electron agree well with theoretical expectations. Measurements are also presented for inclusive transitions to $^{12}N$ excited states, $^{12}C(\\nu_e,e^-)^{12}N^*$ and compared with theoretical expectations. The measured cross section, $(4.5\\pm0.4\\pm0.6)\\times10^{-42}$ cm$^2$, is somewhat lower than previous measurements and than a continuum random phase approximation calculation. It is in better agreement with a recent shell model calculation.']",['2001-09-14']
148,['eng'],"['Bodek, Arie', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bolton, T', 'Brau, J E', 'Buchholz, D']",['Extraction of R=sigma_L/sigma_T from CCFR Neutrino and Antinetrino Differential Cross Sections'],['Particle Physics - Experimental Results'],"['talk, Bologna 2001/04/27', 'neutrino nucleus, interaction', 'antineutrino nucleus, interaction', 'neutrino/mu', 'iron', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'nucleon, structure function', 'momentum spectrum, parton', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105067'],['We report on the extraction of R=sigam_L/sigma_T from CCFR neutrino and antineutrino-Iron differential cross sections. R as measured in neutrno scattering is in agreement with $R$ as measured in muon and electron scattering. All data on R for Q2 > 1 GeV2 are in agreement with a NNLO QCD calculation which uses NNLO PDFs and includes target mass effects. We report on the first measurements of R in the low x and Q2 < 1 GeV2 region (where an anomalous large rise in R for nuclear targets has been observed by the HERMES collaboration).'],['2001-05-23']
149,['eng'],"['Affolder, T']",['Search for Narrow Diphoton Resonances and for gamma-gamma+W/Z Signatures in p\\bar p Collisions at sqrt(s)=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'narrow resonance, search for', 'photon, pair production', 'intermediate boson, associated production', 'mass spectrum, two-photon', 'channel cross section, branching ratio', 'upper limit', 'supersymmetry, symmetry breaking', 'sparticle, Goldstino', 'Higgs particle, radiative decay', 'Higgs particle, mass', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'anti-p p --> 2photon anything', 'anti-p p --> W 2photon anything', 'anti-p p --> Z0 2photon anything', 'Higgs particle --> 2photon', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105066'],"[""We present results of searches for diphoton resonances produced both inclusively and also in association with a vector boson (W or Z) using 100 pb^{-1} of p\\bar p collisions using the CDF detector. We set upper limits on the product of cross section times branching ratio for both p\\bar p\\to\\gamma\\gamma + X and p\\bar p\\to\\gamma\\gamma + W/Z. Comparing the inclusive production to the expectations from heavy sgoldstinos we derive limits on the supersymmetry-breaking scale sqrt{F} in the TeV range, depending on the sgoldstino mass and the choice of other parameters. Also, using a NLO prediction for the associated production of a Higgs boson with a W or Z boson, we set an upper limit on the branching ratio for H\\to\\gamma\\gamma. Finally, we set a lower limit on the mass of a `bosophilic' Higgs boson (e.g. one which couples only to \\gamma, W, and Z$ bosons with standard model couplings) of 82 GeV/c^2 at 95% confidence level.""]",['2001-05-23']
150,['eng'],"['Karlen, D A', 'Burkhardt, H']",['Investigation of vacuum polarization in t-channel radiative Bhabha scattering'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, elastic scattering', 'photon, radiation', 'vacuum polarization', 'fundamental constant, fine structure', 'electroweak interaction, validity test', 'numerical calculations', 'magnetic detector, BaBar', 'SLAC PEP Stor', 'magnetic detector, OPAL', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105065'],"['We discuss the possibility of a precision measurement of vacuum polarization in t-channel radiative Bhabha scattering at a high luminosity collider. For illustration, the achievable precision is estimated for the BaBar experiment at PEP-II and for the OPAL experiment at LEP.']",['2001-05-23']
151,['eng'],"['Musy, M']",['Quartic and neutral IVB couplings at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'Z0, electroproduction', 'neutrino, pair production', 'photon, associated production', 'coupling, (4gauge boson)', 'channel cross section, energy dependence', 'electroweak interaction, validity test', 'magnetic detector, ALEPH', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W- photon', 'electron positron --> neutrino antineutrino 2photon', 'electron positron --> Z0 2photon', '130-208 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105063'],['The study of charged and neutral boson vertices has been performed in different production channels at the LEP experiments. Decay rates and kinematic properties of these events are exploited to set constraints on the corresponding gauge couplings.'],['2001-05-23']
152,['eng'],"['Rosca, A']",['Search for non-SM Higgses at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, multiplet', 'doublet, 2', 'Higgs particle, pair production', 'Higgs particle, decay modes', 'supersymmetry', 'Higgs particle, mass', 'lower limit', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'electron positron --> 2Higgs particle', 'Higgs particle --> quark antiquark', 'Higgs particle --> 2photon', 'Higgs particle --> tau neutrino/tau', 'Higgs particle --> W Higgs particle', 'Higgs particle --> 2Higgs particle', 'Higgs particle --> W+ W-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105062'],"['The four LEP experiments, ALEPH, DELPHI, L3 and OPAL, have searched for Higgs bosons predicted by a large number of extensions of the Standard Model. Flavor independent searches are presented for the h$^{0}$Z$^{0}$ process in which the h$^{0}$ decays hadronically. Search results are also presented for fermiophobic Higgs bosons, invisibly decaying Higgs bosons, charged Higgs bosons and the neutral Higgs bosons in the MSSM.']",['2001-05-23']
153,['eng'],"['Mandelkern, M']",['Luminosity Measurement at PEP-N'],['Particle Physics - Experimental Results'],"['talk, Stanford 2001/04/30', 'electron positron, storage ring', 'beam monitoring, luminosity', 'electron positron, elastic scattering', 'bremsstrahlung', 'Cherenkov counter', 'SLAC PEP Stor']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105060', 'http://www.slac.stanford.edu/econf/C010430/t14.html']","['The PEP-N experiment requires a fast on-line luminosity monitor of modest accuracy plus an off-line method of determining integrated luminosity with accuracy of 0.01 for each pb$^{-1}$. We propose the PEP-2 monitor, based on observing single bremsstrahlung at zero degrees to the positron direction at collision for the former and the use of Bhabha scatters at polar angles $>$.03 radians for the latter requirement.']",['2001-09-14']
154,['eng'],"['Fernández, P A M', 'Bethke, Siegfried', 'Biebel, O', 'Kluth, S']",['Tests of Power Corrections for Event Shapes in e+e- Annihilation'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'hadron, multiple production', 'event shape analysis', 'quantum chromodynamics, perturbation theory', 'effect, hadronization', 'correction, nonperturbative', 'parametrization', 'strong interaction, coupling constant', 'energy dependence', 'numerical calculations, interpretation of experiments', '14-189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105059'],"['A study of perturbative QCD calculations combined with power corrections to model hadronisation effects is presented. The QCD predictions are fitted to differential distributions and mean values of event shape observables measured in e+e- annihilation at centre-of-mass energies from 14 to 189 GeV. We investigate the event shape observables thrust, heavy jet mass, C-parameter, total and wide jet broadening and differential 2-jet rate and observe a good description of the data by the QCD predictions. The strong coupling constant alpha_S(M_Z) and the free parameter of the power correction calculations alpha_0(2 GeV) are measured to be alpha_S(M_Z) = 0.1171 +/- 0.0032/0.0020 and alpha_0(2 GeV) = 0.513 +/- 0.066/0.045. The predicted universality of alpha_0 is confirmed within the uncertainties of the measurements.']",['2001-05-22']
155,['eng'],"['De Groot, N']",['SLD electroweak physics results'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, charm', 'quark, beauty', 'Z0, branching ratio', 'asymmetry', 'track data analysis, charge', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105058'],"['In this paper we present three updates to heavy flavour results from the SLD detector at SLAC. These results are preliminary, based on our full 1993-1998 dataset of 550 000 hadronic Z0 decays produced with an average electron polarisation of 73%. The new measurements are of the hadronic branching fractions into heavy quarks (Rb, Rc), the b quark asymmetry (Ab) using jet charge, and the heavy quark asymmetries (Ab and Ac) using vertex charge and kaons.']",['2001-05-22']
156,['eng'],"['García-Abia, P']",['Search for charged Higgs bosons in L3'],['Particle Physics - Experimental Results'],"['talk, Rome 2001/04/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, pair production', 'Higgs particle, hadronic decay', 'Higgs particle, leptonic decay', 'Higgs particle, mass', 'lower limit', 'mass spectrum', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2Higgs particle', 'Higgs particle --> charm strangeness', 'Higgs particle --> tau neutrino/tau', '200-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105057'],"['A search for pair-produced charged Higgs bosons is performed with the L3 detector at LEP using data collected at centre-of-mass energies between 200 and 209 GeV, corresponding to an integrated luminosity of 217.8 pb^-1. We observe an excess of events in the H+-H -> cscs and cs\\tau\\nu channels in the mass region around 68 GeV, which is most significant at low values of the H+ -> \\tau\\nu branching ratio. Including data taken at lower centre-of-mass energies, the excess is compatible with a 4.4\\sigma fluctuation in the background. Interpreting this excess as a statistical fluctuation in the background, lower limits on the charged Higgs mass are derived at the 95% confidence level. They vary from 67.1 to 84.9 GeV as a function of the H+ -> \\tau\\nu branching ratio. These results are PRELIMINARY.']",['2001-05-22']
157,['eng'],"['Braibant-Giacomelli, S']",['Other searches at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'sparticle, decay', 'neutralino, LSP', 'supersymmetry, symmetry breaking', 'R parity, violation', 'gravitino, LSP', 'technicolor', 'lepton, excited state', 'leptoquark', 'experimental results', 'CERN LEP Stor', '209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105056'],"['During the year 2000, LEP has been operated at centre-of-mass energies up to sqrt(s) = 209 GeV. New particle searches have been performed using these data samples. Model independent limits on the production cross-sections and mass limits in the context of the Minimal Supersymmetric Standard Model (MSSM) assuming R-parity violation and in the context of gauge-mediated supersymmetry breaking theories (GMSB) are presented. Searches for technicolor, excited leptons and leptoquarks are also reviewed.']",['2001-09-14']
158,['eng'],"['Lourenço, C']",['Searching for Quark Matter at the CERN SPS'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 2001/01/15', 'p nucleus, nuclear reaction', 'beryllium', 'scattering, heavy ion', 'lead', 'quark, matter', 'quark gluon, plasma', 'production, strangeness', 'production, charm', 'J/psi(3100), yield', 'dependence, impact parameter', 'lepton, pair production', 'critical phenomena', 'symmetry, chiral', 'experimental results', 'CERN SPS', '< 158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105053'],"['This article gives a brief overview of some recent advances in our understanding of the physics of dense strongly interacting matter, from measurements done at the CERN SPS. The presently available results are very interesting, and are likely to reflect the production of a new state of matter in central Pb-Pb collisions, at the highest SPS energies. However, important questions require further work. Particular emphasis is given to developments made since the Quark Matter 1999 conference, and to issues that justify the continuation of the SPS heavy ion physics program beyond year 2000.']",['2001-05-21']
159,['eng'],"['Faccini, R']",['New results on sin 2beta & BBbar mixing from BaBar'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, branching ratio', 'rho(770)', 'a1(1260)', 'J/psi(3100)', 'psi(3685)', 'Kobayashi-Maskawa angle, unitarity', 'B+, lifetime', 'B0, lifetime', 'lifetime, ratio', 'B0 anti-B0, oscillation', 'time dependence', 'violation, CP', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> psi mesons K', 'B --> charmed meson pi', 'B --> charmed meson rho(770)', 'B --> charmed meson a1(1260)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105051'],"['The BABAR detector, which operates at the SLAC PEPII asymmetric e+e- collider at energies near the Y(4S) resonance has collected about 23M B-anti-B pairs in year 2000. Based on this data sample, we present the first study of sin(2b), with samples of B^0 --> J/psi K0S, B^0 --> psi(2S) K0S and B^0 --> J/psi K0L decays. The measured value is 0.34+-0.20+-0.05. In addition, we present preliminary measurements of charged and neutral B meson lifetimes and B^0-anti-B^0 oscillation frequency.']",['2001-05-21']
160,['eng'],"['Elia, D']",['Results on cascade production in lead-lead interactions from the NA57 experiment'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'p nucleus, nuclear reaction', 'scattering, heavy ion', 'lead', 'hadron, multiple production', 'production, strangeness', 'Xi-, hadronic decay', 'yield, (Xi- Antixi-)', 'central region', 'dependence, impact parameter', 'mass spectrum, (Lambda pi)', 'mass spectrum, transverse', 'transverse momentum, rapidity dependence', 'experimental results', 'CERN SPS', '40, 160 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105049'],"['The NA57 experiment has been designed to study the production of strange and multi-strange particles in Pb-Pb and p-Be collisions at the CERN SPS. The predecessor experiment WA97 has measured an enhanced abundance of strange particles in Pb-Pb collisions relative to p-A reactions at 160 GeV/c per nucleon beam momentum. NA57 has extended the WA97 measurements to investigate the evolution of the strangeness enhancement pattern as a function of the beam energy and over a wider centrality range. In this paper, we report results on cascade production for about the 60% most central collisions at 160 GeV/c per nucleon.']",['2001-05-21']
161,['eng'],"['Astier, P', 'Autiero, D', 'Baldisseri, A', 'Baldo-Ceolin, Massimilla', 'Banner, M', 'Bassompierre, Gabriel', 'Besson, N', 'Bird, I', 'Blumenfeld, B', 'Bobisut, F', 'Bouchez, J', 'Boyd, S', 'Bueno, A G', 'Bunyatov, S A', 'Camilleri, L L', 'Cardini, A', 'Cattaneo, Paolo Walter', 'Cavasinni, V', 'Cervera-Villanueva, A', 'Chukanov, A', 'Collazuol, G', 'Conforto, G', 'Conta, C', 'Contalbrigo, M', 'Cousins, R D', 'Daniels, D C', 'Degaudenzi, H M', 'Del Prete, T', 'De Santo, A', 'Dignan, T', 'Di Lella, Luigi', 'do Couto e Silva, E', 'Dumarchez, J', 'Ellis, M', 'Fazio, T', 'Feldman, G J', 'Ferrari, R', 'Ferrère, D', 'Flaminio, Vincenzo', 'Fraternali, M', 'Gaillard, Jean-Marc', 'Gangler, E', 'Geiser, A', 'Geppert, D', 'Gibin, D', 'Gninenko, S N', 'Godley, A', 'Gómez-Cadenas, J J', 'Gosset, J', 'Gössling, C', 'Gouanère, M', 'Grant, A', 'Graziani, G', 'Guglielmi, A M', 'Hagner, C', 'Hernando, J', 'Hubbard, D', 'Hurst, P', 'Hyett, N', 'Iacopini, E', 'Joseph, C L', 'Juget, F R', 'Kirsanov, M M', 'Klimov, O L', 'Kokkonen, J', 'Kovzelev, A', 'Krasnoperov, A V', 'Kustov, D V', 'Kuznetsov, V E', 'Lacaprara, S', 'Lachaud, C', 'Lakic, B', 'Lanza, A', 'La Rotonda, L', 'Laveder, M', 'Letessier-Selvon, A A', 'Lévy, J M', 'Linssen, L', 'Ljubicic, A', 'Long, J', 'Lupi, A', 'Marchionni, A', 'Martelli, F', 'Méchain, X', 'Mendiburu, J P', 'Meyer, J P', 'Mezzetto, M', 'Mishra, S R', 'Moorhead, G F', 'Naumov, D', 'Nédélec, P', 'Nefedov, Yu', 'Nguyen-Mau, C', 'Orestano, D', 'Pastore, F', 'Peak, L S', 'Pennacchio, E', 'Pessard, H', 'Petti, R', 'Placci, Alfredo', 'Polesello, G', 'Pollmann, D', 'Polyarush, A Yu', 'Popov, B', 'Poulsen, C', 'Rico, J', 'Riemann, P', 'Roda, C', 'Rubbia, André', 'Salvatore, F', 'Schahmaneche, K', 'Schmidt, B', 'Schmidt, T', 'Sevior, M E', 'Sillou, D', 'Soler, F J P', 'Sozzi, G', 'Steele, D', 'Stiegler, U', 'Stipcevic, M', 'Stolarczyk, T', 'Tareb-Reyes, M', 'Taylor, G N', 'Tereshchenko, V V', 'Toropin, A N', 'Touchard, A M', 'Tovey, S N', 'Tran, M T', 'Tsesmelis, Emmanuel', 'Ulrichs, J', 'Vacavant, L', 'Valdata-Nappi, M', 'Valuev, V Yu', 'Vannucci, François', 'Varvell, K E', 'Veltri, M', 'Vercesi, V', 'Vidal-Sitjes, G', 'Vieira, J M', 'Vinogradova, T G', 'Weber, F V', 'Weisse, T', 'Wilson, F F', 'Winton, L J', 'Yabsley, B D', 'Zaccone, H', 'Zuber, K', 'Zuccon, P']",['A study of backward going $p$ and $\\pi^{-}$ in $\\nu_{\\mu}CC$ interactions with the NOMAD detector'],['Particle Physics - Experimental Results'],"['neutrino nucleus, inclusive reaction', 'neutrino/mu', 'carbon', 'charged current', 'pi-, neutrinoproduction', 'p, neutrinoproduction', 'wide-angle', 'momentum spectrum', 'yield, (p pi-)', 'differential cross section, slope', 'energy dependence', 'angular dependence', 'momentum dependence', 'multiple scattering', 'multiplicity', 'correlation, short-range', 'drift chamber, target', 'magnetic detector, experimental results', 'CERN SPS']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ep-2001-038', 'http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105048']","['Backward proton and $\\pi^-$ production has been studied in \\numucc interactions with carbon nuclei. Detailed analyses of the momentum distributions, of the production rates, and of the general features of events with a backward going particle, have been carried out in order to understand the mechanism producing these particles. The backward proton data have been compared with the predictions of the reinteraction and the short range correlation models.']",['2001-06-07']
162,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Albrecht, Z', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amapane, N', 'Amato, S', 'Anashkin, E', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Anjos, N', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Ballestrero, A', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Behrmann, A', 'Bellunato, T F', 'Belokopytov, Yu A', 'Belous, K S', 'Benekos, N C', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Berntzon, L', 'Bertrand, D', 'Besançon, M', 'Besson, N', 'Bilenky, S M', 'Bloch, D', 'Blom, H M', 'Bol, J', 'Bonesini, M', 'Boonekamp, M', 'Booth, P S L', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Bracko, M', 'Branchini, P', 'Brenner, R A', 'Brodet, E', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buschmann, P', 'Caccia, M', 'Calvi, M', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Cattai, A', 'Cavallo, F R', 'Chapkin, M M', 'Charpentier, P', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Shlyapnikov, P', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Chung, S H', 'Cieslik, K', 'Collins, P', 'Contri, R', 'Cosme, G', 'Cossutti, F', 'Costa, M', 'Crawley, H B', 'Crennell, D J', 'Croix, J', 'Cuevas-Maestro, J', 'Czellar, S', ""D'Hondt, J"", 'Dalmau, J', 'Davenport, M', 'Da Silva, W', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Espirito-Santo, M C', 'Fanourakis, G K', 'Fassouliotis, D', 'Feindt, Michael', 'Fernández, J', 'Ferrer, A', 'Ferrer-Ribas, E', 'Ferro, F', 'Firestone, A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Geralis, T', 'Ghodbane, N', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Grosdidier, G', 'Grzelak, K', 'Guy, J', 'Haag, C', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hajduk, Z', 'Hallgren, A', 'Hamacher, K', 'Hamilton, K', 'Hansen, J', 'Harris, F J', 'Haug, S', 'Hauler, F', 'Hedberg, V', 'Heising, S', 'Herquet, P', 'Herr, H', 'Hertz, O', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Hughes, G J', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Jeans, D', 'Johansson, E K', 'Jonsson, P', 'Joram, Christian.', 'Juillot, P', 'Jungermann, L', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kernel, G', 'Kersevan, B P', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kinvig, A', 'Kjaer, N J', 'Klapp, O', 'Kluit, P M', 'Kokkinias, P', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kriznic, E', 'Krumshtein, Z', 'Kubinec, P', 'Kucewicz, W', 'Kucharczyk, M', 'Kurowska, J', 'Lamsa, J W', 'Laugier, J P', 'Leder, Gerhard', 'Ledroit, F', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lemonne, J', 'Lenzen, Georg', 'Lepeltier, V', 'Lethuillier, M', 'Libby, J', 'Liebig, W', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Maltezos, S', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'Merle, E', 'Meroni, C', 'Meyer, W T', 'Myagkov, A', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Moch, M', 'Mönig, K', 'Monge, M R', 'Montenegro, J F', 'Moraes, D', 'Morettini, P', 'Morton, G', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mundim, L M', 'Murray, W J', 'Myatt, Gerald', 'Myklebust, T', 'Nassiakou, M', 'Navarria, Francesco Luigi', 'Nawrocki, K', 'Negri, P', 'Némécek, S', 'Neufeld, N', 'Nicolaidou, R', 'Niezurawski, P', 'Nikolenko, M', 'Nomokonov, V P', 'Nygren, A', 'Oblakowska-Mucha, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Österberg, K', 'Ouraou, A', 'Oyanguren, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Peralta, L', 'Perepelitsa, V F', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Poireau, V', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Rehn, J', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Ripp-Baudot, I', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salmi, L', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Savoy-Navarro, Aurore', 'Schwanda, C', 'Schwemling, P', 'Schwering, B', 'Schwickerath, U', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Sekulin, R L', 'Sette, G', 'Shellard, R C', 'Siebel, M', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Smadja, G', 'Smirnov, N', 'Smirnova, O G', 'Smith, G R', 'Sokolov, A', 'Solovyanov, O', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Squarcia, S', 'Stanescu, C', 'Stanitzki, M', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Szumlak, T', 'Tabarelli de Fatis, T', 'Taffard, A', 'Tegenfeldt, F', 'Terranova, F', 'Timmermans, J', 'Tinti, N', 'Tkatchev, L G', 'Tobin, M', 'Todorova-Nová, S', 'Tomé, B', 'Tortora, L', 'Tortosa, P', 'Treille, D', 'Tristram, G', 'Trochimczuk, M', 'Troncon, C', 'Turluer, M L', 'Tyapkin, I A', 'Tyapkin, P', 'Tzamarias, S', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'Van der Velde, C', 'van Dam, P', 'Van den Boeck, W', 'Van Doninck, W K', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Remortel, N', 'Van Vulpen, I B', 'Vegni, G', 'Ventura, L', 'Venus, W', 'Verbeure, F', 'Verdier, P', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Washbrook, A J', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zinchenko, A I', 'Zoller, P', 'Zumerle, G', 'Zupan, M']",['A Measurement of the Tau Topological Branching Ratios'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, pair production', 'tau-, semileptonic decay', 'tau-, branching ratio', 'particle identification, (K pi)', 'charged particle, multiplicity', 'neutral particle, multiplicity', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105047'],"['Using data collected in the DELPHI detector at LEP-1, measurements of the inclusive tau branching ratios for decay modes containing one, three, or five charged particles have been performed, giving the following results: B_1 = B(\\tau^- -> (particle)^- \\geq 0pi^0 \\geq 0K^0 \\nu_\\tau(\\bar{\\nu})) = (85.316 +/- 0.093 +/- 0.049)%; B_3 = B(\\tau^- -> 2h^-h^+ \\geq 0pi^0 \\geq 0K^0 \\nu_\\tau) = (14.569 +/- 0.093 +/- 0.048)%; B_5 = B(\\tau^- -> 3h^-2h^+ \\geq 0pi^0 \\geq 0K^0 \\nu_\\tau) = (0.115 +/- 0.013 +/- 0.006)%, where h is either a charged pi or K meson. The first quoted uncertainties are statistical and the second systematic.']",['2001-05-21']
163,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Etzion, E', 'Fabbri, F', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kramer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Moed, S', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rozen, Y', 'Runge, K', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Ujvári, B', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Determination of the b Quark Mass at the Z Mass Scale'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'mass, beauty', 'yield, (3jet)', 'jet, particle identification', 'dependence, flavor', 'energy dependence', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tables', 'bibliography', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105046'],"['In hadronic decays of Z bosons recorded with the OPAL detector at LEP, events containing b quarks were selected using the long lifetime of b flavoured hadrons. Comparing the 3-jet rate in b events with that in d u,s and c quark events, a significant difference was observed. Using Order(alpha_s squared) calculations for massive quarks, this difference was used to determine the b quark mass in the MSbar renormalisation scheme at the scale of the Z boson mass. By combining the results from seven different jet finders the running b quark mass was determined to be mb(MZ) = (2.67 +/- 0.03(stat) +0.29/-0.37(syst) +/- 0.19(theo.)) GeV. Evolving this value to the b quark mass scale itself yields mb(mb) = (3.95 +0.52/-0.62) GeV, consistent with results obtained at the b quark production threshold. This determination confirms the QCD expectation of a scale dependent quark mass. A constant mass is ruled out by 3.9 standard deviations.']",['2001-09-14']
164,['eng'],"['Holzner, A G']",['Charged Higgs at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, charged particle', 'Higgs particle, pair production', 'Higgs particle, decay modes', 'Higgs particle, mass', 'lower limit', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2Higgs particle', 'Higgs particle --> tau neutrino/tau', 'Higgs particle --> charm strangeness', '183-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105045'],"['The four LEP experiments Aleph, Delphi, L3 and Opal updated their searches for pair production of charged Higgs bosons using more than 210/pb luminosity collected per experiment in the year 2000. Combining it with previously collected data, a significant deviation from background (equivalent to 4.4 sigma) is found by the L3 collaboration for low values of the branching ratio H+/- -> tau nu around masses of about 68 GeV. This excess is however not seen by the other LEP collaborations and thus a lower limit on the charged Higgs mass is set at 78.5 GeV at 95% confidence level. All results reported here are still preliminary.']",['2001-05-18']
165,['eng'],[],['The BABAR Detector'],['Particle Physics - Experimental Results'],"['electron positron, colliding beam detector', 'semiconductor detector, vertex', 'drift chamber, wire', 'scintillation counter, crystal', 'cesium, iodine', 'particle identification', 'drift chamber, gas', 'electrode, impedance', 'tracks, energy loss', 'Cherenkov counter, ring imaging', 'trigger', 'data acquisition', 'electronics', 'programming', 'magnetic detector, BaBar', 'SLAC PEP Stor', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105044'],"['BABAR, the detector for the SLAC PEP-II asymmetric e+e- B Factory operating at the upsilon 4S resonance, was designed to allow comprehensive studies of CP-violation in B-meson decays. Charged particle tracks are measured in a multi-layer silicon vertex tracker surrounded by a cylindrical wire drift chamber. Electromagentic showers from electrons and photons are detected in an array of CsI crystals located just inside the solenoidal coil of a superconducting magnet. Muons and neutral hadrons are identified by arrays of resistive plate chambers inserted into gaps in the steel flux return of the magnet. Charged hadrons are identified by dE/dx measurements in the tracking detectors and in a ring-imaging Cherenkov detector surrounding the drift chamber. The trigger, data acquisition and data-monitoring systems, VME- and network-based, are controlled by custom-designed online software. Details of the layout and performance of the detector components and their associated electronics and software are presented.']",['2001-05-18']
166,['eng'],"['Roland, C']",['First Results from the PHOBOS Experiment at RHIC'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'nucleus nucleus, colliding beams', 'scattering, heavy ion', 'gold', 'hadron, multiple production', 'charged particle, multiplicity', 'energy dependence', 'dependence, impact parameter', 'angular distribution, anisotropy', 'quark gluon, plasma', 'yield, (particle antiparticle)', 'rapidity, density', 'potential, chemical', 'magnetic detector, PHOBOS', 'experimental results', 'Brookhaven RHIC Coll', '56, 130 GeV-cms/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105043'],"['PHOBOS is one of four experiments studying Au-Au collisions at RHIC. During the first running period RHIC provided Au+Au collisions at $\\sqrt{s_{_{NN}}}$ = 56 GeV and 130 GeV. The data collected during this period allowed us to study the energy and centrality dependence of particle production, the anisotropy of the final state azimuthal distribution and particle ratios at mid-rapidity.']",['2001-09-14']
167,['eng'],"['Sielaff, J']",['DONUT'],['Particle Physics - Experimental Results'],"['neutrino nucleus, interaction', 'neutrino/tau', 'charged current', 'tau, semileptonic decay', 'tau, leptonic decay', 'track data analysis', 'nuclear emulsion', 'spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105042'],['The DONUT collaboration has observed four events in a hybrid emulsion spectrometer consistent with tau neutrino charged-current interactions. The resulting tau lepton is identified by its decay into a single charged particle. The expected background of charm decays and secondary interactions is .34 +/- >.05 events. The probability that all tau neutrino candidates are due to background proceesses is 1.1 x 10-4.'],['2001-05-17']
168,['eng'],"['Church, M']",['Substantial Upgrades to Tevatron Luminosity'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'anti-p p, storage ring', 'luminosity, upgrade', 'proton synchrotron, booster', 'anti-p, particle source', 'energy, upgrade', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105041'],"['Over the next 6 years the CDF and D0 collaborations have the goal of collecting 15 fb-1 of data in collider Run II. This will require a number of ambitious upgrades to the Fermilab accelerator complex, some of which have been completed, some of which are currently being commissioned, and some of which are under development but have not yet been installed. This paper describes the major accelerator upgrades required to reach this Run II luminosity goal.']",['2001-05-17']
169,['eng'],"['Çuhadar-Dönszelmann, T']",['NA48'],['Particle Physics - Experimental Results'],"['talk', 'K0, rare decay', 'K0, radiative decay', 'K0, semileptonic decay', 'K0(S), secondary beam', 'K0(L), secondary beam', 'K0, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'CERN SPS', 'K0(S) --> 2photon', 'K0 --> pi+ pi- positron electron', 'K0(S) --> pi0 positron electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105040'],['Recent results on the kaon rare decays measured in NA48 experiment at CERN are presented.'],['2001-05-17']
170,['eng'],"['Landsberg, G L']",['Extra Dimensions and More'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, annihilation', 'electron p, elastic scattering', 'space-time, higher-dimensional', 'graviton, search for', 'numerical calculations, interpretation of experiments', 'CERN LEP Stor', 'DESY HERA Stor', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105039'],"['One of the most stimulating recent ideas in particle physics involves a possibility that our universe has additional compactified spatial dimensions, perhaps as large as 1 mm. In this review, we discuss the results of recent experimental searches for such large extra dimensions, as well as new developments in this field.']",['2001-05-17']
171,['eng'],"['Nesom, G']",['B Hadron Production and b-bbar Correlations in Z0 Decays at SLD'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'gluon, fragmentation', 'quark, beauty', 'quark, pair production', 'quark, fragmentation function', 'B anti-B, energy spectrum', 'moment', 'quark antiquark, correlation', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'gluon --> 2beauty', 'Z0 --> 2beauty', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105038'],"['We present results of three SLD analyses: our final determination of the rate of gluon splitting into b-bbar, an improved measurement of the inclusive b quark fragmentation function in Z0 decays, and a preliminary first measurement of the energy correlation between the two leading B hadrons in Z0 decays. Our results are obtained using hadronic \\z0decays produced in e+e- annihilations at the Stanford Linear Collider (SLC) between 1996 and 1998 and collected in the SLC Large Detector (SLD). In this period, we used an upgraded vertex detector with wide acceptance and excellent impact parameter resolution, thus improving considerably our tagging capability for low-energy B hadrons.']",['2001-09-14']
172,['eng'],"['Kang, H']","['Production of pi^+-, K^+-, p and p-bar in Quark, Antiquark and Gluon Jets']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'gluon, radiation', 'jet', 'charged particle, multiple production', 'particle identification, flavor', 'track data analysis, vertex', 'yield, (anti-p p K pi)', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105037'],"['We present measurements of identified charged hadron production over a wide momentum range using the SLD Cherenkov Ring Imaging Detector. In addition to studying particle production in flavor-inclusive Z^0 decays, we compare the production in decays into light, c and b flavor events. We also examine particle production in gluon jets with that in light quark jets. The jet flavors are selected by using displaced vertex information.']",['2001-05-16']
173,['eng'],"['Onderwater, C J G']",['g-2 measurement at BNL E821'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'muon+, magnetic moment', 'muon+, polarized beam', 'muon, storage ring', 'electroweak interaction, validity test', 'magnetic field, external field', 'muon+, leptonic decay', 'positron, energy spectrum', 'yield, time dependence', 'scintillation counter, fibre', 'experimental results', 'Brookhaven Lab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105036'],"['The muon (g-2) experiment at BNL has completed four data runs for the positive muon, beginning in 1997 and has just finished its first run for the negative muon. Recently the analysis of a 1.3 ppm result based on the 1999 run was completed and published (a_\\mu^+ = 11,659,202(14)(6) x 10^-10). The result shows a tantalizing discrepancy with the Standard Model prediction of 2.6 times the combined experimental and theoretical uncertainty. The muon (g-2) experiment at BNL is ultimately aimed at measuring the anomalous magnetic moment of the muon with a relative uncertainty of 0.35 ppm.']",['2001-05-16']
174,['eng'],"['Varga, D']",['Recent Results on Strangeness Production from CERN Experiment NA49'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'p p, inclusive reaction', 'p nucleus, inclusive reaction', 'scattering, heavy ion', 'carbon', 'silicon', 'sulfur', 'lead', 'hadron, multiple production', 'production, strangeness', 'yield, (K+ pi+)', 'energy dependence', 'Xi-, yield', 'hyperon, enhancement', 'magnetic spectrometer, experimental results', 'CERN SPS', '40 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105035'],['New results from NA49 on the production of strangeness in elementary and nuclear reactions are presented. New measurements of charged kaon and pion production have been obtained from 40 AGeV Pb+Pb collisions. The evolution of strange meson yields in nucleus-nucleus interactions is studied as a function of collision energy and system size. Cascade baryon yields are presented for a wide range of hadronic interactions including first measurements in p+p and centrality controlled p+Pb collisions.'],['2001-05-16']
175,['eng'],"['García-Abia, P']",['Standard Model Higgs Search Strategy at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'fusion, W W', 'fusion, Z0 Z0', 'data analysis method', 'statistical analysis', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'electron positron --> Higgs particle neutrino antineutrino', 'electron positron --> Higgs particle positron electron', '200-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105034'],"['The Standard Model Higgs boson has been searched for by the four LEP experiments in the last twelve years. The data collected at LEP in the year 2000 suggest the first observation of a Higgs boson. In this letter, I describe the basic concepts of the Higgs search at LEP, with emphasis in the statistical method used to combine the results from the LEP experiments.']",['2001-05-16']
176,['eng'],"['Costanzo, D']",['Prospects for Higgs studies at LHC'],['Detectors and Experimental Techniques'],"['talk, Les Arcs 2001/03/10', 'p p, interaction', 'luminosity', 'Higgs particle, search for', 'supersymmetry', 'Higgs particle, mass', 'Higgs particle, decay modes', 'photon, pair production', 'quark, beauty', 'quark, pair production', 'intermediate boson, pair production', 'intermediate boson, leptonic decay', 'Higgs particle, width', 'magnetic detector, ATLAS', 'magnetic detector, CMS', 'numerical calculations', 'proposed experiment, CERN LHC Coll', '14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105033'],['A major goal of the future Large Hadron Collider will be the Higgs boson search. In this paper the discovery In this paper the discovery potential is described as a function of the Higgs mass showing that a Standard Model Higgs boson can be discovered after less than two years of running of the collider. The MSSM Higgs searches and the precision achievable on the measurement of the Higgs boson parameters are also discussed.'],['2001-05-16']
177,['eng'],"['Kawamoto, T']",['Electroweak data and Standard Model Fit Results'],['Particle Physics - Experimental Results'],"['review, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'anti-p p, colliding beams', 'neutrino nucleon, interaction', 'electroweak interaction, validity test', 'Z0, electroproduction', 'Z0, width', 'Z0, decay modes', 'angular distribution, asymmetry', 'tau, polarization', 'Weinberg angle', 'Higgs particle, mass', 'W, pair production', 'mass, truth', 'strong interaction, coupling constant', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'Batavia TEVATRON PS', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105032'],"['Most recent tests of the Standard Model of the electroweak interaction are reported using data from the four LEP experiments ALEPH, DELPHI, L3 and OPAL, the SLD experiment at SLC, the Tevatron ppbar experiments CDF and D0, and the NuTeV neutrino experiment. Consistency of the Standard Model is studied. The value of the Higgs mass is inferred from a global fit.']",['2001-05-16']
178,['eng'],"['Link, J M']",['A measurement of branching ratios of $D^+$ and $D^+_s$ hadronic decays to four-body final states containing a $K_S$'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium, oxygen', 'charmed meson, photoproduction', 'charmed meson, hadronic decay', 'final state, (4meson)', 'K0(S), hadronic decay', 'D+, branching ratio', 'D/s+, branching ratio', 'forward spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> K0(S) K 2pi', 'D+ --> K0(S) K+ K- pi+', 'D+ --> K0(S) 2pi+ 2pi-', 'D/s+ --> K0(S) K+ pi+ pi-', 'D/s+ --> K0(S) K- 2pi+', 'D/s+ --> K0(S) K- 2pi+', 'K0(S) --> pi+ pi-', 'approx. 180 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105031'],"['We have studied hadronic four-body decays of $D^+$ and $D^+_s$ mesons with a $K_S$ in the final state using data recorded during the 1996-1997 fixed-target run at Fermilab high energy photoproduction experiment FOCUS. We report a new branching ratio measurement of $\\Gamma(D^+\\to K_S K^-\\pi^+\\pi^+)/\\Gamma(D^+\\to K_S \\pi^+\\pi^+\\pi^-)=0.0768\\pm0.0041\\pm0.0032$. We make the first observation of three new decay modes with branching ratios $\\Gamma(D^+\\to K_S K^+\\pi^+\\pi^-)/\\Gamma(D^+\\to K_S \\pi^+\\pi^+\\pi^-)=0.0562\\pm0.0039\\pm0.0040$, $\\Gamma(D^+\\to\\K_S K^+ K^-\\pi^+)/\\Gamma(D^+\\to K_S \\pi^+\\pi^+\\pi^-)=0.0077\\pm0.0015\\pm0.0009$, and $\\Gamma(D^+_s\\to K_S K^+\\pi^+\\pi^-)/\\Gamma(D^+_s\\to K_S K^-\\pi^+\\pi^+)=0.586\\pm0.052\\pm0.043$, where in each case the first error is statistical and the second error is systematic.']",['2001-05-16']
179,['eng'],"['Dubrovin, M']",['First Measurement of the D*+ Width'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D*(2010), width', 'decay, energy', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105030'],['We have made the first measurement of the D*+ width using 9/fb of e+e- data collected near the Y4S resonance by the CLEO II.V detector. Our method uses advanced tracking techniques and a reconstruction method that takes advantage of the small vertical size of the CESR beam spot to measure the energy release distribution from the D*+ -> D0 pi+ decay. Our preliminary result is Gamma(D*+) = 96 +- 4 (Statistical) +- 22 (Systematic) keV.'],['2001-05-15']
180,['eng'],"['Barrow, S P']",['Electroproduction of the $\\Lambda(1520)$ hyperon'],['Particle Physics - Experimental Results'],"['electron p, exclusive reaction', 'Lambda(1520), electroproduction', 'K+, associated production', 'Lambda(1520), hadronic decay', 'K, angular distribution', 'momentum transfer, spectra', 'helicity', 'magnetic spectrometer, experimental results', 'Newport News CEBAF Linac', 'electron p --> Lambda(1520) K+ electron', 'Lambda(1520) --> p K-', '4.05-4.46 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105029'],"[""The reaction $ep \\to e'K^+\\Lambda(1520)$ with $\\Lambda(1520) \\to p'K^-$ was studied at electron beam energies of 4.05, 4.25, and 4.46 GeV, using the CLAS detector at the Thomas Jefferson National Accelerator Facility. The cos$\\theta_{K^+}$, $\\phi_{K^+}$, $Q^2$, and $W$ dependencies of $\\Lambda$(1520) electroproduction are presented for the kinematic region 0.9 $<$ $Q^2$ $<$ 2.4 GeV$^2$ and 1.95 $<$ $W$ $<$ 2.65 GeV. Also, the $Q^2$ dependence of the $\\Lambda$(1520) decay angular distribution is presented for the first time. The cos$\\theta_{K^+}$ angular distributions suggest {\\it t}-channel diagrams dominate the production process. Fits to the $\\Lambda$(1520) {\\it t}-channel helicity frame decay angular distributions indicate the $m_{z}=\\pm{1/2}$ parentage accounts for about 60% of the total yield, which suggests this reaction has a significant contribution from {\\it t}-channel processes with either K$^+$ exchange or longitudinal coupling to an exchanged K$^*$. The $Q^2$ dependence of the $\\Lambda$(1520) production cross section is the same as that observed for $\\Lambda$(1116) photo- and electroproduction.""]",['2001-05-15']
181,['eng'],"['Sanders, D A']",['Rare and forbidden dilepton decays of D mesons (E791)'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'pi- nucleus, inclusive reaction', 'D, hadroproduction', 'D, rare decay', 'D, semileptonic decay', 'D, leptonic decay', 'D+, branching ratio', 'D/s+, branching ratio', 'D0, branching ratio', 'upper limit', 'neutral current, flavor changing', 'flavor, violation', 'lepton number, violation', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105028'],"['We summarize the results of two recent searches for flavor-changing neutral current, lepton-flavor violating, and lepton-number violating decays of D+, Ds, and D0 mesons (and their antiparticles) into modes containing muons and electrons. Using data from Fermilab charm hadroproduction experiment E791, we examined D+ and Ds pi,l,l and K,l,l decay modes and the D0 dilepton decay modes containing either l+,l-, a rho0, K*0, or phi vector meson, or a non-resonant pi,pi, K,pi, or K,K pair of pseudoscalar mesons. No evidence for any of these decays was found. Therefore, we presented branching-fraction upper limits at 90% confidence level for the 51 decay modes examined. Twenty-six of these modes had no previously reported limits, and eighteen of the remainder were reported with significant improvements over previously published results.']",['2001-05-15']
182,['eng'],"['Knuteson, B']",['Sleuth'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'anti-p p, colliding beams', 'anti-p p, interaction', 'transverse momentum, high', 'new particle, search for', 'new interaction, search for', 'data analysis method', 'exclusive reaction, final state', 'background', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105027'],"['How can we search for new physics when we only vaguely know what it should look like? How can we perform an unbiased yet data-driven search? If we see apparently anomalous events in our data, how can we quantify their ""interestingness"" a posteriori? We present an analysis strategy (Sleuth) that simultaneously addresses each of these questions, and we demonstrate its application to over thirty exclusive final states in data collected by D0 in Run I of the Fermilab Tevatron.']",['2001-05-15']
183,['eng'],"['Parashar, N']",['The D0 Run II Detector and Physics Prospects'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 2001/02/18', 'anti-p p, colliding beams', 'four-pi-detector, DZERO', 'upgrade, proposed', 'semiconductor detector, vertex', 'semiconductor detector, microstrip', 'scintillation counter, fibre', 'superconducting, solenoid', 'trigger', 'data acquisition', 'quark, truth', 'quark, beauty', 'sparticle, search for', 'proposed experiment, Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105026'],"['The D0 Detector at Fermilab is currently undergoing an extensive upgrade to participate in the Run II data taking which shall begin on March 1, 2001. The design of the detector meets the requirements of the high luminosity environment provided by the accelerator. This paper describes the upgraded detector subsystems and gives a brief outline of the physics prospects associated with the upgrade.']",['2001-05-15']
184,['eng'],"['Lin, C J S']",['B physics at the Z peak (SLD)'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'beautiful particle, lifetime', 'lifetime, ratio', 'B+', 'B0, mass difference', 'B/s, mass difference', 'Lambda/b0', 'B, semileptonic decay', 'yield, charm', 'B, branching ratio', 'Kobayashi-Maskawa angle, unitarity', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'experimental results', 'magnetic detector, SLD', 'SLAC SLC Linac', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105025'],"['Recent B physics results from LEP and SLD are reviewed. In particular, results of B lifetimes, semileptonic B decays, charm counting, CKM matrix elements, and mixing are presented.']",['2001-05-15']
185,['eng'],"['Tajima, H']","['B CP-Violation, Mixing and Lifetime Results from Belle']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0 anti-B0, interference', 'B0, mass difference', 'B, semileptonic decay', 'B, hadronic decay', 'time dependence', 'B0, lifetime', 'B+, lifetime', 'violation, CP', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105024'],"['Recent results on the $B$ CP-violation parameter $\\sin2\\phi_1$, the $B^0_d$-$\\overline{B}^0_d$ mixing parameter $\\Delta m_d$ and $B$-meson lifetimes are reported. The results are based on 10.5 $fb^{-1}$ of data collected with the Belle detector at KEKB. Using both semileptonic and hadronic decay modes the neutral and charged $B$-meson lifetimes are measured to be $\\taubz=1.548\\pm0.035 (\\mathrm{stat.})$~ps and $\\taubm=1.656\\pm0.038 (\\mathrm{stat.})$~ps. The oscillation frequency $\\Delta m_d$ for $B^0_d$-$\\overline{B}^0_d$ mixing is measured to be $0.522\\pm0.026 (\\mathrm{stat.})$~ps$^{-1}$ using semileptonic modes and $0.527\\pm0.032 (\\mathrm{stat.})$~ps$^{-1}$ using hadronic modes. The above results are preliminary. The time evolution of $B^0_d$ decays into $J/\\psi K^0_S$, $\\psi(2S) K^0_S$, $\\chi_{c1} K^0_S$, $\\eta_{c} K^0_S$, $J/\\psi K^0_L$ and $J/\\psi \\pi^0$ modes are studied to obtain $\\sin2\\phi_1$. Using 282 fully reconstructed events, $\\sin2\\phi_1$ is measured to be']",['2001-05-15']
186,['eng'],"['Toshito, T']",['Super-K atmospheric neutrino results'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'neutrino/mu, cosmic radiation', 'neutrino, oscillation', 'neutrino/tau', 'neutrino, sterile', 'neutrino, mass difference', 'angular distribution', 'neutrino nucleon, interaction', 'charged current', 'Cherenkov counter, water', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105023'],"['We present atmospheric neutrino results from a 79 kiloton year (1289 days) exposure of the Super-Kamiokande detector. Our data are well explained by $\\nu_{\\mu} \\to \\nu_{\\tau}$ 2-flavor oscillations. We have been attempting to discriminate between the possible oscillating partners of the muon neutrino as being either the tau neutrino or the sterile neutrino. Pure $\\nu_\\mu\\to\\nu_s$ oscillation is disfavored at 99% C.L.. Moreover, we performed the appearance search for charged current tau neutrino interactions in the upward-going samples. Our data is consistent with $\\nu_{\\tau}$ appearance at roughly the two-sigma level.']",['2001-05-15']
187,['eng'],"['Wang, C H']",['A Study of B meson Decays to Charm at Belle'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, semileptonic decay', 'final state, charm', 'quarkonium, charm', 'charmed meson', 'Kobayashi-Maskawa angle', 'B, branching ratio', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105022'],"['With ~10fb$^{-1}$ data from Belle, the results of b to c and u decays have been represented here. Several decay modes have been studied, which include charmonium, semileptonic decay and Cabibbo-suppressed decays mode. The preliminary results and the measurements of KM matrix elements will also be presented here.']",['2001-09-14']
188,['eng'],"['Koehler, K U']",['Polarisation of e from mu decays at PSI'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'muon+, polarized beam', 'muon+, leptonic decay', 'positron, polarization', 'polarization, transverse', 'polarization, longitudinal', 'energy dependence', 'electron positron, annihilation', 'time dependence', 'angular dependence', 'spin, rotator', 'time reversal', 'Michel parameter', 'experimental results', 'PSI Cycl']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105021'],"['In the standard model of electroweak interactions the positrons from the decay of polarized positive muons are mainly longitudinally polarized. The measurement of the two transverse polarization components PT1 and PT2 is a sensitive tool to look for contributions from additional, exotic interactions. The energy dependence of PT1 yields the low energy Michel parameter eta and thus an improved model-independent value of the Fermi coupling constant. A non-zero value PT2 would be the first observation of time reversal violation in a purely leptonic decay. The muon decay experiment at the Paul Scherrer Institut is the first experiment to measure all three positron polarization components, PT1, PT2, and the longitudinal polarization component PL. In this contribution results from a small data-sample taken in 1999 are presented. The values obtained are PT1 = (5 +- 16)*10^(-3), PT2 = (1 +- 16)*10^(-3), and PL = 1.09 +- 0.15. More than ten times more data was taken in October/November 2000, the analysis of which will further reduce the statistical errors.']",['2001-05-14']
189,['eng'],"['Aganiants, A O']",['The Growth of Interaction Cross-Section of 4.3 GeV Electrons in Excited Crystals'],['Particle Physics - Experimental Results'],"['electron nucleus, nuclear reaction', 'carbon, crystal', 'crystal, excited state', 'effect, nonlinear', 'photon, radiation', 'radiation, yield', 'radiation, energy loss', 'ionization chamber', 'scintillation counter', 'experimental results', 'Erevan ES', '4.3 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105020'],"['The microscopic properties of the interactions of relativistic electrons were observed to alter when macro-conditions, such as the crystal vacuum, were changed. A qualitative explanation of the phenomenon is given.']",['2001-05-14']
190,['eng'],"['Schietinger, T']",['Charmless Hadronic B Decays at BABAR'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 2001/02/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'meson, pair production', 'final state, (3meson)', 'final state, (0charm)', 'B0, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105019'],"[""We present several searches for charmless hadronic two-body and three-body decays of B mesons from electron-positron annihilation data collected by the BABAR detector near the Upsilon(4S) resonance. We report the preliminary branching fractions BR(B0 --> pi+pi-) = (4.1 +/- 1.0 +/- 0.7) x 10^-6, BR(B0 --> K+pi-) = (16.7 +/- 1.6 +/- 1.3) x 10^-6, BR(B0 --> rho-/+ pi+/-) = (49 +/- 13 +6 -5) x 10^-6, BR(B+ --> eta' K+) = (62 +/- 18 +/- 8) x 10^-6, and present upper limits for nine other decays.""]",['2001-09-14']
191,['eng'],"['Cavoto, G']",['Measurements of Charmless Hadronic B Decays Branching Fraction at BABAR'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'meson, pair production', 'pi', 'K', 'K*(892)', 'Phi(1020)', 'B0, branching ratio', 'B+, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105018'],"['We present preliminary measurements of the branching fractions for charmless hadronic decays of B mesons into two-body final states with kaons, pions and a phi resonance. The measurements are based on a data sample of approximately 23 million B-anti-B pairs collected by the BABAR detector at the PEP-II asymmetric B Factory at SLAC.']",['2001-05-11']
192,['eng'],"['Drollinger, V']",['Finding H0 -> bbbar at the LHC'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'p p, colliding beams', 'p p, interaction', 'Higgs particle, search for', 'Higgs particle, neutral particle', 'quark, truth', 'quark, pair production', 'W, hadroproduction', 'Higgs particle, associated production', 'Higgs particle, hadronic decay', 'quark, beauty', 'supersymmetry', 'proposed experiment, CMS', 'numerical calculations, CERN LHC Coll', '14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105017'],"['We have investigated the sensitivity of CMS for finding the Higgs boson in the H0 -> bbbar channel. An excellent b-tagging performance and a good jet resolution are the main requirements needed for a successful event selection. In the Standard Model (SM), the ttbar H0 -> l+- nu qqbar bbbar bbbar channel is accessible, if the Higgs mass is lighter than m(H0) = 125 GeV, already during the first years of the LHC. Also, most of the MSSM (Minimal Supersymmetric Standard Model) parameter space can be covered. The W+- H0 -> l+- nu bbbar channel is only accessible with high luminosity at the LHC. In both channels the mass can be determined with a precision of a few per cent and the Higgs couplings at the level of 10%.']",['2001-05-11']
193,['eng'],"['Alavi-Harati, A', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barbosa, R F', 'Barker, A R', 'Barrio, M', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hamm, J', 'Hanagaki, K', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jensen, D A', 'Kessler, R', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Qi, X R', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Shields, J', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Swallow, E C', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Turner, S E', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['First Measurement of Form Factors of the Decay Xi0->Sigma+ e- anti-nu/e'],['Particle Physics - Experimental Results'],"['Xi0, semileptonic decay', 'form factor, decay', 'form factor, vector', 'form factor, axial-vector', 'form factor, magnetic', 'second-class current', 'form factor, ratio', 'Sigma+, polarization', 'Sigma+, hadronic decay', 'correlation, (electron antineutrino)', 'electron, energy spectrum', 'symmetry, SU(3)', 'symmetry, flavor', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'Xi0 --> Sigma+ electron antineutrino/e', 'Sigma+ --> p pi0']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105016'],"['We present the first measurement of the form factor ratios g1/f1 (direct axial-vector to vector), g2/f1 (second class current) and f2/f1 (weak magnetism) for the decay Xi0 -> Sigma+ e- anti-nu/e using the KTeV (E799) beam line and detector at Fermilab. From the Sigma+ polarization measured with the decay Sigma+ -> p pi0 and the e- - anti-nu/e correlation, we measure g1/f1 to be 1.32 +0.21-0.17(stat.) +/- 0.05(syst.), assuming the SU(3)f (flavor) values for g2/f1 and f2/f1. Our results are all consistent with exact SU(3)f symmetry.']",['2001-05-11']
194,['eng'],"['Collar, J I']",['A new approach to neutrino and WIMP detection using telecom-grade electrooptic and fiber-optic components'],['Particle Physics - Experimental Results'],"['neutrino, particle identification', 'WIMP, particle identification', 'astrophysics, missing-mass', 'WIMP, search for', 'nucleus, recoil', 'effect, acoustic', 'optics, fibre', 'optics, interference', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105015'],"['The dense energy deposition from a low-energy nuclear recoil produces, via the thermoacoustic effect, a brief yet intense pressure pulse that can be used for WIMP or neutrino detection in some fiber-optic devices sensitive to acoustooptic disturbances. Several possible detection schemes are described: all of them are inspired by modern fiber-optic sensor technologies and share common characteristics of low-cost and expected insensitivity to minimum-ionizing backgrounds.']",['2001-05-11']
195,['eng'],"['Abe, K', 'Adachi, I', 'Aihara, H', 'Asai, M', 'Asano, Y', 'Aso, T', 'Aulchenko, V M', 'Aushev, T', 'Bakich, A M', 'Banas, E', 'Bartel, W', 'Behari, S', 'Behera, P K', 'Beiline, D', 'Bondar, A E', 'Bozek, A', 'Browder, T E', 'Casey, B C K', 'Chang, P', 'Chao, Y', 'Cheon, B G', 'Choi, S K', 'Choi, Y', 'Dragic, J', 'Drutskoy, A G', 'Eidelman, S', 'Enari, Y', 'Fang, F', 'Fujii, H', 'Fukunaga, C', 'Fukushima, M', 'Garmash, A', 'Gordon, A', 'Gotow, K', 'Guo, R', 'Haba, J', 'Hamasaki, H', 'Hanagaki, K', 'Hara, K', 'Hara, T', 'Hastings, N C', 'Hayashii, H', 'Hazumi, M', 'Heenan, E M', 'Higasino, Y', 'Higuchi, I', 'Higuchi, T', 'Hirano, H', 'Hojo, T', 'Hoshi, Y', 'Hou, S R', 'Hou, W S', 'Hsu, S C', 'Huang, H C', 'Igarashi, Y', 'Iijima, T', 'Ikeda, H', 'Inami, K', 'Ishikawa, A', 'Ishino, H', 'Itoh, R', 'Iwai, G', 'Iwasaki, H', 'Iwasaki, Y', 'Jackson, D J', 'Jalocha, P', 'Jang, H K', 'Jones, M', 'Kagan, R', 'Kakuno, H', 'Kaneko, J', 'Kang, J H', 'Kang, J S', 'Kapusta, P', 'Katayama, N', 'Kawai, H', 'Kawai, H', 'Kawamura, N', 'Kawasaki, T', 'Kichimi, H', 'Kim, D W', 'Kim, H J', 'Kim, S K', 'Kim, T H', 'Kinoshita, K', 'Kobayashi, S', 'Koishi, S', 'Krokovnyi, P P', 'Kulasiri, R', 'Kumar, S', 'Kuzmin, A', 'Kwon, Y J', 'Lange, J S', 'Lee, S H', 'Liventsev, D', 'Lu, R S', 'Marlow, D', 'Matsubara, T', 'Matsui, S', 'Matsumoto, S', 'Matsumoto, T', 'Mikami, Y', 'Miyabayashi, K', 'Miyake, H', 'Miyata, H', 'Moloney, G R', 'Moorhead, G F', 'Mori, S', 'Mori, T', 'Murakami, A', 'Nagamine, T', 'Nagasaka, Y', 'Nagashima, Y', 'Nakadaira, T', 'Nakano, E', 'Nakao, M', 'Nam, J W', 'Narita, S', 'Natkaniec, Z', 'Neichi, K', 'Nishida, S', 'Nitoh, O', 'Noguchi, S', 'Nozaki, T', 'Ogawa, S', 'Ohshima, T', 'Okabe, T', 'Okuno, S', 'Olsen, S L', 'Ozaki, H', 'Pakhlov, P', 'Palka, H', 'Park, C S', 'Park, C W', 'Park, H', 'Peak, L S', 'Peters, M', 'Piilonen, L E', 'Prebys, E J', 'Rodríguez, J L', 'Root, N', 'Rózanska, M', 'Rybicki, K', 'Sagawa, H', 'Sakai, Y', 'Sakamoto, H', 'Satapathy, M', 'Satpathy, A', 'Schrenk, S', 'Semenov, S V', 'Senyo, K', 'Sevior, M E', 'Shibuya, H', 'Shwartz, B A', 'Stanic, S', 'Sugi, A', 'Sugiyama, A', 'Sumisawa, K', 'Sumiyoshi, T', 'Suzuki, J I', 'Suzuki, K', 'Suzuki, S', 'Suzuki, S Y', 'Swain, S K', 'Takahashi, T', 'Takasaki, F', 'Takita, M', 'Tamai, K', 'Tamura, N', 'Tanaka, J', 'Tanaka, M', 'Tanaka, Y', 'Taylor, G N', 'Teramoto, Y', 'Tomoto, M', 'Tomura, T', 'Tovey, S N', 'Trabelsi, K', 'Tsuboyama, T', 'Tsukamoto, T', 'Uehara, S', 'Ueno, K', 'Unno, Y', 'Uno, S', 'Ushiroda, Y', 'Vahsen, S E', 'Varvell, K E', 'Wang, C H', 'Wang, J G', 'Wang, M Z', 'Watanabe, Y', 'Won, E', 'Yabsley, B D', 'Yamada, Y', 'Yamaga, M', 'Yamaguchi, A', 'Yamamoto, H', 'Yamashita, Y', 'Yamauchi, M', 'Yanaka, S', 'Yoshida, K', 'Yusa, Y', 'Yuta, H', 'Zhang, C C', 'Zhang, J', 'Zhao, H W', 'Zheng, Y', 'Zhilich, V N', 'Zontar, D']",['Observation of B->J/psi K1(1270)'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'J/psi(3100)', 'K1(1270), hadronic decay', 'intermediate state, (rho(770)0 K0)', 'B0, branching ratio', 'B+, branching ratio', 'upper limit', 'K1(1400)', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> J/psi(3100) K1(1270)', 'K1(1270) --> K0 pi+ pi-', 'approx. 10.6 Gev-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105014', 'http://bsunsrv1.kek.jp/conferences/ICHEP2000/papers/conf0004.ps']","['We report the first observation of the exclusive decay process B->J/psi K1(1270) using a sample of 11.2M BBbar meson pairs collected in the Belle detector at the KEKB asymmetric e+e- collider. We measure branching fractions of Bf(B0 -> J/psi K10(1270) = (1.30 +-0.34 +-0.31)x10^-3 and Bf(B+ -> J/psi K1+(1270) = (1.80 +-0.34 +-0.39)x10-3, where the first error is statistical and the second systematic. These modes constitute approximately 15% of the total number of B -> J/psiX decays. No evidence is seen for B -> J/psi K1(1400) and we set an upper limit on this branching fraction. The K1(1270) -> K0pi+pi- decays have a substantial K0rho0 intermediate state component that may be useful for CP violation studies.']",['2001-05-10']
196,['eng'],"['Hans, R M']",['Mixing and CP violation in the charm & tau sectors(CLEO)'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'D0, electroproduction', 'D0, hadronic decay', 'pseudoscalar meson, pair production', 'D0 anti-D0, interference', 'violation, CP', 'D0, lifetime', 'anti-D0, lifetime', 'lifetime, difference', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D0 --> K+ K-', 'D0 --> pi+ pi-', 'D0 --> K+ pi- pi0', 'D0 --> K0(S) pi0', 'D0 --> 2pi0', 'D0 --> 2K0(S)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105013'],"['Recent CLEO results on neutral charm meson decays presented at the XXXVIth Rencontres de Moriond are discussed. We find no evidence of CP asymmetry in five different two-body decay modes of the D0 to pairs of light pseudo-scalar mesons. We present a measurement of the mixing parameter y_CP = -0.011 +- 0.025 +- 0.014 by searching for a lifetime difference between the CP neutral K+ pi- final state and the CP even K+ K- and pi+ pi- final states. Finally, we describe the first measurement of the rate of wrong-sign D0 to K+ pi- pi0 decay: R_WS = (0.43 +0.11 -0.10 +- 0.07)%.']",['2001-09-14']
197,['eng'],"['Figiel, J']",['Vector meson production at HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'positron p, colliding beams', 'positron p, inclusive reaction', 'vector meson, electroproduction', 'vector meson, photoproduction', 'p, dissociation', 'momentum transfer, high', 'rho(770)', 'Phi(1020)', 'J/psi(3100)', 'differential cross section, momentum transfer', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105012'],"['New results on elastic electroproduction and proton-dissociative photoproduction at large t of rho, phi and J/psi mesons are presented. They are interpreted within perturbative QCD.']",['2001-05-09']
198,['eng'],"['Bai, J Z', 'Chiang Huan Ching', 'Peng, G X', 'Wang, J X', 'Zhu Jun Jie', 'Ban, Y', 'Bian, J G', 'Chang, J F', 'Chen, A D', 'Chen, H F', 'Chen, H S', 'Chen Jia Chao', 'Chen, X D', 'Chen, Y B', 'Cheng, B S', 'Chi, S P', 'Chu, Y P', 'Cui, X Z', 'Dai, Y S', 'Dong, L Y', 'Du, Z Z', 'Fu, H Y', 'Fu, L P', 'Gao, C S', 'Gu, S D', 'Guo, Y N', 'Guo, Z J', 'Han, S W', 'Han, Y', 'He, J', 'He, J T', 'He, K L', 'He, M', 'He, X', 'Hong, T', 'Heng, Y K', 'Hu, G Y', 'Hu, H M', 'Hu, Q H', 'Hu, T', 'Huang, G S', 'Huang, X P', 'Huang, Y Z', 'Ji, X B', 'Jiang, C H', 'Jin, Y', 'Ke, Z J', 'Lai, Y F', 'Li, D', 'Li, H B', 'Li, H H', 'Li, J', 'Li, J C', 'Li, P Q', 'Li, Q J', 'Li, R Y', 'Li, W', 'Li, W G', 'Li Xiao Nan', 'Li Xue Qian', 'Liu, B', 'Liu, F', 'Liu, H M', 'Liu, J', 'Liu, J P', 'Liu, T R', 'Liu, R G', 'Liu, Y', 'Liu, Z X', 'Lu, G R', 'Lu, F', 'Lu, J G', 'Lu, Z J', 'Luo, X L', 'Ma, E C', 'Ma, F C', 'Ma, J M', 'Mao, Z P', 'Meng, X C', 'Mo, X H', 'Nie, J', 'Nie, Z D', 'Qi, N D', 'Qi, X R', 'Qian, C D', 'Qiu, J F', 'Que, Y K', 'Rong, G', 'Shao, Y Y', 'Shen, B W', 'Shen, D L', 'Shen, H', 'Shen, X Y', 'Sheng, H Y', 'Shi, F', 'Shi, H Z', 'Song, X F', 'Sun, H S', 'Sun, L F', 'Sun, Y Z', 'Tang, S Q', 'Tang, X', 'Tong, G L', 'Wang, J', 'Wang, J Z', 'Wang, L', 'Wang, L S', 'Wang, M', 'Wang, M', 'Wang, P', 'Wang, P L', 'Wang, S M', 'Wang, W F', 'Wang, Y Y', 'Wang, Z Y', 'Wei, C L', 'Wu, N', 'Xi, D M', 'Xia, X M', 'Xie, X X', 'Xu, G F', 'Xu, Y', 'Xue, S T', 'Yan, M L', 'Yan, W B', 'Yan, W G', 'Yang, C M', 'Yang, C Y', 'Yang, G A', 'Yang, H X', 'Yang, X F', 'Ye, M H', 'Ye Shu Wei', 'Ye, Y X', 'Yu, C S', 'Yu, C X', 'Yu, G W', 'Yuan, Y', 'Zeng, Y', 'Zhang Bing Yun', 'Zhang, C C', 'Zhang, D H', 'Zhang, H L', 'Zhang, H Y', 'Zhang, J', 'Zhang, J W', 'Zhang, L', 'Zhang, L S', 'Zhang, P', 'Zhang, Q J', 'Zhang, S Q', 'Zhang, X Y', 'Zhang, Y Y', 'Zhang, Z P', 'Zhao, D X', 'Zhao, H W', 'Zhao, J', 'Zhao Jia Wei', 'Zhao, P P', 'Zhao Wei Ren', 'Zhao, Y B', 'Zhao, Z G', 'Zheng Jian Ping', 'Zheng Lin Sheng', 'Zheng Zhi Peng', 'Zhong, X C', 'Zhou, B Q', 'Zhou, G M', 'Zhou, L', 'Zhu, K J', 'Zhu, Q M', 'Zhu, Y C', 'Zhu, Y S', 'Zhu, Z A', 'Zhuang, B A', 'Zou Bing Song']",['Study of N* Production from J/Psi--> p pbar eta'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'J/psi(3100), electroproduction', 'J/psi(3100), hadronic decay', 'partial wave analysis', 'nucleon resonance, mass', 'nucleon resonance, width', 'N(1535)', 'N(1650)', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'J/psi(3100) --> p anti-p eta', '3.1 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105011'],"['Data are presented on the reaction J/psi--> p pbar eta using 7.8 million J/psi triggers collected by the BEjing Spectrometer (BES). A partial wave analysis is performed. A clear enhancement near the p eta(pbar eta) threshold is observed. It is fitted with a JP=1/2- resonance with mass $M= 1530\\pm 10$ MeV and width $\\Gamma = 95\\pm 25$ MeV. In addition, there is a peak around 1650 MeV with JP=1/2- preferred also, fitted with $M =1647\\pm 20$ MeV and $\\Gamma = 145^{+80}_{-45}$ MeV. These two N* resonances are believed to be the two well established states, S11(1535) and S11(1650), respectively. It is the first partial wave study of the production of these resonances from J/psi decays.']",['2001-05-09']
199,['eng'],"['Krawczyk, M', 'Söldner-Rembold, S', 'Wing, M']",['Reach of future colliders in probing the structure of the photon'],['Particle Physics - Experimental Results'],"['talk', 'electron p, deep inelastic scattering', 'photon, direct production', 'electron positron, inelastic scattering', 'photon, structure function', 'photon electron, interaction', 'model, parton', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105010'],"['A comparison of the potentials of ep and e^+e^-$machines to probe the structure of the photon is performed. In particular, the kinematic reach of a proposed future ep facility, THERA, is compared with those of current colliders, LEP and HERA, and with the proposed linear collider, TESLA. THERA like HERA will use a proton beam of 920 GeV but with an increased electron beam energy of 250 GeV allowing higher scales, Q^2, and lower values of parton momentum fraction in the photon, x_\\gamma, to be probed.']",['2001-09-14']
200,['eng'],"['Ciulli, V']",['Studies of b-quark fragmentation'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, fragmentation', 'fragmentation function', 'B, semileptonic decay', 'B, hadronic decay', 'magnetic detector, ALEPH', 'CERN LEP Stor', 'magnetic detector, SLD', 'SLAC SLC Linac', 'experimental results', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105008'],['I will review new studies of b-quark fragmentation performed at the Z peak by ALEPH and SLD. An improved sensitivity to distinguish between fragmentation model and more accurate measurements of the mean b-hadron scaled energy have been obtained.'],['2001-09-14']
201,['eng'],"['Verzi, V']","['W couplings, WW and WZ cross-sections (LEP)']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'gauge boson, pair production', 'W', 'Z0', 'photon', 'intermediate boson, leptonic decay', 'intermediate boson, hadronic decay', 'coupling, (3gauge boson)', 'final state, (4fermion)', 'electroweak interaction, validity test', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', 'electron positron --> W electron neutrino', 'electron positron --> 2Z0', 'electron positron --> Z0 photon', '183-208 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105007'],"['In its second phase, LEP has given the unique opportunity to study four fermion processes never observed before. This papers deals with a preliminary study of $WW$, $We\\nu$, $ZZ$ and $Z\\gamma^\\star$ production in $e^+e^-$ collisions. Measurement results on $WW$ cross section, $W$ branching fractions, $WWV$ ($V=Z/\\gamma$) anomalous couplings and $W$ average polarization in $WW$ events are presented. Moreover cross section measurements for $We\\nu$, $ZZ$ and $Z\\gamma^\\star$ production and limits on $ZZZ$ and $ZZ\\gamma$ anomalous couplings are reported. All the results are in good agreement with the Standard Model expectations.']",['2001-09-14']
202,['eng'],"['Liu, Y', 'Chen, C P', 'Li, H B', 'Tang, C H', 'Chang, C Y', 'Hou, L', 'Lai, W P', 'Li, J', 'Lin, S T', 'Luo, C S', 'Qiu, J F', 'Sheng, H Y', 'Wang Chao Cheng', 'Wang, M Z', 'Wang Shui Cai', 'Wong, H T', 'Xin, B', 'Yue, Q', 'Zhao, D X', 'Zhao, S Q', 'Zhou, Z Y', 'Zhuang, B A']",['Studies of Prototype CsI(Tl) Crystal Scintillators for Low-Energy Neutrino Experiments'],['Particle Physics - Experimental Results'],"['neutrino, counters and detectors', 'scintillation counter, crystal', 'cesium, iodine', 'fabrication', 'radiation, yield', 'astrophysics, missing-mass', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105006'],"['Crystal scintillators provide potential merits for the pursuit of low-energy low-background experiments. A CsI(Tl) scintillating crystal detector is being constructed to study low-energy neutrino physics at a nuclear reactor, while projects are underway to adopt this technique for dark matter searches. The choice of the geometrical parameters of the crystal modules, as well as the optimization of the read-out scheme, are the results of an R&D program. Crystals with 40 cm in length were developed. The detector requirements and the achieved performance of the prototypes are presented. Future prospects for this technique are discussed.']",['2001-05-03']
203,['eng'],"['Iijima, T']",['Study of Rare B Meson Decays at Belle'],['Particle Physics - Experimental Results'],"['talk, Ago Town 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, rare decay', 'meson, pair production', 'D', 'D*(2010)', 'K', 'K*(892)', 'final state, (0charm)', 'neutral current, flavor changing', 'B, branching ratio', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> charmed meson strange meson', 'B --> 2pseudoscalar meson', 'B --> strange meson lepton+ lepton-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105005'],"[""In this paper, we briefly review results on rare decays of $B$ mesons from the Belle experiment, based on 10.4 fb$^{-1}$ data collected on the $\\Upsilon$(4S) resonance. The topics include measurements of Cabibbo suppressed decays $B \\to D^{(*)} K^{(*)}$, charmless two-body decays $B \\to \\pi\\pi$, $K\\pi$, $KK$ and $B \\to \\eta^{'} h (h = K^+, \\pi^+, K^0)$, and a search for flavor changing neutral current decays $B \\to K^{(*)} \\ell^{+} \\ell^{-}$.""]",['2001-05-03']
204,['eng'],"['Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Poling, R A', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Benslama, K', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Nelson, H N', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Alexander, J P', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Schwarthoff, H', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J']",['Rate Measurement of $D^{0}\\to K^{+}\\pi^{-}\\pi^{0}$ and Constraints on $D^{0} - \\overline{D^{0}}$ Mixing'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'D0, branching ratio', 'particle identification, flavor', 'time dependence', 'D0 anti-D0, interference', 'violation, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D0 --> K+ pi- pi0', 'D0 --> K- pi+ pi0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105002'],"['We present an observation and rate measurement of the decay D0 -> K+pi-pi0 produced in 9/fb of e+e- collisions near the Upsilon(4S) resonance. The signal is inconsistent with an upward fluctuation of the background by 4.9 standard deviations. We measured the rate of D0 -> K+pi-pi0 normalized to the rate of D0bar -> K+pi-pi0 to be 0.0043 +0.0011 -0.0010 (stat) +/- 0.0007 (syst). This decay can be produced by doubly-Cabibbo-suppressed decays or by the D0 evolving into a D0bar through mixing, followed by a Cabibbo-favored decay to K+pi-pi0. We also found the CP asymmetry A=(8 +25 -22)% to be consistent with zero.']",['2001-05-02']
205,['eng'],"['Aubert, Bernard', 'Boutigny, D', 'Gaillard, Jean-Marc', 'Hicheur, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Palano, A', 'Chen, G P', 'Chen Jia Chao', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Fan, Q', 'Gill, M S', 'Gowdy, S J', 'Gritsan, A', 'Groysman, Y', 'Jacobsen, R G', 'Kadel, R W', 'Kadyk, J A', 'Kerth, L T', 'Kluth, S', 'Kolomensky, Yu G', 'Kral, J F', 'Le Clerc, C', 'Levi, M E', 'Liu, T', 'Lynch, G', 'Meyer, A B', 'Mir, L M', 'Momayezi, M', 'Oddone, P J', 'Perazzo, A', 'Pripstein, M', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Telnov, A V', 'Wenzel, W A', 'Bright-Thomas, P G', 'Harrison, T J', 'Hawkes, C M', 'Kirk, A', 'Knowles, D J', ""O'Neale, S W"", 'Penny, R C', 'Watson, A T', 'Watson, N K', 'Deppermann, T', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Barlow, N R', 'Bhimji, W', 'Chevalier, N', 'Clark, P J', 'Cottingham, W N', 'De Groot, N', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'Jolly, S', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Telnov, V I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M', 'McMahon, S', 'Stoker, D P', 'Ahsan, A', 'Arisaka, K', 'Buchanan, C D', 'Chun, S', 'Branson, J G', 'MacFarlane, D B', 'Prell, S', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Campagnari, C', 'Dahmes, B', 'Hart, P A', 'Kuznetsova, N P', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Turri, M', 'Walkowiak, W', 'Williams, D C', 'Wilson, M G', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoretskii, A', 'Hitlin, D G', 'Metzler, S', 'Oyang, J', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Bloom, P', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J D', 'Sen, S', 'Smith, J G', 'Van Hoek, W C', 'Wagner, D L', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Wilson, R J', 'Zhang, J', 'Brandt, T', 'Brose, J', 'Colberg, T', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Maly, E', 'Müller-Pfefferkorn, R', 'Otto, S', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Roussot, E', ""T'Jampens, S"", 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di, F', 'Lodovico', 'Khan, A', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Falbo, M', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E', 'Anulli, F', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Xie, Y', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Fabbricatore, P', 'Farinon, S', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Musenich, R', 'Pallavicini, M', 'Parodi, R', 'Passaggio, S', 'Pastore, F', 'Patrignani, C', 'Pia, M G', 'Priano, C', 'Robutti, E', 'Santroni, A', 'Morii, M', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'Meyer, W T', 'Rosenberg, E I', 'Benkebil, M', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Lacker, H M', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', 'Shi, X', 'Van Bibber, K', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'Payne, D J', 'Sloane, R J', 'Touramanis, C', 'Aspinwall, M L', 'Bowerman, D A', 'Dauncey, P D', 'Egede, U', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R', 'Nash, J A', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Potter, R J L', 'Shorthouse, H W', 'Strother, P', 'Vidal, P B', 'Williams, M I', 'Cowan, G', 'George, S', 'Green, M G', 'Kurup, A', 'Marker, C E', 'McGrath, P', 'McMahon, T R', 'Ricciardi, S', 'Salvatore, F', 'Scott, I', 'Vaitsas, G', 'Brown, D', 'Davis, C L', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Forti, A C', 'Fullwood, J', 'Jackson, F', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Weatherall, J H', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Schieck, J R', 'Blaylock, G', 'Dallapiccola, C', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R R', 'Lin, C S', 'Moore, T B', 'Stängle, H', 'Willocq, S', 'Wittlin, J', 'Brau, B', 'Cowan, R', 'Sciolla, G', 'Taylor, F', 'Yamamoto, R K', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Eschenberg, V', 'Kroeger, R A', 'Reidy, J', 'Sanders, D A', 'Summers, D J', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cartaro, C', 'Cavallo, N', 'De, G', 'Nardo', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Paolucci, P', 'Piccolo, D', 'Sciacca, C', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Brau, J E', 'Frey, R', 'Iwasaki, M', 'Sinev, N B', 'Strom, D', 'Colecchia, F', 'Dal Corso, F', 'Dorigo, A', 'Galeazzi, F', 'Margoni, M', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Rotondo, M', 'Simonetto, F', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Hamon, O', 'Le Diberder, F', 'Leruste, P', 'Lory, J', 'Roos, L', 'Stark, J', 'Versille, S', 'Manfredi, P F', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Martínez-Vidal, F', 'Morganti, M', 'Neri, N', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Walsh, J', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Cavoto, G', 'Del Re, D', 'Faccini, R', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Voena, C', 'Christ, S', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M S', 'Plano, R J', 'Adye, T', 'Franek, B J', 'Geddes, N I', 'Gopal, Gian P', 'Xella, S M', 'Aleksan, R', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Copty, N K', 'Purohit, M V', 'Singh, H', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Aston, D', 'Baird, K', 'Bartelt, J', 'Bloom, Elliott D', 'Boyarski, A M', 'Bulos, F', 'Calderini, G', 'Convery, M R', 'Coupal, D P', 'Coward, D H', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Field, R C', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kelsey, M H', 'Kim, P', 'Kocian, M L', 'Langenegger, U', 'Leith, D W G S', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'Manzin, G', 'Marsiske, H', 'Menke, S', 'Messner, R', 'Moffeit, K C', 'Mount, R', 'Müller, D R', ""O'Grady, C P"", 'Petrak, S', 'Quinn, Helen R', 'Ratcliff, B N', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Serbo, V V', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Stelzer, J', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Trunov, A G', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'Wisniewski, W J', 'Young, C C', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'Henderson, R', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Prest, M', 'Vallazza, E', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'De, A', 'Silva', 'Kowalewski, R V', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Hu, H', 'Johnson, J R', 'Liu, R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Sekula, S J', 'Von Wimmersperg-Töller, J H', 'Wu, S L', 'Yu, Z', 'Zobernig, H G', 'Kordich, T M B', 'Neal, H']",['Measurement of the decays B-->phi K and B-->phi K^*'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'Phi(1020)', 'K*(892)', 'B0, branching ratio', 'B+, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> Phi(1020) K', 'B --> Phi(1020) K*(892)', 'B+ --> Phi(1020) pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105001'],"['We have observed the decays B-->phi K and phi K^* in a sample of over 45 million B mesons collected with the BABAR detector at the PEP-II collider. The measured branching fractions are BF(B^+ --> phi K^+) = (7.7^{+1.6}_{-1.4}+/- 0.8) x 10^{-6}, BF(B^0 --> phi K^0) = (8.1^{+3.1}_{-2.5}+/- 0.8) x 10^{-6}, BF(B^+ --> phi K^{*+}) = (9.7^{+4.2}_{-3.4}+/- 1.7) x 10^{-6} and BF(B^0 --> phi K^{*0}) = (8.6^{+2.8}_{-2.4}+/- 1.1) x 10^{-6}. We also report the upper limit BF(B^+ --> phi pi^+) < 1.4 x 10^{-6}$ (90% CL).']",['2001-05-02']
206,['eng'],"['Tanaka, J']",['Measurements of Charmed Meson Lifetimes and Search for $D^0$-$\\overline{D}^0$ Mixing with the Belle Experiment'],['Particle Physics - Experimental Results'],"['talk, Ago Town 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, electroproduction', 'charmed meson, hadronic decay', 'particle identification, flavor', 'D0, lifetime', 'D+, lifetime', 'D/s+, lifetime', 'lifetime, ratio', 'D0 anti-D0, interference', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104053'],"['The lifetimes of charmed mesons have been measured using 11.1fb$^{-1} of data collected with the Belle detector at KEKB. Each candidate is fully reconstructed to identify the flavor of the charmed meson. The lifetimes are measured to be $\\tau(D^0)=(414.5\\pm1.7)$ fs, $\\tau(D^+)=(1029\\pm12)$ fs and $\\tau(D_s^+)=(488.4^{+7.8}_{-7.7})$ fs, where the error is statistical only. The mixing parameter $y_{CP}$ is also measured to be $y_{CP}=(1.16^{+1.67}_{-1.65}(stat.))%$ through the lifetime difference of $D^0$ mesons decaying into CP-mixed states and CP eigenstates.']",['2001-05-01']
207,['eng'],"['Sachs, K']",['Tests of QED with Multi-Photonic Final States'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 2001/02/18', 'electron positron, annihilation', 'radiative correction', 'photon, multiple production', 'quantum electrodynamics, validity test', 'channel cross section, energy dependence', 'channel cross section, ratio', 'differential cross section, angular dependence', 'mass spectrum, (2photon)', 'Higgs particle, electroproduction', 'Higgs particle, radiative decay', 'Higgs particle, coupling', 'Higgs particle, mass', 'Higgs particle, width', 'numerical calculations', 'interpretation of experiments, CERN LEP Stor', 'electron positron --> 2photon', 'electron positron --> 3photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104052'],['In the Standard Model the process e+e- -> gamma-gamma is fully described by QED. Measurements of the differential cross-sections from the four LEP experiments are compared to the QED expectation and limits are set on parameters describing physics beyond the Standard Model. Three-photon events are used for a direct search for a photonically decaying resonance produced together with a photon.'],['2001-05-01']
208,['eng'],"['Abe, K', 'Adachi, I', 'Byoung Sup Ahn', 'Aihara, H', 'Akatsu, M', 'Alimonti, G', 'Asano, Y', 'Aso, T', 'Aulchenko, V M', 'Aushev, T', 'Bakich, A M', 'Bartel, W', 'Behari, S', 'Behera, P K', 'Beiline, D', 'Bondar, A E', 'Bozek, A', 'Browder, T E', 'Casey, B C K', 'Chang, P', 'Chao, Y', 'Cheon, B G', 'Choi, S K', 'Choi, Y', 'Eidelman, S', 'Enari, Y', 'Enomoto, R', 'Fang, F', 'Fujii, H', 'Fukunaga, C', 'Fukushima, M', 'Garmash, A', 'Gordon, A', 'Gotow, K', 'Guo, R', 'Haba, J', 'Hamasaki, H', 'Hanagaki, K', 'Handa, F', 'Hara, K', 'Hara, T', 'Hastings, N C', 'Hayashii, H', 'Hazumi, M', 'Heenan, E M', 'Higuchi, I', 'Higuchi, T', 'Hirano, H', 'Hojo, T', 'Hoshi, Y', 'Hou, W S', 'Hsu, S C', 'Huang, H C', 'Igarashi, Y', 'Iijima, T', 'Ikeda, H', 'Inami, K', 'Ishikawa, A', 'Ishino, H', 'Itoh, R', 'Iwai, G', 'Iwasaki, H', 'Iwasaki, Y', 'Jackson, D J', 'Jalocha, P', 'Jang, H K', 'Jones, M', 'Kagan, R', 'Kakuno, H', 'Kaneko, J', 'Kang, J H', 'Kang, J S', 'Katayama, N', 'Kawai, H', 'Kawai, H', 'Kawasaki, T', 'Kichimi, H', 'Kim, D W', 'Hee Joung Kim', 'Kim, H J', 'Hyunwoo Kim', 'Kim, S K', 'Kinoshita, K', 'Kobayashi, S', 'Krokovnyi, P P', 'Kulasiri, R', 'Kumar, S', 'Kuzmin, A', 'Kwon, Y J', 'Lange, J S', 'Lee, M H', 'Lee, S H', 'Liventsev, D', 'Lu, R S', 'Marlow, D', 'Matsubara, T', 'Matsumoto, S', 'Matsumoto, T', 'Miyabayashi, K', 'Miyake, H', 'Miyata, H', 'Moloney, G R', 'Mori, S', 'Mori, T', 'Murakami, A', 'Nagamine, T', 'Nagasaka, Y', 'Nakadaira, T', 'Nakano, E', 'Nakao, M', 'Nam, J W', 'Narita, S', 'Neichi, K', 'Nishida, S', 'Nitoh, O', 'Noguchi, S', 'Nozaki, T', 'Ogawa, S', 'Ohshima, T', 'Okabe, T', 'Okuno, S', 'Olsen, S L', 'Ozaki, H', 'Pakhlov, P', 'Palka, H', 'Park, C S', 'Park, C W', 'Park, H', 'Peak, L S', 'Peters, M', 'Piilonen, L E', 'Rodríguez, J L', 'Root, N', 'Rózanska, M', 'Rybicki, K', 'Ryuko, J', 'Sagawa, H', 'Sakai, Y', 'Sakamoto, H', 'Satapathy, M', 'Satpathy, A', 'Schrenk, S', 'Semenov, S V', 'Senyo, K', 'Sevior, M E', 'Shibuya, H', 'Shwartz, B A', 'Sidorov, V', 'Singh, J B', 'Stanic, S', 'Sugi, A', 'Sugiyama, A', 'Sumisawa, K', 'Sumiyoshi, T', 'Suzuki, J I', 'Suzuki, K', 'Suzuki, S', 'Suzuki, S Y', 'Swain, S K', 'Takahashi, T', 'Takasaki, F', 'Takita, M', 'Tamai, K', 'Tamura, N', 'Tanaka, J', 'Tanaka, M', 'Taylor, G N', 'Teramoto, Y', 'Tomoto, M', 'Tomura, T', 'Tovey, S N', 'Trabelsi, K', 'Tsuboyama, T', 'Tsukamoto, T', 'Uehara, S', 'Ueno, K', 'Unno, Y', 'Uno, S', 'Ushiroda, Y', 'Usov, Y', 'Vahsen, S E', 'Varner, G', 'Varvell, K E', 'Wang Chao Cheng', 'Wang, C H', 'Wang, J G', 'Wang, M Z', 'Watanabe, Y', 'Won, E', 'Yabsley, B D', 'Yamada, Y', 'Yamaga, M', 'Yamaguchi, A', 'Yamamoto, H', 'Yamashita, Y', 'Yamauchi, M', 'Yanaka, S', 'Yokoyama, M', 'Yoshida, K', 'Yusa, Y', 'Yuta, H', 'Zhang, C C', 'Zhang, J', 'Zhao, H W', 'Zheng, Y', 'Zhilich, V N', 'Zontar, D']",['Observation of Cabibbo suppressed $B \\to D^{(*)}K^-$ decays at Belle'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'D*(2010)', 'B, branching ratio', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> D K-', 'B --> D*(2010) K-', 'B --> charmed meson pi-', 'approx. 10.6 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104051', 'http://bsunsrv1.kek.jp/conferences/ICHEP2000/papers/conf0010.ps']","['Cabibbo-suppressed decays $B \\to D^{(*)} K^-$ using a 10.4 fb$^{-1}$ data sample accumulated at the $\\Upsilon(4S)$ resonance with the Belle detector at the KEKB $e^+ e^-$ storage ring. The high-momentum particle identification system of Belle is used to isolate signals for $B\\to D^0 K^-$, $D^+K^-$, $D^{*0}K^-$ and $D^{*+}K^-$ from the $B\\to D^{(*)}\\pi^-$ decay processes which have much larger branching fractions. We report ratios of Cabibbo-suppressed to Cabibbo-favored branching fractions of: ${\\cal B}(B^- \\to D^0 K^-)/{\\cal B}(B^- \\to D^0\\pi^-) = 0.079\\pm0.009\\pm0.006$; ${\\cal B}(\\bar{B^0} \\to D^+ K^-)/{\\cal B}(\\bar{B^0} \\to D^+\\pi^-) = 0.068\\pm0.015\\pm0.007$; ${\\cal B}(B^-\\to D^{*0}K^-)/{\\cal B}(B^-\\to D^{*0}\\pi^-) = 0.078 \\pm 0.019 \\pm 0.009$; and ${\\cal B}(\\bar{B}^0\\to D^{*+}K^-)/{\\cal B}(\\bar{B}^0\\to D^{*+}\\pi^-)= 0.074 \\pm 0.015 \\pm 0.006$. The first error is statistical and the second is systematic. These are the first reported observations of the $B\\to D^+K^-$, $D^{*0}K^-$ and $D^{*+}K^-$ decay processes.']",['2001-05-01']
209,['eng'],"['Wu, N']",['BES R measurements and $J/\\psi$ decays'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'cross section, hadronic', 'energy dependence', 'J/psi(3100), hadronic decay', 'J/psi(3100), branching ratio', 'mass spectrum, (pi+ pi-)', 'sigma meson, search for', 'omega(783)', 'f0(975)', 'f2(1270)', 'magnetic detector, BES', 'experimental results', 'Beijing Stor', 'electron positron --> J/psi(3100)', 'J/psi(3100) --> omega(783) pi+ pi-', '2-5 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104050'],"['R measurement results in 2--5 GeV region by BESII is reported in this talk. The study on $\\sigma$ particle in $J/\\psi \\to \\omega \\pi^+ \\pi^-$, based on $7.8 \\times 10^6$ BESI $J/\\psi$ data, is also reported.']",['2001-05-01']
210,['eng'],"['Boix, G']","['Bs Physics at LEP, SLD, and CDF']",['Particle Physics - Experimental Results'],"['talk, Ago Town 2001/02/19', 'electron positron, annihilation', 'p p, inclusive reaction', 'B/s, electroproduction', 'B/s, hadroproduction', 'B/s, mass difference', 'B/s, width', 'B/s0 anti-B/s0, oscillation', 'B/s, hadronic decay', 'decay, exclusive reaction', 'B/s, semileptonic decay', 'decay, inclusive reaction', 'numerical calculations, interpretation of experiments', 'CERN LEP Stor', 'SLD', 'CDF']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104048'],"['The current status of the experimental knowledge of $\\Bs$ meson physics is reviewed. Results from LEP and CDF on the width difference $\\dgs$ are presented, the corresponding average is found to be in good agreement with the present theoretical estimation. The $\\Bs$ oscillations have not yet been resolved, despite the progress recently achieved by SLD and ALEPH. The world combination, including results from the LEP experiments, SLD and CDF, is presented, together with the expected and observed lower limit on the $\\Bs$ oscillation frequency. A tantalizing hint of an oscillation is observed around $\\dms\\sim17 \\psin$, near future results could increase the significance of this hint.']",['2001-04-30']
211,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Albrecht, Z', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amapane, N', 'Amato, S', 'Anashkin, E', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Anjos, N', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Ballestrero, A', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Behrmann, A', 'Bellunato, T F', 'Belokopytov, Yu A', 'Belous, K S', 'Benekos, N C', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Berntzon, L', 'Bertrand, D', 'Besançon, M', 'Besson, N', 'Bilenky, S M', 'Bloch, D', 'Blom, H M', 'Bol, L', 'Bonesini, M', 'Boonekamp, M', 'Booth, P S L', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bracko, M', 'Branchini, P', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buschmann, P', 'Caccia, M', 'Calvi, M', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chapkin, M M', 'Charpentier, P', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Shlyapnikov, P', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Cieslik, K', 'Collins, P', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Costa, M', 'Crawley, H B', 'Crennell, D J', 'Croix, J', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', ""D'Hondt, J"", 'Dalmau, J', 'Davenport, M', 'Da Silva, W', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Espirito-Santo, M C', 'Fanourakis, G K', 'Fassouliotis, D', 'Feindt, Michael', 'Fernández, J', 'Ferrer, A', 'Ferrer-Ribas, E', 'Ferro, F', 'Firestone, A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Geralis, T', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Grosdidier, G', 'Grzelak, K', 'Guy, J', 'Haag, C', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Hansen, J', 'Harris, F J', 'Haug, S', 'Hauler, F', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hertz, O', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Hughes, G J', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Jeans, D', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Jungermann, L', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kernel, G', 'Kersevan, B P', 'Khokhlov, Yu A', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kinvig, A', 'Kjaer, N J', 'Klapp, O', 'Kluit, P M', 'Kokkinias, P', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kriznic, E', 'Krumshtein, Z', 'Kubinec, P', 'Kucharczyk, M', 'Kurowska, J', 'Lamsa, J W', 'Laugier, J P', 'Leder, Gerhard', 'Ledroit, F', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liebig, W', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Maltezos, S', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Merle, E', 'Meroni, C', 'Meyer, W T', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Moch, M', 'Mönig, K', 'Monge, M R', 'Montenegro, J F', 'Moraes, D', 'Morettini, P', 'Morton, G', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mundim, L M', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Nassiakou, M', 'Navarria, Francesco Luigi', 'Nawrocki, K', 'Negri, P', 'Némécek, S', 'Neufeld, N', 'Nicolaidou, R', 'Niezurawski, P', 'Nikolenko, M', 'Nomokonov, V P', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Österberg, K', 'Ouraou, A', 'Oyanguren, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Peralta, L', 'Perepelitsa, V F', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Poireau, V', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Rehn, J', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Ripp-Baudot, I', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salmi, L', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Savoy-Navarro, Aurore', 'Schwanda, C', 'Schwemling, P', 'Schwering, B', 'Schwickerath, U', 'Scuri, F', 'Sedykh, Yu', 'Segar, A M', 'Sekulin, R L', 'Sette, G', 'Shellard, R C', 'Siebel, M', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Smadja, G', 'Smirnov, N', 'Smirnova, O G', 'Smith, G R', 'Sokolov, A', 'Solovyanov, O', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Squarcia, S', 'Stanescu, C', 'Stanitzki, M', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Taffard, A', 'Tegenfeldt, F', 'Terranova, F', 'Timmermans, J', 'Tinti, N', 'Tkatchev, L G', 'Tobin, M', 'Todorova-Nová, S', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tortosa, P', 'Treille, D', 'Tristram, G', 'Trochimczuk, M', 'Troncon, C', 'Turluer, M L', 'Tyapkin, I A', 'Tyapkin, P', 'Tzamarias, S', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'Van der Velde, C', 'van Dam, P', 'Van den Boeck, W', 'Van Doninck, W K', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Remortel, N', 'Van Vulpen, I B', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verdier, P', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Washbrook, A J', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zinchenko, A I', 'Zoller, P', 'Zumerle, G', 'Zupan, M']",['Measurement of the Mass and Width of the W Boson in $e^+ e^-$ Collisions at $\\sqrt{s}$ = 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, leptonic decay', 'W, hadronic decay', 'W, mass', 'W, width', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'tables', 'electron positron --> W+ W-', 'W --> quark antiquark', 'W --> lepton neutrino', '189 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104047', 'http://delphiwww.cern.ch/~pubxx/delwww/www/delsec/conferences/osaka/paper_658_1.ps.gz']","['A measurement of the W mass and width has been performed by the DELPHI collaboration using the data collected during 1998. The data sample has an integrated luminosity of 155 pb^{-1} and an average centre-of-mass energy of 188.6 GeV. Results are obtained by applying the method of direct reconstruction of the mass of the W from its decay products in both the W+W- -> lvqq and W+W- -> qqqq channels. The W mass result for the 1998 data set is M_W = 80.387 +/- 0.087 (stat) +/- 0.034 (syst) +/- 0.017 (LEP) +/- 0.035 (FSI) GeV/c2, where FSI represents the uncertainty due to final state interaction effects in the qqqq channel, and LEP represents that arising from the knowledge of the beam energy of the accelerator. Combining this result with those previously published by the DELPHI collaboration gives the result M_W = 80.359 +/- 0.074 (stat) +/- 0.032 (syst) +/- 0.017 (LEP) +/- 0.033 (FSI) GeV/c2. The combined value for the W width is \\Gamma_W = 2.266 +/- 0.176 (stat) +/- 0.056 (syst) +/- 0.052 (FSI) GeV/c2.']",['2001-04-28']
212,['eng'],"['Ushiroda, Y']",['Radiative B Meson Decay'],['Particle Physics - Experimental Results'],"['talk, Ago Town 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, radiative decay', 'B, branching ratio', 'upper limit', 'rho(770)', 'K*(892)', 'K*2(1430)', 'production, strangeness', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> K*(892) photon', 'B --> K*2(1430) photon', 'B --> rho(770) photon', 'B --> strangeness photon anything', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104045'],"['We studied radiative B meson decays with the Belle detector. We measured the following branching fractions; Br(B->K*0(892)\\gamma) = (49.6 \\pm 6.7 \\pm 4.5) x 10^{-6}, Br(B->K*+(892)\\gamma) = (38.9 \\pm 9.3 \\pm 4.1) x 10^{-6}, Br(B->Xs\\gamma) = (3.39 \\pm 0.53 \\pm 0.42 +0.51-0.55) x 10^{-4}. We also set an upper limit for B -> \\rho\\gamma as Br(B->\\rho\\gamma)/Br(B->K*(892)\\gamma) < 0.19 at 90% confidence level.']",['2001-04-28']
213,['eng'],"['Alavi-Harati, A', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barker, A R', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hamm, J', 'Hanagaki, K', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jensen, D A', 'Kessler, R', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Shields, J', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Swallow, E C', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Turner, S E', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['Measurements of the rare decay K_{L} -> e^{+} e^{-} e^{+} e^{-}'],['Particle Physics - Experimental Results'],"['K0(L), rare decay', 'intermediate state, (2photon)', 'mass spectrum, (2positron 2electron)', 'angular correlation', 'mass spectrum, (positron electron)', 'violation, CP', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> 2positron 2electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104043'],"['We observe 441 K_{L} -> e^{+} e^{-} e^{+} e^{-} candidate events with a background of 4.2 events and measure B(K_{L} -> e^{+} e^{-} e^{+} e^{-}) = (3.72 \\pm 0.18(stat) \\pm 0.23(syst)) \\times 10^{-8} in the KTeV/E799II experiment at Fermilab. Using the distribution of the angle between the planes of the e^{+} e^{-} pairs, we measure the CP parameters beta_{CP} = -0.23 \\pm 0.09(stat) \\pm 0.02(syst) and gamma_{CP} = -0.09 \\pm 0.09(stat) \\pm 0.02(syst). We also present the first detailed study of the e^{+} e^{-} invariant mass spectrum in this decay mode.']",['2001-04-25']
214,['eng'],"['Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Poling, R A', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Benslama, K', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Alexander, J P', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Mahlke-Krüger, H', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Schwarthoff, H', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R']",['Experimental Investigation of the Two-Photon Widths of the $\\chi_{c0}$ and the $\\chi_{c2}$ Mesons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'chi mesons, charm', 'chi mesons, photoproduction', 'chi mesons, hadronic decay', 'mass spectrum, (2pi+ 2pi-)', 'chi/c0(3415), width', 'chi/c2(3555), width', 'width, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> chi/c0(3415) positron electron', 'electron positron --> chi/c2(3555) positron electron', 'chi mesons --> 2pi+ 2pi-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104042'],"['Using 12.7 $fb^{-1}$ of data collected with the CLEO detector at CESR, we observed two-photon production of the $c \\bar c$ states $\\chi_{c0}$ and $\\chi_{c2}$ in their decay to $\\pi^+ \\pi^- \\pi^+ \\pi^-$. We measured $\\Gamma_{\\gamma\\gamma}(\\chi_{c}) \\times {\\mathcal B}(\\chi_{c} \\to \\pi^+\\pi^-\\pi^+\\pi^-)$ to be 75 +- 13 (stat) +- 8 (syst) eV for the $\\chi_{c0}$ and 6.4 +- 1.8 (stat) +- 0.8 (syst) eV for the $\\chi_{c2}$ implying $\\Gamma_{\\gamma\\gamma}(\\chi_{c0})$ = 3.76 +- 0.65 (stat) +- 0.41 (syst) +- 1.69 (br) keV and $\\Gamma_{\\gamma\\gamma}(\\chi_{c2})$ = 0.53 +- 0.15 (stat) +- 0.06 (syst) +- 0.22 (br) keV. Also, cancelation of dominant experimental and theoretical uncertainties permits a precise comparison of $\\Gamma_{\\gamma\\gamma}(\\chi_{c0})/\\Gamma_{\\gamma\\gamma}(\\chi_{c2})$, evaluated to be 7.4 +- 2.4 (stat) +- 0.5 (syst) +- 0.9 (br), with QCD-based predictions.']",['2001-04-24']
215,['eng'],"['Bozek, A']",['Charmless B Decays Involving Vector Mesons in Belle'],['Particle Physics - Experimental Results'],"['talk, Ise-Shima 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'meson, pair production', 'vector meson', 'pseudoscalar meson', 'B, branching ratio', 'upper limit', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104041'],"['Using the data sample of 10.5 fb-1 collected by the Belle detector, we searched for two-body charmless decays involving vector mesons. The clear signal signature of B+ -> phi K+ is seen and its branching fraction is measured to be (1.39+.32-.30 +- 0.2) X 10-5. The evidence for B+ -> rho pi+, B0 -> rho- pi+ and B+ -> phi K*+ is reported and their branching fractions are determined. No significant signals are observed for B0 -> phi K0S, -> phi K*0, -> rho- K+, B+ -> rho K+, -> omega pi+ and -> omega K+ only the 90% C.L. upper limits are given.']",['2001-04-24']
216,['eng'],"['Yang, U K', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie']",['Extraction of R = sigma_L/sigma_T from CCFR nu_mu-Fe and nubar_mu-Fe differential cross sections'],['Particle Physics - Experimental Results'],"['neutrino nucleus, inclusive reaction', 'antineutrino nucleus, inclusive reaction', 'neutrino/mu', 'iron', 'differential cross section', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'nucleon, structure function', 'quantum chromodynamics, perturbation theory', 'small-x', 'momentum transfer, low', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104040'],['We report on the extraction of R=sigma_L/sigma_T from CCFR nu_mu-Fe and nubar_mu-Fe differential cross sections. The CCFR differential cross sections do not show the deviations from the QCD expectations that are seen in the CDHSW data at very low and very high x. R as measured in nu_mu scattering is in agreement with R as measured in muon and electron scattering. All data on R for Q^2 > 1 GeV^2 are in agreement with a NNLO QCD calculation which includes target mass effects. We report on the first measurements of R in the low x and Q^2 < 1 GeV^2 region (where an anomalous large rise in R for nuclear targets has been observed by the HERMES collaboration).'],['2001-04-24']
217,['eng'],"['Leksanov, A', 'Alster, J', 'Asryan, G A', 'Averichev, Y', 'Barton, D', 'Baturin, V', 'Bukhtoyarova, N', 'Carroll, A', 'Heppelmann, S', 'Kawabata, T', 'Makdisi, Y I', 'Minina, E', 'Navon, I', 'Malki, A', 'Nicholson, H', 'Ogawa, A', 'Panebratsev, Yu A', 'Piasetzky, E', 'Schetkovsky, A', 'Shimansky, S S', 'Tang, A', 'Watson, J W', 'Yoshida, H', 'Zhalov, D']","['Energy Dependence of Nuclear Transparency in C(p,2p) Scattering']",['Particle Physics - Experimental Results'],"['p p, interaction', 'p nucleus, inclusive reaction', 'carbon', 'p, emission', 'color, transparency', 'momentum dependence', 'nucleon, momentum spectrum', 'magnetic spectrometer, experimental results', 'Brookhaven PS', '6.0-14.5 GeV/c, 90 degrees']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104039'],"['The transparency of carbon for (p,2p) quasi-elastic events was measured at beam energies ranging from 6 to 14.5 GeV at 90 degrees c.m. The four momentum transfer squared q*q ranged from 4.8 to 16.9 (GeV/c)**2. We present the observed energy dependence of the ratio of the carbon to hydrogen cross sections. We also apply a model for the nuclear momentum distribution of carbon to normalize this transparency ratio. We find a sharp rise in transparency as the beam energy is increased to 9 GeV and a reduction to approximately the Glauber level at higher energies.']",['2001-04-23']
218,['eng'],"['Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Fleming, B T', 'Frey, R', 'Formaggio, J A', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McDonald, J', 'McNulty, C', 'McFarland, K S', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Suwonjandee, N', 'Tzanov, M', 'Vakili, M', 'Vaitaitis, A G', 'Yang, U K', 'Yu, J', 'Zeller, G P', 'Zimmerman, E D']",['Observation of an Anomalous Number of Dimuon Events in a High Energy Neutrino Deam'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'beryllium', 'neutrino, secondary beam', 'new particle, search for', 'heavy lepton, neutral particle', 'neutrino, sterile', 'neutralino', 'mass, lower limit', 'final state, dimuon', 'final state, (muon electron)', 'final state, (pi muon)', 'production, upper limit', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104037'],"[""A search for long-lived neutral particles (N^0's) with masses above 2.2 GeV/c^2 that decay into at least one muon has been performed using an instrumented decay channel at the NuTeV experiment at Fermilab. Data were examined for particles decaying into the final states mu mu, mu e, and mu pi. Three mu mu events were observed over an expected Standard Model background of 0.069 +/- 0.010 events; no events were observed in the other modes.""]",['2001-04-20']
219,['eng'],"['Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Sartorelli, G', 'Zichichi, Antonino', 'Aghuzumtsyan, G', 'Brock, I', 'Goers, S', 'Hartmann, H', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Kind, O', 'Paul, E', 'Rautenberg, J', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Brook, N H', 'Cole, J E', 'Foster, B', 'Heath, G P', 'Heath, H F', 'Robins, S A', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Wing, M', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Helbich, M', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowal, M', 'Kowalski, T', 'Mindur, B', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Borras, K', 'Chiochia, V', 'Crittenden, J A', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Geiser, A', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hebbel, K', 'Hillert, S', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Labes, H', 'Löhr, B', 'Mankel, R', 'Martens, J', 'Martínez, M', 'Milite, M', 'Moritz, M', 'Notz, D', 'Petrucci, M C', 'Polini, A', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Stonjek, S', 'Wolf, G', 'Wollmer, U', 'Whitmore, J J', 'Wichmann, R', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Bamberger, Andreas', 'Benen, A', 'Coppola, N', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bell, M', 'Bussey, Peter J', 'Doyle, A T', 'Glasman, C', 'Lee, S W', 'Lupi, A', 'McCance, G J', 'Saxon, D H', 'Skillicorn, Ian O', 'Bodmann, B', 'Gendner, N', 'Holm, U', 'Salehi, H', 'Wick, K', 'Yildirim, A', 'Ziegler, A', 'Carli, T', 'Garfagnini, A', 'Gialas, I', 'Lohrmann, E', 'Foudas, C', 'Goncalo, R', 'Long, K R', 'Metlica, F', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Barakbaev, A N', 'Boos, E G', 'Pokrovskiy, N S', 'Zhautykov, B O', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Son, D', 'Barreiro, F', 'García, G', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Vázquez, M E', 'Barbi, M S', 'Corriveau, F', 'Padhi, S', 'Stairs, D G', 'Tsurugai, T', 'Antonov, A', 'Bashkirov, V', 'Danilov, P', 'Dolgoshein, B A', 'Gladkov, D', 'Sosnovtsev, V V', 'Suchkov, S', 'Dementiev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Levchenko, B B', 'Lukina, O Yu', 'Proskuryakov, A S', 'Shcheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tassi, E', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Brümmer, N', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Ferrando, J', 'Grosse-Knetter, J', 'Matsushita, T', 'Rigby, M', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dusini, S', 'Limentani, S', 'Longhin, A', 'Parenti, A', 'Posocco, M', 'Stanco, L', 'Turcato, M', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Saull, P R B', 'Toothacker, W S', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Williams, D C', 'Park, I H', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Gabareen, A', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Kohno, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Matsuzawa, K', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Mirea, A', 'Sabetfakhri, A', 'Butterworth, J M', 'Gwenlan, C', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Plucinsky, P P', 'Smalska, B', 'Tymieniecka, T', 'Ukleja, J', 'Zakrzewski, J A', 'Adamus, M', 'Sztuk, J', 'Deppe, O', 'Eisenberg, Y', 'Gladilin, L K', 'Hochman, D', 'Karshon, U', 'Breitweg, J', 'Chapin, D', 'Cross, R', 'Kcira, D', 'Lammers, S', 'Reeder, D D', 'Smith, W H', 'Deshpande, A A', 'Dhawan, S K', 'Straub, V W', 'Hughes, P B', 'Bhadra, S', 'Catterall, C D', 'Frisken, W R', 'Hall-Wilton, R', 'Khakzad, M', 'Menary, S R']",['Multiplicity moments in deep inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, electroproduction', 'charged particle, multiplicity', 'multiplicity, moment', 'angular dependence', 'momentum dependence', 'transverse momentum, dependence', 'quantum chromodynamics, perturbation theory', 'duality, parton hadron', 'effect, hadronization', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104036'],"['Multiplicity moments of charged particles in deep inelastic E+P scattering have been measured with the ZEUS detector at HERA using an integrated luminosity of 38.4 pb^{-1}$. The moments for Q^2 > 1000 GeV^2 were studied in the current region of the Breit frame. The evolution of the moments was investigated as a function of restricted regions in polar angle and, for the first time, both in the transverse momentum and in absolute momentum of final-state particles. Analytic perturbative QCD predictions in conjunction with the hypothesis of Local Parton-Hadron Duality (LPHD) reproduce the trends of the moments in polar-angle regions, although some discrepancies are observed. For the moments restricted either in transverse or absolute momentum, the analytic results combined with the LPHD hypothesis show considerable deviations from the measurements. The study indicates a large influence of the hadronisation stage on the multiplicity distributions in the restricted phase-space regions studied here, which is inconsistent with the expectations of the LPHD hypothesis.']",['2001-04-20']
220,['eng'],"['Krcmar, M', 'Krecak, Z', 'Ljubicic, A', 'Stipcevic, M', 'Bradley, D A']",['A Novel Approach to the Search for Solar Axions Using Li-7'],['Particle Physics - Experimental Results'],"['axion, solar', 'axion, search for', 'strong interaction, CP', 'scattering, axion nucleus', 'lithium, excited nucleus', 'energy levels, transition', 'transition, magnetic', 'photon, energy spectrum', 'axion, mass', 'upper limit', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104035'],"['We describe a novel approach to the search for solar, near-monochromatic hadronic axions, the latter being suggested to be created in the solar core during M1 transitions between the first excited level of Li-7, at 478 keV, and the ground state. As a result of Doppler broadening, in principle these axions can be detected via resonant absorption by the same nuclide on the Earth. Excited nuclei of Li-7 are produced in the solar interior by Be-7 electron capture and thus the axions are accompanied by emission of Be-7 solar neutrinos of energy 384 keV. An experiment was made which has yielded an upper limit on hadronic axion mass of 32 keV at the 95% confidence level.']",['2001-04-20']
221,['eng'],"['Suleymanov, M K', 'Abdinov, O B', 'Angelov, N S', 'Vodopyanov, A S']",['Transition to the region of central collisions and critical phenomena'],['Particle Physics - Experimental Results'],"['p nucleus, nuclear reaction', 'nucleus nucleus, nuclear reaction', 'helium', 'carbon', 'dependence, impact parameter', 'hadron, multiple production', 'nucleus, fragmentation', 'critical phenomena', 'quark gluon, string model', 'charge, dependence', 'positive particle, multiplicity', 'pi-, multiplicity', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104033'],['The experimental results on the relation between the processes of total disintegration of nuclei (or the cases with central collisions) and the critical phenomena which can occur in the region of high degree of nuclear disintegration or of collision centrality are discussed.'],['2001-04-19']
222,['eng'],"['Back, B B', 'Baker, M D', 'Barton, D S', 'Betts, R R', 'Bindel, R', 'Budzanowski, A', 'Busza, W', 'Carroll, A', 'Decowski, M P', 'García, E', 'George, N', 'Gulbrandsen, K H', 'Gushue, S', 'Halliwell, C', 'Heintzelman, G A', 'Henderson, C', 'Holynski, R', 'Hofman, D J', 'Holzman, B', 'Johnson, E', 'Kane, J', 'Katzy, J M', 'Khan, N A', 'Kucewicz, W', 'Kulinich, P A', 'Lin, W T', 'Manly, S L', 'McLeod, D', 'Michalowski, J', 'Mignerey, A C', 'Mülmenstädt, J', 'Nouicer, R', 'Olszewski, A', 'Pak, R', 'Park, I C', 'Pernegger, H', 'Reed, C', 'Remsberg, L P', 'Reuter, M', 'Roland, C', 'Roland, G', 'Rosenberg, L J', 'Sarin, P', 'Sawicki, P', 'Skulski, W', 'Steadman, S G', 'Stephans, G S F', 'Steinberg, P', 'Stodulski, M', 'Sukhanov, A', 'Tang, J L', 'Teng, R', 'Trzupek, A', 'Vale, C J', 'van Nieuwenhuizen, G J', 'Verdier, R', 'Wadsworth, B', 'Wolfs, F L H', 'Wosiek, B', 'Wozniak, K', 'Wuosmaa, A H', 'Wyslouch, B']",['Ratios of charged antiparticles to particles near mid-rapidity in Au+Au collisions at sqrt(s_NN) = 130 GeV'],['Particle Physics - Experimental Results'],"['nucleus nucleus, colliding beams', 'scattering, heavy ion', 'gold', 'charged particle, multiple production', 'yield, (particle antiparticle)', 'pi', 'K', 'p', 'potential, chemical', 'energy loss, momentum dependence', 'magnetic detector, PHOBOS', 'experimental results', 'Brookhaven RHIC Coll', '130 GeV-cms/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104032'],"['We have measured the ratios of antiparticles to particles for charged pions, kaons and protons near mid-rapidity in central Au+Au collisions at sqrt(s_NN) = 130 GeV. For protons, we observe pbar/p = 0.60 +/- 0.04 (stat.) +/- 0.06 (syst.) in the transverse momentum range 0.15 < p_T < 1.0 GeV/c. This leads to an estimate of the baryo-chemical potential mu_B of 45 MeV, a factor of 5-6 smaller than in central Pb+Pb collisions at sqrt(s_NN) = 17.2 GeV.']",['2001-04-19']
223,['eng'],"['Hadig, T']",['ep Physics at High Q-squared'],['Particle Physics - Experimental Results'],"['review, Stanford 2000/08/14', 'electron p, colliding beams', 'positron p, colliding beams', 'electron p, inclusive reaction', 'positron p, inclusive reaction', 'momentum transfer, high', 'neutral current', 'charged current', 'differential cross section, momentum transfer', 'interference, (Z0 photon)', 'p, structure function', 'electroweak interaction, validity test', 'lepton quark, interaction', 'resonance, search for', 'supersymmetry', 'R parity, violation', 'leptoquark', 'quark, truth', 'final state, (jet lepton missing-energy)', 'magnetic detector, ZEUS', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104031'],"['This article summarizes a talk presented at the SLAC Summer Institute 2000, SLAC, Stanford, USA. The HERA ep collider allows the measurement of the proton structure and tests of the Standard Model in a large region of phase space that has not been accessible before. Such tests provide the framework for the H1 and ZEUS Collaborations to look for physics beyond the Standard Model.']",['2001-04-18']
224,['eng'],"['Abe, K', 'Abe, K', 'Adachi, I', 'Byoung Sup Ahn', 'Aihara, H', 'Akatsu, M', 'Alimonti, G', 'Asano, Y', 'Aso, T', 'Aulchenko, V M', 'Aushev, T', 'Bakich, A M', 'Bartel, W', 'Behari, S', 'Behera, P K', 'Beiline, D', 'Bondar, A E', 'Bozek, A', 'Browder, T E', 'Casey, B C K', 'Chang, P', 'Chao, Y', 'Chen, K F', 'Cheon, B G', 'Choi, S K', 'Choi, Y', 'Eidelman, S', 'Enari, Y', 'Enomoto, R', 'Fang, F', 'Fujii, H', 'Fukushima, M', 'Garmash, A', 'Gordon, A', 'Gotow, K', 'Guo, R', 'Haba, J', 'Hamasaki, H', 'Hanagaki, K', 'Handa, F', 'Hara, K', 'Hara, T', 'Hastings, N C', 'Hayashii, H', 'Hazumi, M', 'Heenan, E M', 'Higuchi, I', 'Higuchi, T', 'Hirano, H', 'Hojo, T', 'Hoshi, Y', 'Hou, W S', 'Hsu, S C', 'Huang, H C', 'Igarashi, Y', 'Iijima, T', 'Ikeda, H', 'Inami, K', 'Ishikawa, A', 'Ishino, H', 'Itoh, R', 'Iwai, G', 'Iwasaki, H', 'Iwasaki, Y', 'Jackson, D J', 'Jalocha, P', 'Jang, H K', 'Jones, M', 'Kakuno, H', 'Kaneko, J', 'Kang, J H', 'Kang, J S', 'Katayama, N', 'Kawai, H', 'Kawai, H', 'Kawasaki, T', 'Kichimi, H', 'Kim, D W', 'Hee Joung Kim', 'Kim, H J', 'Hyunwoo Kim', 'Kim, S K', 'Kinoshita, K', 'Kobayashi, S', 'Krokovnyi, P P', 'Kulasiri, R', 'Kumar, S', 'Kuzmin, A', 'Kwon, Y J', 'Lange, J S', 'Lee, M H', 'Lee, S H', 'Liventsev, D', 'Lu, R S', 'Marlow, D', 'Matsubara, T', 'Matsumoto, S', 'Matsumoto, T', 'Mikami, Y', 'Miyabayashi, K', 'Miyake, H', 'Miyata, H', 'Moloney, G R', 'Mori, S', 'Mori, T', 'Murakami, A', 'Nagamine, T', 'Nagasaka, Y', 'Nakadaira, T', 'Nakano, E', 'Nakao, M', 'Nam, J W', 'Narita, S', 'Nishida, S', 'Nitoh, O', 'Noguchi, S', 'Nozaki, T', 'Ogawa, S', 'Ohshima, T', 'Okabe, T', 'Okuno, S', 'Olsen, S L', 'Ozaki, H', 'Pakhlov, P', 'Palka, H', 'Park, C S', 'Park, C W', 'Park, H', 'Peak, L S', 'Peters, M', 'Piilonen, L E', 'Rodríguez, J L', 'Root, N', 'Rózanska, M', 'Rybicki, K', 'Ryuko, J', 'Sagawa, H', 'Sakai, Y', 'Sakamoto, H', 'Satapathy, M', 'Satpathy, A', 'Schrenk, S', 'Semenov, S V', 'Senyo, K', 'Sevior, M E', 'Shibuya, H', 'Shwartz, B A', 'Sidorov, V', 'Singh, J B', 'Stanic, S', 'Sugi, A', 'Sugiyama, A', 'Sumisawa, K', 'Sumiyoshi, T', 'Suzuki, J I', 'Suzuki, K', 'Suzuki, S', 'Suzuki, S Y', 'Swain, S K', 'Tajima, H', 'Takahashi, T', 'Takasaki, F', 'Takita, M', 'Tamai, K', 'Tamura, N', 'Tanaka, J', 'Tanaka, M', 'Taylor, G N', 'Teramoto, Y', 'Tomoto, M', 'Tomura, T', 'Tovey, S N', 'Trabelsi, K', 'Tsuboyama, T', 'Tsukamoto, T', 'Uehara, S', 'Ueno, K', 'Unno, Y', 'Uno, S', 'Ushiroda, Y', 'Usov, Y', 'Vahsen, S E', 'Varner, G', 'Varvell, K E', 'Wang Chao Cheng', 'Wang, C H', 'Wang, J G', 'Wang, M Z', 'Watanabe, Y', 'Won, E', 'Yabsley, B D', 'Yamada, Y', 'Yamaga, M', 'Yamaguchi, A', 'Yamamoto, H', 'Yamashita, Y', 'Yamauchi, M', 'Yanaka, S', 'Yokoyama, M', 'Yusa, Y', 'Yuta, H', 'Zhang, C C', 'Zhang, J', 'Zhao, H W', 'Zheng, Y', 'Zhilich, V N', 'Zontar, D']","['Measurement of Branching Fractinos for B->\\pi\\pi, K\\pi and KK Decays']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B0, branching ratio', 'B+, branching ratio', 'upper limit', 'final state, (0charm)', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> 2p', 'B --> K p', 'B --> 2K', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104030'],"['We report measurements of the branching fractions for $B^0\\to\\pi^+\\pi^-$, $K^+\\pi^-$, $K^+K^-$ and $K^0\\pi^0$, and $B^+\\to\\pi^+\\pi^0$, $K^+\\pi^0$, $K^0\\pi^+$ and $K^+\\overline{K}{}^0$. The results are based on 10.4 fb$^{-1}$ of data collected on the $\\Upsilon$(4S) resonance at the KEKB $e^+e^-$ storage ring with the Belle detector, equipped with a high momentum particle identification system for clear separation of charged $\\pi$ and $K$ mesons. We find ${\\cal B}(B^0\\to\\pi^+\\pi^-) =(0.56^{+0.23}_{-0.20}\\pm 0.04)\\times 10^{-5}$ ${\\cal B}(B^0\\to K^+\\pi^-) =(1.93^{+0.34 +0.15}_{-0.32 -0.06})\\times 10^{-5}$, ${\\cal B}(B^+\\to K^+\\pi^0) =(1.63^{+0.35 +0.16}_{-0.33 -0.18})\\times 10^{-5}$, ${\\cal B}(B^+\\to K^0\\pi^+) =(1.37^{+0.57 +0.19}_{-0.48 -0.18})\\times 10^{-5}$, and ${\\cal B}(B^0\\to K^0\\pi^0) =(1.60^{+0.72 +0.25}_{-0.59 -0.27})\\times 10^{-5}$, where the first and second errors are statistical and systematic. We also set upper limits of ${\\cal B}(B^+\\to\\pi^+\\pi^0)<1.34\\times 10^{-5}$, ${\\cal B}(B^0\\to K^+K^-)<0.27\\times 10^{-5}$, and ${\\cal B}(B^+\\to K^+\\overline{K}{}^0)<0.50\\times 10^{-5}$ at the 90% confidence level.']",['2001-04-18']
225,['eng'],"['Formaggio, J A', 'Yu, J', 'Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J M', 'Drucker, R B', 'Fleming, B T', 'Foster, J', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McDonald, J', 'McFarland, K S', 'McNulty, C', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H M', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Suwonjandee, N', 'Vakili, M', 'Vaitaitis, A G', 'Yang, U K', 'Zeller, G P', 'Zimmerman, E D']",['Search for the Lepton Number Violating Process nu_mu-bar e^- -> mu^- nu_e-bar'],['Particle Physics - Experimental Results'],"['neutrino, secondary beam', 'antineutrino electron, interaction', 'neutrino electron, interaction', 'neutrino/mu', 'flavor, violation', 'weak interaction, model', 'channel cross section, ratio', 'upper limit', 'experimental results', 'Batavia TEVATRON PS', 'antineutrino/mu electron --> muon- antineutrino/e', 'neutrino/mu electron --> muon- neutrino/e', '800 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104029'],"['The NuTeV experiment at Fermilab has used a sign-selected neutrino beam to perform a search for the lepton number violating process nu_mu-bar e^- -> mu^- nu_e-bar, and to measure the cross-section of the Standard Model inverse muon decay process nu_mu e^- -> mu^- nu_e. NuTeV measures the inverse muon decay asymptotic cross-section sigma/E to be 13.8 +/- 1.2 +/- 1.4 x 10^-42 cm^2/GeV. The experiment also observes no evidence for lepton number violation and places one of the most restrictive limits on the LNV/IMD cross-section ratio at < 1.7% at 90% C.L. for V-A couplings and < 0.6% for scalar couplings.']",['2001-04-17']
226,['eng'],"['Höcker, A']",['Hadronic B Decays to Charmless Final States and to J/psi K*'],['Particle Physics - Experimental Results'],"['talk, Ise-Shima 2000/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'J/psi(3100)', 'final state, (0charm)', 'B, branching ratio', 'upper limit', 'decay, amplitude analysis', 'final-state interaction', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> J/psi(3100) K*(892)', 'B0 --> pi+ pi-', 'B0 --> K+ pi-', 'B0 --> K+ K-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104028'],"['Preliminary results from the BABAR experiment on charmless B decays to charged pions or kaons, and the measurement of the B -> J/psi K* decay amplitudes are presented. The data sample, collected at the asymmetric-energy B-factory PEP-II at SLAC, comprises a total number of 22.7 million Y(4S) decays, corresponding to an integrated on-resonance luminosity of approximately 21 fb-1. We measure the following CP-averaged branching fractions: BR(B -> pi+pi-) = (4.1 +- 1.0(stat) +- 0.7(sys))xE-6 BR(B -> K+pi-) = (16.7 +- 1.6(stat) +1.2-1.7(sys))xE-6 and an upper limit of BR(B -> K+K-) < 2.5xE-6, at 90% confidence limit. The measurement of the J/psi K* decay amplitudes results in R_\\perp = 0.160 +- 0.032(stat) +- 0.036(sys), and reveals a dominant longitudinal component. The phase of the longitudinal amplitude shows evidence for non-vanishing final state interaction.']",['2001-04-16']
227,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Albrecht, Z', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amapane, N', 'Amato, S', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Ballestrero, A', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Behrmann, A', 'Beillière, P', 'Belokopytov, Yu A', 'Belous, K S', 'Benekos, N C', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Berntzon, L', 'Bertrand, D', 'Besançon, M', 'Bilenky, S M', 'Bizouard, M A', 'Bloch, D', 'Blom, H M', 'Bonesini, M', 'Boonekamp, M', 'Booth, P S L', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bourdarios, C', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Bracko, M', 'Branchini, P', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buran, T', 'Buschbeck, Brigitte', 'Buschmann, P', 'Cabrera, S', 'Caccia, M', 'Calvi, M', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chapkin, M M', 'Charpentier, P', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Shlyapnikov, P', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Cieslik, K', 'Collins, P', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Costa, M', 'Crawley, H B', 'Crennell, D J', 'Crépé, S', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', ""D'Hondt, J"", 'Dalmau, J', 'Davenport, M', 'Da Silva, W', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Dolbeau, J', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Duperrin, A', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Espirito-Santo, M C', 'Fanourakis, G K', 'Fassouliotis, D', 'Feindt, Michael', 'Fernández, J', 'Ferrer, A', 'Ferrer-Ribas, E', 'Ferro, F', 'Firestone, A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Geralis, T', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Gris, P', 'Grosdidier, G', 'Grzelak, K', 'Guy, J', 'Haag, C', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Hansen, J', 'Harris, F J', 'Hauler, F', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Huber, M', 'Hughes, G J', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Janik, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Jeans, D', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Jungermann, L', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kernel, G', 'Kersevan, B P', 'Khokhlov, Yu A', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kinvig, A', 'Kjaer, N J', 'Klapp, O', 'Klein, H', 'Kluit, P M', 'Kokkinias, P', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kriznic, E', 'Krumshtein, Z', 'Kubinec, P', 'Kurowska, J', 'Kurvinen, K L', 'Lamsa, J W', 'Lane, D W', 'Lapin, V', 'Laugier, J P', 'Lauhakangas, R', 'Leder, Gerhard', 'Ledroit, F', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liebig, W', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Lörstad, B', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Maltezos, S', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Meroni, C', 'Meyer, W T', 'Myagkov, A', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Moch, M', 'Møller, R', 'Mönig, K', 'Monge, M R', 'Moraes, D', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mulet-Marquis, C', 'Muresan, R', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Naraghi, F', 'Nassiakou, M', 'Navarria, Francesco Luigi', 'Nawrocki, K', 'Negri, P', 'Neufeld, N', 'Nicolaidou, R', 'Nielsen, B S', 'Niezurawski, P', 'Nikolenko, M', 'Nomokonov, V P', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Orazi, G', 'Österberg, K', 'Ouraou, A', 'Oyanguren, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Pavel, T', 'Pegoraro, M', 'Peralta, L', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Poireau, V', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Rames, J', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Rehn, J', 'Reid, D', 'Reinertsen, P L', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Ripp-Baudot, I', 'Røhne, O M', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Savoy-Navarro, Aurore', 'Schwemling, P', 'Schwering, B', 'Schwickerath, U', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Seibert, N', 'Sekulin, R L', 'Sette, G', 'Shellard, R C', 'Siebel, M', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Smadja, G', 'Smirnova, O G', 'Smith, G R', 'Solovyanov, O', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Squarcia, S', 'Stanescu, C', 'Stanitzki, M', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Taffard, A', 'Tegenfeldt, F', 'Terranova, F', 'Timmermans, J', 'Tinti, N', 'Tkatchev, L G', 'Tobin, M', 'Todorova-Nová, S', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tortosa, P', 'Tranströmer, G', 'Treille, D', 'Tristram, G', 'Trochimczuk, M', 'Troncon, C', 'Turluer, M L', 'Tyapkin, I A', 'Tyapkin, P', 'Tzamarias, S', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'van Dam, P', 'Van den Boeck, W', 'Van Doninck, W K', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Remortel, N', 'Van Vulpen, I B', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verdier, P', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Walck, C', 'Washbrook, A J', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zinchenko, A I', 'Zoller, P', 'Zumerle, G', 'Zupan, M']",['Measurement of $V_{cb}$ from the decay process $\\bar{B^0} \\to D^{*+} \\ell^- \\bar{\\nu}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'anti-B0, semileptonic decay', 'anti-B0, branching ratio', 'Kobayashi-Maskawa angle', 'form factor, decay', 'Isgur-Wise function', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'anti-B0 --> D*(2010) lepton antineutrino', 'D*(2010) --> D0 pi+', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104026'],"['A new precise measurement of |V_{cb}| and of the branching ratio BR(\\bar{B^0} -> D^{*+} \\ell^- \\bar{\\nu_\\ell}) has been performed using a sample of about 5000 semileptonic decays \\bar{B^0} -> D^{*+} \\ell^- \\bar{\\nu_\\ell}, selected by the DELPHI detector at LEP I by tagging the soft pion from D^{*+} -> D^0 \\pi^+. The results are: V_{cb}=(39.0 +/- 1.5 (stat.) ^{+2.5}_{-2.6} (syst. exp.) +/- 1.3 (syst. th.)) x 10^{-3} BR(\\bar{B^0} -> D^{*+} \\ell^- \\bar{\\nu_\\ell})=(4.70 +/- 0.13 (stat.) ^{+0.36} _{-0.31} (syst. exp.))% The analytic dependences of the differential cross-section and of the Isgur Wise form factor as functions of the variable w = v_{B^0}.v_{D^*} have also been obtained by unfolding the experimental resolution.']",['2001-04-16']
228,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Ajinenko, I', 'Albrecht, Z', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amapane, N', 'Amato, S', 'Anashkin, E', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Anjos, N', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Ballestrero, A', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Behrmann, A', 'Belokopytov, Yu A', 'Benekos, N C', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Berntzon, L', 'Bertrand, D', 'Besançon, M', 'Besson, N', 'Bilenky, S M', 'Bloch, D', 'Blom, H M', 'Bol, L', 'Bonesini, M', 'Boonekamp, M', 'Booth, P S L', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Bracko, M', 'Branchini, P', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buschmann, P', 'Caccia, M', 'Calvi, M', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chapkin, M M', 'Charpentier, P', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Shlyapnikov, P', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Cieslik, K', 'Collins, P', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Costa, M', 'Crawley, H B', 'Crennell, D J', 'Croix, J', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', ""D'Hondt, J"", 'Dalmau, J', 'Davenport, M', 'Da Silva, W', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Espirito-Santo, M C', 'Fanourakis, G K', 'Fassouliotis, D', 'Feindt, Michael', 'Fernández, J', 'Ferrer, A', 'Ferrer-Ribas, E', 'Ferro, F', 'Firestone, A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Geralis, T', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Grosdidier, G', 'Grzelak, K', 'Guy, J', 'Haag, C', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Hansen, J', 'Harris, F J', 'Haug, S', 'Hauler, F', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hertz, O', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Hughes, G J', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Jeans, D', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Jungermann, L', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kernel, G', 'Kersevan, B P', 'Khokhlov, Yu A', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kinvig, A', 'Kjaer, N J', 'Klapp, O', 'Kluit, P M', 'Kokkinias, P', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kriznic, E', 'Krumshtein, Z', 'Kubinec, P', 'Kucharczyk, M', 'Kurowska, J', 'Lamsa, J W', 'Laugier, J P', 'Leder, Gerhard', 'Ledroit, F', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lemonne, J', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liebig, W', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Maltezos, S', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Merle, E', 'Meroni, C', 'Meyer, W T', 'Myagkov, A', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Moch, M', 'Mönig, K', 'Monge, M R', 'Montenegro, J F', 'Moraes, D', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mundim, L M', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Nassiakou, M', 'Navarria, Francesco Luigi', 'Nawrocki, K', 'Negri, P', 'Némécek, S', 'Neufeld, N', 'Nicolaidou, R', 'Niezurawski, P', 'Nikolenko, M', 'Nomokonov, V P', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Österberg, K', 'Ouraou, A', 'Oyanguren, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Peralta, L', 'Perepelitsa, V F', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Poireau, V', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Rehn, J', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Ripp-Baudot, I', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Rovelli, T', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salmi, L', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Savoy-Navarro, Aurore', 'Schwanda, C', 'Schwemling, P', 'Schwering, B', 'Schwickerath, U', 'Scuri, F', 'Sedykh, Yu', 'Segar, A M', 'Sekulin, R L', 'Sette, G', 'Shellard, R C', 'Siebel, M', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Smadja, G', 'Smirnov, N', 'Smirnova, O G', 'Smith, G R', 'Solovyanov, O', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Squarcia, S', 'Stanescu, C', 'Stanitzki, M', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Taffard, A', 'Tegenfeldt, F', 'Terranova, F', 'Timmermans, J', 'Tinti, N', 'Tkatchev, L G', 'Tobin, M', 'Todorova-Nová, S', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tortosa, P', 'Treille, D', 'Tristram, G', 'Trochimczuk, M', 'Troncon, C', 'Turluer, M L', 'Tyapkin, I A', 'Tyapkin, P', 'Tzamarias, S', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'van Dam, P', 'Van den Boeck, W', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Remortel, N', 'Van Vulpen, I B', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verdier, P', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Washbrook, A J', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zinchenko, A I', 'Zoller, P', 'Zumerle, G', 'Zupan, M']",['Search for a fermiophobic Higgs at LEP 2'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, neutral particle', 'Higgs particle, multiplet', 'doublet, 2', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, pair production', 'Higgs particle, radiative decay', 'Higgs particle, hadronic decay', 'final state, ((n)photon)', 'final state, (quark antiquark (n)photon)', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104025'],"['Higgs bosons predicted by the fermiophobic scenario within Two Higgs Doublets Models were searched for in the data collected by the DELPHI detector at centre-of-mass energies between 189 GeV and 202 GeV, corresponding to a total integrated luminosity of 380 pb^{-1}. No signal was found and confidence limits were derivedwska, Agni']",['2001-04-16']
229,['eng'],"['Huang, H C']",['K+K- and KsKs Production in Two-Photon Collisions at Belle'],['Particle Physics - Experimental Results'],"['talk, Ise-Shima 2001/02/19', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'K, pair production', 'mass spectrum, (K+ K-)', 'mass spectrum, (2K0(S))', 'f2(1525)', 'mass enhancement, (1750)', 'f4(2220)', 'partial wave analysis', 'width, branching ratio', 'upper limit', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'electron positron --> K+ K- positron electron', 'electron positron --> 2K0(S) positron electron', '10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104024'],"['The production of a kaon pair ($K^+ K^-$ and $K^0_S K^0_S$) in two-photon processes has been measured using the Belle detector at the electron-positron collider KEKB. We have obtained the invariant-mass distribution of the processes between 1.3 and 2.3 GeV. A broad bump structure around 1.7 GeV in the $K^0_S K^0_S$ channel is confirmed, while, in the $K^+ K^-$ channel, a bump structure is seen near 1.9 GeV. The angular distribution of the final-state kaons is analyzed to explore the spin(-helicity) structure in each invariant-mass region for the two processes. Contributions from existing and postulated resonances are discussed.']",['2001-04-16']
230,['eng'],"['Maravin, Y']",['Search for CP violation in tau decays'],['Particle Physics - Experimental Results'],"['talk, Nashville 2001/03/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'amplitude analysis', 'invariance, CP', 'scalar particle, exchange', 'Higgs particle, multiplet', 'experimental results', 'magnetic detector, CLEO', 'Cornell CESR Stor', 'magnetic detector, BELLE', 'KEK TRISTAN Stor', 'tau --> pi pi0 neutrino/tau', 'tau --> K pi neutrino/tau', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104023'],"['The results of the searches for CP non-conservation in the decays of tau leptons are presented. No evidence of violation of CP symmetry is observed neither in CLEO nor in BELLE data. Interpretation of these results is done within the framework of a model with a scalar boson exchange. Limits on the imaginary part of the coupling constant \\Lambda, parameterizing the relative contribution of diagrams that would lead to CP violation, are -0.046 <\\Im(\\Lambda) < 0.022 at 90% C.L. and |\\Im(\\Lambda)| < 1.7 at 90% C.L. in tau-> pi pi^0 nu_{\\tau} and tau-> K pi^0 nu_{\\tau} modes, respectively.']",['2001-04-12']
231,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Albrecht, Z', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amapane, N', 'Amato, S', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Behrmann, A', 'Beillière, P', 'Belokopytov, Yu A', 'Belous, K S', 'Benekos, N C', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Bertini, D', 'Bertrand, D', 'Besançon, M', 'Bigi, M', 'Bilenky, S M', 'Bizouard, M A', 'Bloch, D', 'Blom, H M', 'Bonesini, M', 'Boonekamp, M', 'Booth, P S L', 'Borgland, A W', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bourdarios, C', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Bracko, M', 'Branchini, P', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buran, T', 'Buschbeck, Brigitte', 'Buschmann, P', 'Cabrera, S', 'Caccia, M', 'Calvi, M', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chabaud, V', 'Chapkin, M M', 'Charpentier, P', 'Chaussard, L', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Shlyapnikov, P', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Cieslik, K', 'Collins, P', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Crawley, H B', 'Crennell, D J', 'Crépé, S', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', 'Dalmau, J', 'Davenport, M', 'Da Silva, W', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Dolbeau, J', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Duperrin, A', 'Durand, J D', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ekspong, Gösta', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Espirito-Santo, M C', 'Fanourakis, G K', 'Fassouliotis, D', 'Fayot, J', 'Feindt, Michael', 'Ferrer, A', 'Ferrer-Ribas, E', 'Ferro, F', 'Fichet, S', 'Firestone, A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Gris, P', 'Grosdidier, G', 'Grzelak, K', 'Guy, J', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Hansen, J', 'Harris, F J', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hessing, T L', 'Heuser, J M', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Huber, M', 'Huet, K', 'Hughes, G J', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Janik, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Jeans, D', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Jungermann, L', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kernel, G', 'Kersevan, B P', 'Khokhlov, Yu A', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kinvig, A', 'Kjaer, N J', 'Klapp, O', 'Klein, H', 'Kluit, P M', 'Kokkinias, P', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kriznic, E', 'Krumshtein, Z', 'Kubinec, P', 'Kurowska, J', 'Kurvinen, K L', 'Lamsa, J W', 'Lane, D W', 'Lapin, V', 'Laugier, J P', 'Lauhakangas, R', 'Leder, Gerhard', 'Ledroit, F', 'Lefébure, V', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lemonne, J', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liebig, W', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Lörstad, B', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Malmgren, T G M', 'Maltezos, S', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Martínez-Vidal, F', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Meroni, C', 'Meyer, W T', 'Myagkov, A', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Moch, M', 'Møller, R', 'Mönig, K', 'Monge, M R', 'Moreau, X', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mulet-Marquis, C', 'Muresan, R', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Naraghi, F', 'Nassiakou, M', 'Navarria, Francesco Luigi', 'Navas, S', 'Nawrocki, K', 'Negri, P', 'Neufeld, N', 'Nicolaidou, R', 'Nielsen, B S', 'Niezurawski, P', 'Nikolenko, M', 'Nomokonov, V P', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Orazi, G', 'Österberg, K', 'Ouraou, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Papageorgiou, K', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Pavel, T', 'Pegoraro, M', 'Peralta, L', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Rames, J', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Rehn, J', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Ripp-Baudot, I', 'Røhne, O M', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Royon, C', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Schwemling, P', 'Schwering, B', 'Schwickerath, U', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Seibert, N', 'Sekulin, R L', 'Shellard, R C', 'Siebel, M', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Smadja, G', 'Smirnova, O G', 'Smith, G R', 'Solovyanov, O', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Squarcia, S', 'Stanescu, C', 'Stanic, S', 'Stanitzki, M', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Taffard, A', 'Tegenfeldt, F', 'Terranova, F', 'Thomas, J', 'Timmermans, J', 'Tinti, N', 'Tkatchev, L G', 'Tobin, M', 'Todorova-Nová, S', 'Tomaradze, A G', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tortosa, P', 'Tranströmer, G', 'Treille, D', 'Tristram, G', 'Trochimczuk, M', 'Troncon, C', 'Turluer, M L', 'Tyapkin, I A', 'Tzamarias, S', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'Van der Velde, C', 'van Dam, P', 'Van den Boeck, W', 'Van Doninck, W K', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Remortel, N', 'Van Vulpen, I B', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Walck, C', 'Washbrook, A J', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zinchenko, A I', 'Zoller, P', 'Zucchelli, G C', 'Zumerle, G']",['Addendum to'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'supersymmetry', 'sparticle, search for', 'sparticle, mass', 'Higgs particle, mass', 'renormalization group', 'parametrization', 'numerical calculations, interpretation of experiments', 'magnetic detector, DELPHI', 'proposed experiment, CERN LEP Stor', '161-189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104021'],['A more general MSSM parameter scan is described'],['2001-04-12']
232,['eng'],"['Giorgini, M', 'Manzoor, S']",['Fragmentation of very high energy heavy ions'],['Particle Physics - Experimental Results'],"['talk, Bologna 2000/05/29', 'scattering, heavy ion', 'lead, fragmentation', 'copper', 'plastics, track sensitive', 'total cross section', 'fission', 'charge exchange', 'experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104019'],"['A stack of CR39 (C12H18O7)n nuclear track detectors with a Cu target was exposed to a 158 A GeV lead ion beam at the CERN-SPS, in order to study the fragmentation properties of lead nuclei. Measurements of the total, break-up and pick-up charge-changing cross sections of ultrarelativistic Pb ions on Cu and CR39 targets are presented and discussed.']",['2001-04-12']
233,['eng'],"['Garmash, A']",['Charmless B decays into three charged track final states'],['Particle Physics - Experimental Results'],"['talk, Ago Town 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B+, hadronic decay', 'B+, branching ratio', 'final state, (3charged particle)', 'final state, (0charm)', 'scalar meson, intermediate state', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B+ --> K+ pi+ pi-', 'B+ --> 2K+ K-', 'B+ --> K- 2pi+', 'B+ --> 2K+ pi-', 'B+ --> K+ K- pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104018'],"['Using a data sample of 10.5 1/fb collected by the Belle detector, three-body charmless decays B+ --> K+h+h- have been studied. The following branching fractions have been obtained: Br(B+ --> K+pi-pi+) = (64.8+-10.0+-7.0) x 10**-6 and Br(B+ --> K+K-K+) = (36.5+-6.1+-5.5) x 10**-6. The upper limits for other combinations of charged kaons and pions have been placed. Analysis of the intermediate two-body states gives evidence for production of scalar resonances in charmless B decays.']",['2001-04-12']
234,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the centrally produced $\\pi0\\pi0\\pi0$ channel in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, exclusive reaction', 'meson resonance, hadroproduction', 'pi0, multiple production', 'mass spectrum, (3pi0)', 'eta', 'pi2(1670)', 'omega(783)', 'a1(1260)', 'a2(1320)', 'meson resonance, hadronic decay', 'meson resonance, branching ratio', 'upper limit', 'calorimeter, GAMS', 'experimental results', 'CERN SPS', 'p p --> 2p 3pi0', '450 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104017'],"['The reaction pp -> pf (pi0pi0pi0) ps has been studied at 450 GeV/c. The pi0pi0pi0 effective mass spectrum shows clear eta(547) and pi2(1670) signals. Branching ratios for the eta(547) and pi_2(1670) are given as well as upper limits for the decays of the omega(782), a1(1260) and a2(1320) into 3pi0.']",['2001-04-11']
235,['eng'],"['Kluth, S']",['Experimental Studies of Power Corrections'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, annihilation', 'hadron, multiple production', 'quantum chromodynamics, perturbation theory', 'effect, hadronization', 'correction, nonperturbative', 'event shape analysis', 'color', 'symmetry, SU(3)', 'cross section, transverse', 'numerical calculations, interpretation of experiments', '14-189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104016'],"['We present recent results from experimental studies of power corrections in the model of Dokshitzer, Marchesini and Webber using data from the process e+e- -> hadrons at several centre-of-mass energies. Fitted O(alpha_S^2)+NLLA QCD predictions combined with power corrections to model hadronisation effects successfully describe differential distributions and mean values of event shape observables. The fit results for the strong coupling constant and the free parameter of the power correction calculations from the various observables are consistent with each other within the uncertainties. The same fits are further employed to study the gauge structure of QCD by additionally varying the QCD colour factors in the fits. The results are consistent with QCD based on the SU(3) symmetry group. A new measurement of the transverse cross section is shown using reanalysed data of the former JADE experiment at DESY and its implications for power correction are discussed.']",['2001-04-11']
236,['eng'],"['Oyama, Y']",['Current Status of the K2K Experiment'],['Particle Physics - Experimental Results'],"['talk, Cairo 2001/01/09', 'neutrino, oscillation', 'neutrino/mu, beam', 'neutrino/mu, energy spectrum', 'beam, flux', 'beam instability', 'ratio, (neutrino/mu neutrino/e)', 'deep underground detector, KAMIOKANDE', 'experimental results', 'KEK PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104014'],['Current status of the K2K (KEK to Kamioka) long-baseline neutrino-oscillation experiment is presented.'],['2001-04-11']
237,['eng'],"['Alekhin, S I', 'Anykeyev, V B', 'Batusov, Yu A', 'Borisov, A', 'Bozhko, N', 'Bunyatov, S A', 'Chernichenko, S K', 'Denisov, O Yu', 'Fachrutdinov, R M', 'Goryachev, V N', 'Kazarinov, Yu M', 'Kirsanov, M M', 'Klimov, O L', 'Kononov, A I', 'Kozhin, A S', 'Krasnoperov, A V', 'Lipajev, V V', 'Mukhin, A I', 'Nefedov, Y A', 'Popov, B A', 'Prakhov, S N', 'Salomatin, Y I', 'Snyatkov, V I', 'Sviridov, Yu M', 'Tereshchenko, V V', 'Tumakov, V L', 'Vovenko, A S']",['Determination of the high-twist contribution to the structure function $xF^{\\nu N}_3$'],['Particle Physics - Experimental Results'],"['neutrino nucleon, interaction', 'antineutrino nucleon, interaction', 'charged current', 'nucleon, structure function', 'x-dependence', 'effect, higher-twist', 'renormalon', 'Serpukhov PS', '67, 70 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104013'],['We extract the high-twist contribution to the neutrino-nucleon structure function $xF_3^{(\\nu+\\bar{\\nu})N}$ from the analysis of the data collected by the IHEP-JINR Neutrino Detector in the runs with the focused neutrino beams at the IHEP 70 GeV proton synchrotron. The analysis is performed within the infrared renormalon (IRR) model of high twists in order to extract the normalization parameter of the model. From the NLO QCD fit to our data we obtained the value of the IRR model normalization parameter $\\Lambda^2_{3}=0.69\\pm0.37~({\\rm exp})\\pm0.16~({\\rm theor})~{\\rm GeV}^2$. We also obtained $\\Lambda^2_{3}=0.36\\pm0.22~({\\rm exp})\\pm0.12~({\\rm theor})~{\\rm GeV}^2$ from a similar fit to the CCFR data. The average of both results is $\\Lambda^2_{3}=0.44\\pm0.19~({\\rm exp})~{\\rm GeV}^2$.'],['2001-04-10']
238,['eng'],"['Anfreville, M', 'Astier, P', 'Authier, M', 'Baldisseri, A', 'Banner, M', 'Besson, N', 'Bouchez, J', 'Castera, A', 'Cloué, O', 'Dumarchez, J', 'Dumps, L', 'Gangler, E', 'Gosset, J', 'Hagner, C', 'Jollec, C', 'Lachaud, C', 'Letessier-Selvon, A A', 'Lévy, J M', 'Linssen, L', 'Meyer, J P', 'Ouriet, J P', 'Passerieux, J P', 'Pédrol, T', 'Placci, Alfredo', 'Poinsignon, J', 'Popov, B', 'Rathouit, P', 'Schahmaneche, K', 'Stolarczyk, T', 'Urós, V', 'Vannucci, François', 'Vo, M K', 'Zaccone, H']",['The Drift Chambers Of The Nomad Experiment'],['Detectors and Experimental Techniques'],"['neutrino nucleus, nuclear reaction', 'neutrino/tau', 'drift chamber, target', 'argon, organic compounds', 'spatial resolution', 'resolution, vertex', 'momentum resolution', 'electronics, amplifier', 'signal processing', 'efficiency', 'gas, control system', 'neutrino, oscillation', 'CERN SPS', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104012'],"['We present a detailed description of the drift chambers used as an active target and a tracking device in the NOMAD experiment at CERN. The main characteristics of these chambers are a large area, a self supporting structure made of light composite materials and a low cost. A spatial resolution of 150 microns has been achieved with a single hit efficiency of 97%.']",['2001-04-10']
239,['eng'],"['Van Remortel, N']",['Bose-Einstein correlations in WW events at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'correlation, two-pion', 'boson, statistics', 'quantum mechanics, coherence', 'experimental results', 'CERN LEP Stor', '172-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104011'],"[""The current status of the LEP results on Bose-Einstein correlations is discussed. Emphasis is given to the measurement of Bose-Einstein correlations between decay products from different W's, in an energy range between 172 and 209 GeV, dependent on the experiment. For the first time all four LEP experiments conclude that no evidence for correlations between pions from different W's is seen at the current level of precision.""]",['2001-04-10']
240,['eng'],"['Baird, A', 'Elsen, E E', 'Fleming, Y H', 'Kolander, M', 'Kolya, S D', 'Meer, D', 'Mercer, D', 'Naumann, J', 'Newman, P R', 'Sankey, D', 'Schoening, A', 'Schultz-Coulon, H C', 'Wissing, C']",['A Fast High Resolution Track Trigger for the H1 Experiment'],['Particle Physics - Experimental Results'],"['tracks', 'trigger', 'drift chamber', 'momentum resolution', 'J/psi(3100), leptonic decay', 'luminosity', 'magnetic detector, H1', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104010'],"['After 2001 the upgraded ep collider HERA will provide an about five times higher luminosity for the two experiments H1 and ZEUS. In order to cope with the expected higher event rates the H1 collaboration is building a track based trigger system, the Fast Track Trigger (FTT). It will be integrated in the first three levels (L1-L3) of the H1 trigger scheme to provide higher selectivity for events with charged particles. The FTT will allow to reconstruct 3-dimensional tracks in the central drift chamber down to 100 MeV/c within the L2 latency of ~ 23 mus. To reach the necessary momentum resolution of ~ 5% (at 1 GeV/c) sophisticated reconstruction algorithms have to be implemented using high density Field Programmable Gate Arrays (FPGA) and their embedded Content Addressable Memories (CAM). The final track parameter optimization will be done using non-iterative fits implemented in DSPs. While at the first trigger level rough track information will be provided, at L2 tracks with high resolution are available to form trigger decisions on topological and other track based criteria like multiplicities and momenta. At the third trigger level a farm of commercial processor boards will be used to compute physics quantities such as invariant masses.']",['2001-04-09']
241,['eng'],"['Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Schwarthoff, H', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A']",['Search for CP Violation in $\\tau\\to \\pi\\pi^{0}\\nu_{\\tau}$ Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'correlation', 'scalar particle, exchange', 'Higgs particle, scalar', 'coupling constant, parametrization', 'violation, CP', 'upper limit', 'angular distribution', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau --> pi pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104009'],"['We search for CP non-conservation in the decays of tau leptons produced via $e^+ e^-$ annihilation at $\\sqrt{s}\\sim$ 10.6 GeV. The method uses correlated decays of pairs of tau leptons, each decaying to the $\\pi \\pi^0 \\nu_{\\tau}$ final state. The search is done within the framework of a model with a scalar boson exchange. In an analysis of a data sample corresponding to 12.2 million produced tau pairs collected with the CLEO detector, we find no evidence of violation of CP symmetry. We obtain a limit on the imaginary part of the coupling constant parameterizing the relative contribution of diagrams that would lead to CP violation to be $-0.046 <\\Im(\\Lambda) < 0.022$ at 90% C.L. This result provides a restriction on CP non-conservation in the tau lepton decays. As a cross check, we study the decay angular distribution and perform a model-independent search for a CP violation effect of a scalar exchange in single $\\tau\\to \\pi\\pi^0\\nu_\\tau$ decays. The limit on the imaginary part of the $\\tau$ scalar coupling is $-0.033 < \\Im(\\Lambda) < 0.089$ at 90% C.L.']",['2001-04-05']
242,['eng'],"['Smith, A B']","['Recent Results From CLEO on D0-D0Bar Mixing, CP Violation in D0 Decays and D*+ Width']",['Particle Physics - Experimental Results'],"['talk, Ise-Shima 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, electroproduction', 'D0, hadronic decay', 'pseudoscalar meson, pair production', 'decay, asymmetry', 'D0 anti-D0, interference', 'invariance, CP', 'D*(2010), hadronic decay', 'D*(2010), width', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D0 --> 2pseudoscalar meson', 'D0 --> K+ pi- pi0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104008'],"['We present preliminary results of several analyses searching for the effects of CP violation and mixing in the decay of $D^0$ mesons. We find no evidence of CP asymmetry in five different two-body decay modes of the $D^0$ to pairs of light pseudo-scalar mesons: $A_{CP}(K^+ K^-) = (+0.05 \\pm 2.18 \\pm 0.84)% $, $A_{CP}(\\pi^+ \\pi^-) = (+2.0 \\pm 3.2 \\pm 0.8)% $, $A_{CP}(K^0_{\\rm S} \\pi^0) = (+0.1 \\pm 1.3)%$, $A_{CP}(\\pi^0 \\pi^0) = (+0.1 \\pm 4.8)%$, and $A_{CP}(K^0_{\\rm S} K^0_{\\rm S}) = (-23 \\pm 19)%$. We present the first measurement of the rate of wrong-sign $D^0 \\to K^+ \\pi^- \\pi^0$ decay: $R = 0.0043^{+0.0011}_{-0.0010} \\pm 0.0007$. We also describe a measurement of the mixing parameter $y_{CP}= {\\Delta\\Gamma\\over 2 \\Gamma}$ by searching for a lifetime difference between the CP neutral $K^{-}\\pi^{+}$ final state and the CP even $K^+K^-$ and $\\pi^+\\pi^-$ final states. Under the assumption that CP is conserved we find $y_{CP} = -0.011 \\pm 0.025 \\pm 0.014$. Finally, we present our measurement of the \\dstarp width: $96 \\pm 4 \\pm 22$~k$e$V.']",['2001-04-04']
243,['eng'],"['Paganis, S D', 'Tang, J L']",['Momentum Resolution Improvement Technique for Silicon Tracking Detectors using dE/dx'],['Detectors and Experimental Techniques'],"['charged particle, energy loss', 'semiconductor detector, momentum resolution', 'magnetic detector, STAR', 'Brookhaven RHIC Coll', 'magnetic detector, ALICE', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104006'],['A technique for improving the momentum resolution for low momentum charged particles in few layer silicon based trackers is presented. The particle momenta are determined from the measured Landau dE/dx distribution and the Bethe-Bloch formula in the 1/beta^2 region. It is shown that a factor of two improvement of the momentum determination is achieved as compared to standard track fitting methods. This improvement is important in large scale heavy ion experiments which cover the low transverse momentum spectra using stand-alone silicon tracking devices with a few planes like the ones used in STAR at RHIC and ALICE at LHC.'],['2001-04-04']
244,['eng'],"['Airapetian, A', 'Akopov, N Z', 'Akopov, N Z', 'Amarian, M', 'Aschenauer, E C', 'Avakian, H', 'Avakian, R', 'Avetisian, A', 'Avetissian, E', 'Bailey, P', 'Bains, B', 'Baturin, V', 'Baumgarten, C', 'Beckmann, M', 'Belostotskii, S', 'Bernreuther, S', 'Bianchi, N', 'Böttcher, H', 'Borisov, A', 'Bouhali, O', 'Bouwhuis, M', 'Brack, J', 'Brauksiepe, S', 'Brückner, W', 'Brüll, A', 'Brunn, I', 'Bulten, H J', 'Capitani, G P', 'Chumney, P', 'Cisbani, E', 'Ciullo, G', 'Court, G R', 'Dalpiaz, P F', 'De Leo, R', 'De Nardo, L', 'De Sanctis, E', 'De Schepper, D', 'Devitsin, E G', 'De Witt-Huberts, P K A', 'Di Nezza, P', 'Dzhordzhadze, V', 'Düren, M', 'Ehrenfried, M', 'Elbakian, G M', 'Ellinghaus, F', 'Ely, J', 'Fantoni, A', 'Feshchenko, A', 'Felawka, L', 'Filippone, B W', 'Fischer, H', 'Fox, B', 'Franz, J', 'Frullani, S', 'Gärber, Y', 'Garibaldi, F', 'Garutti, E', 'Gavrilov, G', 'Karibian, V', 'Golendukhin, A', 'Graw, G', 'Grebenyuk, O', 'Green, P W', 'Greeniaus, L G', 'Gute, A', 'Haeberli, W', 'Hafidi, K', 'Hartig, M', 'Hasch, D', 'Heesbeen, D', 'Heinsius, F H', 'Henoch, M', 'Hertenberger, R', 'Hesselink, W H A', 'Hofman, G J', 'Holler, Y', 'Holt, R J', 'Hommez, B', 'Iarygin, G', 'Izotov, A A', 'Jackson, H E', 'Jgoun, A', 'Jung, P', 'Kaiser, R', 'Kanesaka, J', 'Kinney, E R', 'Kiselev, A', 'Kitching, P', 'Kobayashi, H', 'Koch, N', 'Königsmann, Kay C', 'Kolster, H', 'Korotkov, V A', 'Kotik, E', 'Kozlov, V', 'Krauss, B', 'Krivokhizhin, V G', 'Kyle, G S', 'Lagamba, L', 'Laziev, A', 'Lenisa, P', 'Liebing, P', 'Lindemann, T', 'Lorenzon, W', 'Maas, A', 'Makins, N C R', 'Marukyan, H O', 'Masoli, F', 'McAndrew, M', 'McIlhany, K', 'Meissner, F', 'Menden, F', 'Meyners, N', 'Miklukho, O', 'Miller, C A', 'Milner, R', 'Muccifora, V', 'Mussa, R', 'Nagaitsev, A P', 'Nappi, E', 'Naryshkin, Yu', 'Nass, A', 'Negodaeva, K', 'Nowak, W D', 'Oganessyan, K A', ""O'Neill, T G"", 'Owen, B R', 'Pate, S F', 'Potashov, S', 'Potterveld, D H', 'Raithel, M', 'Rakness, G', 'Rappoport, V', 'Redwine, R P', 'Reggiani, D', 'Reolon, A R', 'Rith, K', 'Robinson, D', 'Rostomyan, A', 'Ruh, M', 'Ryckbosch, D', 'Sakemi, Y', 'Sanjiev, I', 'Sato, F', 'Savin, I A', 'Scarlett, C', 'Schäfer, A', 'Schill, C', 'Schmidt, F', 'Schnell, G', 'Schüler, K P', 'Schwind, A', 'Seibert, J', 'Seitz, B', 'Shibata, T A', 'Shutov, V', 'Simani, M C', 'Simon, A', 'Sinram, K', 'Steffens, E', 'Steijger, J J M', 'Stewart, J', 'Stösslein, U', 'Suetsugu, K', 'Taroian, S P', 'Terkulov, A R', 'Teryaev, O V', 'Tessarin, S', 'Thomas, E', 'Tipton, B', 'Tytgat, M', 'Urciuoli, G M', 'Van den Brand, J F J', 'van der Steenhoven, G', 'Van de Vyver, R', 'Van Hunen, J J', 'Vetterli, M C', 'Vikhrov, V V', 'Vincter, M G', 'Visser, J', 'Weiskopf, C', 'Wendland, J', 'Wilbert, J', 'Wise, T', 'Yen, S', 'Yoneyama, S', 'Zohrabyan, H G']",['Single-spin Azimuthal Asymmetries in Electroproduction of Neutral Pions in Semi-inclusive Deep-inelastic Scattering'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'p, polarized target', 'polarization, longitudinal', 'pi0, electroproduction', 'analyzing power', 'spin, asymmetry', 'energy dependence', 'x-dependence', 'transverse momentum, dependence', 'fragmentation function', 'quark, polarization', 'polarization, transverse', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', '27.5 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104005'],['A single-spin asymmetry in the azimuthal distribution of neutral pions relative to the lepton scattering plane has been measured for the first time in deep-inelastic scattering of positrons off longitudinally polarized protons. The analysing power in the sin(phi) moment of the cross section is 0.019 +/- 0.007(stat.) +/- 0.003(syst.). This result is compared to single-spin asymmetries for charged pion production measured in the same kinematic range. The pi^0 asymmetry is of the same size as the pi^+ asymmetry and shows a similar dependence on the relevant kinematic variables. The asymmetry is described by a phenomenological calculation based on a fragmentation function that represents sensitivity to the transverse polarization of the struck quark.'],['2001-04-04']
245,['eng'],"['Danilov, M', 'Laptin, L', 'Tichomirov, I', 'Titov, M L', 'Zaitsev, Yu']",['Aging tests of the proportional wire chambers using Ar\\/CF4\\/CH4 (74'],['Particle Physics - Experimental Results'],"['muon, drift chamber', 'proportional chamber, wire', 'argon, organic compounds', 'carbon, fluorine', 'gas, admixture', 'radiation, damage', 'electron, drift velocity', 'magnetic detector, HERA-B', 'DESY HERA Stor', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0107080'],"['The Muon Detector of the HERA-B experiment at DESY is a gaseous detector that provides muon identification in a high-rate hadronic environment. We present our studies on the properties of several fast gases, Ar/CF4/CH4 (74:20:6), Ar/CF4/CH4 (67:30:3) and Ar/CF4/CO2 (65:30:5), which have been found to fulfill muon detection requirements. The severe radiation environment of the HERA-B experiment leads to the maximum charge deposit on a wire, within the muon detector, of 200 mC/cm per year. For operation in such an environment, the main criteria for the choice of gas turned out to be stability against aging. An overview of aging results from laboratory setups and experimental detectors for binary and ternary mixtures of Ar, CH4, CF4 and CO2 is presented and the relevance of the various aging results is discussed. Since it is not clear how to extrapolate aging results from small to large areas of irradiation, the lifetime of aluminum proportional chambers was studied under various conditions. In this paper we provide evidence that aging results depend not only upon the total collected charge. It was found that the aging rate for irradiation with $Fe^{55}$ X-rays and 100 MeV $\\alpha$-particles may differ by more than two orders of magnitude.']",['2001-07-31']
246,['eng'],"['Patrignani, C']","[""On the Particle Data Group evaluation of Psi' and chi_c Branching Ratios""]",['Particle Physics - Experimental Results'],"['chi mesons, charm', 'chi mesons, hadronic decay', 'chi mesons, radiative decay', 'chi mesons, branching ratio', 'psi(3685), radiative decay', 'J/psi(3100), leptonic decay', 'psi mesons, branching ratio', 'data analysis method, error', 'tables', 'numerical calculations, interpretation of experiments', 'psi(3685) --> chi mesons photon', 'J/psi(3100) --> lepton+ lepton-', 'chi mesons --> p anti-p', 'chi mesons --> 2photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104003'],"[""I propose a new evaluation of $\\psi'(2S)$ and $\\chi_c(1P)$ branching ratios which avoids the inconsistencies found in the procedure adopted by the Particle Data Group. These inconsistencies explain the apparent technique-dependent discrepancies between the available determinations of the ${\\cal B}(\\chi_c(1P)\\to p\\bar p)$ and $\\Gamma(\\chi_c(1P)\\to \\gamma\\gamma)$ under the hypotesis of a systematic error in the current values of the $\\psi'(2S)\\to\\chi_c(1P)\\gamma$ branching ratios. In the process I also noticed that Particle Data Group has not restated many of the older measurements, when necessary, for the new value of ${\\cal B}(J/\\psi\\to l^+l^-)$, which significantly affects the evaluation of some relevant $\\psi'(2S)$ and $\\chi_c(1P)$ exclusive branching ratios.""]",['2001-04-03']
247,['eng'],"['Kulchitskii, Yu A']",['Hadron Energy Reconstruction for the ATLAS Calorimetry in the Framework of the Non-parametrical Method'],['Particle Physics - Experimental Results'],"['calorimeter, electromagnetic', 'lead, liquid argon', 'calorimeter, hadronic', 'iron', 'scintillation counter', 'hadron, energy', 'energy resolution', 'statistical analysis', 'magnetic detector, ATLAS', 'CERN LHC Coll', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104002'],"['This paper discusses hadron energy reconstruction for the ATLAS barrel prototype combined calorimeter (consisting of a lead-liquid argon electromagnetic part and an iron-scintillator hadronic part) in the framework of the non-parametrical method. The non-parametrical method utilizes only the known $e/h$ ratios and the electron calibration constants and does not require the determination of any parameters by a minimization technique. Thus, this technique lends itself to an easy use in a first level trigger. The reconstructed mean values of the hadron energies are within $\\pm 1%$ of the true values and the fractional energy resolution is $[(58\\pm3)% /\\sqrt{E}+(2.5\\pm0.3)%]\\oplus (1.7\\pm0.2)/E$. The value of the $e/h$ ratio obtained for the electromagnetic compartment of the combined calorimeter is $1.74\\pm0.04$ and agrees with the prediction that $e/h > 1.7$ for this electromagnetic calorimeter. Results of a study of the longitudinal hadronic shower development are also presented. The data have been taken in the H8 beam line of the CERN SPS using pions of energies from 10 to 300 GeV.']",['2001-04-03']
248,['eng'],"['Airapetian, A', 'Akopov, N Z', 'Akopov, N Z', 'Amarian, M', 'Arrington, J', 'Aschenauer, E C', 'Avakian, H', 'Avakian, R', 'Avetisian, A', 'Avetissian, E', 'Bailey, P', 'Bains, B', 'Baumgarten, C', 'Beckmann, M', 'Belostotskii, S', 'Bernreuther, S', 'Bianchi, N', 'Böttcher, H', 'Borisov, A', 'Bouwhuis, M', 'Brack, J', 'Brauksiepe, S', 'Braun, B', 'Brückner, W', 'Brüll, A', 'Budz, P', 'Bulten, H J', 'Capitani, G P', 'Carter, P', 'Chumney, P', 'Cisbani, E', 'Court, G R', 'Dalpiaz, P F', 'De Leo, R', 'De Nardo, L', 'De Sanctis, E', 'De Schepper, D', 'Devitsin, E G', 'De Witt-Huberts, P K A', 'Di Nezza, P', 'Dzhordzhadze, V', 'Düren, M', 'Dvoredsky, A P', 'Elbakian, G M', 'Ely, J', 'Fantoni, A', 'Feshchenko, A', 'Ferro-Luzzi, M', 'Fiedler, K', 'Filippone, B W', 'Fischer, H', 'Fox, B', 'Franz, J', 'Frullani, S', 'Gärber, Y', 'Garibaldi, F', 'Garutti, E', 'Gavrilov, G', 'Karibian, V', 'Golendukhin, A', 'Graw, G', 'Grebenyuk, O', 'Green, P W', 'Greeniaus, L G', 'Gute, A', 'Haeberli, W', 'Hartig, M', 'Hasch, D', 'Heesbeen, D', 'Heinsius, F H', 'Henoch, M', 'Hertenberger, R', 'Hesselink, W H A', 'Hoffmann-Rothe, P', 'Hofman, G J', 'Holler, Y', 'Holt, R J', 'Hommez, B', 'Hoprich, W', 'Iarygin, G', 'Ihssen, H', 'Iodice, M', 'Izotov, A A', 'Jackson, H E', 'Jgoun, A', 'Kaiser, R', 'Kanesaka, J', 'Kinney, E R', 'Kiselev, A', 'Kitching, P', 'Kobayashi, H', 'Koch, N', 'Königsmann, Kay C', 'Kolster, H', 'Korotkov, V A', 'Kotik, E', 'Kozlov, V', 'Krivokhizhin, V G', 'Kyle, G S', 'Lagamba, L', 'Laziev, A', 'Lenisa, P', 'Lindemann, T', 'Lorenzon, W', 'Makins, N C R', 'Martin, J W', 'Marukyan, H O', 'Masoli, F', 'McAndrew, M', 'McIlhany, K', 'McKeown, R D', 'Meissner, F', 'Menden, F', 'Metz, A', 'Meyners, N', 'Miklukho, O', 'Miller, C A', 'Milner, R', 'Muccifora, V', 'Mussa, R', 'Nagaitsev, A P', 'Nappi, E', 'Naryshkin, Yu', 'Nass, A', 'Nowak, W D', ""O'Neill, T G"", 'Openshaw, R', 'Ouyang, J', 'Owen, B R', 'Pate, S F', 'Potashov, S', 'Potterveld, D H', 'Rakness, G', 'Redwine, R P', 'Reggiani, D', 'Reolon, A R', 'Ristinen, R', 'Rith, K', 'Robinson, D', 'Rostomyan, A', 'Ruh, M', 'Ryckbosch, D', 'Sakemi, Y', 'Sato, F', 'Savin, I A', 'Scarlett, C', 'Schäfer, A', 'Schill, C', 'Schmidt, F', 'Schmitt, M', 'Schnell, G', 'Schüler, K P', 'Schwind, A', 'Seibert, J', 'Shibata, T A', 'Shin, T', 'Shutov, V', 'Simani, M C', 'Simon, A', 'Sinram, K', 'Steffens, E', 'Steijger, J J M', 'Stewart, J', 'Stösslein, U', 'Suetsugu, K', 'Sutter, M F', 'Tallini, H A', 'Taroian, S P', 'Terkulov, A R', 'Tessarin, S', 'Thomas, E', 'Tipton, B', 'Tytgat, M', 'Urciuoli, G M', 'Van den Brand, J F J', 'van der Steenhoven, G', 'Van de Vyver, R', 'Van Hunen, J J', 'Vetterli, M C', 'Vikhrov, V V', 'Vincter, M G', 'Visser, J', 'Volk, E', 'Weiskopf, C', 'Wendland, J', 'Wilbert, J', 'Wise, T', 'Woller, K', 'Yoneyama, S', 'Zohrabyan, H G']",['Multiplicity of Charged and Neutral Pions in Deep-Inelastic Scattering of 27.5 GeV Positrons on Hydrogen'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'pi, electroproduction', 'pi, multiplicity', 'yield, (pi+ pi- pi0)', 'momentum transfer, dependence', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'positron p --> pi anything', '27.5 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0104004'],[],['2001-04-03']
249,['eng'],"['Bozzi, C']",['B Mixing and Lifetime Measurements with the BaBar Detector'],['Particle Physics - Experimental Results'],"['talk, Ago Town 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0 anti-B0, interference', 'B, hadronic decay', 'B, semileptonic decay', 'B0, lifetime', 'B+, lifetime', 'lifetime, ratio', 'B0, mass difference', 'particle identification, flavor', 'charge, dilepton', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103046'],"['Recent BaBar measurements on lifetime and mixing of B mesons are reported. Various techniques are used, ranging from the full reconstruction of hadronic B decays, to partial reconstruction techniques, and to a totally inclusive approach with dilepton events. The results presented are based on a data sample collected by BaBar during the 1999-2000 data taking, and should be considered as preliminary.']",['2001-03-29']
250,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kamer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R J', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Precision Neutral Current Asymmetry Parameter Measurements from the Tau Polarization at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, electroproduction', 'tau, semileptonic decay', 'tau, leptonic decay', 'tau, polarization', 'polarization, asymmetry', 'angular distribution, asymmetry', 'neutral current, parametrization', 'lepton, universality', 'electroweak interaction, mixing angle', 'coupling constant, vector', 'coupling constant, axial-vector', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> tau+ tau-', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103045'],"['Measurements of the tau lepton polarization and forward-backward polarization asymmetry near the Z resonance using the OPAL detector are described. The measurements are based on analyses of tau -> e nu_e nu_tau, tau -> mu nu_mu nu_tau, tau -> pi nu_tau, tau -> rho nu_tau and tau -> a1 nu_tau decays from a sample of 144810 e+e- -> tau+ tau- candidates corresponding to an integrated luminosity of 151 pb-1. Assuming that the tau lepton decays according to V-A theory, we measure the average tau polarization near Ecm = MZ to be <Ptau> = (-14.10 +/- 0.73 +/- 0.55)% and the tau polarization forward-backward asymmetry to be Afb = (-10.55 +/- 0.76 +/- 0.25)%, where the first error is statistical and the second systematic. Taking into account the small effects of the photon propagator, photon-Z interference and photonic radiative corrections, these results can be expressed in terms of the lepton neutral current asymmetry parameters: Atau = 0.1456 +/- 0.0076 +/- 0.0057, Ae = 0.1454 +/- 0.0108 +/- 0.0036. These measurements are consistent with the hypothesis of lepton universality and combine to give Al = 0.1455 +/- 0.0073. Within the context of the Standard Model this combined result corresponds to sin^2(theta)(lept,effective) = 0.23172 +/- 0.00092. Combing these results with those from the other OPAL neutral current measurements yields a value of sin^2(theta)(lept,effective) = 0.23211 +/- 0.00068.']",['2001-03-28']
251,['eng'],"['Akhmetshin, R R', 'Anashkin, E V', 'Aulchenko, V M', 'Banzarov, V S', 'Baratt, A', 'Barkov, L M', 'Baru, S E', 'Bashtovoy, N S', 'Bondar, A E', 'Bondarev, D V', 'Bragin, A V', 'Chernyak, D V', 'Eidelman, S I', 'Fedotovich, G V', 'Gabyshev, N I', 'Grebeniuk, A A', 'Grigoriev, D N', 'Hughes, V W', 'Ignatov, F V', 'Karpov, S V', 'Kazanin, V F', 'Khazin, B I', 'Koop, I A', 'Krokovnyi, P P', 'Kurdadze, L M', 'Kuzmin, A S', 'Logashenko, I B', 'Lukin, P A', 'Lysenko, A P', 'Mikhailov, K Yu', 'Milshtein, A I', 'Nesterenko, I N', 'Okhapkin, V S', 'Otboev, A V', 'Perevedentsev, E A', 'Popov, A S', 'Root, N I', 'Ruban, A A', 'Ryskulov, N M', 'Shamov, A G', 'Shatunov, Yu M', 'Shwartz, B A', 'Sibidanov, A L', 'Sidorov, V A', 'Skrinsky, A N', 'Smakhtin, V P', 'Snopkov, I G', 'Solodov, E P', 'Stepanov, P Yu', 'Sukhanov, A Yu', 'Thompson, J A', 'Valishev, A A', 'Yudin, Yu V', 'Zverev, S G']",['Study of the Process $e^+ e^\\to\\eta \\gamma$ in c.m. Energy Range 600-1380 MeV at CMD-2'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'eta, electroproduction', 'photon, associated production', 'eta, hadronic decay', 'channel cross section, energy dependence', 'vector meson, intermediate state', 'vector meson, radiative decay', 'vector meson, branching ratio', 'rho(770)', 'omega(783)', 'Phi(1020)', 'magnetic detector, CMD', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> eta photon', 'eta --> 3pi0', 'vector meson --> eta photon', '0.60-1.38 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103043'],"[""The cross section of the process e+ e- ---> eta gamma has been measured in the 600-1380 MeV c.m. energy range with the CMD-2 detector. The following branching ratios have been determined: B(rho ---> eta gamma) = (3.28 +- 0.37 +- 0.23) 10^{-4}, B(omega ---> eta gamma) = (5.10 +- 0.72 +- 0.34) 10^{-4}, B(phi --> eta gamma) = (1.287 +- 0.013 +- 0.063) 10^{-2}. Evidence for the rho'(1450) ---> eta gamma decay has been obtained for the first time.""]",['2001-03-27']
252,['eng'],"['Abe, K', 'Abe, K', 'Adachi, I', 'Byoung Sup Ahn', 'Aihara, H', 'Akatsu, M', 'Alimonti, G', 'Aoki, K', 'Asai, K', 'Asano, Y', 'Aso, T', 'Aulchenko, V M', 'Aushev, T', 'Bakich, A M', 'Banas, E', 'Bartel, W', 'Behari, S', 'Behera, P K', 'Beiline, D', 'Bondar, A E', 'Bozek, A', 'Browder, T E', 'Casey, B C K', 'Chang, P', 'Chao, Y', 'Cheon, B G', 'Choi, S K', 'Choi, Y', 'Doi, Y', 'Dragic, J', 'Drutskoy, A G', 'Eidelman, S', 'Enari, Y', 'Enomoto, R', 'Fang, F', 'Fujii, H', 'Fukunaga, C', 'Fukushima, M', 'Garmash, A', 'Gordon, A', 'Gotow, K', 'Guler, H', 'Guo, R', 'Haba, J', 'Hamasaki, H', 'Hanagaki, K', 'Handa, F', 'Hara, K', 'Hara, T', 'Haruyama, T', 'Hastings, N C', 'Hayashi, K', 'Hayashii, H', 'Hazumi, M', 'Heenan, E M', 'Higasino, Y', 'Higuchi, I', 'Higuchi, T', 'Hirano, H', 'Hojo, T', 'Hoshi, Y', 'Hou, W S', 'Hsu, S C', 'Huang, H C', 'Ichizawa, S', 'Igarashi, Y', 'Iijima, T', 'Ikeda, H', 'Ikeda, K', 'Inami, K', 'Ishikawa, A', 'Ishino, H', 'Itoh, R', 'Iwai, G', 'Iwasaki, H', 'Iwasaki, Y', 'Jackson, D J', 'Jalocha, P', 'Jang, H K', 'Jones, M', 'Kagan, R', 'Kakuno, H', 'Kaneko, J', 'Kang, J H', 'Kang, J S', 'Kapusta, P', 'Katayama, N', 'Kawai, H', 'Kawamura, N', 'Kawasaki, T', 'Kichimi, H', 'Kim, D W', 'Hee Joung Kim', 'Kim, H J', 'Hyunwoo Kim', 'Kim, S K', 'Kinoshita, K', 'Korotushenko, K', 'Krokovnyi, P P', 'Kulasiri, R', 'Kumar, S', 'Kuniya, T', 'Kurihara, E', 'Kuzmin, A', 'Kwon, Y J', 'Lange, J S', 'Lee, M H', 'Lee, S H', 'Li, H B', 'Liventsev, D', 'Lu, R S', 'Manabe, A', 'Matsubara, T', 'Matsui, S', 'Matsumoto, S', 'Matsumoto, T', 'Mikami, Y', 'Misono, K', 'Miyabayashi, K', 'Miyake, H', 'Miyata, H', 'Moffitt, L C', 'Moloney, G R', 'Moorhead, G F', 'Mori, S', 'Murakami, A', 'Nagamine, T', 'Nagasaka, Y', 'Nagashima, Y', 'Nakadaira, T', 'Nakano, E', 'Nakao, M', 'Nam, J W', 'Narita, S', 'Natkaniec, Z', 'Neichi, K', 'Nishida, S', 'Nitoh, O', 'Noguchi, S', 'Nozaki, T', 'Ogawa, S', 'Ohshima, T', 'Ohshima, Y', 'Okabe, T', 'Okazaki, T', 'Okuno, S', 'Olsen, S L', 'Ostrowicz, W', 'Ozaki, H', 'Palka, H', 'Park, C S', 'Park, C W', 'Park, H', 'Peak, L S', 'Peters, M', 'Piilonen, L E', 'Prebys, E J', 'Rodríguez, J L', 'Root, N', 'Rózanska, M', 'Rybicki, K', 'Ryuko, J', 'Sagawa, H', 'Sakai, Y', 'Sakamoto, H', 'Satapathy, M', 'Satpathy, A', 'Schrenk, S', 'Semenov, S V', 'Senyo, K', 'Sevior, M E', 'Shibuya, H', 'Shwartz, B A', 'Sidorov, V', 'Singh, J B', 'Stanic, S', 'Sugi, A', 'Sugiyama, A', 'Sumisawa, K', 'Sumiyoshi, T', 'Suzuki, K', 'Suzuki, S', 'Suzuki, S Y', 'Swain, S K', 'Tajima, H', 'Takahashi, T', 'Takasaki, F', 'Takita, M', 'Tamai, K', 'Tamura, N', 'Tanaka, J', 'Tanaka, M', 'Tanaka, Y', 'Taylor, G N', 'Teramoto, Y', 'Tomoto, M', 'Tomura, T', 'Tovey, S N', 'Trabelsi, K', 'Tsuboyama, T', 'Tsujita, Y', 'Tsukamoto, T', 'Uehara, S', 'Ueno, K', 'Ujiie, N', 'Unno, Y', 'Uno, S', 'Ushiroda, Y', 'Usov, Y', 'Vahsen, S E', 'Varner, G', 'Varvell, K E', 'Wang Chao Cheng', 'Wang, C H', 'Wang, M Z', 'Wang, T J', 'Watanabe, Y', 'Won, E', 'Yabsley, B D', 'Yamada, Y', 'Yamaga, M', 'Yamaguchi, A', 'Yamamoto, H', 'Yamaoka, H', 'Yamaoka, Y', 'Yamashita, Y', 'Yamauchi, M', 'Yanaka, S', 'Yokoyama, M', 'Yoshida, K', 'Yusa, Y', 'Yuta, H', 'Zhang, C C', 'Zhang, J', 'Zheng, Y', 'Zhilich, V N']",['A Measurement of the Branching Fraction for the Inclusive B --> X(s) gamma Decays with Belle'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, radiative decay', 'B, branching ratio', 'K', 'K*(892)', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> strange meson photon anything', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103042'],['We have measured the branching fraction of the inclusive radiative B meson decay B --> X(s) gamma to be Br(B->X(s)gamma)=(3.36 +/- 0.53(stat) +/- 0.42(sys) +0.50-0.54(th)) x 10^{-4}. The result is based on a sample of 6.07 x 10^6 BBbar events collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric e^+e^- storage ring.'],['2001-03-27']
253,['eng'],"['Heinson, A P']",['A Search for Single Top Quark Production at DZero'],['Particle Physics - Experimental Results'],"['talk, Tver 2000/09/14', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, hadroproduction', 'final state, ((n)jet lepton)', 'channel cross section, upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> truth beauty anything', 'anti-p p --> truth beauty quark anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105004'],"['We present details of a search for electroweak production of single top quarks in the electron+jets and muon+jets decay channels. The measurements use \\~90 pb^-1 of data from Run 1 of the Fermilab Tevatron collider, collected at 1.8 TeV with the DZero detector. We use events that include a tagging muon, implying the presence of a b jet, to set an upper limit at the 95% confidence level on the cross section for the s-channel process ppbar->tb+X of 39 pb. The upper limit for the t-channel process ppbar->tqb+X is 58 pb.']",['2001-09-14']
254,['eng'],"['Heinson, A P']",['Search for Electroweak Production of Single Top Quarks at DZero'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, hadroproduction', 'final state, ((n)jet lepton)', 'channel cross section, upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> truth beauty anything', 'anti-p p --> truth beauty quark anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105003'],"['This paper discusses a search for electroweak production of single top quarks in the electron+jets and muon+jets decay channels. The measurements use ~90 pb^-1 of data from Run 1 of the Fermilab Tevatron collider, collected at 1.8 TeV with the DZero detector. We use events that include a tagging muon, implying the presence of a b jet, to set an upper limit at the 95% confidence level on the cross section for the s-channel process ppbar->tb+X of 39 pb. The upper limit for the t-channel process ppbar->tqb+X is 58 pb.']",['2001-05-02']
255,['eng'],"['Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P']",['Search for $\\B^{0}\\to \\pi^{0}\\pi^{0}$ Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'pi0, pair production', 'B0, branching ratio', 'upper limit', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B0 --> 2pi0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103040'],"[""We report on the observation of Bbar -> D(*) pi+ pi- pi- pi^0 decays. The branching ratios for D*+ and D*0 are (1.72+/-0.14+/-0.24)% and (1.80+/-0.24+/-0.27)%, respectively. Each final state has a D* omega pi- component, with branching ratios (0.29+/-0.03+/-0.04)% and (0.45+/-0.10+/-0.07)% for the D*+ and D*0 modes, respectively. We also observe B -> D omega pi- decays. The branching ratios for D+ and D0 are (0.28+/-0.05+/-0.04)% and (0.41+/-0.07+/-0.06)%, respectively. A spin parity analysis of the D omega pi- final state prefers a wide 1^- resonance. A fit to the omega pi- mass spectrum finds a central mass of (1349+/-25^{+10}_{-5}) MeV and width of (547+/-86^{+46}_{-45}) MeV. We identify this object as the rho(1450) or the \\rho'.""]",['2001-03-26']
256,['eng'],"['Bourilkov, D']",['Two-fermion and Two-photon Final States at LEP2 and Search for Extra Dimensions'],['Particle Physics - Experimental Results'],"['review, La Thuile 2001/03/04', 'electron positron, colliding beams', 'electron positron, annihilation', 'fermion, pair production', 'photon, pair production', 'electroweak interaction, validity test', 'fermion, composite', 'muon, magnetic moment', 'string model', 'membrane model', 'new interaction, search for', 'space-time, higher-dimensional', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103039'],"['For the first time the experiments ALEPH, DELPHI, L3 and OPAL have presented preliminary results for fermion-pair and photon-pair production in e+e- collisions on the full LEP2 data set. The details of the experimental measurements and results from their LEP-wide combination are presented. No statistically significant deviations from the Standard Model expectations are observed and lower limits, some obtained in dedicated analyses, for new physics phenomena at 95 % confidence level are derived. The scales of contact interactions are constrained to lie above 10-20 TeV, depending on the helicity structure. The Standard Model has thus been tested at LEP2 down to distances 10^{-19} - 10^{-20} m. This has many implications, one example being the interpretation of the new result on the anomalous magnetic moment of the muon as coming from muon substructure. For gamma-gamma final states the QED cut-offs are Lambda_+ > 0.44 TeV and Lambda_- > 0.37 TeV. In a combined analysis, using e+e- and gamma-gamma final states, the most stringent lower limits to date, M_s^+ > 1.13 TeV (lambda = +1) and M_s^- > 1.39 TeV (lambda = -1), on the low gravity effective Planck scale are set. Constrains on the scales of string models like TeV strings and D-branes are derived. In the last case the lower limit is 1.5 - 4 TeV, depending on the coupling strength.']",['2001-03-23']
257,['eng'],"['von Törne, E', 'Burns, J', 'Duboscq, J E', 'Eckhart, E', 'Honscheid, K', 'Kass, R', 'Larsen, D', 'Rush, C J', 'Smith, S', 'Thayer, J B']",['The Power Supply System of the CLEO III Silicon Detector'],['Particle Physics - Experimental Results'],"['semiconductor detector, microstrip', 'semiconductor detector, power supply', 'electronics, readout', 'electronics, background', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103037'],['The CLEO III detector has recently commenced data taking at the Cornell electron Storage Ring (CESR). One important component of this detector is a 4 layer double-sided silicon tracker with 93% solid angle coverage. This detector ranges in size and number of readout channels between the LEP and LHC silicon detectors. In order to reach the detector performance goals of signal-to-noise ratios greater than 15:1 low noise front-end electronics together with highly regulated low noise power supplies were used. In this paper we describe the low-noise power supply system and associated monitoring and safety features used by the CLEO III silicon tracker.'],['2001-03-22']
258,['eng'],"['Ryd, A']",['A study of time-dependent CP-violating asymmetries in B0 --> J/psi K0S and B0 --> psi(2S) K0S decays'],['Particle Physics - Experimental Results'],"['talk, Sea of Galilee 2000/09/13', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'psi mesons, leptonic decay', 'K0(S), hadronic decay', 'violation, CP', 'particle identification, flavor', 'Kobayashi-Maskawa angle, unitarity', 'neural network', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> J/psi(3100) K0(S)', 'B0 --> psi(3685) K0(S)', 'psi mesons --> lepton+ lepton-', 'K0(S) --> 2pi', '10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103036'],['BABAR has studied the time dependent asymmetries in the the decays B0 -> J/psi K0S and B0 -> psi(2S) K0S in a data set of 9.0 fb^-1 taken at the Y(4S)resonance. In these channels we reconstruct 168 events of which 120 are flavor tagged and used in a likelihood fit where we determine sin2beta. The flavor of the other neutral $B$ mesons is tagged using information primarily from identified leptons and Kaons. A neural network is used to recover events without any clear Kaon or lepton signature. A preliminary result of sin2beta=0.12+/-0.37+/-0.09 is obtained.'],['2001-03-22']
259,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Ajinenko, I', 'Albrecht, Z', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amapane, N', 'Amato, S', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Ballestrero, A', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Behrmann, A', 'Beillière, P', 'Belokopytov, Yu A', 'Benekos, N C', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Bertrand, D', 'Besançon, M', 'Bigi, M', 'Bilenky, S M', 'Bizouard, M A', 'Bloch, D', 'Blom, H M', 'Bonesini, M', 'Boonekamp, M', 'Booth, P S L', 'Borgland, A W', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bourdarios, C', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Bracko, M', 'Branchini, P', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buran, T', 'Buschbeck, Brigitte', 'Buschmann, P', 'Cabrera, S', 'Caccia, M', 'Calvi, M', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chabaud, V', 'Charpentier, P', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Shlyapnikov, P', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Cieslik, K', 'Collins, P', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Crawley, H B', 'Crennell, D J', 'Crépé, S', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', 'Davenport, M', 'Da Silva, W', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Dolbeau, J', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Duperrin, A', 'Durand, J D', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ekspong, Gösta', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Espirito-Santo, M C', 'Fanourakis, G K', 'Fassouliotis, D', 'Fayot, J', 'Feindt, Michael', 'Ferrer, A', 'Ferrer-Ribas, E', 'Ferro, F', 'Fichet, S', 'Firestone, A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J A', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Geralis, T', 'Gerdyukov, L N', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Gris, P', 'Grosdidier, G', 'Grzelak, K', 'Guy, J', 'Haag, C', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Hansen, J', 'Harris, F J', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hessing, T L', 'Heuser, J M', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Huber, M', 'Huet, K', 'Hughes, G J', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Janik, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Jeans, D', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Jungermann, L', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kernel, G', 'Kersevan, B P', 'Khokhlov, Yu A', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kinvig, A', 'Kjaer, N J', 'Klapp, O', 'Klein, H', 'Kluit, P M', 'Kokkinias, P', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kriznic, E', 'Krumshtein, Z', 'Kubinec, P', 'Kurowska, J', 'Kurvinen, K L', 'Lamsa, J W', 'Lane, D W', 'Lapin, V', 'Laugier, J P', 'Lauhakangas, R', 'Leder, Gerhard', 'Ledroit, F', 'Lefébure, V', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lemonne, J', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liebig, W', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Lörstad, B', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Malmgren, T G M', 'Maltezos, S', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Martínez-Vidal, F', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Meroni, C', 'Meyer, W T', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Moch, M', 'Møller, R', 'Mönig, K', 'Monge, M R', 'Moraes, D', 'Moreau, X', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mulet-Marquis, C', 'Muresan, R', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Naraghi, F', 'Nassiakou, M', 'Navarria, Francesco Luigi', 'Navas, S', 'Nawrocki, K', 'Negri, P', 'Neufeld, N', 'Nicolaidou, R', 'Nielsen, B S', 'Niezurawski, P', 'Nikolenko, M', 'Nomokonov, V P', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Orazi, G', 'Österberg, K', 'Ouraou, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Pavel, T', 'Pegoraro, M', 'Peralta, L', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Rames, J', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Rehn, J', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Ripp-Baudot, I', 'Røhne, O M', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Royon, C', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Schwemling, P', 'Schwering, B', 'Schwickerath, U', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Seibert, N', 'Sekulin, R L', 'Shellard, R C', 'Siebel, M', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Smadja, G', 'Smirnov, N', 'Smirnova, O G', 'Smith, G R', 'Sokolov, A', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Squarcia, S', 'Stanescu, C', 'Stanic, S', 'Stanitzki, M', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Taffard, A', 'Tegenfeldt, F', 'Terranova, F', 'Thomas, J', 'Timmermans, J', 'Tinti, N', 'Tkatchev, L G', 'Tobin, M', 'Todorova-Nová, S', 'Tomaradze, A G', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tortosa, P', 'Tranströmer, G', 'Treille, D', 'Tristram, G', 'Trochimczuk, M', 'Troncon, C', 'Turluer, M L', 'Tyapkin, I A', 'Tyapkin, P', 'Tzamarias, S', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'Van der Velde, C', 'van Dam, P', 'Van den Boeck, W', 'Van Doninck, W K', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Remortel, N', 'Van Vulpen, I B', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verdier, P', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Walck, C', 'Washbrook, A J', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zinchenko, A I', 'Zoller, P', 'Zucchelli, G C', 'Zumerle, G']",['Search for supersymmetric partners of top and bottom quarks at $\\sqrt{s}$= 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'squark, search for', 'squark, truth', 'squark, beauty', 'squark, decay', 'neutralino, LSP', 'R parity, invariance', 'squark, mass', 'lower limit', 'electroweak interaction, validity test', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'squark --> beauty neutralino', 'squark --> charm neutralino', '183, 189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103034'],"['Searches for supersymmetric partners of top and bottom quarks are presented using data taken by the DELPHI experiment at LEP in 1997 and 1998. No deviations from standard model expectations are observed in these data sets, which are taken at centre-of-mass energies of 183 GeV and 189 GeV and correspond to integrated luminosities of 54 pb^{-1} and 158 pb^{-1}. These results are used in combination with those obtained by DELPHI at lower centre-of-mass energies to exclude regions in the squark-neutralino mass plane at 95% confidence level.']",['2000-09-25']
260,['eng'],"['Fukuda, S', 'Fukuda, Y', 'Ishitsuka, M', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kobayashi, K', 'Koshio, Y', 'Miura, M', 'Moriyama, S', 'Nakahata, M', 'Nakayama, S', 'Okada, A', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, H', 'Takeuchi, Y', 'Toshito, T', 'Totsuka, Y', 'Yamada, S', 'Desai, S V', 'Earl, M A', 'Kearns, E T', 'Messier, M D', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Goldhaber, M', 'Barszczak, T', 'Casper, David William', 'Gajewski, W', 'Kropp, W R', 'Mine, S', 'Liu, D', 'Price, L R', 'Smy, M B', 'Sobel, H W', 'Vagins, M R', 'Ganezer, K S', 'Keig, W E', 'Ellsworth, R W', 'Tasaka, S', 'Kibayashi, A', 'Learned, J G', 'Matsuno, S', 'Takemori, D', 'Hayato, Y', 'Ishii, T', 'Kobayashi, T', 'Nakamura, K', 'Obayashi, Y', 'Oyama, Y', 'Sakai, A', 'Sakuda, M', 'Kohama, M', 'Suzuki, A T', 'Inagaki, T', 'Nakaya, T', 'Nishikawa, K', 'Haines, T J', 'Blaufuss, E', 'Dazeley, S A', 'Lee, K B', 'Svoboda, R', 'Chen, M L', 'Goodman, J A', 'Guillian, G', 'Sullivan, G W', 'Turcan, D', 'Habig, A', 'Hill, J', 'Jung, C K', 'Martens, K', 'Malek, M', 'Mauger, C', 'McGrew, C', 'Sharkey, E', 'Viren, B M', 'Yanagisawa, C', 'Mitsuda, C', 'Miyano, K', 'Saji, C', 'Shibata, T', 'Kajiyama, Y', 'Nagashima, Y', 'Nitta, K', 'Takita, M', 'Yoshida, M', 'Kim, H I', 'Kim, S B', 'Yoo, J', 'Okazawa, H', 'Ishizuka, T', 'Etoh, M', 'Gando, Y', 'Hasegawa, T', 'Inoue, K', 'Ishihara, K', 'Maruyama, T', 'Shirai, J', 'Suzuki, A', 'Koshiba, M', 'Hatakeyama, Y', 'Ichikawa, Y', 'Koike, M', 'Nishijima, K', 'Fujiyasu, H', 'Ishino, H', 'Morii, M', 'Watanabe, Y', 'Golebiewska, U', 'Kielczewska, D', 'Boyd, S C', 'Stachyra, A L', 'Wilkes, R J', 'Young, K K']",['Constraints on Neutrino Oscillations Using 1258 Days of Super-Kamiokande Solar Neutrino Data'],['Particle Physics - Experimental Results'],"['neutrino, solar', 'neutrino, flux', 'neutrino electron, elastic scattering', 'electron, energy spectrum', 'angular dependence', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103033'],"['We report the result of a search for neutrino oscillations using precise measurements of the recoil electron energy spectrum and zenith angle variations of the solar neutrino flux from 1258 days of neutrino-electron scattering data in Super-Kamiokande. The absence of significant zenith angle variation and spectrum distortion places strong constraints on neutrino mixing and mass difference in a flux-independent way. Using the Super-Kamiokande flux measurement in addition, two allowed regions at large mixing are found.']",['2001-03-21']
261,['eng'],"['Fukuda, S', 'Fukuda, Y', 'Ishitsuka, M', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kobayashi, K', 'Koshio, Y', 'Miura, M', 'Moriyama, S', 'Nakahata, M', 'Nakayama, S', 'Okada, A', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, H', 'Takeuchi, Y', 'Toshito, T', 'Totsuka, Y', 'Yamada, S', 'Desai, S V', 'Earl, M A', 'Kearns, E T', 'Messier, M D', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Goldhaber, M', 'Barszczak, T', 'Casper, David William', 'Gajewski, W', 'Kropp, W R', 'Mine, S', 'Liu, D W', 'Price, L R', 'Smy, M B', 'Sobel, H W', 'Vagins, M R', 'Ganezer, K S', 'Keig, W E', 'Ellsworth, R W', 'Tasaka, S', 'Kibayashi, A', 'Learned, J G', 'Matsuno, S', 'Takemori, D', 'Hayato, Y', 'Ishii, T', 'Kobayashi, T', 'Nakamura, K', 'Obayashi, Y', 'Oyama, Y', 'Sakai, A', 'Sakuda, M', 'Kohama, M', 'Suzuki, A T', 'Inagaki, T', 'Nakaya, T', 'Nishikawa, K', 'Haines, T J', 'Blaufuss, E', 'Dazeley, S A', 'Lee, K B', 'Svoboda, R', 'Chen, M L', 'Goodman, J A', 'Guillian, G', 'Sullivan, G W', 'Turcan, D', 'Habig, A', 'Hill, J', 'Jung, C K', 'Martens, K', 'Malek, M', 'Mauger, C', 'McGrew, C', 'Sharkey, E', 'Viren, B M', 'Yanagisawa, C', 'Mitsuda, C', 'Miyano, K', 'Saji, C', 'Shibata, T', 'Kajiyama, Y', 'Nagashima, Y', 'Nitta, K', 'Takita, M', 'Yoshida, M', 'Kim, H I', 'Kim, S B', 'Yoo, J', 'Okazawa, H', 'Ishizuka, T', 'Etoh, M', 'Gando, Y', 'Hasegawa, T', 'Inoue, K', 'Ishihara, K', 'Maruyama, T', 'Shirai, J', 'Suzuki, A', 'Koshiba, M', 'Hatakeyama, Y', 'Ichikawa, Y', 'Koike, M', 'Nishijima, K', 'Fujiyasu, H', 'Ishino, H', 'Morii, M', 'Watanabe, Y', 'Golebiewska, U', 'Kielczewska, D', 'Boyd, S C', 'Stachyra, A L', 'Wilkes, R J', 'Young, K K']",['Solar 8B and hep Neutrino Measurements from 1258 Days of Super-Kamiokande Data'],['Particle Physics - Experimental Results'],"['neutrino, solar', 'neutrino, flux', 'flux, time variation', 'neutrino electron, elastic scattering', 'electron, energy spectrum', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103032'],"[""Solar neutrino measurements from 1258 days of data from the Super-Kamiokande detector are presented. The measurements are based on recoil electrons in the energy range 5.0-20.0MeV. The measured solar neutrino flux is 2.32 +- 0.03(stat.) +0.08-0.07(sys.)*10^6cm^{-2}s^{-1}, which is 45.1+-0.5(stat.)+1.6-1.4(sys.)% of that predicted by the BP2000 SSM. The day vs night flux asymmetry is 0.033+-0.022(stat.)+0.013-0.012(sys .). The recoil electron energy spectrum is consistent with no spectral distortion (\\chi^2/d.o.f. = 19.0/18). The seasonal variation of the flux is consistent with that expected from the eccentricity of the Earth's orbit (\\chi^2/d.o.f. = 3.7/7). For the hep neutrino flux, we set a 90% C.L. upper limit of 40 *10^3cm^{-2}s^{-1}, which is 4.3 times the BP2000 SSM prediction.""]",['2001-03-21']
262,['eng'],"['Towell, R S', 'McGaughey, P L', 'Awes, T C', 'Beddo, M E', 'Brooks, M L', 'Brown, C N', 'Bush, J D', 'Carey, T A', 'Chang, T H', 'Cooper, W E', 'Gagliardi, C A', 'Garvey, G T', 'Geesaman, D F', 'Hawker, E A', 'He Xiao Chun', 'Isenhower, L D', 'Kaplan, D M', 'Kaufman, S B', 'Kirk, P N', 'Koetke, D D', 'Kyle, G S', 'Lee, D M', 'Lee, W M', 'Leitch, M J', 'Makins, N C R', 'Moss, J M', 'Müller, B A', 'Nord, P M', 'Papavassiliou, V', 'Park, B K', 'Peng, J C', 'Petitt, G', 'Reimer, P E', 'Sadler, M E', 'Sondheim, W E', 'Stankus, P W', 'Thompson, T N', 'Tribble, R E', 'Vasilev, M A', 'Wang, Y C', 'Wang, Z F', 'Webb, J C', 'Willis, J L', 'Wise, D K', 'Young, G R']",['Improved Measurement of the $\\overline{d}/\\overline{u}$ Asymmetry in the Nucleon Sea'],['Particle Physics - Experimental Results'],"['p nucleon, inclusive reaction', 'hydrogen, liquid', 'deuterium, liquid', 'muon, pair production', 'Drell-Yan process', 'nucleon, structure function', 'antiquark, sea', 'asymmetry, (up down)', 'momentum spectrum, parton', 'parametrization', 'sum rule, Gottfried', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'tables', 'bibliography', '800 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103030'],"['Measurements of the ratio of Drell-Yan yields from an 800 \\rm{GeV/c} proton beam incident on liquid hydrogen and deuterium targets are reported. Approximately 360,000 Drell-Yan muon pairs remained after all cuts on the data. From these data, the ratio of anti-down ($\\bar{d}$) to anti-up ($\\bar{u}$) quark distributions in the proton sea is determined over a wide range in Bjorken-$x$. These results confirm previous measurements by E866 and extend them to lower $x$. From these data, $(\\bar{d}-\\bar{u})$ and $\\int(\\bar{d}-\\bar{u} )dx$ are evaluated for $0.015<x<0.35$. These results are compared with parameterizations of various parton distribution functions, models and experimental results from NA51, NMC, and HERMES.']",['2001-03-21']
263,['eng'],"['Nakamura, I']",['Higgs in OPAL'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2001/03/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, mass', 'lower limit', 'Higgs particle, hadronic decay', 'Higgs particle, leptonic decay', 'Z0, decay modes', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'Higgs particle --> 2beauty', 'Higgs particle --> tau+ tau-', 'Z0 --> quark antiquark', 'Z0 --> lepton antilepton', '192-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103029'],"['A search for the Standard Model Higgs boson with the OPAL detector at LEP was reported. The analysis was based on the full data sample collected at center-of-mass energies of 192-209 GeV in 1999 and 2000, corresponding to an integrated luminosity of approximately 426 /pb. The data shows an excess in a range of 95-120 GeV. The data slightly favour the hypothesis that a signal is present, but also that the data are consistent with the background hypothesis. A lower bound of 109.7 GeV is obtained on the Higgs boson mass at the 95% confidence level.']",['2001-03-21']
264,['eng'],"['Mohapatra, A']",['A High-Pt Trigger for the HERA-B Experiment'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'p nucleus, inclusive reaction', 'target, internal', 'quark, beauty', 'B, decay modes', 'transverse momentum, high', 'trigger, efficiency', 'magnetic detector, HERA-B', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103028'],"['We have constructed a high-$p_T$ trigger for the HERA-B experiment at DESY. The HERA-B experiment produces B mesons by inserting wire targets into the halo of the proton beam circulating in HERA. The high-\\pt trigger records events that contain tracks that have high transverse momentum with respect to the beam. Such a trigger is efficient for recording $B \\to \\pi^+\\pi^-$, $B \\to K^-\\pi^+$, $B_s \\to K^+ K^-$, $B_s \\to D_s^-\\pi^+$, and other topical hadronic B decays. These decays provide sensitivity to the internal angles $\\alpha$ and $\\gamma$ of the CKM unitarity triangle, and they also can be used to measure or constrain the $B_s$-$\\bar B_s$ mixing parameter $x_s$.']",['2001-03-20']
265,['eng'],"['Suleymanov, M K', 'Abdinov, O B', 'Angelov, N S', 'Anoshin, A I', 'Vodopyanov, A S', 'Kuznetsov, A A', 'Sadigov, Z Y']",['Transition to the region of central collisions'],['Particle Physics - Experimental Results'],"['talk, Dubna 2000/09/25', 'scattering, heavy ion', 'carbon', 'central region', 'charged particle, multiple production', 'p, multiplicity', 'positive particle, multiplicity', 'dependence, impact parameter', 'charge, dependence', 'quark gluon, string model', 'bubble chamber(heavy liquid), experimental results', 'Dubna PS', '4.2 GeV/c/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103027'],"['The experimental results on the behaviour of the characteristics of secondary particles depending on the disintegration degree of nuclei are used to determine the region of central collisions. It was therefore possible that : - the correlation between the prosesses of total disintegration of nuclei and the central collisions of nuclei had been shown; - the existence of the regime change points in the behaviour of the considered characteristics of secondary particles depending on the disintegration degree of nuclei had been observed in the other earlier experiments as well. The number of all protons in 12CC-interactions at the momentum of 4.2 A GeV/c obtained from the 2-m propane bubble chamber exposed at the Dubna machine is considered as a disintegration degree of nuclei. The experimental results demonstrate that there are cases corresponding to the critical phenomena among the events with the central collisions of nuclei. For 12CC-interaction the behaviour of the number of the events, depending on Q also depends on the number of fragments and has a two-steps form. This result could be explained by the existence of nuclear clusters. The experimental results on the relation between the number of events, the angular distributions of protons and full number of protons are presented for 12CC-interactions at the momentum of 4.2 A GeV/c. The influence of nuclear fragmentation process on the results is also considered. The obtained results confirm the assumption that there exist the critical phenomena among the central collisions and it is necessary to use a percolation approach for the full description of the central collisions.']",['2001-03-20']
266,['eng'],"['Takayama, K', 'Kishiro, J', 'Sakuda, M', 'Wake, M']",['Superbunch Hadron Colliders'],['Particle Physics - Experimental Results'],"['p p, storage ring', 'storage ring, proposed', 'proton synchrotron, induction', 'experimental methods, bunching', 'beam transport, colliding beams', 'scattering, beam-beam', 'luminosity']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103024'],"['A novel concept of a high luminosity hadron collider is proposed. This would be a typical application of an induction synchrotron being newly developed. Extremely long bunches, referred to as superbunches, are generated by a multi- bunch stacking method employing barrier buckets at the injection into the collider, and are accelerated to the collider energy with an step-voltage induced in the induction gaps. Superbunches intersect with each other, yielding a luminosity of more than $10^{35} /cm^2/sec$. A combination of vertical crossing and horizontal crossing can be used in order to avoid any significant beam-beam tune shift.']",['2001-03-19']
267,['eng'],"['Nicollerat, A S']",['Prospects of measuring gluon fusion and weak boson fusion cross sections at the LHC with CMS (diploma thesis)'],['Particle Physics - Experimental Results'],"['thesis', 'p p, interaction', 'Higgs particle, hadroproduction', 'intermediate boson, fusion', 'gluon gluon, fusion', 'Higgs particle, decay modes', 'W, pair production', 'Z0, pair production', 'intermediate boson, leptonic decay', 'intermediate boson, hadronic decay', 'magnetic detector, CMS', 'CERN LHC Coll', 'numerical calculations, Monte Carlo', 'quark quark --> Higgs particle 2quark', 'gluon gluon --> Higgs particle', 'Higgs particle --> 2W', 'Higgs particle --> 2Z0', '14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103023'],['The possibility to observe a Higgs boson having a mass between 300 and 600 GeV and to measure its couplings to vector bosons and top quark with CMS at the LHC is studied. Six different signatures are analyzed. The possibility to separate the Higgs events produced through weak boson fusion from the Higgs produced through gluon fusion using the forward going jets emitted in the weak boson fusion process is discussed for each of these different channels. The results are then used to determine the possible statistical errors on the ratio between the two Higgs decay branching fractions when it decays into Ws and into Zs and the possible statistical errors on the weak boson fusion and gluon fusion cross sections after one year of LHC running.'],['2001-03-19']
268,['eng'],"['Alexander, J P', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Schwarthoff, H', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Poling, R A', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Benslama, K', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H']","['First Observation of $\\bar{b}\\to D^{(*)}\\rho^{\\prime-}$, $ \\rho^{\\prime-}\\to \\omega\\pi^{-}$']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'anti-B, hadronic decay', 'D*(2010)', 'D', 'omega(783)', 'anti-B, branching ratio', 'spin, parity', 'mass spectrum, (omega(783) pi-)', 'meson resonance, mass', 'meson resonance, width', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'anti-B --> D*(2010) pi+ 2pi- pi0', 'anti-B --> D omega(783) pi-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103021'],"[""We report on the observation of Bbar -> D(*) pi+ pi- pi- pi^0 decays. The branching ratios for D*+ and D*0 are (1.72+/-0.14+/-0.24)% and (1.80+/-0.24+/-0.27)%, respectively. Each final state has a D* omega pi- component, with branching ratios (0.29+/-0.03+/-0.04)% and (0.45+/-0.10+/-0.07)% for the D*+ and D*0 modes, respectively. We also observe B -> D omega pi- decays. The branching ratios for D+ and D0 are (0.28+/-0.05+/-0.04)% and (0.41+/-0.07+/-0.06)%, respectively. A spin parity analysis of the D omega pi- final state prefers a wide 1^- resonance. A fit to the omega pi- mass spectrum finds a central mass of (1349+/-25^{+10}_{-5}) MeV and width of (547+/-86^{+46}_{-45}) MeV. We identify this object as the rho(1450) or the \\rho'.""]",['2001-03-16']
269,['eng'],"['Damgov, J', 'Genchev, V', 'Mavrodiev, S C']",['Non-linear energy calibration of CMS calorimeters for single pions'],['Particle Physics - Experimental Results'],"['calorimeter, calibration', 'calibration, nonlinear', 'energy resolution', 'calorimeter, electromagnetic', 'scintillation counter, crystal', 'lead, tungsten', 'copper, zinc', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103019'],['CMS calorimeter energy calibration was done in the full CMS simulated geometry for the pseudorapidity region eta = 0. The samples of single pion events were generated with a set of incident energies from 10 GeV to 3 TeV. The analysis of the simulated data shows that standard calibration using just sampling coefficients for calorimeter parts with different sampling ratio gives nonlinear calorimeter response. Non-linear calibration technique was applied for improving calorimeter energy resolution and restoring the calorimeter linearity.'],['2001-03-16']
270,['eng'],"['de Jong, P']",['Colour Reconnection in W Decays'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'charged particle, multiplicity', 'color, recombination', 'jet, multiple production', 'particle flow', 'W, mass', 'numerical calculations, Monte Carlo', 'interpretation of experiments, CERN LEP Stor', '183-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103018'],['The studies of colour reconnection in e+e- -> WW -> 4 jets events at LEP are reviewed. It is shown that the analysis of the particle- and energy flow between jets is sensitive to realistic model predictions. The effects on the W mass measurement are discussed.'],['2001-03-15']
271,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kamer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, C', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R J', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the Branching Ratio for $D_{s} \\to \\tau\\nu_{\\tau}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, charm', 'quark, pair production', 'D/s*(2110), radiative decay', 'D/s-, leptonic decay', 'D/s-, decay constant', 'D/s-, branching ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'D/s*(2110) --> D/s- photon', 'D/s- --> tau- antineutrino/tau', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103012'],['Using about 3.9 million hadronic Z decays from e+e- collisions recorded by the OPAL detector at LEP at centre-of-mass energies near MZ the branching ratio for the decay D_s -> tau nu_tau has been measured to be (7.0 +/- 2.1(stat) +/- 2.0 (syst))%. This result can be used to derive the decay constant of the D_s meson: f(D_s) = 286 +/- 44(stat) +/- 41(syst) MeV.'],['2001-03-13']
272,['eng'],"['Gan, K K']",['A Novel Optical Package for ATLAS Pixel Detector'],['Detectors and Experimental Techniques'],"['talk, Columbus 2000/08/09', 'semiconductor detector, pixel', 'semiconductor detector, readout', 'optics, fibre', 'semiconductor, optical', 'radiation, laser', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103011'],['An optical package of novel design has been developed for the ATLAS pixel detector. The package contains two VCSELs and one PIN diode to transmit and receive optical signals. The design is based on a simple connector-type concept and is made of radiation-hard material. Several packages have been fabricated and show promising results.'],['2001-03-13']
273,['eng'],"['Gan, K K']",['Tau2000 Conference Summary'],['Particle Physics - Experimental Results'],"['conference, review', 'Victoria 2000/09/18', 'lepton, universality', 'charged current', 'neutral current', 'coupling constant', 'tau, semileptonic decay', 'CVC model, validity test', 'rho(1450)', 'tau, magnetic moment', 'mass, strangeness', 'tau, electric moment', 'neutrino/tau, particle identification', 'neutrino, oscillation', 'neutrino, cosmic radiation', 'flavor, violation', 'interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103010'],"['This is a review of some of the highlights of the 6th workshop on the physics of the tau lepton and its neutrino. This includes the test of lepton universality, measurement of Lorentz Structure, study of hadronic decays, direct evidence of tau neutrino, status of neutrino oscillations, and search for neutrinoless decays. This review concludes with a look at the prospect for tau physics in the future.']",['2001-03-13']
274,['eng'],"['Ferbel, T']","['Search for ""large"" extra dimensions at the Tevatron']",['Particle Physics - Experimental Results'],"['talk, Cairo 2001/01/09', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electron, pair production', 'photon, pair production', 'space-time, higher-dimensional', 'spontaneous compactification', 'Kaluza-Klein model', 'graviton, exchange', 'rapidity spectrum', 'transverse energy, energy spectrum', 'mass', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103009'],"['We report on a search for extra spatial dimensions compactified at radii that are vast compared to those of the Planck length, and even larger than the distance corresponding to the scale of electroweak symmetry breaking. The study is based on the suggestion that there may be only a single mass scale appropriate to particle phenomena, this being the effective Planck scale M_S, which also serves as the scale for electroweak symmetry breaking. The only results that have been presented thus far from the Tevatron are based on data for e^+e^- and \\gamma\\gamma production at D\\O, and provide the most restrictive lower limits to date on M_S of \\approx 1 TeV.']",['2001-03-09']
275,['eng'],"['Arneodo, F']","['The ICARUS Experiment, A Second-Generation Proton Decay Experiment and Neutrino Observatory at the Gran Sasso Laboratory']",['Particle Physics - Experimental Results'],"['p, decay modes', 'muon, cosmic radiation', 'muon, angular distribution', 'muon, flux', 'neutrino, cosmic radiation', 'neutrino, solar', 'neutrino, particle identification', 'neutrino, oscillation', 'supernova', 'neutrino, luminosity', 'calorimeter, liquid argon', 'efficiency', 'deep underground detector, Gran Sasso', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103008'],"['The final phase of the ICARUS physics program requires a sensitive mass of liquid Argon of 5000 tons or more. The T600 detector stands today as the first living proof that such large detector can be built and that liquid Argon imaging technology can be implemented on such large scales. After the successful completion of a series of technical tests to be performed at the assembly hall in Pavia, the T600 detector will be ready to be transported into the LNGS tunnel. The operation of the T600 at the LNGS will allow us (1) to develop the local infrastructure needed to operate our large detector (2) to start the handling of the underground liquid argon technology (3) to study the local background (4) to start the data taking with an initial liquid argon mass that will reach in a 5-6 year program the multi-kton goal. The T600 is to be considered as the first milestone on the road towards a total sensitive mass of 5000 tons: it is the first piece of the detector to be complemented by further modules of appropriate size and dimensions, in order to reach in a most efficient and rapid way the final design mass. In this document, we describe the physics program that will be accomplished within the first phase of the program.']",['2001-03-08']
276,['eng'],"['Kudenko, Yu G']",['Search for T-violation in K^+ --> pi^0 mu^+ nu and K^+ --> mu^+ nu gamma Decays'],['Particle Physics - Experimental Results'],"['talk, Moscow 2000/11/27', 'K+, separated beam', 'K+, semileptonic decay', 'K+, radiative decay', 'at rest', 'muon+, polarization', 'polarization, transverse', 'time reversal, violation', 'pi0, energy', 'asymmetry, energy dependence', 'neutrino, mass spectrum', 'spectrometer, experimental results', 'KEK PS', 'K+ --> pi0 muon+ neutrino', 'K+ --> pi0 muon+ photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103007'],['The recent progress in search for T-violating transverse muon polarization in the decays K^+ --> pi^0 mu^+ nu and K^+ --> mu^+ nu gamma in the on-going experiment E246 at KEK is reported. Future prospects in polarization measurements are also discussed.'],['2001-03-07']
277,['eng'],"['Korzhavina, I A']",['Measurement of D*+/- diffractive cross sections in photoproduction at HERA'],['Particle Physics - Experimental Results'],"['talk, Moscow 2000/11/27', 'positron p, colliding beams', 'positron p, inclusive reaction', 'D*(2010), photoproduction', 'diffraction', 'D*(2010), hadronic decay', 'channel cross section', 'differential cross section', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> D*(2010) p positron anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103003'],"[""The first measurement of D*+/- meson diffractive photoproduction cross sections has been performed with the ZEUS detector at the HERA $ep$ collider, using an integrated luminosity of 38 pb^-1. The measurement has been performed for photon--proton center-of-mass energies in the range 130 < W < 280 GeV and photon virtualities Q^2 < 1 GeV^2. D*+/- mesons have been reconstructed with p_T(D*)>2 GeV and -1.5<\\eta(D*)<1.5 from the decay channel D*+ --> D^0 \\pi^+_s with D^0 --> K-\\pi^+ (+c.c.). The diffractive component has been selected with 0.001<x_Pom<0.018. The measured diffractive cross section in this kinematic range is: \\sigma_(ep --> e'D*Xp') = 0.74 +/- 0.21 (stat.)^{+0.27}_{-0.18} (syst.) +/-0.16 (p. diss.) ~nb (ZEUS preliminary). Measured integrated and differential cross sections have been compared to theoretical expectations.""]",['2001-03-06']
278,['eng'],"['Abe, K', 'Satpathy, M', 'Yamamoto, H']",['Time-dependent angular analyses of B decays'],['Particle Physics - Experimental Results'],"['B0, pair production', 'B0, hadronic decay', 'anti-B0, hadronic decay', 'vector meson, pair production', 'polarization', 'helicity', 'time dependence', 'angular distribution', 'interference, final state', 'violation, CP']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103002'],"['When both B0 and B0bar can decay to the same final state composed of two vectors, the interference between them and those among three polarization states result in intricate phenomena. In this note we derive the time and angular distributions for general B to Va Vb processes in a form convenient for actual analyses. We then apply them to specific examples and clarify the CP violating parameters obtainable in the D* rho and J/\\psi K* final states. The time distributions for the D*pi final states are also discussed.']",['2001-03-05']
279,['eng'],"['Ahn, S H', 'An, S', 'Aoki, S', 'Berns, H G', 'Bhang, H C', 'Boyd, S', 'Casper, David William', 'Chikamatsu, T', 'Choi, J H', 'Echigo, S', 'Etoh, M', 'Fujii, K', 'Fukuda, S', 'Fukuda, Y', 'Gajewski, W', 'Golebiewska, U', 'Hara, T', 'Hasegawa, T', 'Hayato, Y', 'Hill, J', 'Hong, S J', 'Ieiri, M', 'Inada, T', 'Inagaki, T', 'Ishida, T', 'Ishii, H', 'Ishii, T', 'Ishino, H', 'Ishitsuka, M', 'Itow, Y', 'Iwashita, T', 'Jang, H I', 'Jang, J S', 'Jeon, E J', 'Jeong, E M', 'Jung, C K', 'Kadowaki, T', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kato, I', 'Kato, Y', 'Kearns, E T', 'Kenmochi, S', 'Khang, B H', 'Kibayashi, A', 'Kielczewska, D', 'Kim, B J', 'Kim, C O', 'Kim, H I', 'Kim, J H', 'Kim, J Y', 'Kim, S B', 'Kishi, S', 'Kitamura, M', 'Kobayashi, K', 'Kobayashi, T', 'Kobayashi, Y', 'Kohama, M', 'Koo, D G', 'Koshio, Y', 'Kropp, W R', 'Kume, G', 'Kusano, E', 'Learned, J G', 'Lee, H K', 'Lee, J W', 'Lee, S B', 'Lim, I T', 'Lim, S H', 'Maesaka, H', 'Martens, K', 'Maruyama, T', 'Matsuno, S', 'Mauger, C', 'McGrew, C', 'Minakawa, M', 'Mine, S', 'Miura, M', 'Miyamoto, S', 'Miyano, K', 'Moriyama, S', 'Mukai, S', 'Nakahata, M', 'Nakamura, K', 'Nakamura, M', 'Nakano, I', 'Nakaya, T', 'Nakayama, S', 'Nakayoshi, K', 'Nishijima, K', 'Nishikawa, K', 'Nishiyama, S', 'Noda, S', 'Noumi, H', 'Obayashi, Y', 'Oh, J K', 'Okada, A', 'Onchi, M', 'Otaki, T', 'Oyama, Y', 'Pac, M Y', 'Park, H', 'Park, S H', 'Park, S K', 'Sakai, A', 'Sakuda, M', 'Sakurai, N', 'Sasao, N', 'Sato, K', 'Scholberg, K', 'Seo, E', 'Sharkey, E', 'Shiino, K', 'Shima, A', 'Shiozawa, M', 'So, H', 'Sobel, H', 'Stachyra, A', 'Stone, J L', 'Sulak, Lawrence R', 'Suzuki, A', 'Suzuki, Y', 'Suzuki, Y', 'Takasaki, M', 'Takatsuki, M', 'Takenaka, K', 'Takeuchi, H', 'Takeuchi, Y', 'Tamura, N', 'Tanaka, K H', 'Tanaka, Y', 'Tashiro, K', 'Tauchi, K', 'Toshito, T', 'Totsuka, Y', 'Tumakov, V', 'Umeda, T', 'Vagins, M R', 'Walter, C W', 'Wilkes, R J', 'Yamada, S', 'Yamaguchi, T', 'Yamanoi, Y', 'Yanagisawa, C', 'Yokoyama, H', 'Yokoyama, H', 'Yoo, J', 'Yoshida, M', 'You, S Y']",['Detection of Accelerator-Produced Neutrinos at a Distance of 250 km'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'neutrino/mu, beam', 'neutrino/mu, energy spectrum', 'neutrino nucleon, interaction', 'charged current', 'time dependence', 'Cherenkov counter, ring imaging', 'experimental results', 'deep underground detector, KAMIOKANDE', 'KEK PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0103001'],"['The KEK to Kamioka long-baseline neutrino experiment (K2K) has begun its investigation of neutrino oscillations suggested by atmospheric neutrino observations. Twenty-eight neutrino events have been detected in coincidence with the expected arrival time of the beam in the 22.5 kt fiducial volume of Super--Kamiokande, the far detector at 250 km distance. The expectation is 37.8+3.5-3.8, derived using measurements of neutrino interactions in a near detector and extrapolation using a beam simulation validated by a measurement of pion kinematics after production and focusing. The background is of order 10^-3 events.']",['2001-03-02']
280,['eng'],"['Schleper, P']",['Soft Hadronic Interactions'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'lepton p, deep inelastic scattering', 'hadron hadron, interaction', 'p, structure function', 'small-x', 'photon, structure function', 'momentum transfer, dependence', 'diffraction, structure function', 'vector meson, photoproduction', 'cross section, energy dependence', 'quantum chromodynamics', 'Altarelli-Parisi equation', 'Lipatov equation', 'gluon, momentum spectrum', 'momentum transfer, low', 'structure function, charm', 'jet, pair production', 'numerical calculations', 'interpretation of experiments, DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102051'],"['Recent developments in soft hadronic interactions are reviewed. Emphasis it put on measurements of the proton structure at low x, photon structure, diffraction and exclusive processes such as vector-meson production and their interpretation in approaches to QCD dynamics like BFKL or CCFM.']",['2001-03-01']
281,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Anthonis, T', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bahr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, B', 'Brown, D P', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coppens, Y R', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dingfelder, J', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Dubak, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Fleming, Y H', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Gerlich, C', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hildebrandt, M', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Kjellberg, P', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Koutouev, R', 'Koutov, A', 'Krehbiel, H', 'Kroseberg, J', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Laycock, P', 'Lebailly, E', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'List, B', 'Lobodzinska, E', 'Lobodzinski, B', 'Loginov, A', 'Loktionova, N', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, U', 'Martyniak, J', 'Maxfield, S J', 'Meer, D', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Meyer, A B', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Peez, M', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Risler, C', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schmitt, S', 'Schneider, M', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Schwanenberger, C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Tsurin, I', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vasilev, S', 'Vazdik, Ya', 'Vichnevski, A', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Werner, M', 'Werner, N', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Searches at HERA for Squarks in R-Parity Violating Supersymmetry'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'sparticle, search for', 'supersymmetry', 'R parity, violation', 'quark', 'fusion, positron', 'squark, decay modes', 'squark, mass', 'lower limit', 'electroweak interaction, validity test', 'supergravity', 'coupling, Yukawa', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102050'],"[""A search for squarks in R-parity violating supersymmetry is performed in e^+p collisions at HERA at a centre of mass energy of 300 GeV, using H1 data corresponding to an integrated luminosity of 37 pb^(-1). The direct production of single squarks of any generation in positron-quark fusion via a Yukawa coupling lambda' is considered, taking into account R-parity violating and conserving decays of the squarks. No significant deviation from the Standard Model expectation is found. The results are interpreted in terms of constraints within the Minimal Supersymmetric Standard Model (MSSM), the constrained MSSM and the minimal Supergravity model, and their sensitivity to the model parameters is studied in detail. For a Yukawa coupling of electromagnetic strength, squark masses below 260 GeV are excluded at 95% confidence level in a large part of the parameter space. For a 100 times smaller coupling strength masses up to 182 GeV are excluded.""]",['2001-03-01']
282,['eng'],"['Goncharov, M', 'Adams, T', 'Alton, A', 'Bolton, T', 'Goldman, J', 'Spentzouris, P', 'Conrad, J', 'Fleming, B T', 'Formaggio, J A', 'Koutsoliotas, S', 'Kim, J H', 'McNulty, C', 'Romosan, A', 'Shaevitz, M H', 'Stern, E G', 'Vaitaitis, A G', 'Zimmerman, E D', 'Johnson, R A', 'Vakili, M', 'Suwonjandee, N', 'Bernstein, R H', 'Bugel, L', 'Lamm, M J', 'Marsh, W', 'Nienaber, P', 'Yu, J', 'De Barbaro, L', 'Buchholz, D', 'Schellman, H', 'Zeller, G P', 'Brau, J E', 'Drucker, R B', 'Frey, R', 'Mason, D', 'McDonald, J E', 'Naples, D', 'Tzanov, M', 'Avvakumov, S', 'De Barbaro, P', 'Bodek, Arie', 'Budd, H S', 'Harris, D A', 'McFarland, K S', 'Sakumoto, W K', 'Yang, U K']",['Precise Measurement of Dimuon Production Cross-Sections in muon neutrino Fe and muon antineutrino Fe Deep Inelastic Scattering at the Tevatron'],['Particle Physics - Experimental Results'],"['neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'muon, pair production', 'charged current', 'quark, charm', 'quark, neutrinoproduction', 'quark, semileptonic decay', 'differential cross section, x-dependence', 'energy dependence', 'experimental results', 'Batavia TEVATRON PS', 'tables', 'neutrino/mu iron --> muon+ muon- anything']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102049'],"['We present measurements of the semi-inclusive cross-sections for muon neutrino and muon antineutrino-nucleon deep inelastic scattering interactions with two oppositely charged muons in the final state. These events dominantly arise from production of a charm quark during the scattering process. The measurement was obtained from the analysis of 5102 muon neutrino-induced and 1458 muon antineutrino-induced events collected with the NuTeV detector exposed to a sign-selected beam at the Fermilab Tevatron. We also extract a cross-section measurement from a re-analysis of 5030 muon neutrino-induced and 1060 muon antineutrino-induced vents collected from the exposure of the same detector to a quad-triplet beam by the CCFR experiment. The results are combined to obtain the most statistically precise measurement of neutrino-induced dimuon production cross-sections to date. These measurements should be of broad use to phenomenologists interested in the dynamics of charm production, the strangeness content of the nucleon, and the CKM matrix element Vcd.']",['2001-02-27']
283,['eng'],"['Abazov, V M', 'Abbott, B', 'Abdesselam, A', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Ahmed, S N', 'Alexeev, G D', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Bacon, T C', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Todorova-Nová, S', 'Barberis, E', 'Baringer, P', 'Barreto, J', 'Bartlett, J F', 'Bassler, U', 'Bauer, D', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Beuselinck, R', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Bos, Kors', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Davis, G A', 'Davis, K', 'De, K', 'De Jong, S J', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Duflot, L', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Filthaut, F', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E', 'Galyaev, A N', 'Gao, M', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hildreth, M D', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Huang, Y', 'Illingworth, R', 'Ito, A S', 'Jaffré, M', 'Jain, S', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Kalinin, A M', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kharchilava, A I', 'Kim, S K', 'Klima, B', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krivkova, P', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kupco, A', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Leggett, C', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Luo, C', 'Maciel, A K A', 'Madaras, R J', 'Malyshev, V L', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Nunnemann, T', ""O'Neil, D C"", 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Papageorgiou, K', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Petroff, P', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Ridel, M', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M', 'Rubinov, P', 'Ruchti, R C', 'Rutherfoord, J P', 'Sabirov, B M', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Sen, N', 'Shabalina, E', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Vertogradov, L S', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yatsunenko, Yu A', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Search for heavy particles decaying into electron-positron pairs in p-pbar collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electron, pair production', 'new particle, search for', 'technicolor', 'technirho', 'techniomega', ""Z'"", 'mass spectrum, (positron electron)', 'mass, lower limit', 'channel cross section, mass', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> positron electron anything', '1800 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102048', 'http://www-d0.fnal.gov/public/run1/ichep2k/meena.ps']","[""We present results of searches for technirho, techniomega, and Z' particles, using the decay channels technirho, techniomega, Z' -> e+e-. The search is based on 124.8 pb-1 of data collected by the D0 detector at the Fermilab Tevatron during 1992-1996. In the absence of a signal, we set 95% C.L. upper limits on the cross sections for the processes p pbar -> technirho, techniomega, Z' -> e+e- as a function of the mass of the decaying particle. For certain model parameters, we exclude the existence of degenerate technirho and techniomega states with masses below about 200 GeV. We exclude a Z' with mass below 670 GeV, assuming that it has the same couplings to fermions as the Z boson.""]",['2001-02-27']
284,['eng'],"['Erdmann, M']",['Determination of the Quark-Antiquark Interactions using Leading Particle Measurements'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'quark, heavy', 'quark, pair production', 'quark antiquark, strong interaction', 'D*(2010), electroproduction', 'B*(5320), electroproduction', 'B, electroproduction', 'rapidity, difference', 'scaling', 'quark, hadronization', 'formation, time', 'quark, mass', 'fragmentation function, leading particle', 'quark antiquark, potential']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102047'],"['Measurements of heavy quark production in electron-positron collisions are used to analyse the strong interactions between quarks and anti-quarks. A scaling behaviour is observed in distributions of the rapidity change of D*, B*, and B mesons. From these distributions information is obtained on the hadron formation time, effective quark masses, and the potential between quark-antiquark pairs. Predictions for fragmentation functions of leading hadrons are presented.']",['2001-02-26']
285,['eng'],"['Battaglia, M', 'Caccia, M', 'Borghi, S', 'Campagnolo, R', 'Domanski, K', 'Grabiec, P', 'Jaroszewicz, B', 'Marczewski, J', 'Tomaszewski, D', 'Kucewicz, W', 'Zalewska, Agnieszka', 'Tammi, K']",['A Pixel Vertex Tracker for the TESLA Detector'],['Particle Physics - Experimental Results'],"['electron positron, colliding beam detector', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'semiconductor detector, readout', 'fabrication', 'spatial resolution', 'numerical calculations, Monte Carlo', 'linear collider, proposed', 'DESY TESLA Linac']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102046'],"['In order to fully exploit the physics potential of a e+e- linear collider, such as TESLA, a Vertex Tracker providing high resolution track reconstruction is required. Hybrid Silicon pixel sensors are an attractive sensor technology option due to their read-out speed and radiation hardness, favoured in the high rate TESLA environment, but have been so far limited by the achievable single point space resolution. A novel layout of pixel detectors with interleaved cells to improve their spatial resolution is introduced and the results of the characterisation of a first set of test structures are discussed. In this note, a conceptual design of the TESLA Vertex Tracker, based on hybrid pixel sensors is presented']",['2001-02-26']
286,['eng'],"['Zarnecki, A F']",['Measurement of the leptoquark Yukawa couplings in e+e- collisions at TESLA'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'new particle, electroproduction', 'leptoquark', 'quantum number', 'photon electron, inclusive reaction', 'Feynman graph', 'electron, pair production', 'jet, pair production', 'mass spectrum', 'transverse momentum, spectra', 'angular distribution', 'coupling, Yukawa', 'numerical calculations, DESY TESLA Linac', '800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102043'],"['Measurement of the Yukawa couplings of the first-generation leptoquarks has been studied for e+e- collisions at TESLA, at sqrt(s)=800 GeV. By combining measurements from different production and decay channels, determination of Yukawa couplings with precision on the few per-cent level is possible. TESLA will be sensitive to very small leptoquark Yukawa couplings not accessible at LHC, down to lambda ~ 0.05 [e]. Distinction between left-handed and right-handed Yukawa couplings is feasible even for leptoquark masses very close to the pair-production kinematic limit.']",['2001-02-23']
287,['eng'],"['Breitweg, J', 'Abe, T', 'Abramowicz, H', 'Adamczyk, L', 'Adamus, M', 'Aghuzumtsyan, G', 'Ahn, S H', 'Amelung, C', 'Antonioli, P', 'Antonov, A', 'Arneodo, M', 'Badgett, W F', 'Bailey, D C', 'Bailey, D S', 'Bamberger, Andreas', 'Barakbaev, A N', 'Barbagli, G', 'Barbi, M S', 'Bari, G', 'Barreiro, F', 'Barret, O', 'Bashkirov, V', 'Basile, M', 'Bauerdick, L A T', 'Bednarek, B', 'Behrens, U', 'Bell, M', 'Bellagamba, L', 'Benen, A', 'Bertolin, A', 'Bienlein, J K', 'Bodmann, B', 'Bokel, C', 'Boogert, S', 'Boos, E G', 'Borras, K', 'Boscherini, D', 'Botje, M', 'Brock, I', 'Brook, N H', 'Brugnera, R', 'Bruni, A', 'Bruni, G', 'Brümmer, N', 'Bussey, Peter J', 'Butterworth, J M', 'Bylsma, B', 'Caldwell, A', 'Capua, M', 'Cara Romeo, G', 'Carli, T', 'Carlin, R', 'Cartiglia, N', 'Chapin, D', 'Chekanov, S', 'Chiochia, V', 'Chwastowski, J', 'Ciborowski, J', 'Ciesielski, R', 'Cifarelli, Luisa', 'Cindolo, F', 'Cirio, R', 'Cloth, P', 'Coboken, K', 'Coldewey, C', 'Cole, J E', 'Contin, A', 'Cooper-Sarkar, A M', 'Coppola, N', 'Cormack, C', 'Corradi, M', 'Corriveau, F', 'Costa, M', 'Crittenden, J A', 'Cross, R', ""D'Agostini, G"", 'Dagan, S', 'Dal Corso, F', 'Danilov, P', 'Dannheim, D', 'De Pasquale, S', 'De Wolf, E', 'Del Peso, J', 'Dementiev, R K', 'Deppe, O', 'Derrick, Malcolm', 'Desler, K', 'Devenish, R C E', 'Dolgoshein, B A', 'Doyle, A T', 'Drews, G', 'Durkin, L S', 'Dusini, S', 'Eisenberg, Y', 'Eisenhardt, S', 'Engelen, J', 'Epperson, D E', 'Ermolov, P F', 'Eskreys, Andrzej', 'Fagerstroem, C P', 'Ferrero, M I', 'Figiel, J', 'Filges, D', 'Foster, B', 'Foudas, C', 'Fox-Murphy, A', 'Fricke, U', 'Fusayasu, T', 'Gabareen, A', 'Gadaj, T', 'Galea, R', 'Gallo, E', 'García, G', 'Garfagnini, A', 'Geiser, A', 'Gendner, N', 'Gialas, I', 'Gilmore, J', 'Ginsburg, C M', 'Giusti, P', 'Gladilin, L K', 'Gladkov, D', 'Glasman, C', 'Goebel, F', 'Goers, S', 'Golubkov, Yu A', 'Goncalo, R', 'González, O', 'Graciani, R', 'Grijpink, S', 'Grosse-Knetter, J', 'Grzelak, G', 'Gwenlan, C', 'Göttlicher, P', 'Haas, T', 'Hain, W', 'Hamatsu, R', 'Hart, J C', 'Hartmann, H', 'Hartner, G F', 'Hayes, M E', 'Heaphy, E A', 'Heath, G P', 'Heath, H F', 'Hebbel, K', 'Heinloth, K', 'Heusch, C A', 'Hilger, E', 'Hillert, S', 'Hirose, T', 'Hochman, D', 'Holm, U', 'Iacobucci, G', 'Iannotti, L', 'Inuzuka, M', 'Irrgang, P', 'Ishii, T', 'Jakob, H P', 'Jelen, K', 'Jeoung, H Y', 'Jones, T W', 'Kananov, S', 'Kappes, A', 'Karshon, U', 'Katkov, I I', 'Katz, U F', 'Kcira, D', 'Kerger, R', 'Khein, L A', 'Kim, C L', 'Kim, J Y', 'Kind, O', 'Kisielewska, D', 'Kitamura, S', 'Klimek, K H', 'Koch, W', 'Koffeman, E', 'Kohno, T', 'Kooijman, P M', 'Koop, T', 'Korotkova, N A', 'Korzhavina, I A', 'Kotanski, Andrzej', 'Kowal, A M', 'Kowalski, H', 'Kowalski, T', 'Krakauer, D A', 'Kreisel, A', 'Kuze, M', 'Kuzmin, V A', 'Kötz, U', 'Labarga, L', 'Labes, H', 'Lane, J B', 'Lee, J H', 'Lee, S B', 'Lee, S W', 'Levi, G', 'Levman, G M', 'Levy, A', 'Lim, H', 'Lim, I T', 'Limentani, S', 'Ling, T Y', 'Liu, W', 'Liu, X', 'Lohrmann, E', 'Long, K R', 'Longhin, A', 'López-Duran-Viani, A', 'Lukina, O Yu', 'Lupi, A', 'Löhr, B', 'Ma, K J', 'MacDonald, N', 'Magill, S', 'Mankel, R', 'Margotti, A', 'Marini, G', 'Markun, P', 'Martens, J', 'Martin, J F', 'Martínez, M', 'Maselli, S', 'Massam, Thomas', 'Mastroberardino, A', 'Matsushita, T', 'Matsuzawa, K', 'Mattingly, M C K', 'Mattingly, S E', 'McCance, G J', 'McCubbin, N A', 'Mellado, B', 'Meyer, A', 'Milite, M', 'Miller, D B', 'Mirea, A', 'Monaco, V', 'Moritz, M', 'Musgrave, B', 'Nagano, K', 'Nania, R', 'Nigro, A', 'Nishimura, T', 'Notz, D', 'Nowak, R J', 'Oh, B Y', 'Okrasinski, J R', 'Olkiewicz, K', 'Pac, M Y', 'Padhi, S', 'Paganis, S', 'Palmonari, F', 'Parenti, A', 'Park, I H', 'Park, S K', 'Paul, E', 'Pavel, N', 'Pawlak, J M', 'Pawlak, R', 'Pelfer, P G', 'Pellegrino, A R', 'Peroni, C', 'Pesci, A', 'Petrucci, M C', 'Pokrovskiy, N S', 'Polini, A', 'Posocco, M', 'Proskuryakov, A S', 'Przybycien, M B', 'Raach, H', 'Rautenberg, J', 'Redondo, I', 'Reeder, D D', 'Repond, J', 'Robins, S A', 'Rodrigues, E', 'Rohde, M', 'Rulikowska-Zarebska, E', 'Ruske, O', 'Ruspa, M', 'Sabetfakhri, A', 'Sacchi, R', 'Sadrozinski, H F W', 'Salehi, H', 'Sampson, S', 'Sartorelli, G', 'Saull, P R B', 'Savin, A A', 'Saxon, D H', 'Schagen, S', 'Schioppa, M', 'Schlenstedt, S', 'Schmidke, W B', 'Schneekloth, U', 'Schnurbusch, H', 'Sciulli, F', 'Scott, J', 'Seiden, A', 'Selonke, F', 'Shah, T P', 'Shcheglova, L M', 'Sinclair, L E', 'Skillicorn, Ian O', 'Smalska, B', 'Smith, W H', 'Solano, A', 'Solomin, A N', 'Son, D', 'Sosnovtsev, V V', 'Staiano, A', 'Stairs, D G', 'Stanco, L', 'Stanek, R', 'Stifutkin, A', 'Stonjek, S', 'Stopa, P', 'Straub, P B', 'Suchkov, S', 'Susinno, G', 'Suszycki, L', 'Sutton, M R', 'Szuba, D', 'Tandler, J', 'Tapper, A D', 'Tapper, R J', 'Tassi, E', 'Terron, J', 'Tiecke, H G', 'Tokushuku, K', 'Toothacker, W S', 'Tsurugai, T', 'Tuning, N', 'Turcato, M', 'Tymieniecka, T', 'Umemori, K', 'Vaiciulis, A W', 'Van Sighem, A', 'Vázquez, M E', 'Velthuis, J J', 'Vlasov, N N', 'Voss, K C', 'Vossebeld, J H', 'Walczak, R', 'Walker, R', 'Waugh, R', 'Weber, A', 'West, B J', 'Whitmore, J J', 'Wichmann, R', 'Wick, K', 'Wieber, H', 'Wiggers, L', 'Wildschek, T', 'Williams, D C', 'Wing, M', 'Wodarczyk, M', 'Wolf, G', 'Wollmer, U', 'Wróblewski, A K', 'Wölfle, S', 'Yamada, S', 'Yamashita, T', 'Yamazaki, Y', 'Yildirim, A', 'Yoshida, R', 'Youngman, C', 'Zakrzewski, J A', 'Zawiejski, L', 'Zeuner, W', 'Zhautykov, B O', 'Zichichi, Antonino', 'Ziegler, A', 'Zotkin, S A']",['Measurement of dijet production in neutral current deep inelastic scattering at high Q**2 and determination of alpha_s'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'neutral current', 'jet, pair production', 'yield, (2jet)', 'differential cross section', 'transverse momentum, dependence', 'quantum chromodynamics, perturbation theory', 'p, structure function', 'momentum spectrum, parton', 'strong interaction, coupling constant', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'tables', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102042'],"['Dijet production has been studied in neutral current deep inelastic e+p scattering for 470 < Q**2 < 20000 GeV**2 with the ZEUS detector at HERA using an integrated luminosity of 38.4 pb**{-1}. Dijet differential cross sections are presented in a kinematic region where both theoretical and experimental uncertainties are small. Next-to-leading-order (NLO) QCD calculations describe the measured differential cross sections well. A QCD analysis of the measured dijet fraction as a function of Q**2 allows both a precise determination of alpha_s(M_Z) and a test of the energy-scale dependence of the strong coupling constant. A detailed analysis provides a realistic estimate of the uncertainties of the NLO QCD cross sections arising from the parton distribution functions of the proton. The value of alpha_s(M_Z), as determined from the QCD fit, is alpha_s(M_Z) = 0.1166 +- 0.0019 (stat.) {+ 0.0024}_{- 0.0033} (exp.)} {+ 0.0057}_{- 0.0044} (th.).']",['2001-02-22']
288,['eng'],"['Link, J M', 'Reyes, M', 'Yager, P M', 'Anjos, J C', 'Bediaga, I', 'Göbel, C', 'Magnin, J', 'Massafferri, A', 'De Miranda, J M', 'Pepe, I M', 'Dos Reis, A C', 'Simão, F R A', 'Carrillo, S', 'Casimiro, E', 'Sánchez-Hernández, A', 'Uribe, C', 'Vázquez, F', 'Cinquini, L', 'Cumalat, J P', ""O'Reilly, B"", 'Ramírez, J E', 'Vaandering, E W', 'Butler, J N', 'Cheung, H W K', 'Gaines, I', 'Garbincius, P H', 'Garren, L A', 'Gottschalk, E E', 'Kasper, P H', 'Kreymer, A E', 'Kutschke, R', 'Bianco, S', 'Fabbri, F L', 'Sarwar, S', 'Zallo, A']",['Measurement of the relative branching ratio BR(\\Xi_c^+ \\to p^+ K^-\\pi^+)\\BR(\\Xi_c^+ \\to \\Xi^- \\pi^+ \\pi^+)'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium', 'charmed particle, photoproduction', 'Xi/c+, hadronic decay', 'Xi/c+, branching ratio', 'mass spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'Xi/c+ --> p K- pi+', 'Xi/c+ --> Xi- 2pi+', 'Xi/c+ --> p K*(892)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102040'],['We report the observation of the Cabibbo suppressed decay \\Xi_c^+ \\to p K^-\\pi^+ using data collected with the FOCUS spectrometer during the 1996--97 Fermilab fixed target run. We find a \\Xi_c^+ signal peak of 202\\pm35 events. We have measured the relative branching ratios BR(\\Xi^+_c\\to p K^-\\pi^+)/BR(\\Xi^+_c\\to\\Xi^-\\pi^+\\pi^+)= 0.234 \\pm 0.047 \\pm 0.022 and BR(\\Xi^+_c\\to p \\bar{K}^*(892)^0)/BR(\\Xi^+_c\\to p K^-\\pi^+)= 0.54 \\pm 0.09 \\pm 0.05 .'],['2001-02-22']
289,['eng'],"['Airapetian, A', 'Akopov, N Z', 'Akopov, N Z', 'Amarian, M', 'Arrington, J', 'Aschenauer, E C', 'Avakian, H', 'Avakian, R', 'Avetisian, A', 'Avetissian, E', 'Bailey, P', 'Bains, B', 'Baumgarten, C', 'Beckmann, M', 'Belostotskii, S', 'Bernreuther, S', 'Bianchi, N', 'Böttcher, H', 'Borisov, A', 'Bouwhuis, M', 'Brack, J', 'Brauksiepe, S', 'Braun, B', 'Brückner, W', 'Brüll, A', 'Budz, P', 'Bulten, H J', 'Capitani, G P', 'Carter, P', 'Chumney, P', 'Cisbani, E', 'Court, G R', 'Dalpiaz, P F', 'De Leo, R', 'De Nardo, L', 'De Sanctis, E', 'De Schepper, D', 'Devitsin, E G', 'De Witt-Huberts, P K A', 'Di Nezza, P', 'Dzhordzhadze, V', 'Düren, M', 'Dvoredsky, A P', 'Elbakian, G M', 'Ely, J', 'Fantoni, A', 'Feshchenko, A', 'Felawka, L', 'Ferro-Luzzi, M', 'Fiedler, K', 'Filippone, B W', 'Fischer, H', 'Fox, B', 'Franz, J', 'Frullani, S', 'Gärber, Y', 'Garibaldi, F', 'Garutti, E', 'Gavrilov, G', 'Karibian, V', 'Golendukhin, A', 'Graw, G', 'Grebenyuk, O', 'Green, P W', 'Greeniaus, L G', 'Gute, A', 'Haeberli, W', 'Hartig, M', 'Hasch, D', 'Heesbeen, D', 'Heinsius, F H', 'Henoch, M', 'Hertenberger, R', 'Hesselink, W H A', 'Hofman, G J', 'Holler, Y', 'Holt, R J', 'Hommez, B', 'Iarygin, G', 'Iodice, M', 'Izotov, A A', 'Jackson, H E', 'Jgoun, A', 'Jung, P', 'Kaiser, R', 'Kanesaka, J', 'Kinney, E R', 'Kiselev, A', 'Kitching, P', 'Kobayashi, H', 'Koch, N', 'Königsmann, Kay C', 'Kolster, H', 'Korotkov, V A', 'Kotik, E', 'Kozlov, V', 'Krivokhizhin, V G', 'Kyle, G S', 'Lagamba, L', 'Laziev, A', 'Lenisa, P', 'Lindemann, T', 'Lorenzon, W', 'Makins, N C R', 'Martin, J W', 'Marukyan, H O', 'Masoli, F', 'McAndrew, M', 'McIlhany, K', 'McKeown, R D', 'Meissner, F', 'Menden, F', 'Metz, A', 'Meyners, N', 'Miklukho, O', 'Miller, C A', 'Milner, R', 'Muccifora, V', 'Mussa, R', 'Nagaitsev, A P', 'Nappi, E', 'Naryshkin, Yu', 'Nass, A', 'Negodaeva, K', 'Nowak, W D', 'Oganessyan, K A', ""O'Neill, T G"", 'Openshaw, R', 'Ouyang, J', 'Owen, B R', 'Pate, S F', 'Potashov, S', 'Potterveld, D H', 'Rakness, G', 'Rappoport, V', 'Redwine, R P', 'Reggiani, D', 'Reolon, A R', 'Ristinen, R', 'Rith, K', 'Robinson, D', 'Rostomyan, A', 'Ruh, M', 'Ryckbosch, D', 'Sakemi, Y', 'Sato, F', 'Savin, I A', 'Scarlett, C', 'Schäfer, A', 'Schill, C', 'Schmidt, F', 'Schnell, G', 'Schüler, K P', 'Schwind, A', 'Seibert, J', 'Seitz, B', 'Shibata, T A', 'Shin, T', 'Shutov, V', 'Simani, C', 'Simon, A', 'Sinram, K', 'Steffens, E', 'Steijger, J J M', 'Stewart, J', 'Stösslein, U', 'Suetsugu, K', 'Sutter, M F', 'Szymanowski, L', 'Taroian, S P', 'Terkulov, A R', 'Teryaev, O V', 'Tessarin, S', 'Thomas, E', 'Tipton, B', 'Tytgat, M', 'Urciuoli, G M', 'Van den Brand, J F J', 'van der Steenhoven, G', 'Van de Vyver, R', 'Van Hunen, J J', 'Vetterli, M C', 'Vikhrov, V V', 'Vincter, M G', 'Visser, J', 'Volk, E', 'Weiskopf, C', 'Wendland, J', 'Wilbert, J', 'Wise, T', 'Yen, S', 'Yoneyama, S', 'Zohrabyan, H G']",['Double-Spin Asymmetry in the Cross Section for Exclusive rho^0 Production in Lepton-Proton Scattering'],['Particle Physics - Experimental Results'],"['electron p, exclusive reaction', 'positron p, deep inelastic scattering', 'positron, polarized beam', 'hydrogen, polarized target', 'polarization, longitudinal', 'rho(770)0, electroproduction', 'cross section, polarization', 'spin, asymmetry', 'vector dominance', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'positron p --> p rho(770)0 positron', 'rho(770)0 --> pi+ pi-', '27.56 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102037'],"['Evidence for a positive longitudinal double-spin asymmetry <A_1^rho> = 0.24 +-0.11 (stat) +-0.02 (syst) in the cross section for exclusive diffractive rho^0(770) vector meson production in polarised lepton-proton scattering was observed by the HERMES experiment. The longitudinally polarised 27.56 GeV HERA positron beam was scattered off a longitudinally polarised pure hydrogen gas target. The average invariant mass of the photon-proton system has a value of <W> = 4.9 GeV, while the average negative squared four-momentum of the virtual photon is <Q^2> = 1.7 GeV^2. The ratio of the present result to the corresponding spin asymmetry in inclusive deep-inelastic scattering is in agreement with an early theoretical prediction based on the generalised vector meson dominance model.']",['2001-04-04']
290,['eng'],"['Bizzeti, A']",['New results from NA48 experiment on neutral kaon rare decays'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'K0, rare decay', 'K0(S), semileptonic decay', 'K0(L), semileptonic decay', 'mass spectrum, (pi+ pi- positron electron)', 'violation, CP', 'magnetic spectrometer, experimental results', 'CERN SPS', 'K0 --> pi+ pi- positron electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102035'],"['Recent results by the NA48 collaboration on neutral kaons rare decays into the pi+ pi- e+ e- final state are presented. A large CP-violating asymmetry A(K_L)=(13.9+-2.7+-2.0)% has been observed in the K_L to pi+ pi- e+ e- decay. The K_S to pi+ pi- e+ e- decay has been observed for the first time, showing no such asymmetry.']",['2001-02-16']
291,['eng'],"['Perl, Martin Lewis', 'Kim, P C', 'Halyo, V', 'Lee, E R', 'Lee, I T', 'Loomba, D', 'Lackner, K S']","['The Search for Stable, Massive, Elementary Particles']",['Particle Physics - Experimental Results'],"['review, experimental results', 'new particle, search for', 'particle, massive', 'particle, stability', 'neutral particle', 'charged particle', 'charge, fractional', 'CHAMP', 'SIMP', 'WIMP', 'mass, lower limit', 'astrophysics, missing-mass', 'astrophysics, model', 'galaxy, production', 'cosmic radiation', 'electron positron, colliding beams', 'anti-p p, colliding beams', 'scattering, heavy ion', 'matter', 'counters and detectors, satellite', 'deep underground detector']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102033'],"['In this paper we review the experimental and observational searches for stable, massive, elementary particles other than the electron and proton. The particles may be neutral, may have unit charge or may have fractional charge. They may interact through the strong, electromagnetic, weak or gravitational forces or through some unknown force. The purpose of this review is to provide a guide for future searches - what is known, what is not known, and what appear to be the most fruitful areas for new searches. A variety of experimental and observational methods such as accelerator experiments, cosmic ray studies, searches for exotic particles in bulk matter and searches using astrophysical observations is included in this review.']",['2001-02-15']
292,['eng'],"['Aubert, Bernard', 'Boutigny, D', 'De Bonis, I', 'Gaillard, Jean-Marc', 'Jérémie, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Palano, A', 'Chen, G P', 'Chen, J C', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Dardin, S', 'Day, C', 'Dow, S F', 'Elioff, T', 'Fan, Q', 'Gaponenko, I', 'Gill, M S', 'Goozen, F R', 'Gowdy, S J', 'Gritsan, A', 'Groysman, Y', 'Jacobsen, R G', 'Jared, R C', 'Kadel, R W', 'Kadyk, J', 'Karcher, A', 'Kerth, L T', 'Kipnis, I', 'Kluth, S', 'Kolomensky, Yu G', 'Kral, J F', 'Lafever, R', 'Le Clerc, C', 'Levi, M E', 'Lewis, S A', 'Lionberger, C', 'Liu, T', 'Long, M', 'Lynch, G', 'Marino, M', 'Marks, K', 'Matuk, C A', 'Meyer, A B', 'Mokhtarani, A', 'Momayezi, M', 'Nyman, M', 'Oddone, P J', 'Ohnemus, J', 'Oshatz, D', 'Patton, S', 'Perazzo, A', 'Peters, C', 'Pope, W', 'Pripstein, M', 'Quarrie, D R', 'Rasson, J E', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Stone, R', 'Telnov, A V', 'Weber, T', 'Wenzel, W A', 'Zisman, M S', 'Bright-Thomas, P G', 'Harrison, T J', 'Hawkes, C M', 'Kirk, A', 'Knowles, D J', ""O'Neale, S W"", 'Watson, A T', 'Watson, N K', 'Deppermann, T', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Barlow, N R', 'Bhimji, W', 'Chevalier, N', 'Clark, P J', 'Cottingham, W N', 'De, N', 'Groot', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'Jolly, S', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Kolachev, G M', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Telnov, V I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M', 'McMahon, S', 'Stoker, D P', 'Ahsan, A', 'Buchanan, C', 'Chun, S', 'Branson, J G', 'MacFarlane, D B', 'Prell, S', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Burke, S', 'Campagnari, C', 'Dahmes, B', 'Hale, D', 'Hart, P A', 'Kuznetsova, N', 'Kyre, S', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Spencer, E N', 'Turri, M', 'Walkowiak, W', 'Williams, D C', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoretskii, A', 'Hanson, J E', 'Hitlin, D G', 'Metzler, S', 'Oyang, J', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S', 'Jayatilleke, S M', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Bloom, P', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Van Hoek, W C', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J', 'Sen, S', 'Smith, J G', 'Wagner, D L', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Warner, D W', 'Wilson, R J', 'Zhang, J', 'Brandt, T', 'Brose, J', 'Colberg, T', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Eckstein, P', 'Futterschneider, H', 'Krause, R', 'Maly, E', 'Müller-Pfefferkorn, R', 'Otto, S', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Fouque, G', 'Gastaldi, F', 'Matricon, P', 'Mora de Freitas, P', 'Renard, C', 'Roussot, E', ""T'Jampens, S"", 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di Lodovico, F', 'Khan, A', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Falbo, M', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E', 'Anulli, F', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Xie, Y', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Pallavicini, M', 'Passaggio, S', 'Pastore, F C', 'Patrignani, C', 'Pia, M G', 'Robutti, E', 'Santroni, A', 'Morii, M', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'McKay, R', 'Meyer, W T', 'Rosenberg, E I', 'Albert, J N', 'Beigbeder, C', 'Benkebil, M', 'Breton, D', 'Cizeron, R', 'Du, S', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Truong, K', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Brooks, A', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', ""O'Connor, T G"", 'Pedrotti, B', 'Shi, X', 'Van Bibber, K', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Yamamoto, B', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'Payne, D J', 'Sloane, R J', 'Touramanis, C', 'Aspinwall, M L', 'Bowerman, D A', 'Dauncey, P D', 'Egede, U', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R', 'Nash, J A', 'Price, D R', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Newman-Coburn, D', 'Potter, R J L', 'Shorthouse, H W', 'Strother, P', 'Vidal, P B', 'Williams, M I', 'Cowan, G', 'George, S', 'Green, M G', 'Kurup, A', 'Marker, C E', 'McGrath, P', 'McMahon, T R', 'Salvatore, F', 'Scott, I', 'Vaitsas, G', 'Brown, D', 'Davis, C L', 'Ford, K', 'Li, Y', 'Pavlovich, J', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Fullwood, J', 'Jackson, F', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Thompson, R J', 'Weatherall, J H', 'Bard, R L', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Schieck, J R', 'Blaylock, G', 'Dallapiccola, C', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R', 'Lin, C S', 'Stängle, H', 'Willocq, S', 'Wittlin, J', 'Brau, B', 'Cowan, R', 'Sciolla, G', 'Taylor, F', 'Yamamoto, R K', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Eschenberg, V', 'Kroeger, R', 'Reep, M', 'Reidy, J', 'Sanders, D A', 'Summers, D J', 'Beaulieu, M', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cavallo, N', 'Cartaro, C', 'De Nardo, G', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Paolucci, P', 'Piccolo, D', 'Sciacca, C', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Heck, J M', 'Brau, J E', 'Frey, R', 'Iwasaki, M', 'Sinev, N B', 'Strom, D', 'Colecchia, F', 'Dal, F', 'Corso', 'Galeazzi, F', 'Martino, M', 'Marzolla, M', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Rotondo, M', 'Simonetto, F', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Bailly, P', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Genat, J F', 'Hamon, O', 'Le Diberder, F', 'Lebbolo, H', 'Leruste, P', 'Lory, J', 'Martin, L', 'Roos, L', 'Stark, J', 'Versille, S', 'Zhang, B', 'Manfredi, P F', 'Ratti, L', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Bosi, F', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Martínez-Vidal, F', 'Morganti, M', 'Neri, N', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Walsh, J', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Fernholz, R', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Sands, B', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Bronzini, F', 'Buccheri, A', 'Bulfon, C', 'Cavoto, G', 'Del Re, D', 'Faccini, R', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Voena, C', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M', 'Plano, R J', 'Adye, T', 'Claxton, B', 'Franek, B', 'Galagedera, S B', 'Geddes, N I', 'Gopal, Gian P', 'Lidbury, J A', 'Xella, S M', 'Aleksan, R', 'Besson, P', 'Bourgeois, P', 'De Domenico, G', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Gosset, L', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Copty, N K', 'Purohit, M V', 'Singh, H', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Aston, D', 'Baird, K', 'Bartelt, J', 'Becla, J', 'Bell, R', 'Bloom, Elliott D', 'Boeheim, C T', 'Boyarski, A M', 'Boyce, R F', 'Bulos, F', 'Burgess, W', 'Byers, B', 'Calderini, G', 'Claus, R', 'Convery, M R', 'Coombes, R', 'Cottrell, L', 'Coupal, D P', 'Coward, D H', 'Craddock, W W', 'De Staebler, H C', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Ecklund, S', 'Fieguth, T H', 'Field, R C', 'Freytag, D R', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Haller, G', 'Hanushevsky, A', 'Harris, J', 'Hasan, A', 'Hewett, J L', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kawahara, H', 'Keller, L', 'Kelsey, M H', 'Kim, P', 'Klaisner, L A', 'Kocian, M L', 'Krebs, H J', 'Kunz, P F', 'Langenegger, U', 'Langeveld, W', 'Leith, D W G S', 'Louie, S K', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'MacDonald, J', 'Manzin, G', 'Marsiske, H', 'McCulloch, M', 'McShurley, D', 'Menke, S', 'Messner, R', 'Metcalfe, S', 'Moffeit, K C', 'Mount, R', 'Müller, D R', 'Nelson, D', 'Nordby, M', ""O'Grady, C P"", ""O'Neill, F G"", 'Oxoby, G', 'Pavel, T', 'Perl, J', 'Petrak, S', 'Putallaz, G', 'Quinn, Helen R', 'Raines, P E', 'Ratcliff, B N', 'Reif, R', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Russell, J J', 'Sapozhnikov, L', 'Saxon, O H', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Seeman, J T', 'Serbo, V V', 'Skarpass Sr, K', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Stelzer, J', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'White, J L', 'Wienands, U', 'Wisniewski, W J', 'Young, C C', 'Zioulas, G', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'De Silva, A', 'Henderson, R', 'Berridge, S', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'Kowalewski, R', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Hu, H', 'Johnson, J R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Wimmersperg-Toeller', 'Wu, S L', 'Yu, Z', 'Zobernig, H G', 'Kordich, T M B', 'Moore, T B', 'Neal, H']",['Measurement of CP-violating asymmetries in B0 decays to CP eigenstates'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'psi mesons, leptonic decay', 'psi(3685), hadronic decay', 'K0, hadronic decay', 'Kobayashi-Maskawa angle, unitarity', 'violation, CP', 'time dependence', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> psi mesons K0(S)', 'B0 --> J/psi(3100) K0(L)', 'psi mesons --> lepton+ lepton-', 'psi(3685) --> J/psi(3100) pi+ pi-', 'K0 --> 2pi', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102030'],"['We present measurements of time-dependent CP-violating asymmetries in neutral B decays to several CP eigenstates. The measurement uses a data sample of 23 million Upsilon(4S)-->B-anti-B decays collected by the BABAR detector at the PEP-II asymmetric B Factory at SLAC. In this sample, we find events where one neutral B meson is fully reconstructed in a CP eigenstate containing charmonium and the flavor of the other neutral B meson is determined from its decay products. The amplitude of the CP-violating asymmetry, which in the Standard Model is proportional to sin2beta, is derived from the decay time distributions in such events. The result is sin2beta=0.34 +/- 0.20 (stat) +/- 0.05 (syst).']",['2001-02-13']
293,['eng'],"['Achasov, M N', 'Beloborodov, K I', 'Berdyugin, A V', 'Bogdanchikov, A G', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Korol, A A', 'Koshuba, S V', 'Lysenko, A P', 'Nesterenko, I N', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V', 'Vasilev, A V']",['Direct measurement of the phi(1020) leptonic branching ratio'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), leptonic decay', 'muon, pair production', 'Phi(1020), branching ratio', 'universality, (muon electron)', 'channel cross section, energy dependence', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> muon+ muon-', '1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102029'],['The process e+e-->mu+mu- has been studied by SND detector at VEPP-2M e+e- collider in the phi(1020)-resonance energy region. The measured effective phi meson leptonic branching ratio: B(phi->l+l-)=sqrt{B(phi->e+e-)*B(phi->mu+mu-)}=(2.89+-0.10+-0.06)*1 0^{-4} agrees well with the PDG value B(phi->e+e-)=(2.91+-0.07)*10^{-4 } confirming mu-e universality. Without additional assumption of mu-e universality the branching ratio B(phi->mu+mu-)=(2.87+-0.20+-0.14)*10^{-4} was obtained.'],['2001-02-13']
294,['eng'],"['Chazal, V', 'Böhm, F', 'Cook, B', 'Henrikson, H', 'Jonkmans, G', 'Paic, A', 'Mascarenhas, N', 'Vogel, P', 'Vuilleumier, J L']",['Investigations of fast neutron production by 190 GeV/c muon interactions on graphite target'],['Particle Physics - Experimental Results'],"['muon nucleus, inclusive reaction', 'carbon', 'n, electroproduction', 'n, angular distribution', 'n, energy spectrum', 'scintillation counter, liquid', 'experimental results', 'CERN SPS', '< 1 GeV']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102028', 'http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=ext&id=ext-2001-010']","['The production of fast neutrons (1 MeV - 1 GeV) in high energy muon-nucleus interactions is poorly understood, yet it is fundamental to the understanding of the background in many underground experiments. The aim of the present experiment (CERN NA55) was to measure spallation neutrons produced by 190 GeV/c muons scattering on carbon target. We have investigated the energy spectrum and angular distribution of spallation neutrons, and we report the result of our measurement of the neutron production differential cross section.']",['2001-02-13']
295,['eng'],"['Schwienhorst, R', 'Rusack, R', 'Ciampa, D', 'Erickson, C', 'Graham, M', 'Heller, K', 'Sielaff, J', 'Trammell, J', 'Wilcox, J', 'Kodama, K', 'Ushida, N', 'Andreopoulos, C', 'Saoulidou, N', 'Tzanakos, G', 'Yager, P', 'Baller, B R', 'Boehnlein, D', 'Freeman, W', 'Lundberg, B', 'Morfin, J', 'Rameika, R', 'Yun, J C', 'Song, J S', 'Yoon, C S', 'Chung, S H', 'Berghaus, P', 'Kubantsev, M', 'Reay, N W', 'Sidwell, R', 'Stanton, N', 'Yoshida, S', 'Aoki, S', 'Hara, T', 'Rhee, J T', 'Hoshino, K', 'Jiko, H', 'Miyanishi, M', 'Komatsu, M', 'Nakamura, M', 'Nakano, T', 'Niwa, K', 'Nonaka, N', 'Okada, K', 'Sato, O', 'Akdogan, T', 'Paolone, V', 'Rosenfeld, C', 'Kulik, A', 'Kafka, T', 'Oliver, W', 'Patzak, T', 'Schneps, J']",['A New Upper Limit for the Tau-Neutrino Magnetic Moment'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'tungsten', 'beam dump', 'neutrino, secondary beam', 'neutrino/tau, magnetic moment', 'upper limit', 'neutrino electron, elastic scattering', 'differential cross section, energy dependence', 'nuclear emulsion, sandwich', 'iron', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102026'],"['Using a prompt neutrino beam in which a nu_tau component was identified for the first time, the nu_tau magnetic moment was measured based on a search for an anomalous increase in the number of neutrino-electron interactions. One such event was observed when 2.3 were expected from background processes giving an upper 90% confidence limit of 3.9x10^-7 Bohr magnetons.']",['2001-02-13']
296,['eng'],"['Acciarri, M', 'Achard, P', 'Adriani, O', 'Aguilar-Benítez de Lugo, M', 'Alcaraz, J', 'Alemanni, G', 'Allaby, James V', 'Aloisio, A', 'Alviggi, M G', 'Ambrosi, G', 'Anderhub, H', 'Andreev, V P', 'Angelescu, T', 'Anselmo, F', 'Arefev, A', 'Azemoon, T', 'Aziz, T', 'Bagnaia, P', 'Bajo, A', 'Baksay, L', 'Balandras, A', 'Baldew, S V', 'Todorova-Nová, S', 'Banerjee, Sw', 'Barczyk, A', 'Barillère, R', 'Bartalini, P', 'Basile, M', 'Batalova, N', 'Battiston, R', 'Bay, A', 'Becattini, F', 'Becker, U', 'Behner, F', 'Bellucci, L', 'Berbeco, R', 'Berdugo, J', 'Berges, P', 'Bertucci, B', 'Betev, B L', 'Bhattacharya, S', 'Biasini, M', 'Biland, A', 'Blaising, J J', 'Blyth, S C', 'Bobbink, Gerjan J', 'Böhm, A', 'Boldizsar, L', 'Borgia, B', 'Bourilkov, D', 'Bourquin, Maurice', 'Braccini, S', 'Branson, J G', 'Brochu, F', 'Buffini, A', 'Buijs, A', 'Burger, J D', 'Burger, W J', 'Cai, X D', 'Capell, M', 'Cara Romeo, G', 'Carlino, G', 'Cartacci, A M', 'Casaus, J', 'Castellini, G', 'Cavallari, F', 'Cavallo, N', 'Cecchi, C', 'Cerrada, M', 'Cesaroni, F', 'Chamizo-Llatas, M', 'Chang, Y H', 'Chaturvedi, U K', 'Chemarin, M', 'Chen, A', 'Chen, G', 'Chen, G M', 'Chen, H F', 'Chen, H S', 'Chiefari, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Civinini, C', 'Clare, I', 'Clare, R', 'Coignet, G', 'Colino, N', 'Costantini, S', 'Cotorobai, F', 'de la Cruz, B', 'Csilling, Akos', 'Cucciarelli, S', 'Dai, T S', 'van Dalen, J A', ""D'Alessandro, R"", 'De Asmundis, R', 'Déglon, P L', 'Degré, A', 'Deiters, K', 'Della Volpe, D', 'Delmeire, E', 'Denes, P', 'De Notaristefani, F', 'De Salvo, A', 'Diemoz, Marcella.', 'Dierckxsens, M', 'Van Dierendonck, D N', 'Dionisi, C', 'Dittmar, Michael', 'Dominguez, A', 'Doria, A', 'Dova, M T', 'Duchesneau, D', 'Dufournaud, D', 'Duinker, P', 'El-Mamouni, H', 'Engler, A', 'Eppling, F J', 'Erné, Frits C', 'Ewers, A', 'Extermann, Pierre', 'Fabre, M', 'Falagán, M A', 'Falciano, S', 'Favara, A', 'Fay, J', 'Fedin, O', 'Felcini, Marta', 'Ferguson, T', 'Fesefeldt, H S', 'Fiandrini, E', 'Field, J H', 'Filthaut, F', 'Fisher, P H', 'Fisk, I', 'Forconi, G', 'Freudenreich, Klaus', 'Furetta, C', 'Galaktionov, Yu', 'Ganguli, S N', 'García-Abia, P', 'Gataullin, M', 'Gau, S S', 'Gentile, S', 'Gheordanescu, N', 'Giagu, S', 'Gong, Z F', 'Grenier, G', 'Grimm, O', 'Grünewald, M W', 'Guida, M', 'van Gulik, R', 'Gupta, V K', 'Gurtu, A', 'Gutay, L J', 'Haas, D', 'Hasan, A', 'Hatzifotiadou, D', 'Hebbeker, T', 'Hervé, Alain', 'Hidas, P', 'Hirschfelder, J', 'Hofer, H', 'Holzner, G', 'Hoorani, H', 'Hou, S R', 'Hu, Y', 'Iashvili, I', 'Jin, B N', 'Jones, L W', 'de Jong, P', 'Josa-Mutuberria, I', 'Khan, R A', 'Käfer, D', 'Kaur, M', 'Kienzle-Focacci, M N', 'Kim, D', 'Kim, J K', 'Kirkby, Jasper', 'Kiss, D', 'Kittel, E Wolfram', 'Klimentov, A', 'König, A C', 'Kopal, M', 'Kopp, A', 'Koutsenko, V F', 'Kräber, M H', 'Krämer, R W', 'Krenz, W', 'Krüger, A', 'Kunin, A', 'Ladrón de Guevara, P', 'Laktineh, I', 'Landi, G', 'Lebeau, M', 'Lebedev, A', 'Lebrun, Philippe.', 'Lecomte, P', 'Lecoq, P', 'Le Coultre, P', 'Lee, H J', 'Le Goff, J M', 'Leiste, R', 'Levchenko, P M', 'Li Chuan', 'Likhoded, S A', 'Lin, C H', 'Lin, W T', 'Linde, F L', 'Lista, L', 'Liu, Z A', 'Lohmann, W', 'Longo, E', 'Lü, Y S', 'Lübelsmeyer, K', 'Luci, C', 'Luckey, D', 'Lugnier, L', 'Luminari, L', 'Lustermann, W', 'Ma, W G', 'Maity, M', 'Malgeri, L', 'Malinin, A', 'Maña, C', 'Mangeol, D J', 'Mans, J', 'Marian, G', 'Martin, J P', 'Marzano, F', 'Mazumdar, K', 'McNeil, R R', 'Mele, S', 'Merola, L', 'Meschini, M', 'Metzger, W J', 'Von der Mey, M', 'Mihul, A', 'Milcent, H', 'Mirabelli, G', 'Mnich, J', 'Mohanty, G B', 'Moulik, T', 'Muanza, G S', 'Muijs, A J M', 'Musicar, B', 'Musy, M', 'Napolitano, M', 'Nessi-Tedaldi, F', 'Newman, H', 'Niessen, T', 'Nisati, A', 'Nowak, H', 'Ofierzynski, R A', 'Organtini, G', 'Oulianov, A', 'Palomares, C', 'Pandoulas, D', 'Paoletti, S', 'Paolucci, P', 'Paramatti, R', 'Park, H K', 'Park, I H', 'Passaleva, G', 'Patricelli, S', 'Paul, T', 'Pauluzzi, M', 'Paus, C', 'Pauss, Felicitas', 'Pedace, M', 'Pensotti, S', 'Perret-Gallix, D', 'Petersen, B', 'Piccolo, D', 'Pierella, F', 'Pieri, M', 'Piroué, P A', 'Pistolesi, E', 'Plyaskin, V', 'Pohl, M', 'Pozhidaev, V', 'Postema, H', 'Pothier, J', 'Prokofiev, D O', 'Prokofev, D', 'Quartieri, J', 'Rahal-Callot, G', 'Rahaman, M A', 'Raics, P', 'Raja, N', 'Ramelli, R', 'Rancoita, P G', 'Ranieri, R', 'Raspereza, A V', 'Raven, G', 'Razis, P A', 'Ren, D', 'Rescigno, M', 'Reucroft, S', 'Riemann, S', 'Riles, K', 'Rodin, J', 'Roe, B P', 'Romero, L', 'Rosca, A', 'Rosier-Lees, S', 'Roth, S', 'Rosenbleck, C', 'Roux, B', 'Rubio, Juan Antonio', 'Ruggiero, G', 'Rykaczewski, H', 'Saremi, S', 'Sarkar, S', 'Salicio, J', 'Sánchez, E', 'Sanders, M P', 'Schäfer, C', 'Shchegelskii, V', 'Schmidt-Kärst, S', 'Schmitz, D', 'Schopper, Herwig Franz', 'Schotanus, D J', 'Schwering, G', 'Sciacca, C', 'Seganti, A', 'Servoli, L', 'Shevchenko, S', 'Shivarov, N', 'Shoutko, V', 'Shumilov, E', 'Shvorob, A V', 'Siedenburg, T', 'Son, D', 'Smith, B', 'Spillantini, P', 'Steuer, M', 'Stickland, D P', 'Stone, A', 'Stoyanov, B', 'Strässner, A', 'Sudhakar, K', 'Sultanov, G G', 'Sun, L Z', 'Sushkov, S V', 'Suter, H', 'Swain, J D', 'Szillasi, Z', 'Sztaricskai, T', 'Tang, X W', 'Tauscher, Ludwig', 'Taylor, L', 'Tellili, B', 'Teyssier, D', 'Timmermans, C', 'Ting, S C C', 'Ting, S M', 'Tonwar, S C', 'Tóth, J', 'Tully, C', 'Tung, K L', 'Uchida, Y', 'Ulbricht, J', 'Valente, E', 'Vesztergombi, György', 'Vetlitskii, I', 'Vicinanza, D', 'Viertel, Gert M', 'Villa, S', 'Vivargent, M', 'Vlachos, S', 'Vodopyanov, I', 'Vogel, H', 'Vogt, H', 'Vorobev, I', 'Vorobyov, A A', 'Vorvolakos, A', 'Wadhwa, M', 'Wallraff, W', 'Wang, M', 'Wang, X L', 'Wang, Z M', 'Weber, A', 'Weber, M', 'Wienemann, P', 'Wilkens, H', 'Wu, S X', 'Wynhoff, S', 'Xia, L', 'Xu, Z Z', 'Yamamoto, J', 'Yang, B Z', 'Yang, C G', 'Yang, H J', 'Yang, M', 'Ye, J B', 'Yeh, S C', 'Zalite, A', 'Zalite, Yu', 'Zhang, Z P', 'Zhu, G Y', 'Zhu, R Y', 'Zichichi, Antonino', 'Zilizi, G', 'Zimmermann, B', 'Zöller, M']",['Total Cross Section in $\\gamma\\gamma$ Collisions at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'hadron, multiple production', 'cross section, energy dependence', 'parametrization', 'Regge poles', 'model, pomeron', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> (n)hadron positron electron', '183-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102025'],['The reaction e+e- -> e+e- gamma* gamma* -> e+e- hadrons for quasi-real photons is studied using data from root(s) = 183 GeV up to 202 GeV. Results on the total cross sections sigma(e+e- -> e+e- hadrons) and sigma(+e- gamma* gamma* -> e+e- hadrons) are given for the two-photon centre-of-mass energies 5 GeV < Wgammagamma < 185 GeV. The total cross section of two real photons is described by a Regge parametrisation. We observe a steeper rise with the two-photon centre-of-mass energy as compared to the hadron-hadron and the photon-proton cross sections. The data are also compared to the expectations of different theoretical models.'],['2001-02-13']
297,['eng'],"['Acciarri, M', 'Achard, P', 'Adriani, O', 'Aguilar-Benítez de Lugo, M', 'Alcaraz, J', 'Alemanni, G', 'Allaby, James V', 'Aloisio, A', 'Alviggi, M G', 'Ambrosi, G', 'Anderhub, H', 'Andreev, V P', 'Angelescu, T', 'Anselmo, F', 'Arefev, A', 'Azemoon, T', 'Aziz, T', 'Bagnaia, P', 'Bajo, A', 'Baksay, L', 'Balandras, A', 'Baldew, S V', 'Todorova-Nová, S', 'Banerjee, Sw', 'Barczyk, A', 'Barillère, R', 'Bartalini, P', 'Basile, M', 'Batalova, N', 'Battiston, R', 'Bay, A', 'Becattini, F', 'Becker, U', 'Behner, F', 'Bellucci, L', 'Berbeco, R', 'Berdugo, J', 'Berges, P', 'Bertucci, B', 'Betev, B L', 'Bhattacharya, S', 'Biasini, M', 'Biland, A', 'Blaising, J J', 'Blyth, S C', 'Bobbink, Gerjan J', 'Böhm, A', 'Boldizsar, L', 'Borgia, B', 'Bourilkov, D', 'Bourquin, Maurice', 'Braccini, S', 'Branson, J G', 'Brochu, F', 'Buffini, A', 'Buijs, A', 'Burger, J D', 'Burger, W J', 'Cai, X D', 'Capell, M', 'Cara Romeo, G', 'Carlino, G', 'Cartacci, A M', 'Casaus, J', 'Castellini, G', 'Cavallari, F', 'Cavallo, N', 'Cecchi, C', 'Cerrada, M', 'Cesaroni, F', 'Chamizo-Llatas, M', 'Chang, Y H', 'Chaturvedi, U K', 'Chemarin, M', 'Chen, A', 'Chen, G', 'Chen, G M', 'Chen, H F', 'Chen, H S', 'Chiefari, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Civinini, C', 'Clare, I', 'Clare, R', 'Coignet, G', 'Colijn, A P', 'Colino, N', 'Costantini, S', 'Cotorobai, F', 'de la Cruz, B', 'Csilling, Akos', 'Cucciarelli, S', 'Dai, T S', 'van Dalen, J A', ""D'Alessandro, R"", 'De Asmundis, R', 'Déglon, P L', 'Degré, A', 'Deiters, K', 'Della Volpe, D', 'Delmeire, E', 'Denes, P', 'De Notaristefani, F', 'De Salvo, A', 'Diemoz, Marcella.', 'Dierckxsens, M', 'Van Dierendonck, D N', 'Dionisi, C', 'Dittmar, Michael', 'Dominguez, A', 'Doria, A', 'Dova, M T', 'Duchesneau, D', 'Dufournaud, D', 'Duinker, P', 'El-Mamouni, H', 'Engler, A', 'Eppling, F J', 'Erné, Frits C', 'Ewers, A', 'Extermann, Pierre', 'Fabre, M', 'Falagán, M A', 'Falciano, S', 'Favara, A', 'Fay, J', 'Fedin, O', 'Felcini, Marta', 'Ferguson, T', 'Fesefeldt, H S', 'Fiandrini, E', 'Field, J H', 'Filthaut, F', 'Fisher, P H', 'Fisk, I', 'Forconi, G', 'Freudenreich, Klaus', 'Furetta, C', 'Galaktionov, Yu', 'Ganguli, S N', 'García-Abia, P', 'Gataullin, M', 'Gau, S S', 'Gentile, S', 'Gheordanescu, N', 'Giagu, S', 'Gong, Z F', 'Grenier, G', 'Grimm, O', 'Grünewald, M W', 'Guida, M', 'van Gulik, R', 'Gupta, V K', 'Gurtu, A', 'Gutay, L J', 'Haas, D', 'Hasan, A', 'Hatzifotiadou, D', 'Hebbeker, T', 'Hervé, Alain', 'Hidas, P', 'Hirschfelder, J', 'Hofer, H', 'Holzner, G', 'Hoorani, H', 'Hou, S R', 'Hu, Y', 'Iashvili, I', 'Jin, B N', 'Jones, L W', 'de Jong, P', 'Josa-Mutuberria, I', 'Khan, R A', 'Käfer, D', 'Kaur, M', 'Kienzle-Focacci, M N', 'Kim, D', 'Kim, J K', 'Kirkby, Jasper', 'Kiss, D', 'Kittel, E Wolfram', 'Klimentov, A', 'König, A C', 'Kopal, M', 'Kopp, A', 'Koutsenko, V F', 'Kräber, M H', 'Krämer, R W', 'Krenz, W', 'Krüger, A', 'Kunin, A', 'Lacentre, P E', 'Ladrón de Guevara, P', 'Laktineh, I', 'Landi, G', 'Lebeau, M', 'Lebedev, A', 'Lebrun, Philippe.', 'Lecomte, P', 'Lecoq, P', 'Le Coultre, P', 'Lee, H J', 'Le Goff, J M', 'Leiste, R', 'Levchenko, P M', 'Li Chuan', 'Likhoded, S A', 'Lin, C H', 'Lin, W T', 'Linde, F L', 'Lista, L', 'Liu, Z A', 'Lohmann, W', 'Longo, E', 'Lü, Y S', 'Lübelsmeyer, K', 'Luci, C', 'Luckey, D', 'Lugnier, L', 'Luminari, L', 'Lustermann, W', 'Ma, W G', 'Maity, M', 'Malgeri, L', 'Malinin, A', 'Maña, C', 'Mangeol, D J', 'Mans, J', 'Marian, G', 'Martin, J P', 'Marzano, F', 'Mazumdar, K', 'McNeil, R R', 'Mele, S', 'Merola, L', 'Meschini, M', 'Metzger, W J', 'Von der Mey, M', 'Mihul, A', 'Milcent, H', 'Mirabelli, G', 'Mnich, J', 'Mohanty, G B', 'Moore, R', 'Moulik, T', 'Muanza, G S', 'Muijs, A J M', 'Musicar, B', 'Musy, M', 'Napolitano, M', 'Nessi-Tedaldi, F', 'Newman, H', 'Niessen, T', 'Nisati, A', 'Nowak, H', 'Ofierzynski, R A', 'Organtini, G', 'Oulianov, A', 'Palomares, C', 'Pandoulas, D', 'Paoletti, S', 'Paolucci, P', 'Paramatti, R', 'Park, H K', 'Park, I H', 'Passaleva, G', 'Patricelli, S', 'Paul, T', 'Pauluzzi, M', 'Paus, C', 'Pauss, Felicitas', 'Pedace, M', 'Pensotti, S', 'Perret-Gallix, D', 'Petersen, B', 'Piccolo, D', 'Pierella, F', 'Pieri, M', 'Piroué, P A', 'Pistolesi, E', 'Plyaskin, V', 'Pohl, M', 'Pozhidaev, V', 'Postema, H', 'Pothier, J', 'Prokofiev, D O', 'Prokofev, D', 'Quartieri, J', 'Rahal-Callot, G', 'Rahaman, M A', 'Raics, P', 'Raja, N', 'Ramelli, R', 'Rancoita, P G', 'Ranieri, R', 'Raspereza, A V', 'Raven, G', 'Razis, P A', 'Ren, D', 'Rescigno, M', 'Reucroft, S', 'Riemann, S', 'Riles, K', 'Rodin, J', 'Roe, B P', 'Romero, L', 'Rosca, A', 'Rosier-Lees, S', 'Roth, S', 'Rosenbleck, C', 'Roux, B', 'Rubio, Juan Antonio', 'Ruggiero, G', 'Rykaczewski, H', 'Saremi, S', 'Sarkar, S', 'Salicio, J', 'Sánchez, E', 'Sanders, M P', 'Schäfer, C', 'Shchegelskii, V', 'Schmidt-Kärst, S', 'Schmitz, D', 'Schopper, Herwig Franz', 'Schotanus, D J', 'Schwering, G', 'Sciacca, C', 'Seganti, A', 'Servoli, L', 'Shevchenko, S', 'Shivarov, N', 'Shoutko, V', 'Shumilov, E', 'Shvorob, A V', 'Siedenburg, T', 'Son, D', 'Smith, B', 'Spillantini, P', 'Steuer, M', 'Stickland, D P', 'Stone, A', 'Stoyanov, B', 'Strässner, A', 'Sudhakar, K', 'Sultanov, G G', 'Sun, L Z', 'Sushkov, S V', 'Suter, H', 'Swain, J D', 'Szillasi, Z', 'Sztaricskai, T', 'Tang, X W', 'Tauscher, Ludwig', 'Taylor, L', 'Tellili, B', 'Teyssier, D', 'Timmermans, C', 'Ting, S C C', 'Ting, S M', 'Tonwar, S C', 'Tóth, J', 'Tully, C', 'Tung, K L', 'Uchida, Y', 'Ulbricht, J', 'Valente, E', 'Vesztergombi, György', 'Vetlitskii, I', 'Vicinanza, D', 'Viertel, Gert M', 'Villa, S', 'Vivargent, M', 'Vlachos, S', 'Vodopyanov, I', 'Vogel, H', 'Vogt, H', 'Vorobev, I', 'Vorobyov, A A', 'Vorvolakos, A', 'Wadhwa, M', 'Wallraff, W', 'Wang, M', 'Wang, X L', 'Wang, Z M', 'Weber, A', 'Weber, M', 'Wienemann, P', 'Wilkens, H', 'Wu, S X', 'Wynhoff, S', 'Xia, L', 'Xu, Z Z', 'Yamamoto, J', 'Yang, B Z', 'Yang, C G', 'Yang, H J', 'Yang, M', 'Ye, J B', 'Yeh, S C', 'Zalite, A', 'Zalite, Yu', 'Zhang, Z P', 'Zhu, G Y', 'Zhu, R Y', 'Zichichi, Antonino', 'Ziegler, F', 'Zilizi, G', 'Zimmermann, B', 'Zöller, M']",['Measurement of the Tau Branching Fractions into Leptons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, pair production', 'tau, leptonic decay', 'tau, branching ratio', 'muon, coupling constant', 'electron, coupling constant', 'charged current', 'coupling constant, ratio', 'strong interaction, coupling constant', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'tau --> electron neutrino/tau antineutrino/e', 'tau --> muon neutrino/tau antineutrino/mu', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102023'],"['Using data collected with the L3 detector near the Z resonance, corresponding to an integrated luminosity of 150pb-1, the branching fractions of the tau lepton into electron and muon are measured to be B(tau->e nu nu) = (17.806 +- 0.104 (stat.) +- 0.076 (syst.)) %, B(tau->mu nu nu) = (17.342 +- 0.110 (stat.) +- 0.067 (syst.)) %. From these results the ratio of the charged current coupling constants of the muon and the electron is determined to be g_mu/g_e = 1.0007 +- 0.0051. Assuming electron-muon universality, the Fermi constant is measured in tau lepton decays as G_F = (1.1616 +- 0.0058) 10^{-5} GeV^{-2}. Furthermore, the coupling constant of the strong interaction at the tau mass scale is obtained as alpha_s(m_tau^2) = 0.322 +- 0.009 (exp.) +- 0.015 (theory).']",['2001-02-13']
298,['eng'],"['Abe, T']",['A study of topological vertexing for heavy quark tagging'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/24', 'electron positron, linear collider', 'linear collider, proposed', 'counters and detectors, vertex', 'resolution, impact parameter', 'spatial resolution, vertex', 'jet', 'particle identification, flavor', 'efficiency', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102022'],['We compare heavy quark tagging and anti-tagging efficiencies for vertex detectors with different inner raddi using the topological vertex technique developed at the SLC/SLD experiment. Charm tagging benefits by going to very small inner radii.'],['2001-02-12']
299,['eng'],"['Turnau, J']",['Photon Structure'],['Particle Physics - Experimental Results'],"['talk, Tver 2000/09/14', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'electron positron, colliding beams', 'exchange, two-photon', 'photon, structure function', 'photon, off-shell', 'quark, momentum spectrum', 'gluon, momentum spectrum', 'x-dependence', 'momentum transfer, dependence', 'jet, pair production', 'differential cross section', 'quantum chromodynamics', 'perturbation theory, higher-order', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102019'],"['Measurements of di-jet production at HERA provide an important test of NLO QCD calculations. It is also a source of information about partonic content of the photon, complementary to the measurements in e+e- experiments. In this article we review the status of the photon structutre studies with particular emphasis on HERA measurements.']",['2001-02-12']
300,['eng'],"['Abashian, A']",['Measurement of the CP Violation Parameter sin(2phi_1) in B^0_d Meson Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'quarkonium, charm', 'quarkonium, decay modes', 'K0, hadronic decay', 'pi0', 'particle identification, flavor', 'violation, CP', 'asymmetry, time dependence', 'Kobayashi-Maskawa angle, unitarity', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B0 --> psi mesons K0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102018'],"['We present a measurement of the Standard Model CP violation parameter sin(2phi_1) based on a 10.5 fb^{-1} data sample collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric e+e- collider. One neutral B meson is reconstructed in the J/psi K_S, psi(2S) K_S, chi_{c1} K_S, eta_c K_S, J/psi K_L or J/psi pi^0 CP-eigenstate decay channel and the flavor of the accompanying B meson is identified from its charged particle decay products. From the asymmetry in the distribution of the time interval between the two B-meson decay points, we determine sin(2phi_1) = 0.58 +0.32-0.34 (stat) +0.09-0.10 (syst).']",['2001-02-12']
301,['eng'],"['Brown, H N', 'Bunce, G M', 'Carey, R M', 'Cushman, P B', 'Danby, G T', 'Debevec, P T', 'Deile, M', 'Deng, H', 'Deninger, W J', 'Dhawan, S K', 'Druzhinin, V P', 'Duong, L', 'Efstathiadis, E F', 'Farley, Francis J M', 'Fedotovich, G V', 'Giron, S', 'Gray, F', 'Grigoriev, D', 'Grosse-Perdekamp, M', 'Grossmann, A', 'Hare, M F', 'Hertzog, D W', 'Hughes, V W', 'Iwasaki, M', 'Jungmann, K', 'Kawall, D', 'Kawamura, M', 'Khazin, B I', 'Kindem, J', 'Krienen, F', 'Kronkvist, I J', 'Larsen, R', 'Lee, Y Y', 'Logashenko, I B', 'McNabb, R', 'Meng, W', 'Mi, J', 'Miller, J P', 'Morse, W M', 'Nikas, D', 'Onderwater, C J G', 'Orlov, Y', 'Ozben, C S', 'Paley, J M', 'Polly, C', 'Pretz, J', 'Prigl, R', 'zu Putlitz, G', 'Redin, S I', 'Rind, O', 'Roberts, B L', 'Ryskulov, N', 'Sedykh, S N', 'Semertzidis, Y K', 'Shatunov, Yu M', 'Sichtermann, E P', 'Solodov, E P', 'Sossong, M', 'Steinmetz, A', 'Sulak, Lawrence R', 'Timmermans, C', 'Trofimov, A V', 'Urner, D', 'Von Walter, P', 'Warburton, D', 'Winn, D', 'Yamamoto, A', 'Zimmerman, D']",['Precise Measurement of the Positive Muon Anomalous Magnetic Moment'],['Particle Physics - Experimental Results'],"['muon+, magnetic moment', 'muon+, polarized beam', 'muon+, storage ring', 'magnetic field', 'muon+, leptonic decay', 'positron, particle identification', 'experimental results', 'Brookhaven PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102017'],"['A precise measurement of the anomalous g value, a_mu=(g-2)/2, for the positive muon has been made at the Brookhaven Alternating Gradient Synchrotron. The result a_mu^+=11 659 202(14)(6) X 10^{-10} (1.3 ppm) is in good agreement with previous measurements and has an error one third that of the combined previous data. The current theoretical value from the standard model is a_mu(SM)=11 659 159.6(6.7) X 10^{-10} (0.57 ppm) and a_mu(exp)-a_mu(SM)=43(16) X 10^{-10} in which a_mu(exp) is the world average experimental value. This difference may be due to physics beyond the standard model.']",['2001-02-09']
302,['eng'],"['Tajima, H']",['Measurements of Heavy Meson Lifetimes with Belle'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, lifetime', 'beautiful meson, lifetime', 'D0', 'D+', 'D/s+', 'anti-B0, semileptonic decay', 'B-, hadronic decay', 'lifetime, ratio', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'anti-B --> D*(2010) lepton antineutrino', 'D*(2010) --> D0 pi', 'B- --> J/psi(3100) K-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102016'],['Charmed and beauty meson lifetimes have been measured using data collected with the Belle detector at KEKB.'],['2001-02-09']
303,['eng'],"['Iwasaki, M', 'Abe, T']",['LCD ROOT Simulation and Analysis Tools'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/24', 'programming, Monte Carlo', 'electron positron, colliding beam detector', 'semiconductor detector, vertex', 'semiconductor detector, microstrip', 'drift chamber, time projection', 'calorimeter, energy resolution', 'momentum resolution', 'resolution, impact parameter', 'electron positron, linear collider', 'linear collider, proposed', 'track data analysis']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102015'],"['The North American Linear Collider Detector group has developed a simulation program package based on the ROOT system. The package consists of Fast simulation, the reconstruction of the Full simulated data, and physics analysis utilities.']",['2001-02-08']
304,['eng'],"['Iwasaki, M']",['Study of Top-quark Production and Decay Vertices with LCD Fast Simulation'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/24', 'electron positron, annihilation', 'quark, truth', 'quark, pair production', 'final state, (4jet lepton)', 'final state, (6jet)', 'coupling, (2truth Z0)', 'coupling, (2truth photon)', 'particle identification, flavor', 'numerical calculations, Monte Carlo', '500 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102014'],"['We report a study of top-quark reconstruction in $e^+e^- \\rightarrow t\\bar{t}$ events at a 500 GeV linear collider using the LCD Fast simulator. The initial study of top-quark anomalous couplings is also reported. The final states of 4 jets and lepton as well as 6 jets are used. Using the 4 jets and lepton final state, we estimate the preliminary sensitivities for form factors at the $\\gamma/Z^0 t\\bar{t}$ vertex. In the 6 jets reconstruction, we show abilities of the top-quark charge identification and the $c$-quark tagging in W decays.']",['2001-02-08']
305,['eng'],"['Ganis, G']",['Dark Matter and SUSY'],['Particle Physics - Experimental Results'],"['talk, Vulcano 2000/05/22', 'electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'supersymmetry', 'astrophysics, missing-mass', 'sparticle, pair production', 'neutralino, mass', 'lower limit', 'Higgs particle, search for', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102013'],"['The negative outcome of searches for supersymmetry performed at LEP have been used to derive indirect constraints on the parameters of the most plausible supersymmetric candidates for cold dark matter, in particular for the lightest neutralino. We review the basic ideas leading to the present lower limit on the lightest neutralino mass of about 37 GeV, with emphasis on the underlying assumptions.']",['2001-02-08']
306,['eng'],"['Wozniak, K', 'Back, B B', 'Baker, M D', 'Barton, D S', 'Basilev, S', 'Baum, R', 'Betts, R R', 'Bialas, A', 'Bindel, R', 'Bogucki, W', 'Budzanowski, A', 'Busza, W', 'Carroll, A', 'Ceglia, M', 'Chang, Y H', 'Chen, A E', 'Coghen, T', 'Conner, C', 'Czyz, W', 'Dabrowski, B', 'Decowski, M P', 'Despet, M', 'Fita, P', 'Fitch, J', 'Friedl, M', 'Galuszka, K', 'Ganz, R E', 'García-Solis, E', 'George, N', 'Godlewski, J', 'Gomes, C', 'Griesmayer, E', 'Gulbrandsen, K H', 'Gushue, S', 'Halik, J', 'Halliwell, C', 'Haridas, P', 'Hayes, A', 'Heintzelman, G A', 'Henderson, C', 'Hollis, R', 'Holynski, R', 'Holzman, B', 'Johnson, E', 'Kane, J', 'Katzy, J M', 'Kita, W', 'Kotula, J', 'Kraner, H W', 'Kucewicz, W', 'Kulinich, P A', 'Law, C', 'Lemler, M A', 'Ligocki, T J', 'Lin, W T', 'Manly, S L', 'McLeod, D', 'Michalowski, J', 'Mignerey, A C', 'Mülmenstädt, J', 'Neal, M', 'Nouicer, R', 'Olszewski, A', 'Pak, R', 'Park, I C', 'Patel, M', 'Pernegger, H', 'Plesko, M', 'Reed, C', 'Remsberg, L P', 'Reuter, M', 'Roland, C', 'Roland, G', 'Ross, D', 'Rosenberg, L J', 'Ryan, J', 'Sanzgiri, A', 'Sarin, P', 'Sawicki, P', 'Scaduto, J', 'Shea, J', 'Sinacore, J', 'Skulski, W', 'Steadman, S G', 'Stephans, G S F', 'Steinberg, P', 'Straczek, A', 'Stodulski, M', 'Strek, M', 'Stopa, Z', 'Sukhanov, A', 'Surowiecka, K', 'Tang, J L', 'Teng, R', 'Trzupek, A', 'Vale, C J', 'van Nieuwenhuizen, G J', 'Verdier, R', 'Wadsworth, B', 'Wolfs, F L H', 'Wosiek, B', 'Wozniak, K', 'Wuosmaa, A H', 'Wyslouch, B', 'Zalewski, Kasper']",['Results from the PHOBOS Experiment on Au+Au Collisions at RHIC'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'scattering, heavy ion', 'gold', 'multiple production', 'central region', 'charged particle, multiplicity', 'rapidity, density', 'magnetic detector, PHOBOS', 'experimental results', 'Brookhaven RHIC Coll', '56, 130 GeV-cms/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102012'],"['PHOBOS is one of four experiments studying the Au-Au interactions at RHIC. The data collected during the first few weeks after the RHIC start-up, using the initial configuration of the PHOBOS detector, were sufficient to obtain the first physics results for the most central collisions of Au nuclei at the center of mass energy of 56 and 130 AGeV. The pseudorapidity density of charged particles near midrapidity is shown and compared with data at lower energies and from $pp$ and $p\\bar{p}$ collisions. The progress of the analysis of the data is also presented.PHOBOS is one of four experiments studying the Au-Au interactions at RHIC. The data collected during the first few weeks after the RHIC start-up, using the initial configuration of the PHOBOS detector, were sufficient to obtain the first physics results for the most central collisions of Au nuclei at the center of mass energy of 56 and 130 AGeV. The pseudorapidity density of charged particles near midrapidity is shown and compared with data at lower energies and from $pp$ and $p\\bar{p}$ collisions. The progress of the analysis of the data is also presented.']",['2001-02-08']
307,['eng'],"['Faus-Golfe, A', 'Haguenauer, M', 'Velasco, J']",['Precise measurement of the total cross section and the Coulomb scattering at the LHC'],['Particle Physics - Experimental Results'],"['talk, Vienna 2000/06/26', 'p p, colliding beams', 'total cross section, measurement', 'scattering, Coulomb', 'elastic scattering, small-angle', 'beam optics, beta function', 'counters and detectors, acceptance', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102011'],"['A precise measurement of the total cross section and the coulomb scattering at the LHC requires the observation of elastically scatteredparticles at extremely small angles (14 microrad, -t < 0.01 GeV**2 for the first case; 3 microrad, -t<0.0006 GeV**2 for the second one). In this paper a very high-beta insertion optics is presented. A feasibility study, including the acceptance of the detectors, for an experiment to be installed in IR1 or IR5, is also presented.']",['2001-02-08']
308,['eng'],"['Lafferty, G D']","['Universality in hadron production in electron-positron, lepton-hadron and hadron-hadron reactions']",['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, annihilation', 'Z0, hadroproduction', 'Z0, hadronic decay', 'lepton hadron, interaction', 'hadron hadron, interaction', 'hadron, multiple production', 'universality, validity test', 'dependence, flavor', 'quantum chromodynamics, perturbation theory', 'duality, quark hadron', 'kinematics, Breit frame', 'model, thermodynamical', 'string model', 'model, cluster', 'interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102009'],"['According to the concept of universality in hadron production, the basic mechanisms of hadron formation are the same in all high-energy e+e-, lh and hh reactions, with differences in the composition of final-state particle types being due only to differences in initial parton flavours and configurations. This concept is discussed in the light of recent data and phenomenology.']",['2001-02-07']
309,['eng'],"['Pitts, K T']",['Electroweak and B Physics Results from the Fermilab Tevatron Collider'],['Particle Physics - Experimental Results'],"['review, Stanford 2000/08/14', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'channel cross section, ratio', 'W, mass', 'Kobayashi-Maskawa angle', 'B0 anti-B0, interference', 'B0, hadronic decay', 'particle identification, flavor', 'violation, CP', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102010'],"['This writeup is an introduction to some of the experimental issues involved in performing electroweak and B physics measurements at the Fermilab Tevatron. In the electroweak sector, we discuss W and Z boson cross section measurements as well as the measurement of the mass of the W boson. For B physics, we discuss measurements of B^0/\\bar{B^0} mixing and CP violation. This paper is geared towards nonexperts who are interested in understanding some of the issues and motivations for these measurements and how the measurements are carried out.']",['2001-02-08']
310,['eng'],"['Schultz-Coulon, H C']",['Jet Physics at HERA'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron p, colliding beams', 'electron p, inclusive reaction', 'jet, electroproduction', 'jet, photoproduction', 'cross section, transverse energy', 'quantum chromodynamics, perturbation theory', 'validity test', 'strong interaction, coupling constant', 'showers, parton', 'final state, (2jet)', 'p, structure function', 'photon, structure function', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102008'],"['Jet production in electron-proton collisions at HERA provides a unique testing ground for Quantum Chromodynamics (QCD). Apart from the determination of the strong coupling constant $\\alpha_s$, ep jet data may especially be used to gain insight into the dynamics of the exchanged parton cascade, whose structure is probed by the high-$E_T$ dijet system; thus information on the parton content of the proton and (quasi-)-real and virtual photons is obtained. This report touches some of these aspects revealed in recent jet data from the HERA experiments which are testing perturbative QCD at the limits of applicability.']",['2001-02-06']
311,['eng'],"['Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'Jain, V', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Schwarthoff, H', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H']",['First Measurement of $\\Gamma(D^{*+})$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D*(2010), radiative decay', 'D*(2010), width', 'coupling constant, strong interaction', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102007'],['We have made the first measurement of the D*+ width using 9/fb of e+e- data collected near the Upsilon(4S) resonance by the CLEO II.V detector. Our method uses advanced tracking techniques and a reconstruction method that takes advantage of the small vertical size of the CESR beam spot to measure the energy release distribution from the D*+ -> D0 pi+ decay. Our preliminary result is Gamma(D*+) = 96 +- 4 (Statistical) +- 22 (Systematic) keV.'],['2001-02-06']
312,['eng'],"['Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Schwarthoff, H', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V']",['Mixing and CP Violation in the Decay of Neutral D Mesons at CLEO'],['Particle Physics - Experimental Results'],"['talk, Ise-Shima 2001/02/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'energy loss', 'violation, CP', 'pseudoscalar meson, pair production', 'D0 anti-D0, interference', 'lifetime, difference', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D0 --> 2pi', 'D0 --> 2K', 'D0 --> K pi', 'D0 --> K+ pi- pi0', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102006'],"['We present preliminary results of several analyses searching for the effects of CP violation and mixing in the decay of D0 mesons. We find no evidence of CP asymmetry in five different two-body decay modes of the D0 to pairs of light pseudo-scalar mesons: A_CP(K+ K-) = (+0.05 +- 2.18 +- 0.84)%, A_CP(pi+ pi-) = (+2.0 +- 3.2 +- 0.8)%, A_CP(K0_S pi0) = (+0.1 +- 1.3)% A_CP(pi0 pi0) = (+0.1 +- 4.8)% and A_CP(K0_S K0_S) = (-23 +- 19)%. We present the first measurement of the rate of wrong-sign D0 -> K+ pi- pi0 decay: R_WS = 0.0043 + 0.0011 - 0.0010 +- 0.0007. Finally, we describe a measurement of the mixing parameter y_CP= Delta Gamma / (2 Gamma) by searching for a lifetime difference between the CP neutral K+ pi- final state and the CP even K+K- and pi+pi- final states. Under the assumption that CP is conserved we find y_CP = -0.011 +- 0.025 +- 0.014.']",['2001-02-06']
313,['eng'],"['Eggers, H C']",['Experimental correlation analysis'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'data analysis method', 'correlation, ((n)particle)', 'phase space', 'statistical analysis', 'multiplicity, moment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102005'],"['Commonalities and differences in correlation analysis in terms of phase space, conditioning and uncorrelatedness are discussed. The Poisson process is not generally appropriate as reference distribution for normalisation and cumulants, so that generalised statistics in terms of arbitrarily defined reference processes must be employed. Consideration of the sampling hierarchy leads us to a classification of current event-by-event observables.']",['2001-02-06']
314,['eng'],"['Sikler, F']",['Recent NA49 results on Pb+Pb collisions at CERN SPS'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'p p, interaction', 'p nucleus, nuclear reaction', 'scattering, heavy ion', 'carbon', 'silicon', 'aluminum', 'lead', 'hadron, multiple production', 'energy loss', 'production, strangeness', 'correlation', 'pi, density', 'Xi-', 'Lambda(1520)', 'Phi(1020)', 'yield, (Phi(1020) K pi)', 'energy dependence', 'dependence, mass number', 'magnetic spectrometer, experimental results', 'CERN SPS', '40, 158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102004'],"['In the spirit of establishing a fair reference for nucleus-nucleus collisions, results on stopping and baryon transfer, correlations of the p+p interaction and their consequences are shown. In the discussion of new results from nucleus-nucleus collisions the emphasis is on strange meson and baryon production at different energies - for the first time at 40 GeV A - with the study of light nuclei.']",['2001-02-06']
315,['eng'],"['Bai, J Z']",['Measurements of the Cross Section for e+e- -> hadrons at Center-of-Mass Energies from 2 to 5 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'cross section, hadronic', 'energy dependence', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', '2-5 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102003'],['We report values of $R = \\sigma(e^+e^-\\to {hadrons})/\\sigma(e^+e^-\\to\\mu^+\\mu^-)$ for 85 center-of-mass energies between 2 and 5 GeV measured with the upgraded Beijing Spectrometer at the Beijing Electron-Positron Collider.'],['2001-02-06']
316,['eng'],"['Abe, K']",['Improved Measurement of the Probability for Gluon Splitting into b bbar in Z0 Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, multiple production', 'final state, (4jet)', 'gluon, fragmentation', 'quark, beauty', 'quark, pair production', 'particle identification, flavor', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'electron positron --> quark antiquark gluon', 'gluon --> 2beauty', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102002'],"['We have measured gluon splitting into bottom quarks, g -> b bbar, in hadronic Z0 decays collected by SLD between 1996 and 1998. The analysis was performed by looking for secondary bottom production in 4-jet events of any primary flavor. 4-jet events were identified, and in each event a topological vertex-mass technique was applied to the two jets closest in angle in order to identify them as b or bbar jets. The upgraded CCD vertex detector gives very high B-tagging efficiency, especially for B hadrons with the low energies typical of this process. We measured the rate of g -> b bbar production per hadronic event, g_bb, to be (2.44+-0.59 (stat) +-0.34 (syst)) X10**-3.']",['2001-02-06']
317,['eng'],"['Allmendinger, T', 'Barker, G', 'Feindt, Michael', 'Haag, C', 'Moch, M']",['BSAURUS- A Package For Inclusive B-Reconstruction in DELPH'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, beauty', 'B, particle identification', 'particle identification, flavor', 'programming', 'track data analysis, vertex', 'decay, path length', 'neural network', 'numerical calculations, Monte Carlo', 'magnetic detector, DELPHI', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102001'],"['BSAURUS is a software package for the inclusive reconstruction of B-hadrons in Z-decay events taken by the DELPHI detector at LEP. The BSAURUS goal is to reconstruct B-decays, by making use of as many properties of b-jets as possible, with high efficiency and good purity. This is achieved by exploiting the capabilities of the DELPHI detector to their extreme, applying wherever possible physics knowledge about B production and decays and combining different information sources with modern tools- mainly artificial neural networks. This note provides a reference of how BSAURUS outputs are formed, how to access them within the DELPHI framework, and the physics performance one can expect.']",['2001-02-02']
318,['eng'],"['Ivanov, E I']",['Observation of exotic meson production in the reaction $ \\pi^{-} p \\to \\eta^{\\prime} \\pi^- p$ at 18 GeV/c'],['Particle Physics - Experimental Results'],"['pi- p, exclusive reaction', 'eta(958), hadroproduction', 'mass spectrum, (eta(958) pi-)', 'meson, exotic', 'partial wave analysis', 'a2(1320)', 'a4(2040)', 'pi1(1600)', 'momentum transfer, dependence', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'pi- p --> eta(958) p pi-', '18 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101058'],"['An amplitude analysis of an exclusive sample of 5765 events from the reaction $\\pi^{-} p \\to \\eta^{\\prime} \\pi^- p$ at 18 GeV/c is described. The $\\eta^{\\prime} \\pi^-$ production is dominated by natural parity exchange and by three partial waves: those with $J^{PC} = 1^{-+}, 2^{++},$ and $4^{++}$. A mass-dependent analysis of the partial-wave amplitudes indicates the production of the $a_2(1320)$ meson as well as the $a_4(2040)$ meson, observed for the first time decaying to $\\eta^{\\prime}\\pi^-$. The dominant, exotic (non-$q\\bar{q}) $ $1^{-+}$ partial wave is shown to be resonant with a mass of $1.597 \\pm 0.010^{+0.045}_{-0.010}$ GeV/c^2 and a width of $0.340 \\pm 0.040 \\pm 0.050$ GeV/c^2 . This exotic state, the $\\pi_1(1600)$, is produced with a $t$ dependence which is different from that of the $a_2(1320)$ meson, indicating differences between the production mechanisms for the two states.']",['2001-02-02']
319,['eng'],"['Todorova-Nová, S']",['Inter-W Bose-Einstein Correlations ... or Not?'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'Z0, pair production', 'intermediate boson, decay modes', 'correlation, two-pion', 'boson, statistics', 'correlation function', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101057'],"[""A critical summary is given of the present status of the study of Bose-Einstein Correlations in W-pair production at LEP II. In particular, the evidence is reviewed for or against the existence of Bose-Einstein correlations between pions originating both from a different of the two W's. If present, such an inter-W interference would not only form a potential bias in the determination of the W mass, but also would provide a laboratory to measure the space-time development of the overlap. If absent, this would drastically change the conventional (Hanbury Brown and Twiss) picture of pion interferometry in high energy physics.""]",['2001-02-02']
320,['eng'],"['Jikia, G', 'Söldner-Rembold, S']",['Light Higgs Production at a Photon Collider'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2000/06/14', 'photon photon, interaction', 'luminosity', 'Higgs particle, photoproduction', 'photon, polarization', 'Higgs particle, decay modes', 'Higgs particle, width', 'background', 'quantum chromodynamics, perturbation theory', 'correction, higher-order', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101056'],['We present a preliminary study of the production of a light Higgs boson with a mass between 120 and 160 GeV in photon-photon collisions at a Compton collider. The event generator for the backgrounds to a Higgs signal due to bbbar and ccbar heavy quark pair production in polarized Gamma-Gamma collisions is based on a complete next-to-leading order (NLO) perturbative QCD calculation. For J_z=0 the large double-logarithmic corrections up to four loops are also included. It is shown that the two-photon width of the Higgs boson can be measured with high statistical accuracy of about 2-10% for integrated Gamma-Gamma luminosity in the hard part of the spectrum of 43 fb-1. From this result the total Higgs boson width can be derived in a model independent way.'],['2001-01-31']
321,['eng'],"['Kuznetsov, V E']",['Higgs and B physics in Run II'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'Higgs particle, search for', 'Higgs particle, hadroproduction', 'channel cross section, mass', 'Higgs particle, decay modes', 'Higgs particle, branching ratio', 'quark, beauty', 'quark, pair production', 'beautiful meson, decay', 'violation, CP', 'B0 anti-B0, interference', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'numerical calculations', 'proposed experiment, Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101055'],"['In Run II at the Tevatron, the major goal of the upgraded CDF and \\dzero detectors is a Higgs search in the mass range of 110-200 GeV. They will also contribute significantly to B physics. Among many possibilities they will be able to measure rare decays of B mesons and improve our knowledge of CP violation in B system through study of B mixing. Various aspects of Higgs and B physics in Run II are discussed here.']",['2001-01-31']
322,['eng'],"['Kolomensky, Yu G']",['First Measurement of the CP-Violating Asymmetries with BABAR'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'violation, CP', 'asymmetry, time dependence', 'particle identification, flavor', 'Kobayashi-Maskawa angle, unitarity', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> J/psi(3100) K0(S)', 'B0 --> psi(3685) K0(S)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101054'],"['We report on a preliminary measurement of time-dependent CP-violating asymmetries in B0 --> J/psi K0S and B0 --> psi(2S) K0S decays recorded by the BABAR detector at the PEP-II asymmetric B Factory at SLAC. The data sample consisted of 9.0 fb-1 collected at the Y(4S) resonance and 0.8 fb-1 off-resonance. One of the pair of neutral B mesons produced at the Y(4S) was fully reconstructed, while the flavor of the other neutral B meson was tagged at the time of its decay. The value of the asymmetry amplitude, sin(2beta), was determined from a maximum likelihood fit to the time distribution of 120 tagged candidates to be sin(2beta) = 0.12 +- 0.37 (stat.) +- 0.09 (syst.) (preliminary).']",['2001-01-30']
323,['eng'],[],['J/psi suppression in Pb-Pb collisions at CERN SPS'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'p nucleus, nuclear reaction', 'scattering, heavy ion', 'lead', 'oxygen', 'sulfur', 'hadron, multiple production', 'J/psi(3100), yield', 'J/psi(3100), leptonic decay', 'critical phenomena, confinement', 'quark gluon, plasma', 'dependence, impact parameter', 'magnetic spectrometer, experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101052'],"['The NA38 and NA50 experiments at the CERN SPS have measured charmonium production in different colliding systems with the aim of observing a phase transition from ordinary hadronic matter towards a state in which quarks and gluons are deconfined (Quark Gluon Plasma, QGP). In fact it was predicted that the J/psi yield should be suppressed in deconfined matter. The analysis of the data collected by the NA50 experiment with Pb-Pb collisions at 158 GeV/c per nucleon shows that the J/psi is anomalously suppressed in central collisions and the observed pattern can be considered as a strong indication for QGP production.']",['2001-01-30']
324,['eng'],"['Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Brabant, P', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J']",['Correlated ${\\Lambda_{c}}^{+}\\overline{{\\ Lambda}_{c}}{-}$ production in $e^{+}e^{-}$ annihilations at $\\sqrt{s}$ $\\approx$ 10.5 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, beauty', 'quark, pair production', 'Lambda/c+, electroproduction', 'Lambda/c+, hadronic decay', 'Lambda/c+, pair production', 'anti-D, associated production', 'channel cross section, ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Lambda/c+ Antilambda/c+', 'electron positron --> anti-D Lambda/c+', 'approx. 10.5 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101051'],"[""Using 13.6/fb of continuum two-jet e+e- -> ccbar events collected with the CLEO detector, we have searched for baryon number correlations at the primary quark level. We have measured the likelihood for a /\\c+ charmed baryon to be produced in the hemisphere opposite a /\\c- relative to the likelihood for a /\\c+ charmed baryon to be produced opposite an anticharmed meson Dbar; in all cases, the reconstructed hadrons must have momentum greater than 2.3 GeV/c. We find that, given a /\\c- (reconstructed in five different decay modes), a /\\c+ is observed in the opposite hemisphere (0.72+/-0.11)% of the time (not corrected for efficiency). By contrast, given a Dbar in one hemisphere, a /\\c+ is observed in the opposite hemisphere only (0.21+/-0.02)% of the time. Normalized to the total number of either /\\c- or Dbar ``tags'', it is therefore 3.52+/-0.45+/-0.42 times more likely to find a /\\c+ opposite a /\\c- than a Dbar meson. This enhancement is not observed in the JETSET 7.3 e+e- -> ccbar Monte Carlo simulation.""]",['2001-01-30']
325,['eng'],"['Schwartz, A J']",['Searches for Rare and Forbidden Decays of Charm'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'pi- nucleus, inclusive reaction', 'platinum', 'carbon', 'charmed meson, hadroproduction', 'charmed meson, semileptonic decay', 'charmed meson, rare decay', 'D0, leptonic decay', 'D+', 'D/s+', 'final state, dilepton', 'charmed meson, branching ratio', 'upper limit', 'neutral current, flavor changing', 'violation, flavor', 'lepton number, violation', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101050'],"['We review results on rare and forbidden decays of D^0, D^+, and D^+_s mesons from experiments at FNAL. The decay modes studied have two leptons in the final state and, if observed, would constitute evidence for flavor-changing neutral-current, lepton-flavor-violating, or lepton-number-violating processes. To date, no evidence for these decays has been observed and upper limits are obtained for their branching fractions. These limits can constrain various extensions to the Standard Model. We present new upper limits from FNAL E791 on the branching fractions for more than two dozen three- and four-body decay modes.']",['2001-01-30']
326,['eng'],"['Wang, Y F', 'Balic, V', 'Gratta, Giorgio', 'Fassò, Alberto', 'Roesler, S', 'Ferrari, A']",['Predicting Neutron Production from Cosmic-ray Muons'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'muon nucleus, nuclear reaction', 'n, yield', 'energy dependence', 'n, energy spectrum', 'numerical calculations, Monte Carlo', 'interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101049'],"['Fast neutrons from cosmic-ray muons are an important background to underground low energy experiments. The estimate of such background is often hampered by the difficulty of measuring and calculating neutron production with sufficient accuracy. Indeed substantial disagreement exists between the different analytical calculations performed so far, while data reported by different experiments is not always consistent. We discuss a new unified approach to estimate the neutron yield, the energy spectrum, the multiplicity and the angular distribution from cosmic muons using the Monte Carlo simulation package FLUKA and show that it gives a good description of most of the existing measurements once the appropriate corrections have been applied.']",['2001-01-30']
327,['eng'],"['Ellison, J']",['The D0 Detector Upgrade and Physics Program'],['Particle Physics - Experimental Results'],"['talk, Tver 2000/09/14', 'luminosity, upgrade', 'semiconductor detector, microstrip', 'scintillation counter, fibre', 'superconducting, solenoid', 'shower detector', 'muon, drift chamber', 'proportional chamber, drift tube', 'trigger', 'data acquisition', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101048'],[],['2001-01-29']
328,['eng'],"['Kress, T']",['Polarization and Spin Alignment in Multihadronic Z0 Decays'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'hadron, multiple production', 'baryon, polarization', 'spin, alignment', 'Lambda', 'Lambda/b0', 'vector meson, helicity', 'helicity, density matrix', 'K*(892)', 'B*(5320)', 'D*(2010)', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101047'],"['The large statistics of millions of hadronic Z0 decays, accumulated by the four LEP experiments between 1989 and 1995, allowed for detailed investigations of the fragmentation process. Inclusive Lambda_b baryons and Lambda hyperons at intermediate and high momentum have been found to show longitudinal polarization. This may be related to the primary quark and antiquark polarization and the hadronization mechanism which produces the leading baryons. Helicity density-matrix elements have been measured for a variety of vector mesons produced inclusively in hadronic Z0 decays. The diagonal elements of some of the light mesons and the D*+- show a preference for a helicity-zero state if the meson carries a large fraction of the available energy. The mechanism which produces such spin alignment in the non-perturbative hadronization of the primary partons to the vector mesons is so far unexplained. For the B* the results are consistent with no spin alignment, which is expected in a picture based on HQET. For some meson species non-diagonal elements have been measured indicating coherence phenomena due to final-state interaction between the primary quark and antiquark.']",['2001-01-26']
329,['eng'],"['Favart, L']",['Deeply Virtual Compton Scattering at HERA'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon p, Compton scattering', 'photon, off-shell', 'quantum chromodynamics, perturbation theory', 'exchange, two-gluon', 'photon, angular distribution', 'channel cross section, energy dependence', 'momentum transfer, dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> p positron photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101046'],"['Results on Deeply Virtual Compton Scattering at HERA measured by the H1 and ZEUS Collaborations are presented. The cross section, measured for the first time, is reported for Q^2 > 2 GeV^2.']",['2001-01-26']
330,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kamer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R J', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A Search for a Narrow Radial Excitation of the $D^{*\\pm}$ Meson'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'search for, narrow resonance', 'charmed meson, excited state', 'postulated particle, D*(2629)', 'production, upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'D*(2629) --> D*(2010) pi+ pi-', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101045'],"[""A sample of 3.73 million hadronic Z decays, recorded with the OPAL detector at LEP in the years 1991-95, has been used to search for a narrow resonance corresponding to the decay of the D*'+/-(2629) meson into D*+/- pi+ pi-. The D*+ mesons are reconstructed in the decay channel D*+ -> D0 pi+ with D0 -> K- pi+. No evidence for a narrow D*'+/-(2629) resonance is found. A limit on the production of D*'+/-(2629) in hadronic Z decays is derived: f(Z -> D*'+/-(2629)) x Br(D*'+ -> D*+ pi+ pi-) < 3.1 x 10^{-3} (95% C.L.)""]",['2001-01-26']
331,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, H', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kamer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R J', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A Simultaneous Measurement of the QCD Colour Factors and the Strong Coupling'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, multiple production', 'quantum chromodynamics', 'color', 'strong interaction, coupling constant', 'angular correlation, (4jet)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101044'],"['Using data from e+e- annihilation into hadrons, taken with the OPAL detector at LEP at the Z pole between 1991 and 1995, we performed a simultaneous measurement of the colour factors of the underlying gauge group of the strong interaction, CF and CA, and the strong coupling, alpha(s). The measurement was carried out by fitting next-to-leading order perturbative predictions to measured angular correlations of 4-jet events together with multi-jet related variables. Our results, CA = 3.02 +/- 0.25 (stat.) +/- 0.49 (syst.) CF = 1.34 +/- 0.13 (stat.) +/- 0.22 (syst.), alpha(s)(M_Z) = 0.120 +/- 0.011 (stat.) +/- 0.020 (syst.), provide a test of perturbative QCD in which the only assumptions are non-abelian gauge symmetry and standard hadronization models. The measurements are in agreement with SU(3) expectations for CF and CA and the world average of alpha(s)(M_Z).']",['2001-01-26']
332,['eng'],"['Achasov, M N', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bogdanchikov, A G', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Drozdetsky, A A', 'Druzhinin, V P', 'Ganyushin, D I', 'Golubev, V B', 'Ivanchenko, V N', 'Koop, I A', 'Korol, A A', 'Koshuba, S V', 'Otboev, A V', 'Pakhtusova, E V', 'Salnikov, A A', 'Shary, V V', 'Serednyakov, S I', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skripkin, A G', 'Valishev, A A', 'Vasilev, A V', 'Velikzhanin, Yu S']",['Search for the radiative decay $\\eta \\to \\pi^0 \\gamma \\gamma$ in the SND experiment at VEPP-2M'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'eta, radiative decay', 'eta, branching ratio', 'upper limit', 'perturbation theory, chiral', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> eta photon', 'eta --> pi0 2photon', '1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101043'],['The $\\eta \\to \\pi^0 \\gamma \\gamma$ decay was investigated by the SND detector at VEPP-2M $e^+e^-$ collider in the reaction $e^+e^-\\to\\phi\\to \\eta\\gamma$. Here we present the results and some details of this study. We report an upper limit (90% c.l.) $Br(\\eta \\to \\pi^0 \\gamma \\gamma)<8.4\\times 10^{-4}$ as our final result. Our upper limit does not contradict the earlier measurement by GAMS spectrometer. To facilitate future studies a rather detailed review of the problem is also given.'],['2001-01-26']
333,['eng'],"['Prigl, R', 'Brown, H N', 'Bunce, G M', 'Carey, R M', 'Cushman, P B', 'Danby, G T', 'Debevec, P T', 'Deng, H', 'Deninger, W J', 'Dhawan, S K', 'Druzhinin, V P', 'Duong, L', 'Earle, W', 'Efstathiadis, E F', 'Farley, Francis J M', 'Fedotovich, G V', 'Giron, S', 'Gray, F', 'Grosse-Perdekamp, M', 'Grossmann, A', 'Haeberlen, U', 'Hare, M', 'Hazen, E S', 'Hertzog, D W', 'Hughes, V W', 'Iwasaki, M', 'Jungmann, K', 'Kawall, D', 'Kawamura, M', 'Khazin, B I', 'Kindem, J', 'Krienen, F', 'Kronkvist, I J', 'Larsen, R', 'Lee, Y Y', 'Liu, W', 'Logashenko, I B', 'McNabb, R', 'Meng, W', 'Mi, J L', 'Miller, J P', 'Morse, W M', 'Neumayer, P', 'Nikas, D', 'Onderwater, C J G', 'Orlov, Y', 'Ozben, C', 'Paley, J M', 'Pai, C', 'Polly, C', 'Pretz, J', 'zu Putlitz, G', 'Redin, S I', 'Rind, O', 'Roberts, B L', 'Ryskulov, N', 'Sedykh, S N', 'Semertzidis, Y K', 'Shatunov, Yu M', 'Sichtermann, E P', 'Solodov, E P', 'Sossong, M', 'Steinmetz, A', 'Sulak, Lawrence R', 'Tanaka, M', 'Timmermans, C', 'Trofimov, A V', 'Urner, D', 'Warburton, D', 'Winn, D', 'Yamamoto, A', 'Zimmerman, D']",['Status of the BNL Muon g-2 Experiment'],['Particle Physics - Experimental Results'],"['talk, Carmel 2000/09/11', 'muon+, polarized beam', 'muon, magnetic moment', 'magnetic field, external field', 'electroweak interaction, validity test', 'muon+, leptonic decay', 'positron, energy spectrum', 'experimental results', 'Brookhaven PS']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101042', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']","['The muon g-2 experiment at Brookhaven has been taking data since 1997. Analyses of the data taken in 1997 and 1998, which include about 2% of the data taken so far, have improved the experimental accuracy in the muon anomalous magnetic moment to a(mu,expt) = 1 165 921(5) x 10**(-9) (4 ppm). The value agrees with standard theory. Analysis of the 1999 data, about 25% of the existing data set, is nearing completion and analysis of the 2000 data has started. The experiment is preparing for another major data taking run, this time storing negative instead of positive muon beams.']",['2001-01-25']
334,['eng'],"['Antonioli, P']",['MONOLITH'],['Particle Physics - Experimental Results'],"['talk, Conca Specchiulla 2000/09/09', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino, energy', 'neutrino, angular distribution', 'magnetic detector, proposed', 'calorimeter', 'resolution', 'deep underground detector, Gran Sasso']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101040'],"[""MONOLITH is a massive magnetized tracking calorimeter, optimized for the detection of atmospheric muon neutrinos, proposed at the Gran Sasso laboratory in Italy. The main goal is to establish (or reject) the neutrino oscillation hypothesis through an explicit observation of the full first oscillation swing (the ``L/E pattern''). Its performance, status and prospects are briefly reviewed.""]",['2001-01-25']
335,['eng'],"['Auerbach, L B', 'Burman, R L', 'Caldwell, D O', 'Church, E D', 'Donahue, J B', 'Fazely, A', 'Garvey, G T', 'Gunasingha, R M', 'Imlay, R', 'Louis, W C', 'Majkic, R', 'Malik, A', 'Metcalf, W', 'Mills, G B', 'Sandberg, V D', 'Smith, D', 'Stancu, I', 'Sung, M', 'Tayloe, R', 'VanDalen, G J', 'Vernon, W', 'Wadia, N', 'White, D H', 'Yellin, S']",['Measurement of electron-neutrino electron elastic scattering'],['Particle Physics - Experimental Results'],"['neutrino electron, elastic scattering', 'neutrino/e, secondary beam', 'charged current', 'neutral current, flavor changing', 'interference', 'channel cross section', 'electroweak interaction, validity test', 'pi+, leptonic decay', 'muon+, leptonic decay', 'neutrino/mu, magnetic moment', 'upper limit', 'scintillation counter, liquid', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101039'],"['The cross section for the elastic scattering reaction nu_e+e- -> nu_e+e- was measured by the Liquid Scintillator Neutrino Detector using a mu+ decay-at-rest nu_e beam at the Los Alamos Neutron Science Center. The standard model of electroweak physics predicts a large destructive interference between the charge current and neutral current channels for this reaction. The measured cross section, sigma_{nu_e e-}=[10.1 +- 1.1(stat.) +- 1.0(syst.)]x E_{nu_e} (MeV) x 10^{-45} cm^2, agrees well with standard model expectations. The measured value of the interference parameter, I=-1.01 +- 0.13(stat.) +- 0.12(syst.), is in good agreement with the standard model expectation of I^{SM}=-1.09. Limits are placed on neutrino flavor-changing neutral currents. An upper limit on the muon-neutrino magnetic moment of 6.8 x 10^{-10} mu_{Bohr} is obtained using the nu_mu and \\bar{nu}_mu fluxes from pi+ and mu+ decay.']",['2001-01-23']
336,['eng'],"['Morales, A', 'Brodzinski, R L', 'Cebrian, S', 'García, E', 'González, D', 'Irastorza, I G', 'Miley, H S', 'Morales, J', 'De Solorzano, A O', 'Puimedón, J', 'Reeves, J H', 'Sarsa, M L', 'Scopel, S', 'Villar, J A']",['Particle Dark Matter and Solar Axion Searches with a small germanium detector at the Canfranc Underground Laboratory'],['Particle Physics - Experimental Results'],"['new particle, search for', 'astrophysics, missing-mass', 'WIMP', 'axion, solar', 'coupling, (axion photon)', 'shielding', 'semiconductor detector, germanium', 'deep underground detector, experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101037'],"['A small, natural abundance, germanium detector (COSME) has been operating recently at the Canfranc Underground Laboratory (Spanish Pyrenees) in improved conditions of shielding and overburden with respect to a previous operation of the same detector. An exposure of 72.7 kg day in these conditions has at present a background improvement of about one order of magnitude compared to the former operation of the detector. These new data have been applied to a direct search for WIMPs and solar axions. New WIMP exclusion plots improving the current bounds for low masses are reported. The paper also presents a limit on the axion-photon coupling obtained from the analysis of the data looking for a Primakoff axion-to-photon conversion and Bragg scattering inside the crystal.']",['2001-01-23']
337,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Baroiant, S', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bell, W H', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A', 'Binkley, M', 'Bisello, D', 'Bishai, M', 'Blair, R E', 'Blocker, C', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'vanden Brink, S', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-, E', 'Geer', 'Budagov, Yu', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Caskey, W', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G', 'Chlebana, F', 'Christofek, L S', 'Chu, M L', 'Chung, Y S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', ""D'Auria, S"", 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demortier, L', 'Deninno, M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erbacher, R D', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Fernández, J P', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Furic, I K', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Glenzinski, D A', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Gorelov, I', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Grim, G', 'Gris, P', 'Groer, L S', 'Grosso--, C', 'Pilcher, J E', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hill, C', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J', 'Ikeda, H', 'Incandela, J', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R', 'Khazins, D', 'Kikuchi, T', 'Kilminster, B', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirby, M', 'Kirk, M', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, J', 'Lancaster, M', 'Lander, R', 'Latino, G', 'LeCompte, T', 'Lee IV, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liu, J B', 'Liu, Y C', 'Litvintsev, D O', 'Lobban, O', 'Lockyer, N', 'Loken, J', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'McKigney, E', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Meyer, A', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Moulik, T', 'Mulhearn, M', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Nachtman, J', 'Nagaslaev, V', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Nelson, T', 'Neu, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Ribon, A', 'Riegler, W', 'Rimondi, F', 'Ristori, L', 'Riveline, M', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R', 'Rossin, R', 'Roy, A', 'Safonov, A', 'Saint-Denis, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sánchez, C', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Sidoti, A', 'Siegrist, J', 'Sill, A', 'Sinervo, P', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Stru-mia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Tesarek, R', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Thompson, A S', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Wilkes, T', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Measurement of the $t\\bar{t}$ production cross section in $p\\bar{p}$ collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'W, leptonic decay', 'final state, ((n)jet lepton neutrino)', 'transverse energy, missing-energy', 'particle identification, beauty', 'mass, truth', 'channel cross section', 'background', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'anti-p p --> 2truth anything', 'truth --> W beauty', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101036'],"['We update the measurement of the top production cross section using the CDF detector at the Fermilab Tevatron. This measurement uses $t\\bar{t}$ decays to the final states $e+\\nu$+jets and $\\mu+\\nu$+jets. We search for $b$ quarks from $t$ decays via secondary-vertex identification or the identification of semileptonic decays of the $b$ and cascade $c$ quarks. The background to the $t\\bar{t}$ production is determined primarily through a Monte Carlo simulation. However, we calibrate the simulation and evaluate its uncertainty using several independent data samples. For a top mass of 175 $GeV/c^2$, we measure $\\sigma_{t\\bar{t}}=5.1 \\pm 1.5$ pb and $\\sigma_{t\\bar{t}}=9.2 \\pm 4.3$ pb using the secondary vertex and the lepton tagging algorithms, respectively. Finally, we combine these results with those from other $t\\bar{t}$ decay channels and obtain $\\sigma_{t\\bar{t}} = 6.5^{+1.7}_{-1.4}$ pb.']",['2001-01-23']
338,['eng'],"['Touramanis, C']",['Physics at BABAR'],['Particle Physics - Experimental Results'],"['talk, Carmel 2000/09/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B0, lifetime', 'B+, lifetime', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'B0 anti-B0, interference', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> psi mesons K', 'psi mesons --> lepton+ lepton-', 'psi(3685) --> J/psi(3100) pi+ pi-', 'approx. 10.6 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101035', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']","['The BABAR detector at the SLAC PEP-II asymmetric e+e- collider has first started collecting data in May 1999. A study of time-dependent CP-violating asymmetries in B0 --> J/psi K0S and B0 --> psi(2S) K0S decays has been performed on a data sample of 9.0fb-1 taken at the Y(4S) resonance and 0.8fb-1 off-resonance, collected through July 2000. The preliminary result sin2beta = 0.12+/-0.37 (stat) +/- 0.09 (syst) is presented here, together with preliminary results on neutral and charged B meson lifetimes and B0B0bar mixing.']",['2001-01-23']
339,['eng'],"['Gershon, T J']",['Measurement of direct CP violation by the NA48 experiment at CERN'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'K0, hadronic decay', 'K0(L), secondary beam', 'K0(S), secondary beam', 'pi, pair production', 'violation, CP', 'magnetic spectrometer, experimental results', 'CERN SPS', 'K0 --> pi+ pi-', 'K0 --> 2pi0']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101034'],"['The NA48 experiment at CERN has performed a measurement of direct CP violation in the neutral kaon system, based on data collected in 1997 and 1998. The preliminary result for the parameter $\\Re(\\epsilon^{\\prime}/\\epsilon)$ is $(14.0 \\pm 4.3) \\times 10^{-4}$.']",['2001-01-23']
340,['eng'],"['Haas, R']",['Search for Susy with Missing Transverse Energy and Jets at CDF'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'anti-p p, colliding beams', 'sparticle, search for', 'R parity, invariance', 'jet, multiple production', 'transverse energy, missing-energy', 'supersymmetry, symmetry breaking', 'gravitino', 'squark, truth', 'squark, beauty', 'sparticle, mass', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> (n)jet missing-energy anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010063'],"['Events with signatures involving large missing transverse energy (MET) are among the quintessential search modes for R-parity conserving supersymmetry. CDF has conducted two recent analyses for supersymmetry which use MET and jets. The MET and monojet signature is employed to determine process independent limits for the production of new physics beyond the Standard Model and then applied to models of spontaneous breaking of supersymmetry to determine limits on the supersymmetry breaking parameter and the gravitino mass. Direct searches for scalar top and scalar bottom quarks within the framework of supersymmetric models are performed using a signature of MET and two heavy flavor jets. Since the data is found to be consistent with Standard Model expectations, limits are determined in the mass planes $m (\\tilde{\\chi}_{1}^{0}) - m (\\tilde{t}_{1})$ and $m (\\tilde{\\chi}_{1}^{0}) - m (\\tilde{b}_{1})$.']",['2000-10-26']
341,['eng'],"['Kinoshita, K']",['CP Results from Belle'],['Particle Physics - Experimental Results'],"['talk, Maagan 2000/09/13', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'Kobayashi-Maskawa angle, unitarity', 'violation, CP', 'B, hadronic decay', 'quarkonium, charm', 'quarkonium, decay modes', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B --> quarkonium K0', 'B --> quarkonium pi0', 'psi mesons --> lepton+ lepton-', 'psi(3685) --> J/psi(3100) pi+ pi-', 'chi/c1(3510) --> J/psi(3100) photon', '10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101033'],"['The Belle detector at KEKB has collected 6.2 fb^{-1} of data at the Upsilon(4S) resonance. Presented here are preliminary measurements, from this data sample, of sin(2phi_1) and other quantities relating to CP.']",['2001-01-22']
342,['eng'],"['Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J']",['Observation of $B\\to \\phi K$ and $B\\to \\phi K^{*}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'Phi(1020)', 'K*(892)', 'K', 'B0, branching ratio', 'B-, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B- --> Phi(1020) K-', 'B0 --> Phi(1020) K0', 'B --> Phi(1020) K*(892)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101032'],"['We have studied two-body charmless hadronic decays of $B$ mesons into the final states phi K and phi K^*. Using 9.7 million $B\\bar{B}$ pairs collected with the CLEO II detector, we observe the decays B- -> phi K- and B0 -> phi K*0 with the following branching fractions: BR(B- -> phi K-)=(5.5 +2.1-1.8 +- 0.6) x 10^{-6} and BR(B0 -> phi K*0)=(11.5 +4.5-3.7 +1.8-1.7) x 10^{-6}. We also see evidence for the decays B0 -> phi K0 and B- -> phi K*-. However, since the statistical significance is not overwhelming for these modes we determine upper limits of <12.3 x 10^{-6} and <22.5 x 10^{-6} (90% C.L.) respectively.']",['2001-01-22']
343,['eng'],"['Klempt, E']","['Glueballs, Hybrids and Q\\bar Q Mesons']",['Particle Physics - Experimental Results'],"['talk, Zuoz 2000/08/13', 'meson, hadron spectroscopy', 'meson, quantum number', 'quark', 'glueball, mass spectrum', 'quantum chromodynamics', 'lattice field theory', 'meson, hybrid', 'meson, exotic', 'meson, multiplet', 'mass formula', 'meson, decay', 'interference, (scalar meson glueball)', 'quark, multiquark', 'anti-p p, annihilation', 'Z0, hadronic decay', 'J/psi(3100), radiative decay', 'meson, decay modes', 'numerical calculations, interpretation of experiments', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101031'],"['Lattice gauge calculations predict the existence of glueballs. In particular a scalar glueball is firmly expected at a mass of about 1730 MeV. This prediction has led to an intense study of scalar isoscalar interactions and to the discovery of new meson resonances. The number of scalar states observed seems to exceed the number of states which can be accommodated in the quark model even when two states, the a_0(980) and f_0(980), are interpreted as K Kbar bound states and are removed from the list. However, none of these states has a decay pattern which is consistent with that of a pure glueball. A reasonable interpretation of the number of states and of their decay pattern is found only when mixing of scalar q qbar states with the scalar glueball is taken into account. In this paper we scrutinize the evidence for these states and their production characteristics. The f_0(1370) - a cornerstone of all qbar q-glueball mixing scenarios - is shown to be likely of non-qbar q nature. The remaining scalar states then do fit into a nonet classification. If this interpretation should be correct there would be no room for resonant scalar gluon-gluon interactions, no room for the scalar glueball. We also discuss the status of mesons with exotic quantum numbers, of mesons which cannot possibly have qbar q structure, and argue that these are, most likely, four-quark states and not excitations of the gluon string providing the binding between quark and antiquark.']",['2001-01-22']
344,['eng'],"['Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z']",['A Search for Charmless $B\\to VV$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'vector meson, pair production', 'rho(770)0', 'K*(892)', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> 2rho(770)0', 'B --> K*(892) rho(770)0', 'B --> 2K*(892)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101029'],"['We have studied two-body charmless decays of the $B$ meson into the final states $\\rho^0 \\rho^0$, $K^{*0} \\rho^0$, $K^{*0} K^{*0}$, $K^{*0} \\bar{K^{*0}}$, $K^{*+} \\rho^0$, $K^{*+} \\bar{K^{*0}}$, and $K^{*+} K^{*-}$ using only decay modes with charged daughter particles. Using 9.7 million $B \\bar{B}$ pairs collected with the CLEO detector, we place 90% confidence level upper limits on the branching fractions, $(0.46-7.0)\\times 10^{-5}$, depending on final state and polarization.']",['2001-01-19']
345,['eng'],"['Castanier, C', 'Gay, P', 'Lutz, P', 'Orloff, J']",['Higgs self coupling measurement in e+e- collisions at center-of-mass energy of 500 GeV'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'Higgs particle, electroproduction', 'Higgs particle, pair production', 'Z0, associated production', 'Higgs particle, coupling', 'vertex function, (3Higgs particle)', 'Higgs particle, mass', 'background', 'channel cross section', 'mass spectrum', 'neural network', 'numerical calculations, Monte Carlo', 'electron positron --> 2Higgs particle Z0', '500 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101028'],['Feasibility of the measurement of the trilinear self-couplings of the Higgs boson is studied. Such a measurement would experimentally determine the structure of the Higgs potential. Full hadronic and semi-leptonic final states of the double-Higgs strahlung have been investigated.'],['2001-01-19']
346,['eng'],[],['Combination procedure for the precise determination of Z boson parameters from results of the LEP experiments'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'electroweak interaction, validity test', 'parametrization', 'Z0, mass', 'Z0, width', 'cross section, hadronic', 'Z0, hadronic decay', 'Z0, leptonic decay', 'angular distribution, asymmetry', 'Weinberg angle', 'statistical analysis', 'interference, (Z0 photon)', 'lepton, universality', 'flavor, 3', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101027'],"['The precise determination of the Z boson parameters from the measurements at the Z resonance by the four collaborations ALEPH, DELPHI, L3 and OPAL in e+e- collisions at the large electron positron collider LEP at CERN is a landmark for precision tests of the electroweak theory. The four experiments measured quantities which were used to extract the mass and width of the Z boson, the hadronic cross-section at the pole of the resonance, the ratio of hadronic and leptonic decay widths, and the leptonic forward-backward asymmetries at the pole. The combination procedure based on these parameters is presented in this paper.']",['2001-01-19']
347,['eng'],"['Nandakumar, R']",['Colour Reconnection at LEP2'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'quark, final-state interaction', 'color, singlet', 'charged particle, multiplicity', 'particle flow', 'numerical calculations', 'interpretation of experiments, CERN LEP Stor', '183-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101026'],['Colour reconnection is the final state interaction between quarks from different sources. It is not yet fully understood and is a source of systematic error for W-boson mass and width measurements in hadronic \\WW decays at LEP2. The methods of measuring this effect and the results of the 4 LEP experiments at $183\\gev\\leq\\rts\\leq 202\\gev$ will be presented.'],['2001-01-19']
348,['eng'],"['Acciarri, M', 'Achard, P', 'Adriani, O', 'Aguilar-Benítez de Lugo, M', 'Alcaraz, J', 'Alemanni, G', 'Allaby, James V', 'Aloisio, A', 'Alviggi, M G', 'Ambrosi, G', 'Anderhub, H', 'Andreev, V P', 'Angelescu, T', 'Anselmo, F', 'Arefev, A', 'Azemoon, T', 'Aziz, T', 'Bagnaia, P', 'Bajo, A', 'Baksay, L', 'Balandras, A', 'Baldew, S V', 'Todorova-Nová, S', 'Banerjee, Sw', 'Barczyk, A', 'Barillère, R', 'Bartalini, P', 'Basile, M', 'Batalova, N', 'Battiston, R', 'Bay, A', 'Becattini, F', 'Becker, U', 'Behner, F', 'Bellucci, L', 'Berbeco, R', 'Berdugo, J', 'Berges, P', 'Bertucci, B', 'Betev, B L', 'Bhattacharya, S', 'Biasini, M', 'Biland, A', 'Blaising, J J', 'Blyth, S C', 'Bobbink, Gerjan J', 'Böhm, A', 'Boldizsar, L', 'Borgia, B', 'Bourilkov, D', 'Bourquin, Maurice', 'Braccini, S', 'Branson, J G', 'Brochu, F', 'Buffini, A', 'Buijs, A', 'Burger, J D', 'Burger, W J', 'Cai, X D', 'Capell, M', 'Cara Romeo, G', 'Carlino, G', 'Cartacci, A M', 'Casaus, J', 'Castellini, G', 'Cavallari, F', 'Cavallo, N', 'Cecchi, C', 'Cerrada, M', 'Cesaroni, F', 'Chamizo-Llatas, M', 'Chang, Y H', 'Chaturvedi, U K', 'Chemarin, M', 'Chen, A', 'Chen, G', 'Chen, G M', 'Chen, H F', 'Chen, H S', 'Chiefari, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Civinini, C', 'Clare, I', 'Clare, R', 'Coignet, G', 'Colino, N', 'Costantini, S', 'Cotorobai, F', 'de la Cruz, B', 'Csilling, Akos', 'Cucciarelli, S', 'Dai, T S', 'van Dalen, J A', ""D'Alessandro, R"", 'De Asmundis, R', 'Déglon, P L', 'Degré, A', 'Deiters, K', 'Della Volpe, D', 'Delmeire, E', 'Denes, P', 'De Notaristefani, F', 'De Salvo, A', 'Diemoz, Marcella.', 'Dierckxsens, M', 'Van Dierendonck, D N', 'Dionisi, C', 'Dittmar, Michael', 'Dominguez, A', 'Doria, A', 'Dova, M T', 'Duchesneau, D', 'Dufournaud, D', 'Duinker, P', 'El-Mamouni, H', 'Engler, A', 'Eppling, F J', 'Erné, Frits C', 'Ewers, A', 'Extermann, Pierre', 'Fabre, M', 'Falagán, M A', 'Falciano, S', 'Favara, A', 'Fay, J', 'Fedin, O', 'Felcini, Marta', 'Ferguson, T', 'Fesefeldt, H S', 'Fiandrini, E', 'Field, J H', 'Filthaut, F', 'Fisher, P H', 'Fisk, I', 'Forconi, G', 'Freudenreich, Klaus', 'Furetta, C', 'Galaktionov, Yu', 'Ganguli, S N', 'García-Abia, P', 'Gataullin, M', 'Gau, S S', 'Gentile, S', 'Gheordanescu, N', 'Giagu, S', 'Gong, Z F', 'Grenier, G', 'Grimm, O', 'Grünewald, M W', 'Guida, M', 'van Gulik, R', 'Gupta, V K', 'Gurtu, A', 'Gutay, L J', 'Haas, D', 'Hasan, A', 'Hatzifotiadou, D', 'Hebbeker, T', 'Hervé, Alain', 'Hidas, P', 'Hirschfelder, J', 'Hofer, H', 'Holzner, G', 'Hoorani, H', 'Hou, S R', 'Hu, Y', 'Iashvili, I', 'Jin, B N', 'Jones, L W', 'de Jong, P', 'Josa-Mutuberria, I', 'Khan, R A', 'Käfer, D', 'Kaur, M', 'Kienzle-Focacci, M N', 'Kim, D', 'Kim, J K', 'Kirkby, Jasper', 'Kiss, D', 'Kittel, E Wolfram', 'Klimentov, A', 'König, A C', 'Kopal, M', 'Kopp, A', 'Koutsenko, V F', 'Kräber, M H', 'Krämer, R W', 'Krenz, W', 'Krüger, A', 'Kunin, A', 'Ladrón de Guevara, P', 'Laktineh, I', 'Landi, G', 'Lebeau, M', 'Lebedev, A', 'Lebrun, Philippe.', 'Lecomte, P', 'Lecoq, P', 'Le Coultre, P', 'Lee, H J', 'Le Goff, J M', 'Leiste, R', 'Levchenko, P M', 'Li Chuan', 'Likhoded, S A', 'Lin, C H', 'Lin, W T', 'Linde, F L', 'Lista, L', 'Liu, Z A', 'Lohmann, W', 'Longo, E', 'Lü, Y S', 'Lübelsmeyer, K', 'Luci, C', 'Luckey, D', 'Lugnier, L', 'Luminari, L', 'Lustermann, W', 'Ma, W G', 'Maity, M', 'Malgeri, L', 'Malinin, A', 'Maña, C', 'Mangeol, D J', 'Mans, J', 'Marian, G', 'Martin, J P', 'Marzano, F', 'Mazumdar, K', 'McNeil, R R', 'Mele, S', 'Merola, L', 'Meschini, M', 'Metzger, W J', 'Von der Mey, M', 'Mihul, A', 'Milcent, H', 'Mirabelli, G', 'Mnich, J', 'Mohanty, G B', 'Moulik, T', 'Muanza, G S', 'Muijs, A J M', 'Musicar, B', 'Musy, M', 'Napolitano, M', 'Nessi-Tedaldi, F', 'Newman, H', 'Niessen, T', 'Nisati, A', 'Nowak, H', 'Ofierzynski, R A', 'Organtini, G', 'Oulianov, A', 'Palomares, C', 'Pandoulas, D', 'Paoletti, S', 'Paolucci, P', 'Paramatti, R', 'Park, H K', 'Park, I H', 'Passaleva, G', 'Patricelli, S', 'Paul, T', 'Pauluzzi, M', 'Paus, C', 'Pauss, Felicitas', 'Pedace, M', 'Pensotti, S', 'Perret-Gallix, D', 'Petersen, B', 'Piccolo, D', 'Pierella, F', 'Pieri, M', 'Piroué, P A', 'Pistolesi, E', 'Plyaskin, V', 'Pohl, M', 'Pozhidaev, V', 'Postema, H', 'Pothier, J', 'Prokofiev, D O', 'Prokofev, D', 'Quartieri, J', 'Rahal-Callot, G', 'Rahaman, M A', 'Raics, P', 'Raja, N', 'Ramelli, R', 'Rancoita, P G', 'Ranieri, R', 'Raspereza, A V', 'Raven, G', 'Razis, P A', 'Ren, D', 'Rescigno, M', 'Reucroft, S', 'Riemann, S', 'Riles, K', 'Rodin, J', 'Roe, B P', 'Romero, L', 'Rosca, A', 'Rosier-Lees, S', 'Roth, S', 'Rosenbleck, C', 'Roux, B', 'Rubio, Juan Antonio', 'Ruggiero, G', 'Rykaczewski, H', 'Saremi, S', 'Sarkar, S', 'Salicio, J', 'Sánchez, E', 'Sanders, M P', 'Schäfer, C', 'Shchegelskii, V', 'Schmidt-Kärst, S', 'Schmitz, D', 'Schopper, Herwig Franz', 'Schotanus, D J', 'Schwering, G', 'Sciacca, C', 'Seganti, A', 'Servoli, L', 'Shevchenko, S', 'Shivarov, N', 'Shoutko, V', 'Shumilov, E', 'Shvorob, A V', 'Siedenburg, T', 'Son, D', 'Smith, B', 'Spillantini, P', 'Steuer, M', 'Stickland, D P', 'Stone, A', 'Stoyanov, B', 'Strässner, A', 'Sudhakar, K', 'Sultanov, G G', 'Sun, L Z', 'Sushkov, S V', 'Suter, H', 'Swain, J D', 'Szillasi, Z', 'Sztaricskai, T', 'Tang, X W', 'Tauscher, Ludwig', 'Taylor, L', 'Tellili, B', 'Teyssier, D', 'Timmermans, C', 'Ting, S C C', 'Ting, S M', 'Tonwar, S C', 'Tóth, J', 'Tully, C', 'Tung, K L', 'Uchida, Y', 'Ulbricht, J', 'Valente, E', 'Vesztergombi, György', 'Vetlitskii, I', 'Vicinanza, D', 'Viertel, Gert M', 'Villa, S', 'Vivargent, M', 'Vlachos, S', 'Vodopyanov, I', 'Vogel, H', 'Vogt, H', 'Vorobev, I', 'Vorobyov, A A', 'Vorvolakos, A', 'Wadhwa, M', 'Wallraff, W', 'Wang, M', 'Wang, X L', 'Wang, Z M', 'Weber, A', 'Weber, M', 'Wienemann, P', 'Wilkens, H', 'Wu, S X', 'Wynhoff, S', 'Xia, L', 'Xu, Z Z', 'Yamamoto, J', 'Yang, B Z', 'Yang, C G', 'Yang, H J', 'Yang, M', 'Ye, J B', 'Yeh, S C', 'Zalite, A', 'Zalite, Yu', 'Zhang, Z P', 'Zhu, G Y', 'Zhu, R Y', 'Zichichi, Antonino', 'Zilizi, G', 'Zimmermann, B', 'Zöller, M']",['Measurement of the Charm Production Cross Section in gamma gamma Collisions at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'quark, charm', 'quark, pair production', 'channel cross section, energy dependence', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2charm positron electron', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101025'],['Open charm production in gamma-gamma collisions is studied with data collected at e+e- centre-of-mass energies from 189 GeV to 202 GeV corresponding to a total integrated luminosity of 410 pb-1. The charm cross section sigma(gamma gamma ---> c c~ X) is measured for the first time as a function of the two-photon centre-of-mass energy in the interval from 5 GeV to 70 GeV and is compared to NLO QCD calculations.'],['2001-01-19']
349,['eng'],"['Kaplan, D M']",['Prospects for low-energy antiproton physics at Fermilab'],['Particle Physics - Experimental Results'],"['talk, Venice 2000/08/20', 'anti-p p, interaction', 'anti-p, particle source', 'violation, CP', 'hyperon, hadroproduction', 'hyperon, pair production', 'Lambda, hadronic decay', 'Xi-, cascade decay', 'hyperon, rare decay', 'quarkonium, charm', 'meson, hybrid', 'proposed experiment, Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101024'],"[""Fermilab has long had the world's most intense antiproton source, but the opportunities for medium-energy antiproton physics have been limited, and those for low-energy antiproton physics nonexistent. The conclusion of E835 brings this era to an end. While the future of antiproton physics at Fermilab remains highly uncertain, developments are occurring that may lead to a low-energy program within the next several years, with the possibility of an improved medium-energy program thereafter. These issues were considered at the recent $\\bar{p}2000$ Workshop at Illinois Institute of Technology. I summarize the current status of the Fermilab antiproton facility, review hyperon {\\em CP} violation as an example of the physics that might be achievable, and discuss future possibilities.""]",['2001-01-18']
350,['eng'],"['Hilgers, M', 'Horisberger, R P']",['Development of a radiation hard version of the Analog Pipeline Chip APC128'],['Particle Physics - Experimental Results'],"['semiconductor detector, vertex', 'semiconductor detector, microstrip', 'electronics, readout', 'integrated circuit', 'electronics, amplifier', 'electronics, background', 'electronics, analog', 'magnetic detector, H1', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101023'],"['The Analog Pipeline Chip (APC) is a low noise, low power readout chip for silicon micro strip detectors with 128 channels containing an analog pipeline of 32 buffers depth. The chip has been designed for operation at HERA with a power dissipation of 300-400 muW per channel and has been used also in several other particle physics experiments. In this paper we describe the development of a radiation hard version of this chip that will be used in the H1 vertex detector for operation at the luminosity upgraded HERA machine. A 128 channel prototyping chip with several amplifier variations has been designed in the radiation hard DMILL technology and measured. The results of various parameter variations are presented in this paper. Based on this, the design choice for the final production version of the APC128-DMILL has been made.']",['2001-01-18']
351,['eng'],"['Bravo, S']",['New results on alpha_s and optimized scales'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'event shape analysis', 'strong interaction, coupling constant', 'jet, multiplicity', 'final state, (4jet)', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101022'],['A summary of the latest alpha_s results at LEP1 and LEP2 from event-shape predictions at Order(alpha2_s) + NLLA is presented. Later these are compared to measurements obtained using the Experimentally Optimized Scale method. Finally the alpha_s measurement from the 4-jet rate is discussed.'],['2001-01-18']
352,['eng'],"['Satpathy, A']",['First Physics Results From Belle'],['Particle Physics - Experimental Results'],"['talk, Prerow 2000/10/01', 'talk, Carmel 2000/09/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, decay modes', 'B, branching ratio', 'Kobayashi-Maskawa angle', 'violation, CP', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', '10.57 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101021', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']","['The Belle detector at the KEK-B asymmetric $e^{+}e^{-}$ collider has recorded 6.2 fb$^{-1}$ data at the $\\Upsilon(4S)$ resonance by July 2000. Using this data sample, several new results on various B meson branching ratio measurements are presented. We also report on the measurement of the Standard Model CP violation parameter $\\sin(2\\phi_{1})$, where $\\phi_{1}$ is one of angles of the CKM triangle. The preliminary result is $\\sin(2\\phi_{1})$ = $0.45^{+0.43 \\pm 0.07}_{-0.44 \\pm 0.08}$.']",['2001-01-18']
353,['eng'],"['Battaglia, M', 'Caccia, M', 'Borghi, S', 'Campagnolo, R', 'Kucewicz, W', 'Palka, H', 'Zalewska, Agnieszka']",['Hybrid pixel detector development for the Linear collider Vertex Detector'],['Particle Physics - Experimental Results'],"['talk, Lyon 2000/10/15', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'spatial resolution', 'electron positron, colliding beam detector', 'electron positron, linear collider', 'linear collider, proposed']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101020'],"['In order to fully exploit the Physics potential of future e+ e- linear collider, a Vertex Detector providing high resolution track reconstruction is required. Hybrid Silicon pixel detectors are an attractive option for the sensor technology due to their read-out speed and radiation hardness but have been so far limited by the achievable single point resolution. A novel layout of hybrid pixel sensor with interleaved cells to improve the spatial resolution has been developed. The characterisation of the first processed prototypes is reported.']",['2001-01-17']
354,['eng'],"['Spurio, M']",['MACRO and the atmospheric neutrino problem'],['Particle Physics - Experimental Results'],"['talk, Faro 2000/09/01', 'neutrino, cosmic radiation', 'neutrino/mu, flux', 'neutrino/mu, energy spectrum', 'neutrino, oscillation', 'neutrino nucleus, interaction', 'charged current', 'muon, angular distribution', 'neutrino, sterile', 'MSW effect', 'deep underground detector, MACRO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101019'],"['After a brief presentation of the MACRO detector we discuss the updated data on atmospheric muon neutrinos, and the interpretation in terms of neutrino oscillations.']",['2001-01-16']
355,['eng'],"['Wong, H T']",['Neutrino Experiments'],['Particle Physics - Experimental Results'],"['talk, Chi-Pen 2000/11/08', 'neutrino, solar', 'neutrino, cosmic radiation', 'neutrino, energy spectrum', 'astrophysics', 'neutrino, mass difference', 'neutrino, mixing angle', 'mass, hierarchy', 'neutrino, oscillation', 'fission, particle source', 'double-beta decay', 'neutrino, beam', 'scintillation counter, crystal', 'experimental results', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101018'],"['This article consists of two parts. The first section presents the highlights on the goals of neutrino physics, status of the current neutrino experiments and future directions and program. The second section describes the theme, program and research efforts for the TEXONO Collaboration among scientists from Taiwan and China.']",['2001-01-16']
356,['eng'],"['Popp, J L']",['The MECO experiment'],['Particle Physics - Experimental Results'],"['talk, Monterey 2000/05/22', 'muon nucleus, capture', 'muonic atom', 'transition, muon electron', 'electron, energy', 'violation, flavor', 'muon nucleus, interaction', 'charged current', 'cross section, ratio', 'upper limit', 'magnet, superconducting', 'drift chamber, drift tube', 'experimental results', 'Brookhaven PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101017'],"['MECO will search for direct evidence of muon and electron flavor violation in the decay of muons in Coulomb bound states via coherent recoil of the nucleus and decay electron. The expected sensitivity to the $\\mu^{-} {\\rm N} \\to e^{-} + {\\rm N}$ branching fraction relative to muon capture $\\mu^{-} {\\rm N}(A,Z) \\to \\nu_{\\mu} + {\\rm N}(A,Z-1)$ is $R_{\\mu e} < 5\\times 10^{-17}$ at 90% confidence level, roughly three to four orders of magnitude lower than current limits. This article provides an overview of the experiment.']",['2001-01-16']
357,['eng'],"['Wynhoff, S']",['Standard Model Physics Results from LEP2'],['Particle Physics - Experimental Results'],"['talk, Carmel 2000/09/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'electroweak interaction, validity test', 'fermion, pair production', 'angular distribution, asymmetry', 'interference, (Z0 photon)', 'new interaction, search for', 'W, electroproduction', 'intermediate boson, pair production', 'W, decay modes', 'W, branching ratio', 'Kobayashi-Maskawa angle', 'W, mass', 'W, width', 'Higgs particle, mass', 'experimental results', 'CERN LEP Stor']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101016', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']","['At LEP2 many Standard Model predictions are tested up to centre-of-mass energies of 209 GeV. Fermion pair production cross sections and asymmetries agree well with the theoretical expectation over the entire energy range. The measurements are used to determine the gamma/Z interference and to search for contact interactions up to 20 TeV. The cross sections for single-W, ZZ and W+W- production agree well with the expectations. The branching fractions of the W boson into hadrons and leptons are determined as well as the CKM matrix element |V_{cs}|. Precise measurements of the W mass and width are presented yielding MW=80.427+-0.046 GeV and GammaW=2.12=_0.11 GeV. All electroweak data are very consistent with the Standard Model predictions. In a combined fit using the recent value of Delta alpha_{had}^(5)(s) the mass of the Higgs boson is constrained to MH=88^{+60}_{-37} GeV.']",['2001-01-15']
358,['eng'],"['Junk, T R']",['Searches at LEP'],['Particle Physics - Experimental Results'],"['talk, Carmel 2000/09/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'Higgs particle, multiplet', 'supersymmetry', 'gaugino', 'squark, truth', 'stau', 'photon, recoil', 'energy spectrum', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, mass', 'Higgs particle, decay modes', 'experimental results', 'CERN LEP Stor', 'approx. 206 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101015', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']","['Searches have been conducted for a broad range of new phenomena by the four experiments ALEPH, DELPHI, L3, and OPAL, at LEP2. Each experiment contributes approximately 150 pb-1 of e+e- annihilation data with a mean sqrt(s) of 205.9 GeV in 2000 to these searches (data prepared for the September 5 LEPC meeting). The statistical procedure for setting limits and evaluating the significance of excesses observed in the data is reviewed. Search results are presented for the Standard Model Higgs boson, the neutral Higgs bosons in the MSSM, charged Higgs bosons, invisibly decaying Higgs bosons produced by Higgs-strahlung, and fermiophobic Higgs bosons. Search results are briefly summarized for gauginos, stops, and staus. The photon recoil spectrum is checked for hints of new physics.']",['2001-01-12']
359,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Couchman, J', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Sen-Gupta, A', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kamer, T', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pahl, C', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Spanó, F', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Tasevsky, M', 'Taylor, R J', 'Teuscher, R J', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vollmer, C F', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for the Standard Model Higgs Boson in $e^{+}e^{-}$ Collisions at $\\sqrt{s}$ = 192-209 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, leptonic decay', 'Higgs particle, hadronic decay', 'Z0, leptonic decay', 'Z0, hadronic decay', 'Higgs particle, mass', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'Higgs particle --> 2beauty', 'Higgs particle --> tau+ tau-', '179-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101014'],"['A search for the Standard Model Higgs boson has been performed with the OPAL detector at LEP based on the full data sample collected at sqrt(s) = 192-209 GeV in 1999 and 2000, corresponding to an integrated luminosity of approximately 426 pb-1. The data are examined for their consistency with the background-only hypothesis and various Higgs boson mass hypotheses. A lower bound of 109.7 GeV is obtained on the Higgs boson mass at the 95% confidence level. At higher masses, the data are consistent with both the background and the signal-plus-background hypotheses.']",['2001-01-12']
360,['eng'],"['Zhao, X']",['Measurement of Vcb and Charmless Hadronic B decays at CLEO'],['Particle Physics - Experimental Results'],"['review, Carmel 2000/09/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'Kobayashi-Maskawa angle, unitarity', 'Feynman graph, penguin', 'asymmetry, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.57 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101013', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']",['The recent results on the measurement of Vcb and charmless hadronic B decays from CLEO are presented.'],['2001-01-11']
361,['eng'],"['Caccia, M', 'Campagnolo, R', 'Battaglia, M', 'Kucewicz, W', 'Palka, H', 'Zalewska, Agnieszka', 'Domanski, K', 'Marczewski, J', 'Tomaszewski, D']",['Characterisation of Hybrid Pixel Detectors with capacitive charge division'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/24', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'spatial resolution', 'electron positron, colliding beam detector', 'electron positron, linear collider', 'linear collider, proposed']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101012'],"['In order to fully exploit the physics potential of the future high energy e+ e- linear collider, a Vertex Tracker providing high resolution track reconstruction is required. Hybrid pixel sensors are an attractive technology due to their fast read-out capabilities and radiation hardness. A novel pixel detector layout with interleaved cells between the readout nodes has been developed to improve the single point resolution. The results of the characterisation of the first processed prototypes are reported.']",['2001-01-11']
362,['eng'],"['Caccia, M']",['The challenge of hybridization'],['Particle Physics - Experimental Results'],"['talk, Genova 2000/06/05', 'semiconductor detector, pixel', 'semiconductor detector, vertex', 'electronics, wire', 'integrated circuit', 'magnetic detector, DELPHI', 'CERN LEP Stor', 'CERN LHC Coll', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101011'],"['Hybridization of pixel detector systems has to satisfy tight requirements: high yield, long term reliability, mechanical stability, thermal compliance and robustness have to go together with low passive mass added to the system, radiation hardness, flexibility in the technology end eventually low cost. The current technologies for the interconnection of the front-end chips and the sensor are reviewed and compared, together with the solutions for the interface to the far-end electronics.']",['2001-01-11']
363,['eng'],"['Trigger, I']",['Constraining CP-Violating TGCs and Measuring W-Polarization at OPAL'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'W, polarization', 'spin, density matrix', 'helicity, amplitude analysis', 'coupling, (3gauge boson)', 'violation, CP', 'numerical calculations', '189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101010'],['A measurement of the polarization of W bosons in semi-leptonically decaying W pairs produced at 189 GeV is presented. Rates of longitudinally and transversely polarized W bosons and correlation between two W bosons are studied. The spin properties of the leptonically decaying W boson in the W pairs was used to measure the CP-violating trilinear gauge boson couplings. These results are compared with Standard Model expectations.'],['2001-01-11']
364,['eng'],"['Vossebeld, J H']",['Recent Results on Particle Production from OPAL'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, electroproduction', 'quark, jet', 'gluon, jet', 'jet, fragmentation', 'dependence, flavor', 'charged particle, multiplicity', 'neutral particle, multiplicity', 'effect, leading particle', 'yield, strangeness', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101009'],"['Three recent OPAL studies are presented in which the fragmentation process in quark and gluon jets and in identified up, down and strange flavour jets is studied. The first is a measurement is of charged particle, pi0, eta and K0 multiplicities in quark and gluon jets. No evidence is found for a particle species dependent multiplicity enhancement in gluon jets. In another study leading pion, kaon, K0, proton and lambda rates have been measured in up, down and strange flavour jets. The results confirm the leading particle effect in the fragmentation of light flavour jets. In addition a direct determination of the strangeness suppression factor has been performed, yielding gamma_s=0.422 +/- 0.049(stat.) +/- 0.059(syst.). In a third study mean charged particle multiplicities were measured for up, down and strange flavoured Z0 decays and found to be identical within the uncertainties of the measurement, as expected from the flavour independence of the strong interaction.']",['2001-01-11']
365,['eng'],"['Przysiezniak, H']",['Precision Electroweak Measurements'],['Particle Physics - Experimental Results'],"['review, Quebec City 2000/05/22', 'electroweak interaction, validity test', 'Higgs particle, mass', 'electron positron, colliding beams', 'electron positron, annihilation', 'anti-p p, colliding beams', 'Z0, electroproduction', 'neutrino nucleon, interaction', 'electron, polarized beam', 'polarization, asymmetry', 'Z0, mass', 'Z0, width', 'Z0, decay modes', 'tau, polarization', 'Weinberg angle', 'fermion, pair production', 'W, pair production', 'W, decay modes', 'coupling, (3gauge boson)', 'W, mass', 'W, width', 'mass, truth', 'muon, magnetic moment', 'atomic physics, parity', 'experimental results', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101008'],"['This talk describes some of the precision electroweak measurements from around the world, namely those related to the Z and W bosons, the top quark mass, sin2 theta_ W at NuTeV, and three other fundamental measurements: alpha-1 m2_ Z, (g-2)_mu at the E821 BNL experiment as well as the atomic parity violation (APV) measurement for the Cesium atom. These and other measurements are set in the context of the Standard Model (SM) and of the electroweak fit predictions. Future prospects for forthcoming experiments are briefly discussed.']",['2001-01-11']
366,['eng'],"['Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Park, W', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J']",['Bounds on the CP Asymmetry in Like-Sign Dileptons from $B^{0}\\bar{B}^{0}$ Meson Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, semileptonic decay', 'charge, dilepton', 'charge, asymmetry', 'violation, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101006'],"['We have measured the charge asymmetry in like-sign dilepton yields from B^0 B^0-bar meson decays using the CLEO detector at the Cornell Electron Storage Ring. We find a_ll = [N(l+l+) - N(l-l-)]/[N(l+l+) + N[l-l-)] = +0.013 +/- 0.050 +/- 0.005 . We combine this result with a previous, independent measurement and obtain Re(epsilon_B)/(1+|epsilon_B|^2) = +0.0035 +/- 0.0103 +/- 0.0015 (uncertainties are statistical and systematic, respectively) for the CP impurity parameter, epsilon_B.']",['2001-01-09']
367,['eng'],"['Mönig, K']",['What is the Case for a Return to the Z-Pole?'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/24', 'electron positron, linear collider', 'linear collider, proposed', 'Z0, electroproduction', 'electroweak interaction, validity test', 'electron, polarized beam', 'polarization, asymmetry', 'Z0, decay modes', 'Z0, width', 'coupling constant, axial-vector', 'Weinberg angle', 'W, mass', 'strong interaction, coupling constant', 'vertex function, (Z0 2beauty)', 'B, hadronic decay', 'Higgs particle, multiplet', 'B/s0 anti-B/s0, interference', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101005'],['The possibilities to run with a linear collider at the Z-pole with high luminosity are examined. Apart from the implications on machine and detector the interest for electroweak and B-physics is discussed.'],['2001-01-09']
368,['eng'],"['Sciolla, G']",['The first physics results from BaBar'],['Particle Physics - Experimental Results'],"['talk, Ferrara 2000/09/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'Kobayashi-Maskawa angle, unitarity', 'psi mesons, leptonic decay', 'psi(3685), hadronic decay', 'chi mesons, radiative decay', 'K, hadronic decay', 'particle identification, beauty', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> psi mesons K', 'B --> chi mesons K', '10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101004'],"['The BaBar experiment and the PEP-II accelerator at SLAC started to take data on May 26, 1999. By the time of this conference, the recorded integrated luminosity was 20 fb^{-1}, of which 8 fb^{-1} were analyzed to provide a first set of physics results. This talk reviews the first measurement of sin2beta and the study of B meson decays to charmonium modes and 2-body charmless decays.']",['2001-01-08']
369,['eng'],"['Diwan, M V', 'Ma, H']",['Tests of the Standard Model Using Muon Polarization Asymmetries in Kaon Decays'],['Particle Physics - Experimental Results'],"['K, decay modes', 'muon, polarization', 'electroweak interaction, asymmetry', 'violation, CP', 'Kobayashi-Maskawa angle', 'n, electric moment', 'electron, electric moment', 'time reversal, violation', 'spin, correlation', 'numerical calculations', 'K0(L) --> muon+ muon-', 'K --> pi muon+ muon-', 'K --> pi neutrino antineutrino', 'K+ --> pi0 muon+ neutrino', 'K+ --> muon+ neutrino photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101003'],"['We have examined the physics and the experimental feasibility of studying various kaon decay processes in which the polarization of a muon in the final state is measured. Valuable information on CP violation, the quark mixing (CKM) matrix, and new physics can be obtained from such measurements. We have considered muon polarization in K_L to mu+ mu- and K to pi mu+ mu- decays. Although the effects are small, or difficult to measure because of the small branching ratios involved, these studies could provide clean measurements of the CKM parameters. The experimental difficulty appears comparable to the observation of K to pi nu barnu. New sources of physics, involving non-standard CP violation, could produce effects observable in these measurements. Limits from new results on the neutron and electron electric dipole moment, and epsilon-prime over epsilon in neutral kaon decays, do not eliminate certain models that could contribute to the signal. A detailed examination of muon polarization out of the decay plane in KMU3 and radiative KMU2 decays also appears to be of interest. With current kaon beams and detector techniques, it is possible to measure the T-violating polarization for KMU3 with uncertainties approaching 0.0001. This level of sensitivity would provide an interesting probe of new physics.']",['2001-01-22']
370,['eng'],"['Telnov, V I']",['Photon collider at TESLA'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/24', 'photon photon, colliding beams', 'photon electron, colliding beams', 'luminosity', 'channel cross section', 'electron positron, linear collider', 'linear collider, proposed', 'radiation, laser', 'Compton scattering, backscatter']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101002'],"['Photon colliders (gamma-gamma, gamma-e) are based on backward Compton scattering of laser light off the high energy electrons of linear colliders. Recent study has shown that the gamma-gamma luminosity in the high energy peak can reach 0.3--0.5 L (e+e-). Typical cross sections of interesting processes in gamma-gamma collisions are higher than those in e+e- collisions by about one order of magnitude, so the number of events in gamma-gamma collisions will be more than that in e+e- collisions. In this paper possible parameters of a photon collider at TESLA and a laser scheme are briefly discussed.']",['2001-01-22']
371,['eng'],"['Grannis, P D']",['Linear Collider Workshop 2000 Summary'],['Particle Physics - Experimental Results'],"['conference, review', 'Batavia 2000/10/24', 'electron positron, linear collider', 'linear collider, proposed', 'Higgs particle, search for', 'supersymmetry, search for', 'electroweak interaction, validity test', 'electroweak interaction, symmetry breaking', 'strong interaction, coupling constant', 'polarized beam', 'photon photon, interaction', 'electron electron, interaction', 'free electron laser']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101001'],"['We summarize some of the main physics questions that will serve to define the linear e+e- collider program, and comment on issues that confront the world community in making such a collider a reality.']",['2001-01-22']
372,['eng'],"['Rizvi, E', 'Sloan, Terence']",['xF3 (gamma-Z) in Charged Lepton Scattering'],['Particle Physics - Experimental Results'],"['lepton nucleon, deep inelastic scattering', 'neutrino nucleon, deep inelastic scattering', 'neutral current', 'nucleon, structure function', 'x-dependence', 'sum rule', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0101007'],['Measurements of the structure function xF3(gamma-Z) are now becoming available in charged lepton deep inelastic scattering at HERA. The correction factors which are necessary to compare these with measurements of xF3(nu N) in neutrino-nucleon scattering are deduced and a comparison is made between the H1 and the CCFR data. A sum rule is derived for the structure function xF3(gamma-Z)measured in charged lepton scattering which is the analogue of the Gross Llewellyn-Smith sum rule for neutrino-nucleon scattering.'],['2001-01-10']
373,['eng'],"['Schilling, F P']",['Diffractive Dijet and 3-Jet Electroproduction at HERA'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'diffraction', 'jet, multiple production', 'final state, (2jet)', 'final state, (3jet)', 'rapidity, gap', 'pomeron, resolved', 'gluon, momentum spectrum', 'quantum chromodynamics, perturbation theory', 'differential cross section', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012065'],"['A new H1 measurement of diffractive dijet and 3-jet production cross sections in diffractive deep inelastic scattering events of the type ep->eXY is presented. The data constrain well the diffractive gluon distribution. At low x-pom, a calculation based on perturbative QCD is in a reasonable agreement with the data.']",['2000-12-29']
374,['eng'],"['Weinstein, A J']",['Semi-hadronic Tau Decays at CLEO'],['Particle Physics - Experimental Results'],"['talk, Victoria 2000/09/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'pi, multiple production', 'CVC model', 'mass spectrum, ((n)pi)', 'amplitude analysis', 'meson resonance', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012064'],"[""This contribution reviews several new or updated results on substructure in semi-hadronic tau decays, recently published by the CLEO Collaboration. These results are all based on data collected with the CLEO detector at Cornell's CESR collider, in the reaction $e^+e^-\\to \\tau^+\\tau^-$ at $\\sqrt{s} \\simeq 10.6$ GeV. Most of these results are based on $\\approx 4.3\\times 10^6$ $\\tau^+\\tau^-$ pairs collected with the CLEO II detector between 1990 --- 1995. Some (where noted) also use $\\approx 8.0\\times 10^6$ $\\tau^+\\tau^-$ pairs collected with the CLEO II.V detector (which includes a silicon vertex detector and better drift chamber tracking) between 1995 --- 1999.""]",['2000-12-28']
375,['eng'],"['Moinester, M A']",['Pion Polarizabilities and Hybrid Meson Structure at CERN COMPASS'],['Particle Physics - Experimental Results'],"['talk, Newport News 2000/12/01', 'photon pi, interaction', 'pi, polarizability', 'K, polarizability', 'Primakoff effect', 'meson, photoproduction', 'meson, hybrid', 'calorimeter, electromagnetic', 'trigger', 'proposed experiment, CERN SPS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012063'],[],['2000-12-26']
376,['eng'],"['Gayler, J']",['Jet Production in DIS at HERA'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'jet, multiple production', 'quantum chromodynamics, perturbation theory', 'angular distribution', 'differential cross section, x-dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012062'],['Data on jet production in deep inelastic e^+ p scattering are presented. The results are compared with pQCD calculations. At low Q^2 no consistent description of the data over all the phase space is available yet. At high Q^2 (>150 GeV^2) the data are well described by pQCD in NLO.'],['2000-12-26']
377,['eng'],"['Womesrley, J']",['QCD at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Carmel 2000/09/11', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'final state, (2jet)', 'final state, (3jet)', 'strong interaction, coupling constant', 'cross section, ratio', 'quantum chromodynamics', 'intermediate boson, hadroproduction', 'Z0, transverse momentum', 'photon, direct production', 'differential cross section, transverse momentum', 'transverse energy, dependence', 'quark, beauty', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> (n)jet anything', 'anti-p p --> intermediate boson anything', 'anti-p p --> W (n)jet anything', '630, 1800 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012061', 'http://www.slac.stanford.edu/econf/C000911/proceedings.html']","['I shall review the present status of Tevatron QCD studies, focusing on the production of jets, vector bosons, photons and heavy quarks. In general there is good agreement between the results of current calculational tools and the experimental data. The major areas of discrepancy arise when the input parton distributions become uncertain (for example, jets at high $E_T$) or when the momentum scales become relatively small (for example, $b$ production at low $p_T$). We can look forward to continued improvement in both calculations and measurements over the next decade. However, fully exploiting the power of the data will require considerable work, both from the experimentalists who must understand and publish all the systematic errors and their correlations, and from the phenomenologists who must understand the level of uncertainty in their calculations and in the parton distributions.']",['2000-12-25']
378,['eng'],"['Jain, V']",['Rare $K^{+}$ Decays from Experiment E787'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'K+, rare decay', 'K+, semileptonic decay', 'K+, radiative decay', 'at rest', 'K+, branching ratio', 'scintillation counter, plastics', 'experimental results', 'proposed experiment', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino', 'K+ --> muon+ neutrino/mu photon', 'K+ --> pi+ pi0 photon', '0 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012060'],"['This paper presents the latest results from experiment E787, at Brookhaven National Laboratory, on K+ -> pi nu/nubar and radiative K+ decays. The result for K+ -> pi nu/nubar uses data collected in runs taken during 1995, 1996 and 1997. In addition, we discuss plans for future measurements of K+ -> pi nu/nubar.']",['2000-12-25']
379,['eng'],"['Muheim, F']",['Status of the LHCb Experiment'],['Particle Physics - Experimental Results'],"['talk, Maagan 2000/09/13', 'semiconductor detector, vertex', 'semiconductor detector, microstrip', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'carbon, fluorine', 'aerogel', 'calorimeter, energy resolution', 'lead', 'iron', 'scintillation counter', 'trigger', 'magnetic detector, LHC-B', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012059'],"['We present the status of the LHCb experiment which will make precision measurements of CP violation in $B$ meson decays. The motivation for the experiment and an overview of the detector design are given. The vertex detector, ring imaging Cherenkov counter, calorimeters, and trigger systems are discussed in detail. We also present the expected physics performance for selected modes.']",['2000-12-25']
380,['eng'],"['Muheim, F']",['Multianode Photo Multipliers for Ring Imaging Cherenkov Detectors'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'photoelectron, amplifier', 'magnetic detector, LHC-B', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012058'],['The 64-channel Multianode Photo Multiplier has been evaluated as a possible choice for the photo detectors of the LHCb Ring Imaging Cherenkov detector.'],['2000-12-25']
381,['eng'],"['Rowson, P C', 'Woods, M']",['Experimental Issues for Precision Electroweak Physics at a High-Luminosity Z Factory'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/24', 'electron positron, linear collider', 'linear collider, proposed', 'luminosity, high', 'electron positron, annihilation', 'Z0, electroproduction', 'electron, polarized beam', 'positron, polarized beam', 'polarization, asymmetry', 'polarization, measurement', 'Weinberg angle', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012055'],"['We discuss the ultimate precision for ALR, and therefore for the weak mixing angle, at a high-luminosity Linear Collider. Drawing on our experience at the SLC, and considering various machine parameter sets for the NLC and for TESLA, it emerges that a compromise between peak luminosity and precision will be a likely outcome. This arises due to the severe requirements on the uncertainty in the luminosity weighted collision energy (Ecm). We consider the cases with and without a polarized positron beam.']",['2000-12-22']
382,['eng'],"['Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Borum, L D', 'Gramaglia, M', 'Jaffe, D E', 'Mahapatra, R', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R']","['Search for CP Violation in $D^{0}\\to K_{S}^{0}\\pi^{0}$, $D^{0}\\to \\pi^{0}\\pi^{0}$ and $D^{0}\\to K_{S}^{0}K_{S}^{0}$']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'particle identification, flavor', 'D0, hadronic decay', 'anti-D0, hadronic decay', 'violation, CP', 'meson, pair production', 'K0(S)', 'pi0', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D*(2010) --> D0 pi', 'D0 --> K0(S) pi0', 'D0 --> 2pi0', 'D0 --> 2K0(S)', '10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012054'],"['We have searched for CP-violating asymmetries in neutral charm meson decays in 13.7 fb^-1 of e^+e^- collision data at sqrt{s} = 10.6 GeV with the CLEO detector. The measured asymmetries in the rate of D0 and D0bar decays to K0sPi0, Pi0Pi0 and K0sK0s final states are (+0.1 +- 1.3)%, (+0.1 +- 4.8)% and (-23 +- 19)%, respectively.']",['2000-12-22']
383,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Anthonis, T', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bahr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, B', 'Brown, D P', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coppens, Y R', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Fleming, Y H', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Glazov, A', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hildebrandt, M', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Koutouev, R', 'Koutov, A', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebailly, E', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'List, B', 'Lobodzinska, E', 'Lobodzinski, B', 'Loginov, A', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, A B', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Risler, C', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schmitt, S', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Schwanenberger, C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Tsurin, I', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vasilev, S', 'Vazdik, Ya', 'Vichnevski, A', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Deep-Inelastic Inclusive ep Scattering at Low x and a Determination of $\\alpha_{s}$'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'small-x', 'neutral current', 'differential cross section', 'p, structure function', 'structure function, longitudinal', 'momentum transfer, dependence', 'Altarelli-Parisi equation', 'quantum chromodynamics, perturbation theory', 'gluon, momentum spectrum', 'strong interaction, coupling constant', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012053'],"['A precise measurement of the inclusive deep-inelastic e^+p scattering cross section is reported in the kinematic range 1.5<= Q^2 <=150 GeV^2 and 3*10^(-5)<= x <=0.2. The data were recorded with the H1 detector at HERA in 1996 and 1997, and correspond to an integrated luminosity of 20 pb^(-1). The double differential cross section, from which the proton structure function F_2(x,Q^2) and the longitudinal structure function F_L(x,Q^2) are extracted, is measured with typically 1% statistical and 3% systematic uncertainties. The measured partial derivative (dF_2(x,Q^2)/dln Q^2)_x is observed to rise continuously towards small x for fixed Q^2. The cross section data are combined with published H1 measurements at high Q^2 for a next-to-leading order DGLAP QCD analysis.The H1 data determine the gluon momentum distribution in the range 3*10^(-4)<= x <=0.1 to within an experimental accuracy of about 3% for Q^2 =20 GeV^2. A fit of the H1 measurements and the mu p data of the BCDMS collaboration allows the strong coupling constant alpha_s and the gluon distribution to be simultaneously determined. A value of alpha _s(M_Z^2)=0.1150+-0. 0017 (exp) +0.0009-0.0005 (model) is obtained in NLO, with an additional theoretical uncertainty of about +-0.005, mainly due to the uncertainty of the renormalisation scale.']",['2000-12-22']
384,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Anthonis, T', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bahr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, B', 'Brown, D P', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coppens, Y R', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Dubak, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Fleming, Y H', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hildebrandt, M', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Kjellberg, P', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Koutouev, R', 'Koutov, A', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Laycock, P', 'Lebailly, E', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'List, B', 'Lobodzinska, E', 'Lobodzinski, B', 'Loginov, A', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Meyer, A B', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Risler, C', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schmitt, S', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Schwanenberger, C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Tsurin, I', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vasilev, S', 'Vazdik, Ya', 'Vichnevski, A', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Measurement of Neutral and Charged Current Cross Sections in Electron-Proton Collisions at High $Q^{2}$'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'electron p, deep inelastic scattering', 'positron p, deep inelastic scattering', 'charged current', 'neutral current', 'differential cross section, x-dependence', 'momentum transfer, dependence', 'energy spectrum', 'electron, angular distribution', 'p, structure function', 'W, propagator', 'propagator, mass', 'electroweak interaction, validity test', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '320 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012052'],"['The inclusive e^-p single and double differential cross sections for neutral and charged current processes are measured with the H1 detector at HERA, in the range of four-momentum transfer squared Q^2 between 150 and 30000 GeV^2, and Bjorken x between 0.002 and 0.65. The data were taken in 1998 and 1999 with a centre-of-mass energy of 320 GeV and correspond to an integrated luminosity of 16.4 pb^(-1). The data are compared with recent measurements of the inclusive neutral and charged current e^+p cross sections. For Q^2>1000 GeV^2 clear evidence is observed for an asymmetry between e^+p and e^-p neutral current scattering and the generalised structure function xF_3 is extracted for the first time at HERA. A fit to the charged current data is used to extract a value for the W boson propagator mass. The data are found to be in good agreement with Standard Model predictions.']",['2000-12-22']
385,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Anthonis, T', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bahr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Berndt, T', 'Bizot, J C', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coppens, Y R', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Fleming, Y H', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hildebrandt, M', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Kjellberg, P', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Koutouev, R', 'Koutov, A', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Laycock, P', 'Lebailly, E', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'List, B', 'Lobodzinska, E', 'Lobodzinski, B', 'Loginov, A', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Meyer, A B', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Risler, C', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schmitt, S', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Schwanenberger, C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Tsurin, I', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vasilev, S', 'Vazdik, Ya', 'Vichnevski, A', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Diffractive Jet Production in Deep-Inelastic $e^{+}p$ Collisions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, multiple production', 'diffraction', 'rapidity, gap', 'momentum transfer, low', 'differential cross section', 'photon, resolved', 'pomeron, exchange', 'pomeron, structure function', 'exchange, two-gluon', 'gluon, momentum spectrum', 'color, dipole', 'Regge poles', 'energy flow', 'differential cross section', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'tables', 'bibliography', 'positron p --> 2jet positron anything', 'positron p --> 3jet positron anything', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012051'],"['A measurement is presented of dijet and 3-jet cross sections in low-|t| diffractive deep-inelastic scattering interactions of the type ep -> eXY, where the system X is separated by a large rapidity gap from a low-mass baryonic system Y. Data taken with the H1 detector at HERA, corresponding to an integrated luminosity of 18.0 pb^(-1), are used to measure hadron level single and double differential cross sections for 4<Q^2<80 GeV^2 x_pom<0.05 and p_(T,jet)>4 GeV. The energy flow not attributed to jets is also investigated. The measurements are consistent with a factorising diffractive exchange with trajectory intercept close to 1.2 and tightly constrain the dominating diffractive gluon distribution. Viewed in terms of the diffractive scattering of partonic fluctuations of the photon, the data require the dominance of qqbarg over qqbar states. Soft colour neutralisation models in their present form cannot simultaneously reproduce the shapes and the normalisations of the differential cross sections. Models based on 2-gluon exchange are able to reproduce the shapes of the cross sections at low x_pom values.']",['2000-12-22']
386,['eng'],"['Nikas, D', 'Castillo, V', 'Kowalski, L A', 'Larsen, R', 'Lazarus, D M', 'Ozben, C', 'Semertzidis, Y K', 'Tsang, T', 'Srinivasan-Rao, T']",['ElectroOptical measurements of ultrashort 45 MeV electron beam bunch'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron, beam', 'bunching, length', 'beam monitoring, length', 'beam monitoring, crystal', 'lithium, niobium', 'radiation, laser', 'photon, polarization']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012050'],['We have made an observation of 45 MeV electron beam bunches using the nondestructive electro-optical (EO) technique. The amplitude of the EO modulation was found to increase linearly with electron beam charge and decrease inversely with the optical beam path distance from the electron beam. The risetime of the signal was bandwidth limited by our detection system to \\~70ps. An EO signal due to ionization caused by the electrons traversing the EO crystal was also observed. The EO technique may be ideal for the measurement of bunch structure with femtosecond resolution of relativistic charged particle beam bunches.'],['2000-12-21']
387,['eng'],"['Airapetian, A', 'Akopov, N Z', 'Akopov, N Z', 'Akushevich, I V', 'Amarian, M', 'Arrington, J', 'Aschenauer, E C', 'Avakian, H', 'Avakian, R', 'Avetisian, A', 'Avetissian, E', 'Bailey, P', 'Bains, B', 'Baumgarten, C', 'Beckmann, M', 'Belostotskii, S', 'Bernreuther, S', 'Bianchi, N', 'Böttcher, H', 'Borisov, A', 'Bouwhuis, M', 'Brack, J', 'Brauksiepe, S', 'Braun, B', 'Brückner, W', 'Brüll, A', 'Budz, P', 'Bulten, H J', 'Capitani, G P', 'Carter, P', 'Chumney, P', 'Cisbani, E', 'Court, G R', 'Dalpiaz, P F', 'De Leo, R', 'De Nardo, L', 'De Sanctis, E', 'De Schepper, D', 'Devitsin, E G', 'De Witt-Huberts, P K A', 'Di Nezza, P', 'Dzhordzhadze, V', 'Düren, M', 'Dvoredsky, A P', 'Elbakian, G M', 'Ely, J', 'Fantoni, A', 'Feshchenko, A', 'Felawka, L', 'Ferro-Luzzi, M', 'Fiedler, K', 'Filippone, B W', 'Fischer, H', 'Fox, B', 'Franz, J', 'Frullani, S', 'Gärber, Y', 'Garibaldi, F', 'Garutti, E', 'Gavrilov, G', 'Karibian, V', 'Golendukhin, A', 'Graw, G', 'Grebenyuk, O', 'Green, P W', 'Greeniaus, L G', 'Gute, A', 'Haeberli, W', 'Hartig, M', 'Hasch, D', 'Heesbeen, D', 'Heinsius, F H', 'Henoch, M', 'Hertenberger, R', 'Hesselink, W H A', 'Hofman, G J', 'Holler, Y', 'Holt, R J', 'Hommez, B', 'Iarygin, G', 'Iodice, M', 'Izotov, A A', 'Jackson, H E', 'Jgoun, A', 'Jung, P', 'Kaiser, R', 'Kanesaka, J', 'Kinney, E R', 'Kiselev, A', 'Kitching, P', 'Kobayashi, H', 'Koch, N', 'Königsmann, Kay C', 'Kolster, H', 'Korotkov, V A', 'Kotik, E', 'Kozlov, V', 'Krivokhizhin, V G', 'Kyle, G S', 'Lagamba, L', 'Laziev, A', 'Lenisa, P', 'Lindemann, T', 'Lorenzon, W', 'Makins, N C R', 'Martin, J W', 'Marukyan, H O', 'Masoli, F', 'McAndrew, M', 'McIlhany, K', 'McKeown, R D', 'Meissner, F', 'Menden, F', 'Metz, A', 'Meyners, N', 'Miklukho, O', 'Miller, C A', 'Milner, R', 'Muccifora, V', 'Mussa, R', 'Nagaitsev, A P', 'Nappi, E', 'Naryshkin, Yu', 'Nass, A', 'Negodaeva, K', 'Nowak, W D', 'Oganessyan, K A', ""O'Neill, T G"", 'Openshaw, R', 'Ouyang, J', 'Owen, B R', 'Pate, S F', 'Potashov, S Yu', 'Potterveld, D H', 'Rakness, G', 'Rappoport, V', 'Redwine, R P', 'Reggiani, D', 'Reolon, A R', 'Ristinen, R', 'Rith, K', 'Robinson, D', 'Rostomyan, A', 'Ruh, M', 'Ryckbosch, D', 'Sakemi, Y', 'Sato, T', 'Savin, I A', 'Scarlett, C', 'Schäfer, A', 'Schill, C', 'Schmidt, F', 'Schnell, G', 'Schüler, K P', 'Schwind, A', 'Seibert, J', 'Seitz, B', 'Shibata, T A', 'Shin, T', 'Shutov, V', 'Simani, M C', 'Simon, A', 'Sinram, K', 'Steffens, E', 'Steijger, J J M', 'Stewart, J', 'Stösslein, U', 'Suetsugu, K', 'Sutter, M F', 'Taroian, S P', 'Terkulov, A R', 'Tessarin, S', 'Thomas, E', 'Tipton, B', 'Tytgat, M', 'Urciuoli, G M', 'Van den Brand, J F J', 'van der Steenhoven, G', 'Van de Vyver, R', 'Van Hunen, J J', 'Vetterli, M C', 'Vikhrov, V V', 'Vincter, M G', 'Visser, J', 'Volk, E', 'Weiskopf, C', 'Wendland, J', 'Wilbert, J', 'Wise, T', 'Yen, S', 'Yoneyama, S', 'Zohrabyan, H G']",['Hadron Formation in Deep-Inelastic Positron Scattering in a Nuclear Environment'],['Particle Physics - Experimental Results'],"['positron nucleus, deep inelastic scattering', 'deuteron', 'nitrogen', 'hadron, multiple production', 'charged particle, multiplicity', 'multiplicity, ratio', 'energy dependence', 'formation, time', 'charge, dependence', 'model, hadronization', 'gluon, bremsstrahlung', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', '27.5 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012049'],"['The influence of the nuclear medium on the production of charged hadrons in semi-inclusive deep-inelastic scattering has been studied by the HERMES experiment at DESY using a 27.5 GeV positron beam. The differential multiplicity of charged hadrons and identified charged pions from nitrogen relative to that from deuterium has been measured as a function of the virtual photon energy \\nu and the fraction z of this energy transferred to the hadron. There are observed substantial reductions of the multiplicity ratio R_M^h at low \\nu and at high z, both of which are well described by a gluon-bremsstrahlung model of hadronization. A significant difference of the \\nu-dependence of R_M^h is found between positive and negative hadrons. This is interpreted in terms of a difference between the formation times of protons and pions using a phenomenological model to describe the \\nu- and z-dependence of R_M^h.']",['2000-12-21']
388,['eng'],"['Link, J M', 'Reyes, M', 'Yager, P M', 'Anjos, J C', 'Bediaga, I', 'Göbel, C', 'Magnin, J', 'Massafferri, A', 'De Miranda, J M', 'Pepe, I M', 'Dos Reis, A C', 'Simão, F R A', 'Carrillo, S', 'Casimiro, E', 'Sánchez-Hernández, A', 'Uribe, C', 'Vázquez, F', 'Cinquini, L', 'Cumalat, J P', ""O'Reilly, B"", 'Ramírez, J E', 'Vaandering, E W', 'Butler, J N', 'Cheung, H W K', 'Gaines, I', 'Garbincius, P H', 'Garren, L A', 'Gottschalk, E E', 'Kasper, P H', 'Kreymer, A E', 'Kutschke, R', 'Bianco, S', 'Fabbri, F L', 'Sarwar, S', 'Zallo, A', 'Cawlfield, C', 'Kim, D Y', 'Rahimi, A', 'Wiss, J', 'Gardner, R', 'Chung, Y S', 'Kang, J S', 'Ko, B R', 'Kwak, J W', 'Lee, K B', 'Park, H', 'Alimonti, G', 'Boschini, M', 'Caccianiga, B', ""D'Angelo, P"", 'Di Corato, M', 'Dini, P', 'Giammarchi, M G', 'Inzani, P', 'Leveraro, F', 'Malvezzi, S', 'Menasce, D', 'Mezzadri, M', 'Milazzo, L', 'Moroni, L', 'Pedrini, D', 'Pontoglio, C', 'Prelz, F', 'Rovere, M', 'Sala, A', 'Sala, S', 'Davenport, T F', 'Agostino, L', 'Arena, V', 'Boca, G', 'Bonomi, G', 'Gianini, G', 'Liguori, G', 'Merlo, M', 'Pantea, D', 'Ratti, S P', 'Riccardi, C', 'Segoni, I', 'Viola, L', 'Vitulo, P', 'Hernández, H', 'López, A M', 'Méndez, H', 'Méndez, L', 'Mirles, M A', 'Montiel, E', 'Olaya, D', 'Paris, A', 'Quinones, J', 'Rivera, C', 'Xiong, W', 'Zhang, Y', 'Wilson, J R', 'Cho, K', 'Handler, T', 'Engh, D', 'Hosack, M', 'Johns, W E', 'Nehring, M S', 'Sheldon, P D', 'Stenson, K', 'Webster, M S', 'Sheaff, M']",['A Study of the Decay $D^{0} \\to K^{+}\\pi^{-}$'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium, oxygen', 'charmed meson, photoproduction', 'D0, hadronic decay', 'mass spectrum, (K pi)', 'D0 anti-D0, interference', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> K+ pi-', 'D0 --> K- pi+', 'approx. 180 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012048'],"['Using a large sample of photoproduced charm mesons from the FOCUS experiment at Fermilab (FNAL-E831), we observe the decay $D^0\\to K^+\\pi^-$ with a signal yield of $149\\pm31$ events compared to a similarly cut sample consisting of $36760 \\pm 195$ $D^0\\to K^-\\pi^+$ events. We use the observed ratio of $D^0\\to K^+\\pi^-$ to $D^0\\to K^-\\pi^+$ $(0.404\\pm 0.085\\pm 0.025)%$ to obtain a relationship between the $D^0$ mixing and doubly Cabibbo suppressed decay parameters.']",['2000-12-21']
389,['eng'],"['Telnov, V I']",['Problems of multi-TeV photon colliders'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2000/06/14', 'photon photon, colliding beams', 'photon electron, colliding beams', 'radiation, laser', 'Compton scattering, backscatter', 'luminosity', 'electron, pair production', 'pair production, coherence', 'beam, radiation']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012047'],"['A high energy photon collider (gamma-gamma, gamma-electron) based on backward Compton scattering of laser light is a very natural supplement to e+e- a linear collider and can significantly enrich the physics program. The region below about one 0.5-1 TeV is very convenient from a technical point of view: wave length of the laser should be about 1 micron, i.e. in the region of most powerful solid state lasers, collision effects do not restrict the gamma-gamma luminosity. In the multi-TeV energy region the situation is more complicated: the optimum laser wave length increases in proportional to the energy, the required flash energy also increases due to nonlinear effects in the Compton scattering; bunch trains are shorter (for warm high gradient linacs), this leads to higher backgrounds; the collision effects (coherent pair e+e- pair creation) restrict the luminosity. These problems and possible solutions are discussed in this paper. A method of laser focusing is considered which allows the decrease of the required laser flash energy and the practical elimination of the problem of nonlinear effects in Compton scattering; a way to reduce collision effects and obtain ultimate gamma-gamma luminosities at multi-TeV photon colliders is suggested.']",['2000-12-21']
390,['eng'],"['Abbott, B', 'Abdesselam, A', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Astur, R', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Bacon, T C', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Todorova-Nová, S', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bauer, D', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Beuselinck, R', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Duflot, L', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fatyga, M K', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gao, M', 'Gavrilov, V', 'Geld, T L', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Illingworth, R', 'Ito, A S', 'Jaffré, M', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Leggett, C', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Luo, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Nunnemann, T', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Papageorgiou, K', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Petroff, P', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Ridel, M', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M', 'Rubinov, P', 'Ruchti, R C', 'Rutherfoord, J P', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Sen, N', 'Shabalina, E', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['High-$p_{T}$ Jets in $p\\overline{p}$ Collisions at $sqrt{s}$ = 630 and 1800 GeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'jet, particle identification', 'transverse momentum, high', 'quantum chromodynamics, perturbation theory', 'channel cross section, ratio', 'angular distribution, (2jet)', 'mass spectrum, (2jet)', 'quark, composite', 'coloron', 'differential cross section, transverse energy', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'bibliography', '630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012046'],"['Results are presented from analyses of jet data produced in pbarp collisions at sqrt{s} = 630 and 1800 GeV collected with the DO detector during the 1994-95 Fermilab Tevatron Collider run. We discuss details of detector calibration, and jet selection criteria in measurements of various jet production cross sections at sqrt{s} = 630 and 1800 GeV. The inclusive jet cross sections, the dijet mass spectrum, the dijet angular distributions, and the ratio of inclusive jet cross sections at sqrt{s} = 630 and 1800 GeV are compared to next-to-leading-order QCD predictions. The order alpha_s^3 calculations are in good agreement with the data. We also use the data at sqrt{s} = 1800 GeV to rule out models of quark compositeness with a contact interaction scale less than 2.2 TeV at the 95% confidence level.']",['2000-12-21']
391,['eng'],"['Duboscq, J E']",['A Biased Review of Tau Neutrino Mass Limits'],['Particle Physics - Experimental Results'],"['talk, Victoria 2000/09/18', 'neutrino/tau, mass', 'upper limit', 'astrophysics', 'neutrino, interference', 'electron positron, annihilation', 'tau, pair production', 'tau, decay modes', 'statistical analysis', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012045'],"['After a quick review of astrophysically relevant limits, I present a summary of MeV scale tau neutrino mass limits derived from accelerator based experiments. I argue that the current published limits appear to be too consistent, and that we therefore cannot conclude that the tau neutrino mass limit is as low as usually claimed. I provide motivational arguments calling into question the assumed statistical properties of the usual maxumum likelihood estimators, and provide a prescription for deriving a more robust and understandable mass limit.']",['2000-12-21']
392,['eng'],"['Kluth, S', 'Fernández, P A M', 'Bethke, Siegfried', 'Pahl, C', 'Pfeifenschneider, P']",['A Measurement of the QCD Colour Factors using Event Shape Distributions at sqrt(s)=14 GeV to 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'quantum chromodynamics, perturbation theory', 'correction, nonperturbative', 'color, vertex function', 'event shape analysis', 'dependence, flavor', 'effect, hadronization', 'strong interaction, coupling constant', 'experimental results', 'CERN LEP Stor', 'tables', 'bibliography', '14-189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012044'],"['Measurements of the QCD colour factors C_A and C_F and of the number of active quark flavours n_f in the process e+e- -> hadrons at high energy are presented. They are based on fits of O(alpha_S**2)+NLLA QCD calculations to distributions of the event shape observables 1-T, C, B_T and B_W measured at centre-of-mass energies from 14 GeV to 189 GeV. Hadronisation effects are approximated with power correction calculations which also depend on the QCD gauge structure. In this approach potential biases from hadronisation models are reduced. Our results for individually measured quantities are n_f = 5.64 +- 1.35, C_A = 2.88 +- 0.27 and C_F = 1.45 +- 0.27 in good agreement with QCD based on the SU(3) symmetry group where n_f=5 for the energies considered here, C_A=3 and C_F=4/3. From simultaneous fits of C_A and C_F we find C_A = 2.84 +- 0.24 and C_F = 1.29 +- 0.18, which is also in good agreement with the QCD expectation.']",['2000-12-21']
393,['eng'],"['Abe, K', 'Adam, I', 'Akimoto, H', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Berger, R', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Cassell, R', 'Chou, A', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Crawford, G', 'Damerell, C J S', 'Daoudi, M', 'Dasu, S', 'De Groot, N', 'De Sangro, R', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Erofeeva, I', 'Eschenburg, V', 'Fahey, S', 'Falciai, D', 'Fernández, J P', 'Flood, K', 'Frey, R', 'Hart, E L', 'Hasuko, K', 'Hertzbach, S S', 'Huffer, M E', 'Huynh, X', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Kajikawa, R', 'Kalelkar, M S', 'Kang, H J', 'Kofler, R R', 'Kroeger, R S', 'Langston, M', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'McKemey, A K', 'Messner, R', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Narita, S', 'Nauenberg, U', 'Neal, H', 'Nesom, G', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Ratcliff, B N', 'Reidy, J', 'Reinertsen, P L', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schumm, B A', 'Schwiening, J', 'Serbo, V V', 'Shapiro, G', 'Sinev, N B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Usher, T', 'Vavra, J', 'Verdier, R', 'Wagner, D L', 'Waite, A P', 'Walston, S', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Wright, T R', 'Yamamoto, R K', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H']",['Time Dependent $B^{0}_{s} - \\overline{^B{0}_{s}}$ Mixing Using Inclusive and Semileptonic B Decays at SLD'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'time dependence', 'angular distribution, asymmetry', 'particle identification, flavor', 'B0, semileptonic decay', 'B/s0, cascade decay', 'B0, mass difference', 'B/s0, mass difference', 'correlation, (D lepton)', 'track data analysis, vertex', 'charge, dipole', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012043'],"['We set a preliminary 95% C.L. exclusion on the oscillation frequency of B0s - B0s-bar mixing using a sample of 400,000 hadronic Z0 decays collected by the SLD experiment at the SLC between 1996 and 1998. The analyses determine the b-hadron flavor at production by exploiting the large forward-backward asymmetry of polarized Z0 -> b b-bar decays as well as information from the hemisphere opposite that of the reconstructed B decay. In one analysis, B decay vertices are reconstructed inclusively with a topological technique and separation between B0s and B0s-bar decays exploits the B0s -> Ds- cascade charge structure. In the other analysis, semileptonic decays are selected and the B decay point is reconstructed by intersecting a lepton track with the trajectory of a topologically reconstructed D meson. The two analyses are combined with a third analysis described elsewhere to exclude the following values of the B0s - B0s-bar mixing oscillation frequency: Delta m_s < 7.6 ps-1 and 11.8 < Delta m_s < 14.8 ps-1 at the 95% confidence level.']",['2000-12-20']
394,['eng'],"['Meyer, A B']",['Heavy Quark Production at HERA'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'positron p, colliding beams', 'quark, charm', 'quark, beauty', 'quark, pair production', 'fusion, photon gluon', 'D*(2010), photoproduction', 'D/s, photoproduction', 'quark, semileptonic decay', 'differential cross section, momentum transfer', 'structure function, charm', 'channel cross section, transverse momentum', 'energy dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '320 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012041'],"['Recent results on heavy flavor production at HERA are presented. New measurements of charm production are available in the region of $ Q^2 <$ 1000 GeV$^2$ for $D^*$ and in the photoproduction limit, $Q^2\\to 0$, for $D_s$. The results are compared to theoretical calculations and the charm proton structure function \\f2cc$(x,Q^2)$ is extracted. A new independent measurement of the $b\\bar{b}$ cross section using a $b$-lifetime tag is reported.']",['2000-12-19']
395,['eng'],"['Kirchner, J J', 'Becker, U J', 'Dinner, A R', 'Fidkowski, K J', 'Wyatt, J H']",['Optimization of drift gases for accuracy in pressurized drift tubes'],['Detectors and Experimental Techniques'],"['drift chamber, drift tube', 'pressure, drift tube', 'magnetic field', 'scaling', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012040'],"['Modern detectors such as ATLAS use pressurized drift tubes to minimize diffusion and achieve high coordinate accuracy. However, the coordinate accuracy depends on the exact knowledge of converting measured times into coordinates. Linear space-time relationships are best for reconstruction, but difficult to achieve in the $E \\propto \\frac{1}{r}$ field. Previous mixtures, which contained methane or other organic quenchers, are disfavored because of ageing problems. From our studies of nitrogen and carbon dioxide, two mixtures with only small deviations from linearity were determined and measured. Scaling laws for different pressures and magnetic fields are also given.']",['2000-12-19']
396,['eng'],[],"['Study of conversion decays phi->etae+e-, eta->e+e-g and eta->pi+pi-e+e- at CMD-2']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), electromagnetic decay', 'Phi(1020), branching ratio', 'eta, electromagnetic decay', 'eta, branching ratio', 'mass spectrum', 'magnetic detector, CMD', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> eta positron electron', 'Phi(1020) --> eta muon+ muon-', 'eta --> 2photon', 'eta --> pi+ pi- positron electron', 'eta --> positron electron photon', 'eta --> 2positron 2electron', '1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012039'],"['Using 15.1 pb^{-1} of data collected by CMD-2 in the phi-meson energy range, the branching ratios of the following conversion decays have been measured: B(\\phi\\to\\eta e^+e^-) = (1.14\\pm0.10\\pm0.06)\\cdot10^{-4}, B(\\eta\\to e^+e^-\\gamma) = (7.10\\pm0.64\\pm0.46)\\cdot10^{-3}, B(\\eta\\to\\pi^+\\pi^-e^+e^-) = (3.7^{+2.5}_{-1.8}\\pm0.3)\\cdot10^{-4}. The upper limits for the following rare conversion decays have been obtained at the 90% confidence level: B(\\phi\\to\\eta\\mu^+\\mu^-) < 9.4\\cdot10^{-6}, B(\\eta\\to e^+e^-e^+e^-) < 6.9\\cdot10^{-5}.']",['2000-12-19']
397,['eng'],"['Zhao, Z G']",['New R values in 2-5 GeV from the BESII at BEPC'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'cross section, hadronic', 'energy dependence', 'magnetic detector, BES', 'experimental results', 'Beijing Stor', '2-5 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012038'],"['We report preliminary $R$ values for all 85 energy points scanned in the energy region of 2-5 GeV with the upgraded Beijing Spectrometer (BESII) at the Beijing Electron Positron Collider (BEPC). The typical uncertainty on the R values we measured is about 7%. The new R values have a significant impact on the predicted mass of the Higgs coming from the global fit to the electroweak data, and will also contribute to the interpretation of the E821 g-2 experiment.']",['2000-12-19']
398,['eng'],"['Weatherall, J']",['The BABAR measurement of sin2beta and its future prospects'],['Particle Physics - Experimental Results'],"['talk, Durham 2000/09/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'anti-B0, hadronic decay', 'violation, CP', 'asymmetry, time dependence', 'particle identification, flavor', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012037'],"['The measurement of sin2beta by the BABAR experiment, where beta is one of the angles of the Unitarity Triangle, is described. Some prospects for the future of the measurement are also discussed.']",['2000-12-19']
399,['eng'],"['Mangeol, D J']",['Moments of the charged-particle multiplicity distribution in Z decays at LEP'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, beauty', 'hadron, multiple production', 'charged particle, multiplicity', 'multiplicity, moment', 'quantum chromodynamics, perturbation theory', 'jet, multiplicity', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012036'],"['The charged-particle multiplicity distribution and its moments have been measured, for all hadronic as well as for light-quark and b-quark events in e+e- collisions at the Z mass. The Hq moments derived from the charged-particle multiplicity distribution are known to exhibit quasi-oscillations when plotted versus the order of the moment. This behavior is predicted by the NNLLA of perturbative QCD for the parton level and, under the assumption of LPHD, also for the hadron level. Using the jet multiplicity distributions in order to vary the dependence on the LPHD hypothesis, we find, however, that at our energy the oscillations only appear for non-perturbative scales. In the absence of confirmation of pQCD, we investigate a more phenomenological answer in the possibility that the features seen in the Hq behavior could be due to the fact that the charged-particle multiplicity derives from a superposition of final states related to the topology of the events. Therefore, the analysis is repeated using charged-particle multiplicity distributions originating from 2-jet and 3-jet events for the full, light- and b-quark samples.']",['2000-12-18']
400,['eng'],"['Kodama, K', 'Ushida, N', 'Andreopoulos, C', 'Saoulidou, N', 'Tzanakos, G', 'Yager, P', 'Baller, B R', 'Böhnlein, D J', 'Freeman, W', 'Lundberg, B', 'Mor, J', 'Rameika, R', 'Yun, J C', 'Song, J S', 'Yoon, C S', 'Chung, S H', 'Berghaus, P', 'Kubantsev, M A', 'Reay, N W', 'Sidwell, R A', 'Stanton, N', 'Yoshida, S', 'Aoki, S', 'Hara, T', 'Rhee, J T', 'Ciampa, D', 'Erickson, C', 'Graham, M', 'Heller, K', 'Rusack, R', 'Schwienhorst, R', 'Siela, J', 'Trammell, J', 'Wilcox, J', 'Hoshino, K', 'Jiko, H', 'Miyanishi, M', 'Komatsu, M', 'Nakamura, M', 'Nakano, T', 'Niwa, K', 'Nonaka, N', 'Okada, K', 'Sato, O', 'Akdogan, T', 'Paolone, V', 'Rosenfeld, C', 'Kulik, A V', 'Kafka, T', 'Oliver, W', 'Patzak, T', 'Schneps, J']",['Observation of Tau Neutrino Interactions'],['Particle Physics - Experimental Results'],"['neutrino, secondary beam', 'neutrino nucleus, interaction', 'neutrino/tau', 'charged current', 'tau, leptonic decay', 'tau, semileptonic decay', 'electroweak interaction, validity test', 'nuclear emulsion, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012035'],['The DONUT experiment has analyzed 203 neutrino interactions recorded in nuclear emulsion targets. A decay search has found evidence of four tau neutrino interactions with an estimated background of 0.34 events. This number is consistent with the Standard Model expectation.'],['2000-12-15']
401,['eng'],"['Chang, T H']",['Angular distribution of J/psi decays in dimuon channel in 800 GeV proton-copper collisions'],['Particle Physics - Experimental Results'],"['Thesis', 'thesis', 'p nucleus, inelastic scattering', 'copper', 'J/psi(3100), hadroproduction', 'J/psi(3100), leptonic decay', 'angular distribution', 'J/psi(3100), polarization', 'polarization, longitudinal', 'polarization, transverse', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'J/psi(3100) --> muon+ muon-', 'p copper --> J/psi(3100) anything', '800 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012034'],"[""The anuglar distribution of $J/\\psi$ decays in the $\\mu^{+}\\mu^{-}$ channel in 800 proton-copper collisions has been measured for $x_F$ > 0.25. The polarization parameter $\\lambda$ is extracted in 1 GeV of $p_T$ and 0.1 of $x_F$ bins for two magnet configugrations with different acceptances. The data indicate that the $J/\\psi$'s are produced with a slight transverse polarization at small $x_F$, which turns to longitudinal at $x_F$ > 0.6. No $p_T$ dependence of $\\lambda$ is observed. Theoretical calculations are needed in order to interpret the measurements.""]",['2000-12-14']
402,['eng'],"['Inoue, Y']",['Measurement of the cross-section and forward-backward charge asymmetry for the b and c-quark in $e^{+} ^e{-}$ annihilation with inclusive muons at sqrt(s) = 58 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, charm', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'channel cross section, ratio', 'angular distribution, asymmetry', 'charge, asymmetry', 'muon, particle identification', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', 'tables', '58 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012033'],"['We have studied inclusive muon events using all the data collected by the TOPAZ detector at sqrt(s)=58 GeV with an integrated luminosity of 273pb-1. From 1328 inclusive muon events, we measured the ratio R_qq of the cross section for qq-bar production to the total hadronic cross section and forward-backward asymmetry A^q_FB for b and c quarks. The obtained results are R_bb = 0.13+-0.02(stat)+-0.01(syst), R_cc = 0.36+-0.05(stat)+-0.05(syst), A^b_FB = -0.20+-0.16(stat)+-0.01(syst) and A^c_FB = -0.17+-0.14(stat)+-0.02(syst), in fair agreement with a prediction of the standard model.']",['2000-12-14']
403,['eng'],"['Tsang, T', 'Castillo, V', 'Kowalski, L A', 'Larsen, R', 'Lazarus, D M', 'Nikas, D', 'Ozben, C', 'Semertzidis, Y K', 'Srinivasan-Rao, T']",['Electro-optical Measurements of Ultrashort 45 MeV Electron Beam Bunches'],['Particle Physics - Experimental Results'],"['electron, beam', 'bunching, length', 'beam monitoring, length', 'beam monitoring, crystal', 'lithium, niobium', 'optics, laser', 'beam, electromagnetic field', 'optics, polarization']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012032'],"['We have measured the temporal duration of 45 MeV picosecond electron beam bunches using a noninvasive electro-optical (EO) technique. The amplitude of the EO modulation was found to increase linearly with electron beam charge and decrease inversely with distance from the electron beam. The risetime of the temporal signal was limited by our detection system to ~70ps. The EO signal due to ionization caused by the electrons traversing the EO crystal was also observed. It has a distinctively long decay time constant and signal polarity opposite to that due to the field induced by the electron beam. The electro-optical technique may be ideal for the measurement of bunch length of femtosecond, relativistic, high energy, charged, particle beams.']",['2000-12-12']
404,['eng'],"['Alavi-Harati, A', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barker, A R', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hamm, J', 'Hanagaki, K', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jensen, D A', 'Kessler, R', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian R"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S R', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Shields, J', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Suzuki, I', 'Swallow, E C', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Turner, S E', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['A Measurement of the Branching Ratio and Asymmetry of the Decay Cascade$^{0} \\to \\Sigma ^{0}/gamma$'],['Particle Physics - Experimental Results'],"['Xi0, radiative decay', 'Xi0, branching ratio', 'angular distribution, asymmetry', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'Xi0 --> Sigma0 photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012031'],"['We have studied the rare weak radiative hyperon decay Cascade0-->Sigma0/gamma in the KTeV experiment at Fermilab. We have identified 4045 signal events over a background of 804 events. The dominant Cascade0-->Lambda/pi0 decay, which was used for normalization, is the only important background source. An analysis of the acceptance of both modes yields a branching ratio of BR(Cascade0-->Sigma0/gamma)=(3.34 +/- 0.05 +/- 0.09) x 10^(-3). By analyzing the final state decay distributions, we have also determined that the Sigma0 emission asymmetry parameter for this decay is alpha = -0.63 +/- 0.09.']",['2000-12-12']
405,['eng'],"['Alimonti, G', 'Arpesella, C', 'Back, H O', 'Balata, M', 'Beau, T', 'Bellini, G', 'Benziger, J B', 'Bonetti, S', 'Brigatti, A', 'Caccianiga, B', 'Cadonati, L', 'Calaprice, F', 'Cecchet, G', 'Chen, M', 'De Bari, A', 'De Haas, E', 'De Kerret, H', 'Donghi, O', 'Deutsch, M', 'Elisei, F', 'Etenko, A', 'Von Feilitzsch, F', 'Fernholz, R C', 'Ford, R', 'Freudiger, B', 'Garagiola, A', 'Galbiati, C', 'Gatti, F', 'Gazzana, S', 'Giammarchi, M G', 'Giugni, D', 'Golubchikov, A', 'Goretti, A', 'Grieb, C', 'Hagner, C', 'Hagner, T', 'Hampel, W', 'Harding, E', 'Hartmann, F', 'Von Hentig, R', 'Hess, H', 'Heusser, G', 'Ianni, A', 'Inzani, P', 'Kidner, S H', 'Kiko, J', 'Kirsten, T', 'Korga, G', 'Korschinek, G', 'Kryn, Didier', 'Lagomarsino, V', 'La Marche, P', 'Laubenstein, M', 'Löser, F', 'Lombardi, P', 'Magni, S', 'Malvezzi, S', 'Maneira, J', 'Manno, I', 'Manuzio, G', 'Masetti, F', 'Mazzucato, U', 'Meroni, E', 'Musico, P', 'Neder, H', 'Neff, M', 'Nisi, S', 'Oberauer, L', 'Obolensky, M', 'Pallavicini, M', 'Papp, L', 'Perasso, L', 'Pocar, A', 'Raghavan, R', 'Ranucci, G', 'Rau, W', 'Razeto, A', 'Resconi, E', 'Riedel, T', 'Sabelnikov, A A', 'Saggese, P', 'Salvo, C', 'Scardaoni, R', 'Schönert, S', 'Schuhbeck, K', 'Seidel, H', 'Shutt, T', 'Simgen, H', 'Sonnenschein, A H', 'Smirnov, O Yu', 'Sotnikov, A', 'Skorokhvatov, M', 'Sukhotin, S V', 'Tartaglia, R', 'Testera, G', 'Vitale, S', 'Vogelaar, R', 'Wójcik, M', 'Zaimidoroga, O A', 'Zakharov, Yu I']",['Science and Technology of BOREXINO'],['Particle Physics - Experimental Results'],"['neutrino, solar', 'neutrino, oscillation', 'neutrino electron, interaction', 'scintillation counter, liquid', 'organic compounds, liquid', 'background, radioactivity', 'data acquisition', 'supersymmetry', 'neutrino, cosmic radiation', 'xenon, double-beta decay', 'deep underground detector, Gran Sasso', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012030'],"[""BOREXINO, a real-time device for low energy neutrino spectroscopy is nearing completion of construction in the underground laboratories at Gran Sasso, Italy (LNGS). The experiment's goal is the direct measurement of the flux of 7Be solar neutrinos of all flavors via neutrino-electron scattering in an ultra-pure scintillation liquid. Seeded by a series of innovations which were brought to fruition by large scale operation of a 4-ton test detector at LNGS, a new technology has been developed for BOREXINO. It enables sub-MeV solar neutrino spectroscopy for the first time. This paper describes the design of BOREXINO, the various facilities essential to its operation, its spectroscopic and background suppression capabilities and a prognosis of the impact of its results towards resolving the solar neutrino problem. BOREXINO will also address several other frontier questions in particle physics astrophysics and geophysics.""]",['2000-12-12']
406,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Baroiant, S', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bell, W H', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Bishai, M', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Caskey, W', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Chung, Y S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', ""D'Auria, S"", 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erbacher, R D', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Fernández, J P', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Furic, I K', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Glenzinski, D A', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Gorelov, I V', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Grim, G P', 'Gris, P', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hill, C', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirby, M', 'Kirk, M', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, J', 'Lancaster, M', 'Lander, R', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Litvintsev, D O', 'Lobban, O', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Meyer, A', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Moulik, T', 'Mulhearn, M', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Nachtman, J', 'Nagaslaev, V', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Nelson, T', 'Neu, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Ribon, A', 'Riegler, W', 'Rimondi, F', 'Ristori, L', 'Riveline, M', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R', 'Rossin, R', 'Roy, A', 'Safonov, A', 'Saint-Denis, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sánchez, C', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tartarelli, G F', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Tesarek, R J', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Thompson, A S', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Wilkes, T', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['First Measurement of the Ratio $B(t \\to Wb)/B(t \\to Wq)$ and Associated Limit on the CKM Element $|V_{tb}|$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'quark, branching ratio', 'Kobayashi-Maskawa angle', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'truth --> W beauty', 'truth --> W quark', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012029'],"['We present the first measurement of the ratio of branching fraction R= B(t-->wb)/B(t-->Wq) from ppbar collisions at sqrt(s)=1.8 TeV. The data set corresponds to 109 pb-1 of data recorded by the Collider Detector at Fermilab during the 1992-1995 Tevatron run. We measure R=0.94+.31-.24 (stat+syst) or R>0.61 (0.56) at 90 (95) %C.L., in agreement with the standard model predictions. This measurement yields a limit of the Cabibbo-Kobayashi-Maskawa quark mixing matrix element Vtb under the assumption of three generation unitarity.']",['2000-12-12']
407,['eng'],"['Rodríguez, J L']",['Measurement of $\\sin{2\\phi_{1}}$ at Belle'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'decay, time', 'Kobayashi-Maskawa angle', 'quarkonium, charm', 'K0', 'particle identification, flavor', 'violation, CP', 'magnetic detector, BELLE', 'experimental results', 'SLAC PEP Stor', 'B0 --> J/psi(3100) K0', 'B0 --> psi(3685) K0(S)', 'B0 --> chi/c1(3510) K0(S)', 'B0 --> J/psi(3100) pi0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012028'],"['With 6.2 fb^-1 of data collected on the Upsilon(4S), Belle reports its first measurement of sin 2\\phi_1 = 0.45^{+0.43}_{-0.44}(stat)^{+0.07}_{-0.09}(sys). The result was obtained by fitting the proper time distribution of flavor tagged and fully reconstructed neutral B mesons decays to five different charmonia plus a Kshort or Klong channels. In this paper the analysis and results will be described briefly.']",['2000-12-12']
408,['eng'],"['Brau, B']",['B decays to final states including $D_{s}^{(*)}$ and $D^{*}$'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'D', 'D*(2010)', 'D/s', 'D/s*(2110)', 'B0, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> 2charmed meson', 'B0 --> D*(2010) pi+', 'B0 --> D*(2010) rho(770)+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012027'],['The e^+e^- annihilation data recorded with the BABAR detector has been used to study B decays to D_s^(*) and D^* mesons. The production fraction of inclusive D_s^(*) and the corresponding momentum spectra have been determined. Exclusive decays B^0 --> D^{*-}D_s^{(*)+} have been identified with a partial reconstruction technique and their branching fractions have been measured. We also report branching fraction measurements for the exclusive hadronic modes B^0 --> D^{*-} pi^+ and B^0 --> D^{*-} rho^+.'],['2000-12-11']
409,['eng'],"['Ferrer-Ribas, E']",['Standard Model Higgs at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, mass', 'lower limit', 'Higgs particle, hadronic decay', 'Higgs particle, leptonic decay', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'Higgs particle --> 2beauty', 'Higgs particle --> tau+ tau-', 'Z0 --> quark antiquark', 'Z0 --> lepton antilepton', '192-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012026'],['In 1999 the LEP experiments collected data at centre of mass energies between 192 and 202 GeV for about 900 pb-1 integrated luminosity. Combined results are presented for the search for the Standard Model Higgs boson. No statistically significant excess has been observed when compared to Standard Model background expectation which can be translated into a lower bound on the mass of the Higgs boson at 107.9 GeV/c^2 at 95 % confidence level.'],['2000-12-11']
410,['eng'],"['Lazarus, D M', 'Castillo, V', 'Kowalski, L A', 'Kraus, D E', 'Larsen, R', 'Magurno, B', 'Nikas, D', 'Ozben, C', 'Semertzidis, Y K', 'Srinivasan-Rao, T', 'Tsang, T']",['First Electrooptical Detection of Charged Particles'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron, beam', 'beam monitoring, crystal', 'lithium, niobium', 'optics, laser', 'beam, electromagnetic field', 'optics, polarization', 'semiconductor, optical']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012025'],"['We have made the first observation of a charged particle beam by means of its electro-optical effect on the polarization of laser light in a birefringent crystal. The modulation of the laser light during the passage of a pulsed electron beam was observed using a fast photodiode and a digital oscilloscope. The fastest rise time measured in a single shot, 120 ps, was limited by the bandwidth of the oscilloscope and the associated electronics. This technology holds promise for detectors of greatly improved spatial and temporal resolution for single relativistic charged particles as well as particle beams.']",['2000-12-08']
411,['eng'],"['Kluth, S']",['Multijet Final States in $e^{+}e^{-}$ Annihilation'],['Particle Physics - Experimental Results'],"['talk, Tihany 2000/10/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, multiple production', 'hadron, multiple production', 'mass, beauty', 'correction, higher-order', 'event shape analysis', 'color', 'quantum chromodynamics, perturbation theory', 'effect, hadronization', 'experimental results', 'DESY PETRA Stor', 'CERN LEP Stor', '35-189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012023'],"['We review the current status of analyses of multijet final states in e+e- annihilation. Results for jet observables from LEP 1, LEP 2 and from the reanalysis of the PETRA experiment JADE will be presented. A determination of the b-quark mass using jet observables will be discussed and tests of power correction models will be shown. Finally determinations of the QCD colour factors from an analysis of event shape distributions at several energy points using power corrections will be discussed.']",['2000-12-08']
412,['eng'],"['Baudis, L', 'Dietz, A', 'Heusser, G', 'Majorovits, B', 'Strecker, H', 'Klapdor-Kleingrothaus, H V']",['GENIUS-TF'],['Particle Physics - Experimental Results'],"['double-beta decay, (0neutrino)', 'astrophysics, missing-mass', 'neutralino', 'WIMP', 'scattering, WIMP nucleon', 'semiconductor detector, germanium', 'nitrogen, liquid', 'background', 'deep underground detector, Gran Sasso', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012022'],"['GENIUS is a proposal for a large scale detector of rare events. As a first step of the experiment, a small test version, the GENIUS test facility, will be build up at the Laboratorio Nazionale del Gran Sasso (LNGS). With about 40 kg of natural Ge detectors operated in liquid nitrogen, GENIUS-TF could exclude (or directly confirm) the DAMA annual modulation signature within about two years of measurement.']",['2000-12-08']
413,['eng'],"['Battaglia, M']",['Physics Case and Challenges for the Vertex Tracker at Future High Energy $e^{+}e^{-}$ Linear Colliders'],['Particle Physics - Experimental Results'],"['talk, Homestead 2000/09/10', 'electron positron, linear collider', 'linear collider, proposed', 'new particle, search for', 'Higgs particle', 'counters and detectors, vertex']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012021'],"['The physics programme of high energy e+e- linear colliders relies on the accurate identification of fermions in order to study in details the profile of the Higgs boson, search for new particles and probe the multi-TeV mass region by means of precise electro-weak measurements and direct searches.']",['2000-12-08']
414,['eng'],"['Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H']",['Evidence of New States Decaying into $\\Xi^{\\prime}_{c}\\pi$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, excited state', 'charmed baryon, electroproduction', 'charmed baryon, hadronic decay', 'charmed baryon, radiative decay', 'charmed baryon, mass difference', 'postulated particle, Xi/c1', 'mass spectrum, mass difference', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012020'],"['Using 13.7 $fb^{-1}$ of data recorded by the CLEO detector at CESR, we report evidence for two new charmed baryons: one decaying into $\\Xi_c^{0 \\prime}\\pi^+$ with the subsequent decay $\\Xi_c^{0 \\prime} \\to \\Xi_c^0 \\gamma$, and its isospin partner decaying into $\\Xi_c^{+ \\prime} \\pi^-$ followed by $\\Xi_c^{+\\prime} \\to \\Xi_c^+\\gamma$. We measure the following mass differences for the two states: $M(\\Xi_c^0 \\gamma \\pi^+)-M(\\Xi_c^0)$=3 18.2+-1.3+-2.9 MeV, and $M(\\Xi_c^+ \\gamma \\pi^-)-M(\\Xi_c^+)$=324.0+-1.3+-3.0 MeV. We interpret these new states as the $J^P = 1/2^- \\Xi_{c1}$ particles, the charmed-strange analogs of the $\\Lambda_{c1}^+(2593)$.']",['2000-12-07']
415,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Beeston, C', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Darling, C L', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Foucher, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hart, P A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Kirk, J', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lee, A M', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Müller, U', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Palmonari, F', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Quast, G', 'Rabbertz, K', 'Raith, B A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, B', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Smith, T J', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Springer, R W', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Tecchio, M', 'Thomas, J', 'Thomson, M A', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsukamoto, T', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Vokurka, E H', 'Voss, H', 'Vossebeld, J H', 'Wagner, A', 'Wagner, D L', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Precise Determination of the Z Resonance Parameters at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, mass', 'Z0, width', 'Z0, hadronic decay', 'Z0, leptonic decay', 'angular distribution, asymmetry', 'interference, (Z0 photon)', 'lepton, universality', 'neutrino, flavor', 'mass, truth', 'Higgs particle, mass', 'strong interaction, coupling constant', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tables', 'bibliography', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012018'],"['This final analysis of hadronic and leptonic cross-sections and of leptonic forward-backward asymmetries in e+e- collisions with the OPAL detector makes use of the full LEP1 data sample comprising 161 pb^-1 of integrated luminosity and 4.5 x 10^6 selected Z decays. An interpretation of the data in terms of contributions from pure Z exchange and from Z-gamma interference allows the parameters of the Z resonance to be determined in a model-independent way. Our results are in good agreement with lepton universality and consistent with the vector and axial-vector couplings predicted in the Standard Model. A fit to the complete dataset yields the fundamental Z resonance parameters: mZ = 91.1852 +- 0.0030 GeV, GZ = 2.4948 +- 0.0041 GeV, s0h = 41.501 +- 0.055 nb, Rl = 20.823 +- 0.044, and Afb0l = 0.0145 +- 0.0017. Transforming these parameters gives a measurement of the ratio between the decay width into invisible particles and the width to a single species of charged lepton, Ginv/Gl = 5.942 +- 0.027. Attributing the entire invisible width to neutrino decays and assuming the Standard Model couplings for neutrinos, this translates into a measurement of the effective number of light neutrino species, N_nu = 2.984 +- 0.013. Interpreting the data within the context of the Standard Model allows the mass of the top quark, mt = 162 +29-16 GeV, to be determined through its influence on radiative corrections. Alternatively, utilising the direct external measurement of mt as an additional constraint leads to a measurement of the strong coupling constant and the mass of the Higgs boson: alfa_s(mZ) = 0.127 +- 0.005 and mH = 390 +750-280 GeV.']",['2000-12-07']
416,['eng'],"['Nolty, R']",['Semi-Contained Neutrino Events in MACRO'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'neutrino nucleon, interaction', 'neutrino/mu, angular distribution', 'charged current', 'scintillation counter, experimental results', 'deep underground detector, MACRO']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012016'],[],['2000-12-07']
417,['eng'],"['Semertzidis, Y K', 'Castillo, V', 'Kowalski, L A', 'Kraus, D E', 'Larsen, R C', 'Lazarus, D M', 'Magurno, B', 'Srinivasan-Rao, T', 'Tsang, T', 'Usack, V']",['Electro-Optical Detection of Charged Particle Beams'],['Particle Physics - Experimental Results'],"['talk, New York 1999/03/29', 'electron, beam', 'beam monitoring, position sensitive', 'optics, laser', 'crystal, optics', 'lithium, niobium', 'optics, polarization', 'Brookhaven Lab']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012014', 'http://documents.cern.ch/archive/electronic/other/uploader/PAC99/thbr4.pdf']","['We have made the first observation of a charged particle beam by means of its electro-optical effect on the propagation of laser light in a birefringent crystal at the Brookhaven National Laboratory Accelerator Test Facility. Polarized infrared light was coupled to a LiNbO3 crystal through a polarization maintaining fiber of 4 micron diameter. An electron beam in 10ps bunches of 1mm diameter was scanned across the crystal. The modulation of the laser light during passage of the electron beam was observed using a photodiode with 45GHz bandwidth. The fastest rise time measured, 120ps, was made in the single shot mode and was limited by the bandwidth of the oscilloscope and the associated electronics. Both polarization dependent and polarization independent effects were observed. This technology holds promise of greatly improved spatial and temporal resolution of charged particle beams.']",['2000-12-06']
418,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Baroiant, S', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bell, W H', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Bishai, M', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Caskey, W', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Chung, Y S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', ""D'Auria, S"", 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erbacher, R D', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Fernández, J P', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Furic, I K', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Glenzinski, D A', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Gorelov, I V', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Grim, G P', 'Gris, P', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hill, C', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirby, M', 'Kirk, M', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, J', 'Lancaster, M', 'Lander, R', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Litvintsev, D O', 'Lobban, O', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Meyer, A', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Moulik, T', 'Mulhearn, M', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Nachtman, J', 'Nagaslaev, V', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Nelson, T', 'Neu, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Ribon, A', 'Riegler, W', 'Rimondi, F', 'Ristori, L', 'Riveline, M', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R', 'Rossin, R', 'Roy, A', 'Safonov, A', 'Saint-Denis, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sánchez, C', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Tesarek, R J', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Thompson, A S', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Wilkes, T', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Measurement of the Two-Jet Differential Cross Section in proton-antiproton Collisions at $\\sqrt{s}$ = 1800 GeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, pair production', 'differential cross section, transverse energy', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'momentum spectrum, parton', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'anti-p p --> 2jet anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012013'],"['A measurement is presented of the two-jet differential cross section, d^3\\sigma/dE_T d\\eta_1 d\\eta_2, at center of mass energy sqrt{s} = 1800 GeV in proton-antiproton collisions. The results are based on an integrated luminosity of 86 pb^-1 collected during 1994-1995 by the CDF collaboration at the Fermilab Tevatron collider. The differential cross section is measured as a function of the transverse energy, E_T, of a jet in the pseudorapidity region 0.1 < |eta_1| < 0.7 for four different pseudorapidity bins of a second jet restricted to 0.1 < |\\eta_2| < 3.0. The results are compared with next-to-leading order QCD calculations determined using the CTEQ4 and MRST sets of parton distribution functions. None of the sets examined in this analysis provides a good description of the data.']",['2000-12-06']
419,['eng'],"['Truöl, P']",['New Results on Rare and Forbidden Semileptonic $K^{+}$ Decays'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'K+, rare decay', 'K+, semileptonic decay', 'violation, flavor', 'pi pi, scattering length', 'K+, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ muon+ electron', 'K+ --> pi+ positron electron neutrino/e']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012012'],"['Experiment E865 at the Brookhaven AGS was set up primarily to search for the lepton flavour violating decay $K^+\\to \\pi^+\\mu^+e^-$ ($K_{\\pi\\mu e}$) with high sensitivity. The flexibility of the apparatus allowed also to obtain more than an order of magnitude larger than previously available event samples on the following decay modes: $ \\pi^+e^+e^- (K_{\\pi ee})$, $\\pi^+\\mu^+\\mu^- (K_{\\pi\\mu\\mu})$, $\\pi^+\\pi^-e^+\\nu_e (K_{e4})$, $\\mu^+e^+e^-\\nu_\\mu$, and $e^+e^+e^-\\nu_e$. The report focusses on the $K_{\\pi\\mu e}$ results and those on other lepton flavour violating decays as well as the $K_{e4}$ data, from which a new, quite precise value for the s-wave $\\pi\\pi$ scattering length can be deduced.']",['2000-12-06']
420,['eng'],"['Unal, G']",['Performances of the NA48 Liquid Krypton calorimeter'],['Particle Physics - Experimental Results'],"['talk', 'calorimeter, electromagnetic', 'krypton', 'ionization chamber, liquid', 'spatial resolution', 'energy resolution', 'K0, hadronic decay', 'violation, CP', 'CERN SPS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012011'],['The NA48 experiments aims at a precise measurement of direct CP violation in the neutral Kaon system. This puts stringent requirements on the electromagnetic calorimeter used to detect photons of average energy 25 GeV. The choice of NA48 is a quasi homogeneous Liquid Krypton calorimeter with fast readout. The operation of this device and the performances achieved are described.'],['2000-12-06']
421,['eng'],"['Abbaneo, D']",['Review of experimental results on neutral B meson oscillations'],['Particle Physics - Experimental Results'],"['review, Rio de Janeiro 2000/10/09', 'B0 anti-B0, oscillation', 'B/s0 anti-B/s0, oscillation', 'beautiful meson, electroproduction', 'beautiful meson, hadroproduction', 'particle identification, flavor', 'B0, mass difference', 'B/s0, mass difference', 'upper limit', 'experimental results', 'Batavia TEVATRON Coll', 'SLAC SLC Linac', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012010'],"['The current status of the experimental knowledge of neutral B meson oscillation is reviewed. The B0d oscillation frequency is precisely measured by SLD, CDF and the LEP experiments. An overview of the analyses and their combination is presented. Preliminary measurements and perspectives at the running B factories are also briefly discussed. The much faster B0s oscillations have not yet been resolved, despite the progress recently by SLD and ALEPH. The world combination is presented, together with the expected and observed lower limit on the B0s oscillation frequency. The ""amplitude method"", used to combine the analyses in order to set the limits, is discussed also as a tool to establish the significance of a possible signal.']",['2000-12-06']
422,['eng'],"['Göbel, C']",['Light mesons and charm decays'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'pi- nucleus, inclusive reaction', 'charmed meson, hadroproduction', 'D+, hadronic decay', 'D/s, hadronic decay', 'meson, hadron spectroscopy', 'decay, amplitude analysis', 'Dalitz plot', 'scalar meson, mass', 'scalar meson, width', 'f0(975)', 'f0(1370)', 'sigma meson', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> 2pi+ pi-', 'D+ --> K- 2pi+', 'D/s+ --> 2pi+ pi-', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012009'],"['We will discuss how the decays of charm mesons can be used to study light mesons spectroscopy, by presenting recent results of Dalitz plot analyses using data from Fermilab experiment E791. Emphasis will be on scalar mesons, which are found to have large contribution to the $D$ decays studied. In addition to the usual extraction of decay fractions and relative phases of the intermediate amplitudes, the Dalitz plot technique is used to measure masses and widths of scalar resonances. From the $D_s$ decay, we obtain masses and widths of $f_0(980)$ and $f_0(1370)$. We find evidence for a light and broad scalar resonance, the $\\sigma$ meson, in $D^+\\to\\pi^-\\pi^+\\pi^+$ decay. Preliminary studies also show evidence for a light and broad resonance, the $\\kappa$ meson, in $D^+\\to K^-\\pi^+\\pi^+$ decay. These results illustrate the potential of charm decays as a laboratory for the study of light mesons.']",['2000-12-06']
423,['eng'],"['Pásztor, G']",['Study of ZZ production at LEP at $\\sqrt{s}$ = 183-209 GeV'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, pair production', 'Z0, hadronic decay', 'Z0, semileptonic decay', 'channel cross section, energy dependence', 'coupling, (3Z0)', 'coupling, (2Z0 photon)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '183-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012008'],"['A study of Z boson pair production in e+e- annihilation using the OPAL detector at LEP is reported. The ZZ production cross-section is measured, limits on anomalous ZZgamma and ZZZ couplings are derived, and constraints on models of low scale quantum gravity in extra spatial dimensions are set.']",['2000-12-05']
424,['eng'],"['Pásztor, G']",['Search for R-parity Violating Decays of Supersymmetric Particles at LEP'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'sparticle, pair production', 'chargino', 'neutralino', 'squark', 'slepton', 'sneutrino', 'sparticle, decay', 'R parity, violation', 'sparticle, mass', 'channel cross section, upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189-209 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012007'],"[""Searches for pair-produced charginos, neutralinos and scalar fermions decaying via R-parity violating / /\\' and /\\'' couplings with the OPAL detector at LEP are presented at sqrt(s)=189 GeV. Partial updates using data up to the highest energies of LEP, sqrt(s)=209 GeV, are also given.""]",['2000-12-05']
425,['eng'],"['Schwartz, A J']",['CP Violation and Mixing Results from FNAL E791'],['Particle Physics - Experimental Results'],"['talk, Ferrara 2000/09/18', 'pi- nucleus, inclusive reaction', 'charmed meson, hadroproduction', 'D+, hadronic decay', 'D0, hadronic decay', 'D0, semileptonic decay', 'D0 anti-D0, interference', 'violation, CP', 'mass spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012006'],"['We review results from FNAL E791 concerning D0-D0bar mixing and CP violation in D meson decays. We have searched for mixing in semileptonic D0 -> K+\\ell-\\bar{\\nu} decays and in hadronic D0 -> K+\\pi- and D0 -> K+\\pi-\\pi+\\pi- decays. We have searched for CP violation in D0 -> K+K- / \\pi+\\pi- and D+ -> \\phi\\pi+ / \\bar{K}^{*0}K+ / K+K-\\pi+ / \\pi+\\pi-\\pi+ decays. Finally, we have measured the difference in decay widths \\Delta\\Gamma between the two mass-eigenstates of the D0-D0bar system. This parameter affects the rate of D0-D0bar mixing. We combine our results with those from other experiments to obtain confidence intervals incorporating all published experimental data.']",['2000-12-20']
426,['eng'],"['Di Lodovico, F']",['First Physics Results at BABAR'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'B0, semileptonic decay', 'Kobayashi-Maskawa angle, unitarity', 'B0, lifetime', 'B0 anti-B0, oscillation', 'B0, mass difference', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> J/psi(3100) K0(S)', 'B0 --> psi(3685) K0(S)', 'B0 --> charmed meson meson', 'B0 --> charmed meson lepton neutrino', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012005'],"['The BABAR detector, which operates at the SLAC PEP-II asymmetric e^+e^- collider at energies near the Y(4S) resonance, started operation on the 26th of May 1999. We present the first study of sin2beta, with samples of B0 --> J/psi K0S and B0 --> psi(2S) K0S decays, using 9.0 fb-1 of data recorded between January and July 2000 at the Y(4S) resonance and 0.8 fb-1 recorded 40 MeV below the Y(4S) resonance. A preliminary result of sin2beta = 0.12+/-0.37 (stat) +/- 0.09 (syst) was obtained. Details of the analysis are given. Moreover, we present measurements of charged and neutral B meson lifetimes and B^0 B^0bar oscillation frequency.']",['2000-12-20']
427,['eng'],"['Engelfried, J', 'Alkhazov, G', 'Atamanchuk, A G', 'Balatz, M Y', 'Bondar, N F', 'Cooper, P S', 'Dauwe, L J', 'Davidenko, G V', 'Dersch, U', 'Dolgolenko, A G', 'Dzyubenko, G B', 'Edelstein, R M', 'Emediato, L', 'Endler, A M F', 'Eschrich, I', 'Escobar, C O', 'Evdokimov, A V', 'Filimonov, I S', 'García, F G', 'Gaspero, M', 'Giller, I', 'Golovtsov, V L', 'Gouffon, P', 'Gülmez, E', 'He Kangling', 'Iori, M', 'Jun, S Y', 'Kaya, M', 'Kilmer, J', 'Kim, V T', 'Kochenda, L M', 'Konorov, I', 'Kozhevnikov, A P', 'Krivshich, A G', 'Krüger, H', 'Kubantsev, M A', 'Kubarovskii, V P', 'Kulyavtsev, A I', 'Kuropatkin, N P', 'Kurshetsov, V F', 'Kushnirenko, A', 'Kwan, S', 'Lach, J', 'Lamberto, A', 'Landsberg, L G', 'Larin, I', 'Leikin, E M', 'Li, Y', 'Luksys, M', 'Lungov, T', 'Maleev, V P', 'Mao, D', 'Mao, C', 'Mao, Z', 'Mathew, P', 'Mattson, M E', 'Matveev, V', 'McCliment, E', 'Moinester, M A', 'Molchanov, V V', 'Morelos, A', 'Nelson, K D', 'Nemitkin, A V', 'Neoustroev, P V', 'Newsom, C', 'Nilov, A P', 'Nurushev, S B', 'Ocherashvili, A', 'Önel, Y M', 'Ozel, E', 'Ozkorucuklu, S', 'Penzo, Aldo L', 'Petrenko, S V', 'Pogodin, P I', 'Procario, M', 'Prutskoi, V A', 'Ramberg, E', 'Rappazzo, G F', 'Razmyslovich, B V', 'Rud, V I', 'Russ, J', 'Schiavon, P', 'Simón, J', 'Sitnikov, A I', 'Skow, D', 'Smith, V J', 'Srivastava, M', 'Steiner, V', 'Stepanov, V', 'Stutte, L', 'Svoiski, M', 'Terentyev, N K', 'Thomas, G P', 'Uvarov, L N', 'Vasilev, A N', 'Vavilov, D V', 'Verebryusov, V S', 'Victorov, V A', 'Vishnyakov, V E', 'Vorobyov, A A', 'Vorwalter, K', 'You, J', 'Zhao Wen Heng', 'Zheng Shu Chen', 'Zukanovich-Funchal, R']",['Recent Results on Charm and Hyperon Physics from SELEX'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'hadron nucleus, inclusive reaction', 'Sigma-, form factor', 'form factor, electric', 'pi-', 'p', 'charmed particle, hadroproduction', 'charmed particle, hadronic decay', 'charmed particle, lifetime', 'Lambda/c+', 'D0', 'D+', 'D/s', 'hyperon, hadroproduction', 'Lambda, polarization', 'Sigma+, polarization', 'differential cross section, x-dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '600 GeV/c']","['http://fnalpubs.fnal.gov/archive/2000/conf/Conf-00-309-E.html', 'http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012004']","[""The SELEX experiment (Fermilab E781) is a 3-stage magnetic spectrometer for the study of charm hadroproduction at large x_F using 600GeV/c Sigma-, pi-, and p beams. New precise measurements of the Lambda_c, D0, and Ds lifetimes are presented. Results on Lambda_c and D_s production for x_F>0.2 are reported as well. The spectrometer was also used for hyperon physics, where we will show measurements of the Sigma- charge radius, the polarization of inclusive produced Lambda's, and the polarization of beam Sigma+.""]",['2000-12-14']
428,['eng'],"['Damgov, J', 'Litov, L']",['Application of Neural Networks for Energy Reconstruction'],['Detectors and Experimental Techniques'],"['calorimeter, readout', 'scintillation counter, crystal', 'lead, tungsten', 'scintillation counter, plastics', 'jet, energy resolution', 'neural network', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012003'],"['The possibility to use Neural Networks for reconstruction of the energy deposited in the calorimetry system of the CMS detector is investigated. It is shown that using feed - forward neural network, good linearity, Gaussian energy distribution and good energy resolution can be achieved. Significant improvement of the energy resolution and linearity is reached in comparison with other weighting methods for energy reconstruction.']",['2000-12-20']
429,['eng'],"['Hoshina, K', 'Fujii, K', 'Khalatyan, N S', 'Nitoh, O', 'Okuno, H', 'Kato, Y', 'Kobayashi, M', 'Kurihara, Y', 'Kuroiwa, H', 'Nakamura, Y', 'Sakieda, K', 'Suzuki, Y', 'Watanabe, T']",['Lorentz Angle Measurement for CO2/Isobutane Gas Mixtures'],['Particle Physics - Experimental Results'],"['electron positron, linear collider', 'linear collider, proposed', 'electron positron, colliding beam detector', 'drift chamber, gas', 'organic compounds', 'magnetic field', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012002'],"['We have developed a Lorentz angle measurement system for cool gas mixtures in the course of our R&D for a proposed JLC central drift chamber (JLC-CDC). The measurement system is characterized by the use of two laser beams to produce primary electrons and flash ADCs to read their signals simultaneously. With this new system, we have measured Lorentz angles for CO2/isobutane gas mixtures with different proportions (95:5, 90:10, and 85:15), varying drift field from 0.6 to 2.0 kV/cm and magnetic field up to 1.5 T. The results of the measurement are in good agreement with GARFIELD/MAGBOLTZ simulations.']",['2000-12-20']
430,['eng'],"['Romalis, M V', 'Griffith, W C', 'Fortson, E Norval']",['A new limit on the permanent electric dipole moment of ^{199}Hg'],['Particle Physics - Experimental Results'],"['atom, electric moment', 'upper limit', 'mercury, atom', 'energy levels, transition', 'electric field, external field', 'magnetic field, external field', 'radiation, laser', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0012001'],"['We present the first results of a new search for a permanent electric dipole moment of the ^{199}Hg atom using a UV laser. Our measurements give d(Hg)= - (1.06 +/- 0.49 +/- 0.40) 10^{-28} e cm. We interpret the result as an upper limit |d(Hg)| < 2.1 10^{-28} e cm (95% C.L.), which sets new constraints on theta_{QCD}, chromo-EDMs of the quarks, and CP violation in Supersymmetric models.']",['2000-12-20']
431,['eng'],"['Appel, J A']",['Review of Heavy-Quark Production at Fixed-Target Experiments'],['Particle Physics - Experimental Results'],"['review, Rio de Janeiro 2000/10/09', 'neutrino nucleus, inclusive reaction', 'photon nucleus, inclusive reaction', 'hadron nucleus, inclusive reaction', 'production, charm', 'production, beauty', 'cross section', 'dependence, mass number', 'quarkonium, heavy', 'quark, hadronization', 'polarization', 'quantum chromodynamics, perturbation theory', 'nonperturbative', 'particle antiparticle, asymmetry', 'transverse momentum, spectra', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011101'],"['An increasingly large amount of quality fixed-target data on heavy-quark production at fixed-target energies is appearing. This data can provide information across a range of physics topics. The topics vary from investigations of QCD predictions to the understanding of the structure of hadrons. Recent results on neutrino, photon, and hadron production of charm and beauty will be reviewed in this context. The greatest insight will come from combining multiple measurements as they relate to the physics topics, and by ensuring that the parameters used in models are consistent with all the measurements. We have not yet really entered the time when this has been done for fixed-target measurements.']",['2000-12-01']
432,['eng'],"['Battaglia, M']",['Jet Flavour Identification at the CLIC Multi-TeV $e^{+}e^{-}$ Collider'],['Detectors and Experimental Techniques'],"['talk, Batavia 2000/10/24', 'electron positron, annihilation', 'quark, beauty', 'quark, pair production', 'jet, electroproduction', 'particle identification, flavor', 'charged particle, multiplicity', 'decay, path length', 'semiconductor detector, vertex', 'numerical calculations, Monte Carlo', '3000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011099'],"['Jet flavour identification in multi-TeV e+e- collisions is expected to provide insights on new phenomena at scales beyond those probed by the LHC. The anticipated high track density and jet collimation represent a new challenge to jet tagging algorithms. A method, based on the sampling of the jet charged multiplicity, sensitive to the long decay length and large decay multiplicity of heavy flavour hadrons is proposed and the expected performances for the tagging of e+e- -> bb events at 3 TeV are discussed.']",['2000-12-01']
433,['eng'],"['Renard, F M', 'Anghinolfi, M', 'Bartalini, O', 'Bellini, V', 'Bocquet, J P', 'Capogni, M', 'Castoldi, M', 'Corvisiero, P', ""D'Angelo, A"", 'Didelez, J P', 'Salvo, R D', 'Gaulard, C', 'Gervino, G', 'Ghio, F', 'Girolami, B', 'Guidal, M', 'Hourany, E', 'Kouznetsov, V', 'Künne, R A', 'Lapik, A', 'Levi-Sandri, P', 'Llères, A', 'Moricciani, D', 'Nedorezov, V G', 'Nicoletti, L', 'Rebreyend, D', 'Rudnev, N', 'Sanzone, M', 'Schärf, C A', 'Sperduto, M L', 'Sutera, M C', 'Taiuti, M', 'Turinge, A', 'Zhao, Q', 'Zucchiatti, A']",['Differential cross section measurement of $\\eta$ photoproduction on the proton from threshold to 1100 MeV'],['Particle Physics - Experimental Results'],"['photon p, exclusive reaction', 'photon, polarized beam', 'eta, photoproduction', 'eta, radiative decay', 'angular distribution', 'channel cross section, energy dependence', 'vector meson, exchange', 'partial wave analysis, multipole', 'model, coupled channel', 'N(1535)', 'four-pi-detector, experimental results', 'Grenoble ESRF', 'photon p --> p eta', '< 1.1 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011098'],"['Measurement of the differential cross section for the reaction p(gamma, eta p) is presented from threshold to 1100 MeV photon laboratory energy. The experiment has been performed using the GRAAL facility in Grenoble. For the first time, the region of the S11(1535) is fully covered, allowing a precise extraction of its width. Above 900 MeV, s-wave dominance disappears while p and d-waves take over. A discussion about their origin is given, suggesting unexpected contribution from vector meson exchange or the need for ""missing"" resonances.']",['2000-12-01']
434,['eng'],"['Schune, M H']",['Physics results from BABAR and prospects'],['Particle Physics - Experimental Results'],"['talk, Ferrara 2000/09/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, semileptonic decay', 'B0, lifetime', 'B+, lifetime', 'B0 anti-B0, interference', 'B0, mass difference', 'Kobayashi-Maskawa angle, unitarity', 'lepton, charge', 'charmed meson, final state', 'B, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'proposed experiment', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011100'],"['The BABAR experiment has been taking data since about one year. Physics results, complementary to those described by G.Sciolla elsewhere in these Proceedings, are presented: various measurements of the neutral and charged B mesons lifetimes, the B^0 mixing frequency, the mistag fractions, and the B --> D_s^(*) X and B^0 --> D_s^(*)+ D^* branching ratios. Some prospects for the close future are shown. All the numbers given here are preliminary.']",['2000-12-01']
435,['eng'],"['Bellantoni, L']","['Rare Decay Results from KTeV and $(\\rho_{CKM}, \\eta_{CKM})$']",['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 2000/10/09', 'K0(L), rare decay', 'K0(L), leptonic decay', 'K0(L), radiative decay', 'K0(L), semileptonic decay', 'Kobayashi-Maskawa angle', 'violation, flavor', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011097'],"['Rare decay results from KTeV are reviewed, emphasizing modes that in principle provide information about the CKM matrix. Our recent results in lepton flavor violating modes are also presented.']",['2000-11-30']
436,['eng'],"['Vuagnin, G']",['B decays to $D_{s}^{(*)}$ and $D^{*}$'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'charmed meson, pair production', 'D*(2010)', 'D/s', 'D/s*(2110)', 'B0, branching ratio', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> 2charmed meson', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011096'],['The e+e- annihilation data recorded with the BABAR detector has been used to study B^0 decays to Ds^(*)+ and D^*-$ mesons. The production fraction of inclusive Ds^(*)+ and the corresponding momentum spectra have been determined. Exclusive decays B^0 --> D^*- Ds^(*)+ have been identified with a partial reconstruction technique and their branching ratios have been measured. Fully reconstructed B^0 decays in the hadronic modes B^0 --> D^*- pi+ andB^0 --> D^*- rho+ have been also studied and the measurement of their absolute branching fractions is reported.'],['2000-11-30']
437,['eng'],"['Fleming, B T', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Formaggio, J A', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McFarland, K S', 'McNulty, C', 'Mishra, S R', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Sciulli, F J', 'Seligman, W G', 'Shaevitz, M H', 'Smith, W H', 'Spentzouris, P', 'Stern, E G', 'Vakili, M', 'Vaitaitis, A G', 'Vakili, M', 'Yang, U K', 'Yu, J', 'Zeller, G P', 'Zimmerman, E D']",['Recent Structure Function Results from CCFR'],['Particle Physics - Experimental Results'],"['talk, Hanoi 2000/07/19', 'neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'charged current', 'nucleon, structure function', 'small-x', 'momentum transfer, low', 'structure function, x-dependence', 'momentum transfer, dependence', 'muon nucleus, deep inelastic scattering', 'iron', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011095'],['A new structure function analysis of CCFR deep inelastic nu-N and nubar-N scattering data is presented for previously unexplored kinematic regions down to Bjorken x=0.0045 and Q^2=0.3 GeV^2. Comparisons to charged lepton scattering data from NMC and E665 experiments are made and the behavior of the structure function F2_nu is studied in the limit Q^2 -> 0'],['2000-11-30']
438,['eng'],"['Fleming, B T', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Formaggio, J A', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McFarland, K S', 'McNulty, C', 'Mishra, S R', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Sciulli, F J', 'Seligman, W G', 'Shaevitz, M H', 'Smith, W H', 'Spentzouris, P', 'Stern, E G', 'Suwonjandee, N', 'Vaitaitis, A G', 'Vakili, M', 'Yang, U K', 'Yu, J', 'Zeller, G P', 'Zimmerman, E D']",['A First Measurement of Low x Low $Q^{2}$ Structure Functions in Neutrino Scattering'],['Particle Physics - Experimental Results'],"['neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'charged current', 'nucleon, structure function', 'small-x', 'momentum transfer, low', 'structure function, x-dependence', 'momentum transfer, dependence', 'muon nucleus, deep inelastic scattering', 'iron', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011094'],['A new structure function analysis of CCFR deep inelastic nu-N and nubar-N scattering data is presented for previously unexplored kinematic regions down to Bjorken x=0.0045 and Q^2=0.3 GeV^2. Comparisons to charged lepton scattering data from NMC and E665 experiments are made and the behavior of the structure function F2_nu is studied in the limit Q^2 -> 0.'],['2000-11-30']
439,['eng'],"['Alavi-Harati, A', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barker, A R', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hamm, J', 'Hanagaki, K', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jensen, D A', 'Kessler, R', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian R"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S R', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Shields, J', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Suzuki, I', 'Swallow, E C', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Turner, S E', 'Uchizawa, T', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['First observation of the decay $K_{L} \\to \\pi^{0}e^{+}e^{-}\\gamma$'],['Particle Physics - Experimental Results'],"['K0(L), radiative decay', 'K0(L), rare decay', 'K0(L), branching ratio', 'perturbation theory, chiral', 'decay, amplitude analysis', 'vector meson, exchange', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi0 positron electron photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011093'],"['We report on the first observation of the decay KL -> pi0 ee gamma by the KTeV E799 experiment at Fermilab. Based upon a sample of 48 events with an estimated background of 3.6 +/- 1.1 events, we measure the KL -> pi0 ee gamma branching ratio to be (2.34 +/- 0.35 +/- 0.13)x10^{-8}. Our data agree with recent O(p^6) calculations in chiral perturbation theory that include contributions from vector meson exchange through the parameter a_V. A fit was made to the KL -> pi0 ee gamma data for a_V with the result -0.67 +/- 0.21 +/- 0.12, which is consistent with previous results from KTeV.']",['2000-11-29']
440,['eng'],"['Andersen, E', 'Blaes, R', 'Brom, J M', 'Cherney, M', 'de la Cruz, B', 'Fernández, C', 'Garabatos, C', 'Garzón, J A', 'Geist, W M', 'Greiner, D E', 'Gruhn, C R', 'Hafidouni, M', 'Hrubec, Josef', 'Jones, P G', 'Judd, E G', 'Kuipers, J P M', 'Ladrem, M', 'Ladrón de Guevara, P', 'Løvhøiden, G', 'MacNaughton, J N', 'Mosquera, J', 'Natkaniec, Z', 'Nelson, J M', 'Neuhofer, Günther', 'Pérez de los Heros, C', 'Pló, M', 'Porth, Paul', 'Powell, B', 'Ramil, A', 'Rohringer, Herbert', 'Sakrejda, I', 'Thorsteinsen, T F', 'Traxler, J', 'Voltolini, C', 'Wozniak, K', 'Yañez, A', 'Zybert, R']",['Measurement of negative particle multiplicity in S-Pb collisions at 200 GeV/c per nucleon with the NA36 TPC'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'sulfur', 'lead', 'hadron, multiple production', 'negative particle, multiplicity', 'drift chamber, time projection', 'experimental results', 'CERN SPS', '200 GeV/c/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011091'],['A high statistics study of the negative multiplicity distribution from S-Pb collisions at 200 GeV/c per nucleon is presented. The NA36 TPC was used to detect charged particles; corrections are based upon the maximum entropy method.'],['2000-11-29']
441,['eng'],"['Abe, K', 'Abe, K', 'Adachi, I', 'Byoung Sup Ahn', 'Aihara, H', 'Akatsu, M', 'Alimonti, G', 'Aoki, K', 'Asai, K', 'Asai, M', 'Asano, Y', 'Aso, T', 'Aulchenko, V M', 'Aushev, T', 'Bakich, A M', 'Banas, E', 'Behari, S', 'Behera, P K', 'Beiline, D', 'Bondar, A E', 'Bozek, A', 'Browder, T E', 'Casey, B C K', 'Chang, P', 'Chao, Y', 'Cheon, B G', 'Choi, S K', 'Choi, Y', 'Doi, Y', 'Dragic, J', 'Eidelman, S', 'Enari, Y', 'Enomoto, R', 'Everton, C W', 'Fang, F', 'Fujii, H', 'Fujita, Y', 'Fukunaga, C', 'Fukushima, M', 'Garmash, A', 'Gordon, A', 'Gotow, K', 'Guler, H', 'Guo, R', 'Haba, J', 'Haji, T', 'Hamasaki, H', 'Hanagaki, K', 'Handa, F', 'Hara, K', 'Hara, T', 'Hastings, N C', 'Hayashi, K', 'Hayashii, H', 'Hazumi, M', 'Heenan, E M', 'Higuchi, I', 'Higuchi, T', 'Hirai, T', 'Hirano, H', 'Hojo, T', 'Hoshi, Y', 'Hou, W S', 'Hsu, S C', 'Huang, H C', 'Huang, Y C', 'Ichizawa, S', 'Igarashi, Y', 'Iijima, T', 'Ikeda, H', 'Ikeda, K', 'Inami, K', 'Inoue, Y', 'Ishikawa, A', 'Ishino, H', 'Itoh, R', 'Iwai, G', 'Iwasaki, H', 'Iwasaki, Y', 'Jackson, D J', 'Jalocha, P', 'Jang, H K', 'Jones, M', 'Kagan, R', 'Kakuno, H', 'Kaneko, J', 'Kang, J H', 'Kang, J S', 'Kapusta, P', 'Kasami, K', 'Katayama, N', 'Kawai, H', 'Kawai, M', 'Kawamura, N', 'Kawasaki, T', 'Kichimi, H', 'Kim, D W', 'Kim, H J', 'Hyunwoo Kim', 'Kim, S K', 'Kinoshita, K', 'Kobayashi, S', 'Koike, S', 'Koishi, S', 'Konishi, H', 'Korotushenko, K', 'Krokovnyi, P P', 'Kulasiri, R', 'Kumar, S', 'Kuniya, T', 'Kurihara, E', 'Kuzmin, A', 'Kwon, Y J', 'Lee, M H', 'Lee, S H', 'Leonidopoulos, C', 'Li, H B', 'Lu, R S', 'Makida, Y', 'Manabe, A', 'Marlow, D', 'Matsubara, T', 'Matsuda, T', 'Matsui, S', 'Matsumoto, S', 'Matsumoto, T', 'Miyabayashi, K', 'Miyake, H', 'Miyata, H', 'Moffitt, L C', 'Mohapatra, A', 'Moloney, G R', 'Moorhead, G F', 'Mori, S', 'Mori, T', 'Murakami, A', 'Nagamine, T', 'Nagasaka, Y', 'Nagashima, Y', 'Nakadaira, T', 'Nakano, E', 'Nakao, M', 'Nakazawa, H', 'Nam, J W', 'Narita, S', 'Natkaniec, Z', 'Neichi, K', 'Nishida, S', 'Nitoh, O', 'Noguchi, S', 'Nozaki, T', 'Ogawa, S', 'Ohshima, T', 'Ohshima, Y', 'Okabe, T', 'Okazaki, T', 'Okuno, S', 'Olsen, S L', 'Ozaki, H', 'Pakhlov, P', 'Palka, H', 'Park, C S', 'Park, C W', 'Park, H', 'Peak, L S', 'Peters, M', 'Piilonen, L E', 'Prebys, E J', 'Raaf, J', 'Rodríguez, J L', 'Root, N', 'Rózanska, M', 'Rybicki, K', 'Ryuko, J', 'Sagawa, H', 'Sakai, Y', 'Sakamoto, H', 'Sakaue, H', 'Satapathy, M', 'Sato, N', 'Satpathy, A', 'Schrenk, S', 'Semenov, S V', 'Sevior, M E', 'Shibuya, H', 'Shwartz, B A', 'Sidorov, A', 'Sidorov, V', 'Stanic, S', 'Sugi, A', 'Sugiyama, A', 'Sumisawa, K', 'Sumiyoshi, T', 'Suzuki, J', 'Suzuki, K', 'Suzuki, S', 'Suzuki, S Y', 'Swain, S K', 'Tajima, H', 'Takahashi, T', 'Takasaki, F', 'Takita, M', 'Tamai, K', 'Tamura, N', 'Tanaka, J', 'Tanaka, M', 'Tanaka, Y', 'Taylor, G N', 'Teramoto, Y', 'Tomoto, M', 'Tomura, T', 'Tovey, S N', 'Trabelsi, K', 'Tsuboyama, T', 'Tsujita, Y', 'Tsukamoto, T', 'Tsukamoto, T', 'Uehara, S', 'Ueno, K', 'Ujiie, N', 'Unno, Y', 'Uno, S', 'Ushiroda, Y', 'Usov, Y', 'Vahsen, S E', 'Varner, G', 'Varvell, K E', 'Wang Chao Cheng', 'Wang, C H', 'Wang, M Z', 'Wang, T J', 'Watanabe, Y', 'Won, E', 'Yabsley, B D', 'Yamada, Y', 'Yamaga, M', 'Yamaguchi, A', 'Yamaguchi, H', 'Yamaoka, H', 'Yamaoka, Y', 'Yamashita, Y', 'Yamauchi, M', 'Yanaka, S', 'Yokoyama, M', 'Yoshida, K', 'Yusa, Y', 'Yuta, H', 'Zhang, C C', 'Zhao, H W', 'Zheng, Y', 'Zhilich, V N']",['Measurement of $B^{0}_{d} - \\overline{B}^{0}_{d}$ mixing rate from the time evolution of dilepton events at the $\\Upsilon(4S)$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, semileptonic decay', 'B0 anti-B0, interference', 'B0, mass difference', 'yield, dilepton', 'charge, dilepton', 'asymmetry', 'time dependence', 'violation, CPT', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011090'],"['We report a determination of the B0d - B0d-bar mixing parameter Delta-m_d based on the time evolution of dilepton yields in Upsilon(4S) decays. The measurement is based on a 5.9 /fb data sample collected by the Belle detector at KEKB. The proper-time difference distributions for same-sign and opposite-sign dilepton events are simultaneously fitted to an expression containing Delta-m_d as a free parameter. Using both muons and electrons, we obtain Delta-m_d = 0.463 +- 0.008(stat.) +- 0.016(sys.) ps^{-1} This is the first determination of Delta-m_d from time evolution measurements at the Upsilon(4S). We also place limits on possible CPT violations.']",['2000-11-29']
442,['eng'],"['Vaiciulis, A W']",['Top Production Properties at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Hanoi 2000/07/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, hadroproduction', 'channel cross section', 'mass spectrum, (quark antiquark)', 'transverse momentum, spectra', 'electroweak interaction, validity test', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']","['http://fnalpubs.fnal.gov/archive/2000/conf/Conf-00-312-E.html', 'http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011088']","['Following the confirmation of the top quark discovery at the Tevatron, the next step is to begin studying its properties. Because the scale of electroweak symmetry breaking is of the same order as the measured top mass, the top quark may be very sensitive to new physics. We describe measurements of the total top-antitop cross section, the top-antitop invariant mass, the top transverse momentum distribution, and single top production from Run 1 data at D0 and CDF. All of these measurements will become more precise in Run 2.']",['2000-12-20']
443,['eng'],"['Ellis, Jonathan Richard']",['The 115 GeV Higgs Odyssey'],['Particle Physics - Experimental Results'],"['Higgs particle, search for', 'Higgs particle, mass', 'electron positron, annihilation', 'hadron hadron, interaction', 'supersymmetry', 'sparticle, mass', 'technicolor', 'new interaction', 'potential, Higgs', 'Higgs particle, coupling', 'numerical calculations', 'interpretation of experiments, CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011086'],"['On his way home from Troy, Odysseus had arrived within reach of Ithaca when a great storm blew up. He was swept away, and only several years later was he able to return to reclaim his rights from the rapacious suitors, with the aid of his son Telemachus. Some wonder whether this epic is repeating itself, if the Higgs weighs 115 GeV. If so, are CMS and ATLAS cast in the role of Telemachus? In this paper, I first discuss how close to Ithaca LEP may have been, the fact that a 115 GeV Higgs boson would disfavour technicolour, its potential implications for supersymmetry, and finally the prospects for completing the Higgs Odyssey.']",['2000-12-20']
444,['eng'],"['Battaglia, M', 'Schulte, D']",['Study of $\\gamma\\gamma$ Background in $e^{+}e^{-} \\to W^{+}W^{-}\\nu\\overline{\\nu} \\to H^{0}\\nu\\overline{\\nu}$ Events at the TESLA $e^{+}e^{-}$ Linear Collider'],['Particle Physics - Experimental Results'],"['talk, Padua 2000//05/05', 'electron positron, annihilation', 'W, pair production', 'neutrino, pair production', 'fusion, W W', 'Higgs particle, production', 'background, two-photon', 'Higgs particle, hadronic decay', 'quark, beauty', 'quark, pair production', 'mass spectrum, (2jet)', 'mass spectrum, recoil', 'numerical calculations, Monte Carlo', 'electron positron --> W+ W- neutrino antineutrino', 'W+ W- --> Higgs particle', 'photon photon --> (n)hadron', '350 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011085'],"['The effect of the overlap of gamma gamma -> hadrons to H nu nu events has been studied for the case of the Tesla e+e- linear collider at 350 GeV. It was found that, due to the significant bunch length and the track extrapolation accuracy provided by the Vertex Tracker, the gamma gamma background to physics events can be substantially reduced, with moderate loss in reconstruction efficiency, by a combination of kinematical and vertex topology observables. The remaining background, being confined to very forward hadron production, does not significantly interfere with the event reconstruction.']",['2000-12-20']
445,['eng'],"['Bandourin, D V', 'Konoplyanikov, V F', 'Skachkov, N B']","['Jet energy scale setting with ""photon+Jet"" events at LHC energies. Minijets and cluster suppression and photon Pt - jet Pt disbalance']",['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'jet, hadroproduction', 'photon, associated production', 'transverse momentum, (jet photon)', 'jet, energy', 'minijet', 'cluster', 'numerical calculations, Monte Carlo', '14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011084'],"['In this paper the study of ""photon+Jet"" events is continued and the event number determination useful for jet energy scale setting with the possible CMS detector hadron calorimeter calibration at LHC is fulfiled. The sources of photon Pt and jet Pt disbalance are exposed. It is shown that the cluster Pt limitation, which is found in an event outside of the jet, can be a good criterion for this disbalance decreasing.']",['2000-12-20']
446,['eng'],"['Hüttmann, K']",['Measurement of the $B^{0}$ and $B^{-}$ meson lifetimes in ALEPH'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'B, semileptonic decay', 'D*(2010)', 'B0, lifetime', 'B-, lifetime', 'correlation, (charmed meson lepton-)', 'D0, hadronic decay', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'B0 --> D*(2010) lepton anything', 'B- --> D0 lepton- anything', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011083'],['The lifetimed of the Bbar0 and B- meson lifetimes are measured using data recorded on the Z peak with the ALEPH detector at LEP. An improved analysis based on partially reconstructed Bbar0 -> D*+l-nubar and B- -> D0l-nubar decays is presented.'],['2000-12-20']
447,['eng'],"['Rosca, A']",['Search for a Higgs Boson Decaying into Two Photons with the L3 Detector at LEP'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, radiative decay', 'mass spectrum, two-photon', 'Z0, hadronic decay', 'Z0, leptonic decay', 'Higgs particle, mass', 'lower limit', 'Higgs particle, branching ratio', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'Higgs particle --> 2photon', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011082'],"['A search is performed for a Higgs boson, decaying into two photons, using the L3 data collected at centre of mass energies between $\\sqrt s$ = 189 and 202 GeV, corresponding to an integrated luminosity of 400 pb$^{-1}$. The processes $e^{+}e^{-}\\to {Zh} \\to {q} \\bar{q} \\gamma \\gamma $, $e^{+}e^{-}\\to {Zh} \\to \\nu \\bar{\\nu} \\gamma \\gamma $, $e^{+}e^{-}\\to {Zh} \\to {l}^{+} {l}^{-} \\gamma \\gamma $ are considered. The observed data are found to be consistent with the expected background from standard physics processes. Limits on the branching fraction of the Higgs boson decay into two photons as a function of the Higgs mass are shown and a lower mass limit on a fermiophobic Higgs is derived.']",['2000-11-24']
448,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Sartorelli, G', 'Zichichi, Antonino', 'Aghuzumtsyan, G', 'Amelung, C', 'Brock, I', 'Coboken, K', 'Goers, S', 'Hartmann, H', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Kind, O', 'Paul, E', 'Rautenberg, J', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Cole, J E', 'Foster, B', 'Heath, G P', 'Heath, H F', 'Robins, S A', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Borras, K', 'Chiochia, V', 'Crittenden, J A', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hebbel, K', 'Hillert, S', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Labes, H', 'Löhr, B', 'Mankel, R', 'Martens, J', 'Martínez, M', 'Milite, M', 'Moritz, M', 'Notz, D', 'Petrucci, M C', 'Polini, A', 'Rohde, M', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Parenti, A', 'Pelfer, P G', 'Bamberger, Andreas', 'Benen, A', 'Coppola, N', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Bell, M', 'Doyle, A T', 'Glasman, C', 'Lee, S W', 'Lupi, A', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bodmann, B', 'Gendner, N', 'Holm, U', 'Salehi, H', 'Wick, K', 'Yildirim, A', 'Carli, T', 'Garfagnini, A', 'Geiser, A', 'Gialas, I', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Boos, E G', 'Pokrovskiy, N S', 'Zhautykov, B O', 'Barakbaev, A N', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Son, D', 'Barreiro, F', 'García, G', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Vázquez, M E', 'Barbi, M S', 'Corriveau, F', 'Padhi, S', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Antonov, A', 'Bashkirov, V', 'Danilov, M V', 'Dolgoshein, B A', 'Gladkov, D', 'Sosnovtsev, V V', 'Suchkov, S', 'Dementiev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Shcheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tassi, E', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dusini, S', 'Limentani, S', 'Longhin, A', 'Posocco, M', 'Stanco, L', 'Turcato, M', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Saull, P R B', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C', 'Park, I H', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Gabareen, A', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Kohno, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Matsuzawa, K', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Mirea, A', 'Sabetfakhri, A', 'Butterworth, J M', 'Gwenlan, C', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Pawlak, R', 'Smalska, B', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A']",['Measurement of open beauty production in photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'quark, beauty', 'quark, photoproduction', 'quark, semileptonic decay', 'ionization, energy loss', 'channel cross section', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet positron electron anything', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011081'],"['The production and semi-leptonic decay of heavy quarks have been studied in the photoproduction process $e^+p -> e^+ + {dijet} + e^- + X with the ZEUS detector at HERA using an integrated luminosity of 38.5 ${\\rm pb^{-1}}$. Events with photon-proton centre-of-mass energies, $W_{\\gamma p}$, between 134 and 269 GeV and a photon virtuality, Q^2, less than 1 ${\\rm GeV^2}$ were selected requiring at least two jets of transverse energy $E_T^{\\rm jet1(2)} >7(6)$ GeV and an electron in the final state. The electrons were identified by employing the ionisation energy loss measurement. The contribution of beauty quarks was determined using the transverse momentum of the electron relative to the axis of the closest jet, $p_T^{\\rm rel}$. The data, after background subtraction, were fit with a Monte Carlo simulation including beauty and charm decays. The measured beauty cross section was extrapolated to the parton level with the b quark restricted to the region of transverse momentum $p_T^{b} > p_T^{\\rm min} =$ 5 GeV and pseudorapidity $|\\eta^{b}| <$ 2. The extrapolated cross section is $1.6 \\pm 0.4 (stat.)^{+0.3}_{-0.5} (syst.) ^{+0.2}_{-0.4} (ext.) {nb}$. The result is compared to a perturbative QCD calculation performed to next-to-leading order.']",['2000-11-23']
449,['eng'],"['Paganis, S D']",['A Luminosity Spectrometer for the Zeus Experiment at HERA'],['Particle Physics - Experimental Results'],"['talk, Annecy 2000/10/09', 'electron p, storage ring', 'luminosity, upgrade', 'luminosity, beam monitoring', 'bremsstrahlung', 'calorimeter', 'scintillation counter', 'tungsten', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011080'],"['The HERA luminosity upgrade is expected to generate two major problems in the current method of luminosity determination which is based on counting brehmsstrahlung photons: damage of the calorimeter monitor due to high primary synchrotron radiation and large multiple event (pile-up) corrections. The luminosity spectrometer presented in this talk, is a novel method that reduces the impact of these problems in the luminosity measurement and is expected to yield a total systematic uncertainty of 1.4%. The spectrometer counts brehmsstrahlung photon conversions in the beam pipe exit window using two small calorimeters (former ZEUS beam pipe calorimeters) symmetrically placed away from the synchrotron radiation plane. The photon conversion rate is measured by counting electron-positron (ep) coincidences in the calorimeters. The ep acceptance is measured using a third calorimeter (6 meter tagger) which tags the brehmsstrahlung electrons. The electron-positron pair is separated by a small dipole magnet.']",['2000-11-23']
450,['eng'],"['Summers, D J']",['Search for Rare 3 and 4-Body $D^{0}$ Decays at FNAL E791'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'pi- nucleus, inclusive reaction', 'charmed meson, hadroproduction', 'D0, rare decay', 'rho(770)', 'K*(892)', 'Phi(1020)', 'D0, branching ratio', 'upper limit', 'violation, flavor', 'lepton number, violation', 'neutral current, flavor changing', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> vector meson lepton+ lepton-', 'D0 --> 2meson lepton+ lepton-', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011079'],"['Limits at the 10**-4 level are reported for rare and forbidden decays of the D0 charm meson to a pair of leptons and either a vector meson or two pseudoscalar mesons. Of these searches, 18 are investigations of decays without previous published results; several others have significantly improved sensitivity over previous results.']",['2000-11-22']
451,['eng'],"['Blazey, G C']",['A QCD Survey $0 \\leq Q^{2} \\leq 10^{5} GeV^{2}$'],['Particle Physics - Experimental Results'],"['review, Columbus 2000/08/09', 'anti-p p, colliding beams', 'electron p, colliding beams', 'electron positron, colliding beams', 'lepton nucleon, deep inelastic scattering', 'p nucleon, interaction', 'jet, hadroproduction', 'jet, electroproduction', 'jet, multiple production', 'mass spectrum, (2jet)', 'momentum transfer, high', 'quantum chromodynamics, validity test', 'perturbation theory, higher-order', 'Lipatov equation', 'nucleon, structure function', 'momentum spectrum, parton', 'strong interaction, coupling constant', 'momentum transfer, dependence', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011078'],"['Selected, recent results, primarily form collider experiments but including some fixed target experiments, are presented as a survey of Quantum Chromodynamics (QCD). The concepts of leading order and next-to-leading order QCD are introduced. Inclusive proton-antiproton jet and dijet production and deep inelastic electron-proton scattering at very large momentum transfer are shown to be in good agreement with perturbative QCD (pQCD). Dijet, three-jet and multi-jet results from proton-antiproton, electron-proton, and electron-electron colliders at moderate Q**2 are also compared to pQCD. BFKL searches from all three colliders are discussed. Recent measurements of structure functions and contributions to the parton distribution functions are presented. New measurements of the strong coupling constant are summarized, the world average is 0.1184 with an uncertainty of 0.0031.']",['2000-11-22']
452,['eng'],"['Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Todorova-Nová, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Copty, N K', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Fernández, A', 'Fox, G F', 'Gagnon, P', 'Göbel, C', 'Gounder, K', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lundberg, B', 'Magnin, J', 'May Tal-Beck, S', 'Meadows, B', 'De Mello-Neto, J R T', 'Mihalcea, D', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'De Oliveira, A B', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Dos Reis, A C', 'Rubin, H A', 'Sanders, D A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Slaughter, A J', 'Sokoloff, M D', 'Solano, J M', 'Stanton, N R', 'Stefanski, R J', 'Stenson, K', 'Summers, D J', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yang, S M', 'Yi, D', 'Yoshida, S', 'Zaliznyak, R', 'Zhang, C']",['Search for Rare and Forbidden Charm Meson Decays $D^{0} \\to V l^{+}l^{-}$ and $hhll$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'D0, hadroproduction', 'D0, semileptonic decay', 'neutral current, flavor changing', 'violation, flavor', 'lepton number, violation', 'lepton, pair production', 'vector meson, production', 'rho(770)0', 'K*(892)', 'Phi(1020)', 'pseudoscalar meson, pair production', 'pi', 'K', 'D0, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> vector meson lepton+ lepton-', 'D0 --> 2pseudoscalar meson lepton+ lepton-', 'D0 --> 2pseudoscalar meson 2lepton+', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011077'],"['We report the results of a search for flavor-changing neutral current, lepton-flavor, and lepton-number violating decays of the 3 and 4-body decay modes of D0 (and its antiparticle) containing muons and electrons. Using data from Fermilab charm hadroproduction experiment E791, we examine modes with two leptons and either a Rho(0), Kstar, or Phi vector meson or a non-resonant Pi Pi, K Pi, or K K pair of pseudoscalar mesons. No evidence for any of these decays is found. Therefore, we present branching-fraction upper limits at 90% confidence level for the 27 decay modes examined (18 new).']",['2000-11-22']
453,['eng'],"['Bauer, G']",['Measurement of $\\Delta-m_{d}$ Using a Probability Based Same-Side Tagger at CDF'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'anti-p p, colliding beams', 'quark, beauty', 'quark, pair production', 'B, semileptonic decay', 'B0, mass difference', 'particle identification, flavor', 'track data analysis, vertex', 'lepton, charge', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B0 --> charmed meson lepton anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011076'],"['A measurement of Delta m_d is performed using inclusive lepton+vertex events at CDF. A probability based Same-Side Tagger was developed to tag the initial b-flavor of the B^0_d, which suppresses tagging on B-decay products. We find Delta m_d = 0.42 +/- 0.09 +/- 0.03 ps^-1.']",['2000-11-22']
454,['eng'],"['Solomey, N']",['Importance of Future Hyperon Beta Decay Experiments'],['Particle Physics - Experimental Results'],"['talk, Chicago 2000/08/03', 'K0, semileptonic decay', 'hyperon, semileptonic decay', 'Xi0', 'Lambda', 'decay, form factor', 'Sigma+, hadronic decay', 'interference, (Sigma0 Lambda)', 'Kobayashi-Maskawa angle', 'magnetic spectrometer, experimental results', 'proposed experiment', 'Batavia TEVATRON PS', 'Xi0 --> Sigma+ lepton- antineutrino', 'K0 --> pi+ lepton- antineutrino', 'Sigma+ --> Lambda positron neutrino', 'Lambda --> p muon- antineutrino/mu']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011074'],"['Recent results from the KTeV experiment at Fermilab using $\\Xi^0$ hyperons have enabled a great leap in improving our understanding of elementary particle physics, especially with the first form-factor measurement from the semi-leptonic decay $\\Xi^0 \\to \\Sigma^+ e^- \\bar{\\nu}$. This decay is a test of whether the standard model contains all of the needed parameters to fully describe hyperon beta decay. It was observed for the first time only in 1997 even though its importance had been explicitly stated in 1961 by the early theories of the standard model as formulated by N. Cabibbo. We have the ability to improve this measurement substantially by making the definitive form-factor measurement with a sample of 30,000 such decays from a forthcoming experiment, which will either show or rule out the existence any additional second class weak currents, an obviously important measurement allowing particle physics to finally put this question to rest. We also have the ability to make a measurement of hyperon compositeness by measuring the charged $\\Sigma^{\\pm}$ beta decay into $\\Lambda^0$, and in addition to search for mass coupling terms in hyperon beta decays where the muon replaces the electron, important for determining the $g_3$ and $f_3$ form-factors. These are the important questions to answer in studying strange baryon decays, and are reviewed in this article.']",['2000-11-22']
455,['eng'],"['Chan, S', 'Eigen, G', 'Lipeles, E', 'Miller, J S', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, H N', 'Nelson, T K', 'Roberts, D', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Boisvert, V', 'Cassel, David G', 'Crowcroft, D S', 'Dickson, M', 'Von Dombrowski, S', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Ogg, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Soffer, A', 'Valant-Spaight, B L', 'Warburton, A', 'Ward, C', 'Athanas, M', 'Avery, P', 'Jones, C D', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Briere, R A', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Selen, M', 'Thaler, J J', 'Edwards, K W', 'Bellerive, A', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Coppage, D', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhou, L', 'Anderson, S', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Alam, M S', 'Athar, S B', 'Ling, Z', 'Mahmood, A H', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lee, J', 'Lorenc, J', 'Schwarthoff, H', 'Wolf, A', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Glenn, S', 'Kwon, Y', 'Lyon, A L', 'Roberts, S', 'Thorndike, E H', 'Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Dambasuren, E', 'Kopp, S E', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Csorna, S E', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J']",['A Measurement of the Decay Asymmetry Parameters in $\\Xi_{c}^{0}\\to \\X^{-}\\pi^{+}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, charm', 'quark, pair production', 'Xi/c0, hadronic decay', 'mass spectrum, (Xi- pi+)', 'angular distribution, asymmetry', 'violation, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Xi/c0 --> Xi- pi+', 'Xi- --> Lambda pi-', '< 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011073'],"['Using the CLEO II detector at the Cornell Electron Storage Ring we have measured the $\\Xi_c^{0}$ decay asymmetry parameter in the decay $\\Xi_c^{0} \\to \\Xi^{-} \\pi^+$. We find $\\alpha_{\\Xi_c^{0}} \\alpha_{\\Xi} = 0.26 \\pm 0.18{(stat)}^{+0.05}_{-0.04}{(syst)}$, using the world average value of $\\alpha_{\\Xi} = -0.456 \\pm 0.014$ we obtain $\\alpha_{\\Xi_c^{0}} = -0.56 \\pm 0.39{(stat)}^{+0.10}_{-0.09}{(syst)}$. The physically allowed range of a decay asymmetry parameter is $-1<\\alpha<+1$. Our result prefers a negative value: $\\alpha_{\\Xi_c^{0}}$ is $<0.1$ at the 90% CL. The central value occupies the middle of the theoretically expected range but is not yet precise enough to choose between models.']",['2000-11-22']
456,['eng'],"['Sarwar, S', 'Link, J M', 'Paolone, V S', 'Reyes, M', 'Anjos, J C', 'Yager, P M', 'Bediaga, I', 'Göbel, C', 'Magnin, J', 'De Miranda, J M', 'Pepe, I M', 'Dos Reis, A C', 'Simão, F R A', 'Carrillo, S', 'Casimiro, E', 'Méndez, H', 'Sánchez-Hernández, A', 'Uribe, C', 'Vásquez, F', 'Cinquini, L', 'Cumalat, J P', 'Ramírez, J E', ""O'Reilly, B"", 'Vaandering, E W', 'Butler, J N', 'Cheung, H W K', 'Gaines, I', 'Garbincius, P H', 'Garren, L A', 'Gottschalk, E E', 'Gourlay, S A', 'Kasper, P H', 'Kreymer, A E', 'Kutschke, R', 'Bianco, S', 'Fabbri, F L', 'Sarwar, S', 'Cawlfield, C', 'Kim, D Y', 'Park, K S', 'Rahimi, A', 'Gardner, R', 'Chung, Y S', 'Kang, J S', 'Ko, B R', 'Kwak, J W', 'Lee, K B', 'Myung, S S', 'Alimonti, G', 'Boschini, M', 'Brambilla, D', 'Caccianiga, B', 'Calandrino, A', ""D'Angelo, P"", 'Di Corato, M', 'Dini, P', 'Giammarchi, M G', 'Inzani, P', 'Leveraro, F', 'Malvezzi, S', 'Menasce, D', 'Mezzadri, M', 'Milazzo, L', 'Moroni, L', 'Pedrini, D', 'Prelz, F', 'Rovere, M', 'Sala, A', 'Sala, S', 'Arena, V', 'Boca, G', 'Bonomi, G', 'Gianini, G', 'Liguori, G', 'Merlo, M', 'Pantea, D', 'Ratti, S P', 'Riccardi, C', 'Torre, P', 'Viola, L', 'Vitulo, P', 'Hernández, Pilar', 'López, A M', 'Méndez, L', 'Mirles, M A', 'Montiel, E', 'Olaya, D', 'Quinones, J', 'Rivera, C', 'Zhang-Mayaguez, Y', 'Copty, N K', 'Purohit, M', 'Cho, K', 'Handler, T', 'Engh, D', 'Johns, W E', 'Hosack, M', 'Nehring, M S', 'Sales, M', 'Sheldon, P D', 'Stenson, K', 'Webster, M S', 'Sheaff, M', 'Kwon, Y']",['Preliminary Results on Charmed Meson Spectroscopy'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'photon nucleus, inclusive reaction', 'beryllium, oxygen', 'charmed meson, photoproduction', 'charmed meson, hadron spectroscopy', 'charmed meson, hadronic decay', 'D*2(2460), mass', 'D*2(2460), width', 'mass spectrum, (D pi)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011072'],['We report the preliminary measurement by the FOCUS Collaboration (E831 at Fermilab) of masses and widths of the L=1 charm mesons $D_2^{*0}$ and $D_2^{*+}$. The fit of the invariant mass distribution requires an additional term to account for a broad structure over background.'],['2000-11-22']
457,['eng'],"['Abbott, B', 'Abdesselam, A', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Bacon, T C', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Todorova-Nová, S', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bauer, D', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Beuselinck, R', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Duflot, L', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Filthaut, F', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gao, M', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Illingworth, R', 'Ito, A S', 'Jaffré, M', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Leggett, C', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Luo, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Nunnemann, T', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Papageorgiou, K', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Petroff, P', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Ridel, M', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P', 'Ruchti, R C', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Sen, N', 'Shabalina, E', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['A Quasi-Model-Independent Search for New High $p_{T}$ Physics at DZero'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, exclusive reaction', 'transverse momentum, high', 'jet, hadroproduction', 'intermediate boson, hadroproduction', 'photon, hadroproduction', 'lepton, hadroproduction', 'transverse energy, missing-energy', 'data analysis method', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011071'],"['We apply a quasi-model-independent strategy (""Sleuth"") to search for new high p_T physics in approximately 100 pb^-1 of ppbar collisions at sqrt(s) = 1.8 TeV collected by the DZero experiment during 1992-1996 at the Fermilab Tevatron. We systematically analyze many exclusive final states and demonstrate sensitivity to a variety of models predicting new phenomena at the electroweak scale. No evidence of new high p_T physics is observed.']",['2000-11-22']
458,['eng'],"['Acciarri, M', 'Achard, P', 'Adriani, O', 'Aguilar-Benítez de Lugo, M', 'Alcaraz, J', 'Alemanni, G', 'Allaby, James V', 'Aloisio, A', 'Alviggi, M G', 'Ambrosi, G', 'Anderhub, H', 'Andreev, V P', 'Angelescu, T', 'Anselmo, F', 'Arefev, A', 'Azemoon, T', 'Aziz, T', 'Bagnaia, P', 'Bajo, A', 'Baksay, L', 'Balandras, A', 'Baldew, S V', 'Todorova-Nová, S', 'Banerjee, Sw', 'Barczyk, A', 'Barillère, R', 'Bartalini, P', 'Basile, M', 'Batalova, N', 'Battiston, R', 'Bay, A', 'Becattini, F', 'Becker, U', 'Behner, F', 'Bellucci, L', 'Berbeco, R', 'Berdugo, J', 'Berges, P', 'Bertucci, B', 'Betev, B L', 'Bhattacharya, S', 'Biasini, M', 'Biland, A', 'Blaising, J J', 'Blyth, S C', 'Bobbink, Gerjan J', 'Böhm, A', 'Boldizsar, L', 'Borgia, B', 'Bourilkov, D', 'Bourquin, Maurice', 'Braccini, S', 'Branson, J G', 'Brochu, F', 'Buffini, A', 'Buijs, A', 'Burger, J D', 'Burger, W J', 'Cai, X D', 'Capell, M', 'Cara Romeo, G', 'Carlino, G', 'Cartacci, A M', 'Casaus, J', 'Castellini, G', 'Cavallari, F', 'Cavallo, N', 'Cecchi, C', 'Cerrada-Canales, M', 'Cesaroni, F', 'Chamizo-Llatas, M', 'Chang, Y H', 'Chaturvedi, U K', 'Chemarin, M', 'Chen, A', 'Chen, G', 'Chen, G M', 'Chen, H F', 'Chen, H S', 'Chiefari, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Civinini, C', 'Clare, I', 'Clare, R', 'Coignet, G', 'Colino, N', 'Costantini, S', 'Cotorobai, F', 'de la Cruz, B', 'Csilling, Akos', 'Cucciarelli, S', 'Dai, T S', 'van Dalen, J A', ""D'Alessandro, R"", 'De Asmundis, R', 'Déglon, P L', 'Degré, A', 'Deiters, K', 'Della Volpe, D', 'Delmeire, E', 'Denes, P', 'De Notaristefani, F', 'De Salvo, A', 'Diemoz, Marcella.', 'Dierckxsens, M', 'Van Dierendonck, D N', 'Dionisi, C', 'Dittmar, Michael', 'Dominguez, A', 'Doria, A', 'Dova, M T', 'Duchesneau, D', 'Dufournaud, D', 'Duinker, P', 'Durán, I', 'El-Mamouni, H', 'Engler, A', 'Eppling, F J', 'Erné, Frits C', 'Ewers, A', 'Extermann, Pierre', 'Fabre, M', 'Falagán, M A', 'Falciano, S', 'Favara, A', 'Fay, J', 'Fedin, O', 'Felcini, Marta', 'Ferguson, T', 'Fesefeldt, H S', 'Fiandrini, E', 'Field, J H', 'Filthaut, F', 'Fisher, P H', 'Fisk, I', 'Forconi, G', 'Freudenreich, Klaus', 'Furetta, C', 'Galaktionov, Yu', 'Ganguli, S N', 'García-Abia, P', 'Gataullin, M', 'Gau, S S', 'Gentile, S', 'Gheordanescu, N', 'Giagu, S', 'Gong, Z F', 'Grenier, G', 'Grimm, O', 'Grünewald, M W', 'Guida, M', 'van Gulik, R', 'Gupta, V K', 'Gurtu, A', 'Gutay, L J', 'Haas, D', 'Hasan, A', 'Hatzifotiadou, D', 'Hebbeker, T', 'Hervé, Alain', 'Hidas, P', 'Hirschfelder, J', 'Hofer, H', 'Holzner, G', 'Hoorani, H', 'Hou, S R', 'Hu, Y', 'Iashvili, I', 'Jin, B N', 'Jones, L W', 'de Jong, P', 'Josa-Mutuberria, I', 'Khan, R A', 'Käfer, D', 'Kaur, M', 'Kienzle-Focacci, M N', 'Kim, D', 'Kim, J K', 'Kirkby, Jasper', 'Kiss, D', 'Kittel, E Wolfram', 'Klimentov, A', 'König, A C', 'Kopal, M', 'Kopp, A', 'Koutsenko, V F', 'Kräber, M H', 'Krämer, R W', 'Krenz, W', 'Krüger, A', 'Kunin, A', 'Ladrón de Guevara, P', 'Laktineh, I', 'Landi, G', 'Lebeau, M', 'Lebedev, A', 'Lebrun, Philippe.', 'Lecomte, P', 'Lecoq, P', 'Le Coultre, P', 'Lee, H J', 'Le Goff, J M', 'Leiste, R', 'Levchenko, P M', 'Li Chuan', 'Likhoded, S A', 'Lin, C H', 'Lin, W T', 'Linde, F L', 'Lista, L', 'Liu, Z A', 'Lohmann, W', 'Longo, E', 'Lü, Y S', 'Lübelsmeyer, K', 'Luci, C', 'Luckey, D', 'Lugnier, L', 'Luminari, L', 'Lustermann, W', 'Ma, W G', 'Maity, M', 'Malgeri, L', 'Malinin, A', 'Maña, C', 'Mangeol, D J', 'Mans, J', 'Marian, G', 'Martin, J P', 'Marzano, F', 'Mazumdar, K', 'McNeil, R R', 'Mele, S', 'Merola, L', 'Meschini, M', 'Metzger, W J', 'Von der Mey, M', 'Mihul, A', 'Milcent, H', 'Mirabelli, G', 'Mnich, J', 'Mohanty, G B', 'Moulik, T', 'Muanza, G S', 'Muijs, A J M', 'Musicar, B', 'Musy, M', 'Napolitano, M', 'Nessi-Tedaldi, F', 'Newman, H', 'Niessen, T', 'Nisati, A', 'Nowak, H', 'Ofierzynski, R A', 'Organtini, G', 'Oulianov, A', 'Palomares, C', 'Pandoulas, D', 'Paoletti, S', 'Paolucci, P', 'Paramatti, R', 'Park, H K', 'Park, I H', 'Passaleva, G', 'Patricelli, S', 'Paul, T', 'Pauluzzi, M', 'Paus, C', 'Pauss, Felicitas', 'Pedace, M', 'Pensotti, S', 'Perret-Gallix, D', 'Petersen, B', 'Piccolo, D', 'Pierella, F', 'Pieri, M', 'Piroué, P A', 'Pistolesi, E', 'Plyaskin, V', 'Pohl, M', 'Pozhidaev, V', 'Postema, H', 'Pothier, J', 'Prokofiev, D O', 'Prokofev, D', 'Quartieri, J', 'Rahal-Callot, G', 'Rahaman, M A', 'Raics, P', 'Raja, N', 'Ramelli, R', 'Rancoita, P G', 'Ranieri, R', 'Raspereza, A V', 'Raven, G', 'Razis, P A', 'Ren, D', 'Rescigno, M', 'Reucroft, S', 'Riemann, S', 'Riles, K', 'Rodin, J', 'Roe, B P', 'Romero, L', 'Rosca, A', 'Rosier-Lees, S', 'Roth, S', 'Rosenbleck, C', 'Rubio, Juan Antonio', 'Ruggiero, G', 'Rykaczewski, H', 'Saremi, S', 'Sarkar, S', 'Salicio, J', 'Sánchez, E', 'Sanders, M P', 'Schäfer, C', 'Shchegelskii, V', 'Schmidt-Kärst, S', 'Schmitz, D', 'Schopper, Herwig Franz', 'Schotanus, D J', 'Schwering, G', 'Sciacca, C', 'Seganti, A', 'Servoli, L', 'Shevchenko, S', 'Shivarov, N', 'Shoutko, V', 'Shumilov, E', 'Shvorob, A V', 'Siedenburg, T', 'Son, D', 'Smith, B', 'Spillantini, P', 'Steuer, M', 'Stickland, D P', 'Stone, A', 'Stoyanov, B', 'Strässner, A', 'Sudhakar, K', 'Sultanov, G G', 'Sun, L Z', 'Sushkov, S V', 'Suter, H', 'Swain, J D', 'Szillasi, Z', 'Sztaricskai, T', 'Tang, X W', 'Tauscher, Ludwig', 'Taylor, L', 'Tellili, B', 'Timmermans, C', 'Ting, S C C', 'Ting, S M', 'Tonwar, S C', 'Tóth, J', 'Tully, C', 'Tung, K L', 'Uchida, Y', 'Ulbricht, J', 'Valente, E', 'Vesztergombi, György', 'Vetlitskii, I', 'Vicinanza, D', 'Viertel, Gert M', 'Villa, S', 'Vivargent, M', 'Vlachos, S', 'Vodopyanov, I', 'Vogel, H', 'Vogt, H', 'Vorobev, I', 'Vorobyov, A A', 'Vorvolakos, A', 'Wadhwa, M', 'Wallraff, W', 'Wang, M', 'Wang, X L', 'Wang, Z M', 'Weber, A', 'Weber, M', 'Wienemann, P', 'Wilkens, H', 'Wu, S X', 'Wynhoff, S', 'Xia, L', 'Xu, Z Z', 'Yamamoto, J', 'Yang, B Z', 'Yang, C G', 'Yang, H J', 'Yang, M', 'Ye, J B', 'Yeh, S C', 'Zalite, A', 'Zalite, Yu', 'Zhang, Z P', 'Zhu, G Y', 'Zhu, R Y', 'Zichichi, Antonino', 'Zilizi, G', 'Zimmermann, B', 'Zöller, M']",['Measurements of the Cross Sections for Open Charm and Beauty Production in $\\gamma\\gamma$ Collisions at $\\sqrt{s}$ = 189-202 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, inclusive reaction', 'quark, charm', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'lepton, particle identification', 'channel cross section, energy dependence', 'quantum chromodynamics', 'perturbation theory, higher-order', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2beauty positron electron anything', 'electron positron --> 2charm positron electron anything', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011070'],"['The production of c and b quarks in gamma-gamma collisions is studied with the L3 detector at LEP with 410 pb^-1 of data, collected at centre-of-mass energies from 189 GeV to 202 GeV. Hadronic final states containing c and b quarks are identified by detecting electrons or muons from their semileptonic decays. The cross sections sigma(e+e- -> e+e- c c~ X) and sigma(e+e- -> e+e- b b~ X) are measured and compared to next-to-leading order perturbative QCD calculations. The cross section of b production is measured in gamma-gamma collisions for the first time. It is in excess of the QCD prediction by a factor of three.']",['2000-11-22']
459,['eng'],"['Giunti, C', 'Laveder, M']",['The Power of Confidence Intervals'],['Particle Physics - Experimental Results'],"['statistical analysis', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011069'],"['We consider the power to reject false values of the parameter in Frequentist methods for the calculation of confidence intervals. We connect the power with the physical significance (reliability) of confidence intervals for a parameter bounded to be non-negative. We show that the confidence intervals (upper limits) obtained with a (biased) method that near the boundary has large power in testing the parameter against larger alternatives and small power in testing the parameter against smaller alternatives are physically more significant. Considering the recently proposed methods with correct coverage, we show that the physical significance of upper limits is smallest in the Unified Approach and highest in the Maximum Likelihood Estimator method. We illustrate our arguments in the specific cases of a bounded Gaussian distribution and a Poisson distribution with known background.']",['2000-11-22']
460,['eng'],"['Abbott, B', 'Abdesselam, A', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Bacon, T C', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Todorova-Nová, S', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bauer, D', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Beuselinck, R', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Duflot, L', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Filthaut, F', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gao, M', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Illingworth, R', 'Ito, A S', 'Jaffré, M', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Leggett, C', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Luo, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Nunnemann, T', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Papageorgiou, K', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Petroff, P', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Ridel, M', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P', 'Ruchti, R C', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Sen, N', 'Shabalina, E', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['A Quasi-Model-Independent Search for New Physics at Large Transverse Momentum'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'transverse momentum, high', 'new particle, search for', 'new interaction, search for', 'transverse energy, missing-energy', 'electroweak interaction, validity test', 'intermediate boson, hadroproduction', 'jet, associated production', 'lepton, multiple production', 'photon, multiple production', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'anti-p p --> muon electron anything', 'anti-p p --> intermediate boson (n)jet', 'anti-p p --> 2lepton photon anything', 'anti-p p --> lepton 2photon anything', 'anti-p p --> 3lepton photon anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011067'],"['We apply a quasi-model-independent strategy (""Sleuth"") to search for new high p_T physics in approximately 100 pb^-1 of ppbar collisions at sqrt(s) = 1.8 TeV collected by the DZero experiment during 1992-1996 at the Fermilab Tevatron. Over thirty-two e mu X, W+jets-like, Z+jets-like, and 3(lepton/photon)X exclusive final states are systematically analyzed for hints of physics beyond the standard model. Simultaneous sensitivity to a variety of models predicting new phenomena at the electroweak scale is demonstrated by testing the method on a particular signature in each set of final states. No evidence of new high p_T physics is observed in the course of this search, and we find that 89% of an ensemble of hypothetical similar experimental runs would have produced a final state with a candidate signal more interesting than the most interesting observed in these data.']",['2000-11-21']
461,['eng'],"['Rubiera, A I']",['Exclusive Measurements in $B \\to D^{*}N\\overline{N}X$'],['Particle Physics - Experimental Results'],"['thesis', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'nucleon, pair production', 'D*(2010)', 'B0, branching ratio', 'decay, amplitude analysis', 'Lambda/c+, intermediate state', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'bibliography', 'B0 --> D*(2010) p anti-p pi+', 'B0 --> D*(2010) anti-n p', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011066'],"['We report the first observation of exclusive decays of the type B to D^* N Nbar X, where N is a nucleon. Using a sample of 9.7 x 10^6 BBbar pairs collected with the CLEO detector operating at the Cornell Electron Storage Ring, we measure the branching fractions B(B^0 to D^*-p pbar pi^+) = (6.5+1.3-1.2 +-1.0) x 10^-4, and B(B^0 to D^*- p nbar) = (14.5+3.4-3.0 +-2.7) x 10^-4. The charge conjugate process is implied in the reconstruction of B^0 to D^*- p nbar, only the mode with the antineutron is used in our measurement because neutrons do not have a distinctive annihilation signature. Antineutrons are used for the first time in the exclusive reconstruction of a B meson. By finding conclusive evidence for the existence of decay modes of the type B to D N Nbar X, we challenge the assumption that the B to Baryons rate is dominated by decays to charmed mesons.']",['2000-11-21']
462,['eng'],"['Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Bornheim, A', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Jaffe, D E', 'Masek, G', 'Paar, H P', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Vogel, H', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Savinov, V', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J']",['Dalitz Analysis of the Decay $D^{0}\\to K^{-}\\pi^{+}\\pi^{0}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'Dalitz plot', 'mass spectrum, (K- pi+ pi0)', 'meson resonance, production', 'K*(892)', 'K*0(1430)', 'K*(1680)', 'rho(1700)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D0 --> K- pi+ pi0', 'D0 --> K*(892) pi', 'D0 --> K- rho(770)', 'D0 --> K*0(1430) pi', 'D0 --> rho(1700) K', 'D0 --> K*(1680) pi', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011065'],"['We use data collected with the CLEO II detector to perform a high-statistics measurement of the resonant substructure in $D^0 \\to K^-\\pi^+\\pi^0$ decays. We find the Dalitz Plot is well represented by a combination of seven quasi-two-body decay channels ($\\bar{K}^{*0} \\pi^0$, $K^- \\rho$, $K^{*-} \\pi^+$, $K^*_0(1430)^-\\pi^+$, $\\bar{K}^*_0(1430)^0 \\pi^0$, $K^- \\rho^+(1700)$, and $K^*(1680)^- \\pi^+$), plus a small non-resonant component. Using the amplitudes and phases from this analysis, we calculate an integrated CP asymmetry of $-0.031 \\pm 0.086$.']",['2000-11-21']
463,['eng'],"['Stefano, P D', 'Bruckmayer, M', 'Bucci, C', 'Cooper, S', 'Cozzini, C', 'Von Feilitzsch, F', 'Frank, T', 'Hauff, D', 'Jagemann, T', 'Jochum, J', 'Keeling, R', 'Kraus, H', 'Marchese, J', 'Pergolesi, D', 'Pröbst, F', 'Ramachers, Y', 'Schnagl, J', 'Seidel, W', 'Sergeyev, I', 'Stark, M', 'Stodolsky, L', 'Uchaikin, S V', 'Wulandari, H']",['The CRESST Experiment'],['Particle Physics - Experimental Results'],"['talk, Verbier 2000/07/17', 'astrophysics, missing-mass', 'WIMP, search for', 'scattering, WIMP nucleus', 'calorimeter', 'scintillation counter', 'cryogenics', 'background']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011064'],"['The CRESST experiment seeks hypothetical WIMP particles that could account for the bulk of dark matter in the Universe. The detectors are cryogenic calorimeters in which WIMPs would scatter elastically on nuclei, releasing phonons. The first phase of the experiment has successfully deployed several 262 g sapphire devices in the Gran Sasso underground laboratories. A main source of background has been identified as microscopic mechanical fracturing of the crystals, and has been eliminated, improving the background rate by up to three orders of magnitude at low energies, leaving a rate close to one count per day per kg and per keV above 10 keV recoil energy. This background now appears to be dominated by radioactivity, and future CRESST scintillating calorimeters which simultaneously measure light and phonons will allow rejection of a great part of it.']",['2000-11-21']
464,['eng'],"['Kamys, B', 'Kulessa, P', 'Ohm, H', 'Pysz, K', 'Rudy, Z', 'Ströher, H', 'Cassing, W']",['Nonmesonic decay of the $\\Lambda$-hyperon in hypernuclei produced by p+Au collisions'],['Particle Physics - Experimental Results'],"['p nucleus, nuclear reaction', 'gold', 'hyperfragment, hadroproduction', 'Lambda, hadronic decay', 'final state, (0meson)', 'Lambda, lifetime', 'experimental results', 'Juelich COSY PS', 'nucleon Lambda --> 2nucleon', '1.9 GeV-kin']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011063'],['The lifetime of the Lambda-hyperon for the nonmesonic decay Lambda N ---> N N has been determined by a measurement at COSY Juelich of the delayed fission of heavy hypernuclei produced in proton - Au collisions at T_p=1.9 GeV. It is found that heavy hypernuclei with mass numbers A= 180 +- 5 and atomic numbers Z= 74 +-2 fission with a lifetime 130ps +- 13ps (stat.) +- 15ps (syst.) . This value together with the results obtained for other heavy hypernuclei in previous investigations indicates (on the confidence level of 0.9) a violation of the phenomenological Delta I = 1/2 rule for Lambda N ---> NN transitions as known from the weak mesonic decays of kaons and hyperons. PACS: {13.30.-a}{Decays of baryons} {13.75.Ev}{Hyperon-nucleon interaction} {21.80}{Hypernuclei} {25.80.Pw}{Hyperon-induced reactions}'],['2000-11-21']
465,['eng'],"['Dror, G', 'Etzion, E']",['Vertex Reconstructing Neural Network at the ZEUS Central Tracking Detector'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/16', 'drift chamber, vertex', 'drift chamber, wire', 'resolution, vertex', 'neural network', 'track data analysis', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011062'],"['An unconventional solution for finding the location of event creation is presented. It is based on two feed-forward neural networks with fixed architecture, whose parameters are chosen so as to reach a high accuracy. The interaction point location is a parameter that can be used to select events of interest from the very high rate of events created at the current experiments in High Energy Physics. The system suggested here is tested on simulated data sets of the ZEUS Central Tracking Detector, and is shown to perform better than conventional algorithms.']",['2000-11-21']
466,['eng'],"['Dror, G', 'Etzion, E']",['Momentum Reconstruction and Triggering in the ATLAS Detector'],['Particle Physics - Experimental Results'],"['talk, Batavia 2000/10/16', 'muon, trigger', 'muon, transverse momentum', 'neural network', 'computer, vector', 'statistical analysis', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011061'],"['A neural network solution for a complicated experimental High Energy Physics problem is described. The method is used to reconstruct the momentum and charge of muons produced in collisions of particle in the ATLAS detector. The information used for the reconstruction is limited to the output of the outer layer of the detector, after the muons went through strong and inhomogeneous magnetic field that have bent their trajectory. It is demonstrated that neural network solution is efficient in performing this task. It is shown that this mechanism can be efficient in rapid classification as required in triggering systems of the future particle accelerators. The parallel processing nature of the network makes it relevant for hardware realization in the ATLAS triggering system.']",['2000-11-21']
467,['eng'],"['Goulianos, K']",['Diffraction in hadron-hadron interactions'],['Particle Physics - Experimental Results'],"['talk, Cetraro 2000/09/02', 'p p, interaction', 'anti-p p, interaction', 'elastic scattering', 'diffraction, dissociation', 'diffraction, structure function', 'differential cross section', 'factorization', 'scaling', 'rapidity, gap', 'Regge poles', 'pomeron, exchange', 'cross section, energy dependence', 'unitarity', 'pomeron, structure function', 'gluon', 'nucleon, structure function', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011060'],"['Results on soft and hard diffraction in $pp$ and $\\bar pp$ collisions are reviewed with emphasis on factorization and scaling properties of differential cross sections. While conventional factorization breaks down at high energies, a scaling behavior emerges, which leads to a universal description of diffractive processes in terms of a (re)normalized rapidity gap probability distribution.']",['2000-11-21']
468,['eng'],"['Goulianos, K']",['The diffractive structure function at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Cetraro 2000/09/02', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'diffraction, structure function', 'small-angle', 'jet, pair production', 'exchange, (2pomeron)', 'W, hadroproduction', 'rapidity, gap', 'quark, beauty', 'quark, hadroproduction', 'J/psi(3100), hadroproduction', 'J/psi(3100), leptonic decay', 'pomeron, structure function', 'gluon', 'anti-p, leading particle', 'factorization, violation', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011059'],['Results on hard diffraction from CDF are reviewed with emphasis on the determination of the diffractive structure function of the (anti)proton from single diffractive and double Pomeron exchange dijet production. Comparison of the diffractive dijet results with predictions based on diffractive deep inelastic scattering at HERA shows a breakdown of conventional QCD factorization. A similar breakdown is observed within the CDF results in comparing the structure functions obtained from single diffraction and double Pomeron exchange.'],['2000-11-21']
469,['eng'],"['Cranmer, K']",['Kernel Estimation in High-Energy Physics'],['Particle Physics - Experimental Results'],"['statistical analysis', 'data analysis method']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011057'],"['Kernel Estimation provides an unbinned and non-parametric estimate of the probability density function from which a set of data is drawn. In the first section, after a brief discussion on parametric and non-parametric methods, the theory of Kernel Estimation is developed for univariate and multivariate settings. The second section discusses some of the applications of Kernel Estimation to high-energy physics. The third section provides an overview of the available univariate and multivariate packages. This paper concludes with a discussion of the inherent advantages of kernel estimation techniques and systematic errors associated with the estimation of parent distributions.']",['2000-11-20']
470,['eng'],"['Csilling, Akos']",['QCD measurements in photon-photon collisions at LEP'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'cross section, hadronic', 'quark, charm', 'quark, pair production', 'D*(2010), photoproduction', 'differential cross section, transverse momentum', 'channel cross section, energy dependence', 'charmed meson, semileptonic decay', 'jet, pair production', 'photon, structure function', 'structure function, charm', 'quantum chromodynamics', 'experimental results', 'CERN LEP Stor', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011056'],"['An overview of the latest results of the LEP collaborations on QCD measurements in photon-photon collisions is presented, including measurements of the total hadronic cross-section, the production of heavy quarks and dijets and the structure functions of real and virtual photons.']",['2000-11-20']
471,['eng'],"['Bianco, S', 'Link, J M', 'Paolone, V S', 'Reyes, M', 'Yager, P M', 'Anjos, J C', 'Bediaga, I', 'Göbel, C', 'Magnin, J', 'De Miranda, J M', 'Pepe, I M', 'Dos Reis, A C', 'Simão, F R A', 'Carrillo, S', 'Casimiro, E', 'Méndez, H', 'Sánchez-Hernández, A', 'Uribe, C', 'Vásquez, F', 'Cinquini, L', 'Cumalat, J P', 'Ramírez, J E', ""O'Reilly, B"", 'Butler, J N', 'Vaandering, E W', 'Cheung, H W K', 'Gaines, I', 'Garbincius, P H', 'Garren, L A', 'Gottschalk, E E', 'Gourlay, S A', 'Kasper, P H', 'Kreymer, A E', 'Kutschke, R', 'Fabbri, F L', 'Sarwar, S', 'Zallo, A', 'Cawlfield, C', 'Kim, D Y', 'Park, K S', 'Rahimi, A', 'Gardner, R', 'Wiss, J', 'Chung, Y S', 'Kang, J S', 'Ko, B R', 'Kwak, J W', 'Lee, K B', 'Myung, S S', 'Park, H', 'Alimonti, G', 'Boschini, M', 'Brambilla, D', 'Caccianiga, B', 'Calandrino, A', ""D'Angelo, P"", 'Di Corato, M', 'Dini, P', 'Giammarchi, M G', 'Inzani, P', 'Leveraro, F', 'Malvezzi, S', 'Menasce, D', 'Mezzadri, M', 'Milazzo, L', 'Moroni, L', 'Pedrini, D', 'Prelz, F', 'Rovere, M', 'Sala, A', 'Sala, S', 'Arena, V', 'Davenport, T F', 'Boca, G', 'Bonomi, G', 'Gianini, G', 'Liguori, G', 'Merlo, M', 'Pantea, D', 'Ratti, S P', 'Riccardi, C', 'Torre, P', 'Viola, L', 'Vitulo, P', 'Hernández, H', 'López, A M', 'Méndez, L', 'Mirles, M A', 'Montiel, E', 'Olaya, D', 'Quinones, J', 'Rivera, C', 'Zhang, Y', 'Copty, N K', 'Purohit, M', 'Wilson, J R', 'Cho, K', 'Handler, T', 'Engh, D', 'Johns, W E', 'Hosack, M', 'Nehring, M S', 'Sales, M', 'Sheldon, P D', 'Stenson, K', 'Webster, M S', 'Sheaff, M', 'Kwon, Y']",['New FOCUS results on charm mixing and CP violation'],['Particle Physics - Experimental Results'],"['talk, Ferrara 2000/09/18', 'photon nucleus, inclusive reaction', 'beryllium, oxygen', 'charmed meson, photoproduction', 'charmed meson, hadronic decay', 'D0, lifetime', 'lifetime, difference', 'D+', 'D*(2010), branching ratio', 'D0 anti-D0, interference', 'violation, CP', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'photon nucleus --> charmed meson anything', 'D0 --> K- pi+', 'D0 --> pi+ pi-', 'D0 --> K+ K-', 'D+ --> K+ K- pi+', 'D*(2010) --> K+ pi+ pi-', 'D*(2010) --> K- 2pi+']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011055'],"['We present a summary of recent results on CP violation and mixing in the charm quark sector based on a high statistics sample collected by photoproduction experiment FOCUS (E831 at Fermilab). We have measured the difference in lifetimes for the $D^0$ decays: $D^0 \\to K^-\\pi^+$ and $D^0 \\to K^-K^+$. This translates into a measurement of the $y_{CP}$ mixing parameter in the $\\d0d0$ system, under the assumptions that $K^-K^+$ is an equal mixture of CP odd and CP even eigenstates, and CP violation is negligible in the neutral charm meson system. We verified the latter assumption by searching for a CP violating asymmetry in the Cabibbo suppressed decay modes $D^+ \\to K^-K^+\\pi^+$, $D^0 \\to K^-K^+$ and $D^0 \\to \\pi^-\\pi^+$. We show preliminary results on a measurement of the branching ratio $\\Gamma(D^{*+}\\to \\pi^+ (K^+\\pi^-))/\\Gamma(D^{*+}\\to \\pi^+ (K^-\\pi^+))$.']",['2000-11-20']
472,['eng'],"['Jessop, C']",['First Results in Exclusive Radiative Penguin Decays at BABAR'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, radiative decay', 'B, semileptonic decay', 'lepton, pair production', 'Feynman graph, penguin', 'B0, branching ratio', 'B+, branching ratio', 'upper limit', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> K*(892) photon', 'B0 --> K*(892) lepton+ lepton-', 'B+ --> K+ lepton+ lepton-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011054'],"['We present a preliminary measurement of the branching fraction of the exclusive penguin decay B^0 -> K^*0 gamma using (8.6+/-0.3) x 10^6 B-anti-B decays BF(B^0 -> K^*0 gamma) = (5.2+/-0.82 (stat.) +/- 0.47 (sys.)) x 10^-5. In addition we search for the related penguin decays with a lepton pair in the final state, B^+ -> K^+ l^+l^-, B^0 -> K^*0 l^+l^-. We find no evidence for these decays in 3.7+/-0.1 x 10^6 B-anti-B decays and set preliminary 90% C.L upper limits of BF(B^+ -> K^+ e^+ e^-) < 12.5 x 10^{-6}, BF(B^+ -> K^+ mu^+ mu^-) < 8.3 x 10^{-6}, BF(B^0 -> K^*0 e^+ e^-) < 24.1 x 10^{-6}, BF(B^0 -> K^*0 mu^+ mu^-) < 24.5 x 10^{-6}.']",['2000-11-20']
473,['eng'],"['Battaglia, M', 'Borghi, S', 'Campagnolo, R', 'Caccia, M', 'Kucewicz, W', 'Jalocha, P', 'Palka, J', 'Zalewska, Agnieszka']",['Hybrid Pixel Detector Development for the Linear Collider Vertex Tracker'],['Particle Physics - Experimental Results'],"['talk, Homestead 2000/09/10', 'electron positron, linear collider', 'linear collider, proposed', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'spatial resolution', 'radiation, damage']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011053'],"['In order to fully exploit the physics potential of the future high energy e+e- linear collider, a Vertex Tracker able to provide particle track extrapolation with very high resolution is needed. Hybrid Si pixel sensors are an attractive technology due to their fast read-out capabilities and radiation hardness. A novel pixel detector layout with interleaved cells has been developed to improve the single point resolution. Results of the characterisation of the first processed prototypes by electrostatic measurements and charge collection studies are discussed.']",['2000-11-17']
474,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thomas, J', 'Thomson, M A', 'Tonnesmann, M', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A Study of $B_{s}$ Meson Oscillation Using $D_{s}^{-}$-Lepton Correlations'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B/s0 anti-B/s0, oscillation', 'B/s0, semileptonic decay', 'correlation, (D/s- lepton+)', 'particle identification, flavor', 'B/s0, mass difference', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011052'],"['From data collected around the Z resonance by the OPAL detector at LEP a sample of Bs decays was obtained using Ds^-l^+ combinations, where the Ds^- was fully reconstructed in the phi pi-, K*0K- and Ks0K- decay channels or partially reconstructed in the phi l- nu (X) decay channel. These events were used to study Bs oscillation. The flavor (b or bbar) at decay was determined from the lepton charge while the flavor at production was determined from a combination of techniques. The expected sensitivity of the experiment is 4.1 ps-1. The experiment was not able to resolve the oscillatory behavior, and we deduced that the Bs oscillation frequency Delta m_s > 1.0 ps-1 at the 95% confidence level.']",['2000-11-17']
475,['eng'],"['Park, H']",['$D^{0}-\\overline{D}^{0}$ Mixing and CP Violation from FOCUS Experiment'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'photon nucleus, inclusive reaction', 'beryllium, oxygen', 'charmed meson, photoproduction', 'charmed meson, hadronic decay', 'D0, lifetime', 'D+', 'D0 anti-D0, interference', 'violation, CP', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> K- pi+', 'D0 --> K+ K-', 'D0 --> pi+ pi-', 'D+ --> K+ K- pi+', 'approx. 180 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011051'],"['Measurement results on $D^0$-$\\bar D^0$ mixing and CP violation are presented. FOCUS is the fixed target experiment at Fermilab and results are based on a high statistics photo-produced charm sample collected during 96-97 run. We reconstructed more than 1 million charmed particles and compared the lifetimes of two $D^0$ meson decays to $K^-\\pi^+$ and $K^-K^+$. We obtained a mixing parameter, $y_{\\rm cp}$, is $(3.42\\pm 1.39\\pm 0.74)%$. We also searched CP asymmetries in $D^+\\to K^-K^+\\pi^+$, $D^0\\to K^-K^+$ and $D^0\\to \\pi^-\\pi^+$ decay modes. We did not see any evidence of CP violation by comparing the decay rates for particle and antiparticle.']",['2000-11-17']
476,['eng'],"['Mellado, B']",['Diffractive Vector Meson Production at HERA'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'positron p, colliding beams', 'vector meson, electroproduction', 'vector meson, photoproduction', 'diffraction', 'rho(770)0', 'omega(783)', 'Phi(1020)', 'J/psi(3100)', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'differential cross section, momentum transfer', 'x-dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011050'],"['The H1 and ZEUS collaborations at HERA report new data on the diffractive production of vector mesons with a many-fold increase of luminosity compared to previous measurements. The new data include photoproduction and electroproduction of $\\rho^0,\\phi,J/\\psi$. The available data on elastic VM production indicate that the interaction scales as $Q^2+M_{V}^2$.']",['2000-11-16']
477,['eng'],"['Mahmood, A H']",['Measurement of the $\\Lambda_{c}^{+}$ Lifetime'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, charm', 'quark, pair production', 'Lambda/c+, electroproduction', 'Lambda/c+, lifetime', 'Lambda/c+, hadronic decay', 'mass spectrum, (p K- pi+)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Lambda/c+ anything', 'Lambda/c+ --> p K- pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011049'],"['The $\\Lambda_{c}^{+}$ lifetime is measured using 9.0 fb$^{-1}$ of $e^+e^-$ annihilation data collected on or just below the $\\Upsilon(4S)$ resonance with the CLEO II.V detector at CESR. Using an unbinned maximum likelihood fit, the $\\Lambda_{c}^{+}$ lifetime is measured to be $(179.6 \\pm 6.9(stat.) \\pm 4.4(syst.))$ fs. The precision of this colliding beam measurement is comparable to other measurements, which are based on fixed target experiments with different systematic errors.']",['2000-11-16']
478,['eng'],"['Cecchini, S', 'Giacomelli, Giorgio', 'Giacomelli, R', 'Hasegan, D', 'Maris, O', 'Popa, V', 'Serra, R', 'Serrazanetti, M', 'Stefanov, L', 'Tasca, L', 'Valeanu, V']",['Limits on radiative decays of solar neutrinos from a measurement during a solar eclipse'],['Particle Physics - Experimental Results'],"['neutrino, solar', 'neutrino, radiative decay', 'neutrino, lifetime', 'lower limit', 'kinematics', 'photon, angular distribution', 'shadowing, lunar', 'imaging', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011048'],"['A search for possible radiative decays of solar neutrinos with emission of photons in the visible range was performed during the total solar eclipse of August 11, 1999. Due to very bad weather conditions our two telescopes were unable to collect useful data; fortunately we obtained several video camera images from a local TV station. An analysis of the digitised images is presented and limits on the lifetime for radiative decay are discussed.']",['2000-11-16']
479,['eng'],"['Wing, M']",['Precise measurement of jet energies with the ZEUS detector'],['Particle Physics - Experimental Results'],"['talk, Annecy 2000/10/09', 'positron p, colliding beams', 'jet, electroproduction', 'jet, transverse energy', 'energy, correction', 'track data analysis, cluster', 'energy flow', 'numerical calculations, Monte Carlo', 'magnetic detector, ZEUS', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011046'],"['A method to correct the jet transverse energy has been developed for the ZEUS detector which attains an uncertainty better than 3%. The procedure is based on a combination of tracking and calorimeter information that optimises the resolution of reconstructed kinematic variables. The selected calorimeter clusters and tracks are referred to as Energy Flow Objects (EFOs). The conservation of energy and momentum in neutral current deep inelastic $e^+p$ scattering events is exploited to determine the required energy corrections by balancing the scattered positron with the hadronic final state. The method has been applied to data and simulated events independently. The corrected EFOs are used as input to a $k_T$-cluster jet algorithm to reconstruct the jets and to determine kinematic variables. In addition, the corrected EFOs allow an improved measurement of the internal structure of a jet.']",['2000-11-16']
480,['eng'],"['Fabbri, F L']",['Results on Charmed Meson Spectroscopy from Focus'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'photon nucleus, inclusive reaction', 'beryllium, oxygen', 'charmed meson, photoproduction', 'charmed meson, hadronic decay', 'D0', 'D+', 'D*(2010)', 'charmed meson, excited state', 'hadron spectroscopy', 'D*2(2460)', 'D1(2420)', 'mass, width', 'mass spectrum', 'forward spectrometer, experimental results', 'Batavia TEVATRON PS', 'approx. 300 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011044'],['We report the preliminary measurement by the FOCUS Collaboration (E831 at Fermilab) of masses and widths of the L=1 charm mesons D_2^{*0} and D_2^{*+}.'],['2000-11-16']
481,['eng'],"['Acciarri, M']",['Higgs Candidates in $e^{+}e^{-}$ Interactions at $\\sqrt{s}$ = 206.6 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Z0, decay modes', 'Higgs particle, mass', 'Higgs particle, hadronic decay', 'quark, pair production', 'quark, beauty', 'neural network', 'track data analysis, vertex', 'final state, (4jet)', 'jet, energy', 'jet, thrust', 'missing-energy', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> Z0 Higgs particle', 'electron positron --> 2quark 2antiquark', 'electron positron --> quark antiquark neutrino antineutrino', '206.06 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011043'],"['In a search for the Standard Model Higgs boson, carried out on 212.5 pb-1 of data collected by the L3 detector at the highest LEP centre-of-mass energies, including 116.5 pb-1 above root(s) = 206GeV, an excess of candidates for the process e+e- -> Z* -> HZ is found for Higgs masses near 114.5GeV. We present an analysis of our data and the characteristics of our strongest candidates.']",['2000-11-15']
482,['eng'],"['Bediaga, I']",['Dalitz plot analysis and branching fraction measurement of $D^{+}$ and $D {s}^{+} \\to\\pi^{-} \\pi^{+} \\pi{+}$'],['Particle Physics - Experimental Results'],"['talk, Valencia 2000/06/27', 'pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'charmed meson, hadroproduction', 'charmed meson, hadronic decay', 'charmed meson, branching ratio', 'D+', 'D/s+', 'Dalitz plot', 'amplitude analysis', 'sigma meson, mass', 'rho(770)0', 'rho(1450)', 'f0(975)', 'f2(1270)', 'f0(1370)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> 2pi+ pi-', 'D/s+ --> 2pi+ pi-', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011042'],"['Fermilab fixed target experiment E791 obtained a sample of $1172 \\pm 61$ events of $D^+ \\to \\pi^- \\pi^+ \\pi^+$ and 848 $\\pm 44$ events of $D_s^+ \\to \\pi^- \\pi^+ \\pi^+$ decays. We find respectively $B (D^+ \\to \\pi^- \\pi^+ \\pi^+) / B (D^+ \\to K^- \\pi^+ \\pi^+) = 0.0311 \\pm 0.0018 ^ {+0.0016}_{-0.0026}$ and $B(D_s^+ \\to \\pi^+ \\pi^- \\pi^+) / B(D_s^+ \\to \\phi \\pi^+) = 0.245 \\pm 0.028^{+0.019}_{-0.012}$. Using a coherent amplitude analysis to fit the Dalitz plot of the $D^+ \\to \\pi^- \\pi^+ \\pi^+$ decay, we find strong evidence for a scalar resonance of mass $478^{+24}_{-23} \\pm 17 $MeV/$c^2$ and width $324^{+42}_{-40} \\pm 21$ MeV/$c^2$, compatible with what is expected for the isoscalar meson $\\sigma$ >. The $D^+ \\to \\sigma(500) \\pi^+$ fraction accounts for approximately half of all three-charged-pion decays of the $D^+$ . From the Dalitz plot analysis of the $D_s^+ \\to \\pi^- \\pi^+ \\pi^+$ decay events, we find significant contributions from the channels $\\rho^0(770)\\pi^+$, $\\rho^0(1450)\\pi^+$, $f_0(980)\\pi^+$, $f_2(1270)\\pi^+$, and $f_0(1370)\\pi^+$. We also present new measurement of the masses and widths of the isoscalar resonances $f_0(980)$ and $f_0(1370)$.']",['2000-11-15']
483,['eng'],"['Abe, K']",['Time Dependent $B_s^0 - \\bar{B_s^0}$ Oscillations Using Exclusively Reconstructed $D_s^+$ Decays at SLD'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B/s0 anti-B/s0, oscillation', 'B/s0, mass difference', 'B/s0, hadronic decay', 'D/s-, hadronic decay', 'track data analysis, vertex', 'decay, path length', 'particle identification, flavor', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'B/s0 --> D/s- anything', 'D/s- --> Phi(1020) pi', 'D/s- --> K*(892) K', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011041'],"['We set a preliminary 95% C.L. exclusion on the oscillation frequency of $B_s^0 - \\bar{B_s^0}$ mixing using a sample of 400,000 hadronic $Z^0$ decays collected by the SLD experiment at the SLC during the 1996-98 run. In this analysis, $B_s^0$ mesons are partially reconstructed by combining a fully reconstructed $D_s$ with other $B_s^0$ decay tracks. The $D_s$ decays are reconstructed via the $\\phi \\pi$ and $K^* K$ channels. The $b$-hadron flavor at production is determined by exploiting the large forward-backward asymmetry of polarized $Z^0 \\to b \\bar{b}$ decays as well as information from the hemisphere opposite to the reconstructed B decay. The flavor of the $B_s^0$ at the decay vertex is determined by the charge of the $D_s$. A total of 361 candidates passed the final event selection cuts. This analysis excludes the following values of the $B_s^0 - \\bar{B_s^0}$ mixing oscillation frequency: $\\Delta m_s < 1.5$ ps$^{-1}$, $2.6 < \\Delta m_s < 4.9$ ps$^{-1}$, and $10.8 < \\Delta m_s < 13.5$ ps$^{-1}$ at the 95% confidence level.']",['2000-11-15']
484,['eng'],"['Boyd, S']",['Recent Results from the K2K (KEK-to-Kamioka) Neutrino Oscillation Experiment'],['Particle Physics - Experimental Results'],"['talk, Victoria 2000/09/18', 'neutrino, oscillation', 'neutrino/mu, secondary beam', 'beam profile', 'beam, energy spectrum', 'neutrino nucleon, interaction', 'dependence, path length', 'neutrino/tau', 'neutrino/e', 'scintillation counter, fibre', 'Cherenkov counter', 'deep underground detector, KAMIOKANDE', 'experimental results', 'KEK PS', '800 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011039'],"['The latest results of the K2K experiment are reported. The results are based on data taken from June, 1999, to June, 2000, corresponding to a total $2.6 \\cdot 10^{19}$ protons on target. Twenty seven fully-contained events in the 22.5 kton fiducial volume of Super-Kamiokande (SK) are observed. The expected number of events is estimated to be 40.3^{+4.7}_{-4.6} assuming the null oscillations hypothesis.']",['2000-11-14']
485,['eng'],"['Solomey, N']",['Neutral Hyperon and H-Dibaryon Results from KTeV'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'hyperon, secondary beam', 'Xi0, semileptonic decay', 'Xi0, radiative decay', 'form factor, decay', 'baryon resonance, dibaryon', 'H baryon, search for', 'electroweak interaction, validity test', 'polarization', 'angular distribution', 'Xi0, branching ratio', 'transition radiation detector, experimental results', 'Batavia TEVATRON PS', 'Xi0 --> Sigma+ lepton- antineutrino', 'Xi0 --> Sigma0 photon', 'Xi0 --> Lambda photon', '800 GeV (p)']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011038'],"['Results from the KTeV experiment at Fermilab using neutral Xi hyperons are presented, especially the first form-factor (FF) measurement from its semi-leptonic decay. This decay, which is an important test of the Standard Model, was observed for the first time using the 1997 KTeV experiment. We also report on the analysis of a large samples of neutral Xi weak radiative decays, and a search for the decay of a lightly bound $H^0$ dibaryon.']",['2000-11-14']
486,['eng'],"['Abbott, B', 'Abdesselam, A', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Bacon, T C', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Todorova-Nová, S', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bauer, D', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Beuselinck, R', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Duflot, L', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gao, M', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Illingworth, R', 'Ito, A S', 'Jaffré, M', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Leggett, C', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Luo, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Nunnemann, T', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Papageorgiou, K', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Petroff, P', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Ridel, M', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Sen, N', 'Shabalina, E', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Inclusive Jet Production in $\\overline{p}p$ Collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'differential cross section, rapidity dependence', 'transverse energy, dependence', 'p, structure function', 'momentum spectrum, parton', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011036'],"['We report a new measurement of the pseudorapidity (eta) and transverse-energy (Et) dependence of the inclusive jet production cross section in pbar b collisions at sqrt(s) = 1.8 TeV using 95 pb**-1 of data collected with the DZero detector at the Fermilab Tevatron. The differential cross section d^2sigma/dEt deta is presented up to |eta| = 3, significantly extending previous measurements. The results are in good overall agreement with next-to-leading order predictions from QCD and indicate a preference for certain parton distribution functions.']",['2000-11-13']
487,['eng'],"['Sefkow, F']",['Open Charm and Beauty Production at HERA'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'positron p, colliding beams', 'electron p, colliding beams', 'charmed meson, electroproduction', 'charmed meson, hadronic decay', 'D1(2420)', 'D*2(2460)', 'D*(2010)', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'fusion, intermediate boson gluon', 'mass difference, spectra', 'differential cross section, x-dependence', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'final state, (2jet)', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'DESY HERA Stor', 'electron p --> charmed meson anything', 'D1(2420) --> D*(2010) pi', 'D*2(2460) --> D*(2010) pi', 'D*(2010) --> D0 pi+', '300-318 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011034'],"['Selected new results from the H1 and ZEUS collaborations on $ep$ interactions at 300 - 318 GeV centre-of-mass energy are presented. The full pre-upgrade integrated luminosity of HERA of 110 pb$^{-1}$ is used. Charm cross sections are measured up to high values of $x_B$ and $Q^2$ and are found to be well described by NLO QCD in the 3 flavour scheme. Orbitally excited $D$ mesons are observed; radial excitations are searched for, but are not seen. The first $b$ cross section measurement is confirmed with a lifetime based method, establishing the excess over NLO QCD.']",['2000-11-13']
488,['eng'],"['Obraztsov, V F', 'Landsberg, G L']",['Prospects for CP-violation searches in the future experiment with RF-separated K+/- beam at U-70'],['Particle Physics - Experimental Results'],"['talk, Ferrara 2000/09/18', 'K+, separated beam', 'RF system, particle separator', 'superconducting', 'K+, rare decay', 'K+, hadronic decay', 'violation, CP', 'experimental results', 'proposed experiment, Serpukhov PS', 'K+ --> 2pi+ pi-', 'K+ --> pi+ 2pi0']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011033'],"['The first description of the experimental program ""OKA"" with RF-separated K+/- beam at Protvino U-70 PS is presented. The parameters of the beam as well as the potential for CP-violation searches are discussed.']",['2000-11-13']
489,['eng'],"['Shen, X']",['Recent Results from BES'],['Particle Physics - Experimental Results'],"['talk, Valencia 2000/06/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'psi mesons, electroproduction', 'psi mesons, hadronic decay', 'psi mesons, radiative decay', 'J/psi(3100), branching ratio', 'psi(3685), branching ratio', 'partial wave analysis', 'photon, energy spectrum', 'K*(892)', 'Phi(1020)', 'f2(1270)', 'f0(1710)', 'cross section, hadronic', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'J/psi(3100) --> K+ K- photon', 'J/psi(3100) --> Phi(1020) pi+ pi-', 'J/psi(3100) --> Phi(1020) K+ K-', 'J/psi(3100) --> K*(892) K', 'psi(3685) --> f2(1270) photon', 'psi(3685) --> f0(1710) photon', 'psi(3685) --> J/psi(3100) pi+ pi-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011032'],"['We report partial wave analysis results for $J/\\psi \\to \\gamma K^+ K^-$ based on $7.8 \\times 10^6$ BESI $J/\\psi$ events, and find $0^{++}$ to be dominant in the $f_J(1710)$ mass region. Some very preliminary results are presented from the $2.2 \\times 10^7$ $J/\\psi$ events newly collected at the upgraded BES(BESII). Using the world largest $\\psi(2S)$ data sample, BES measures branching ratios of $\\psi(2S)$ radiative and hadronic decays. The preliminary R values measured by BESII in the 2-5 GeV energy region are also presented.']",['2000-11-13']
490,['eng'],"['Olsen, J']",['Charmless Hadronic B Decays at BABAR'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, rare decay', 'final state, (0charm)', 'final state, (2meson)', 'final state, (3meson)', 'B0, branching ratio', 'B+, branching ratio', 'upper limit', 'rho(770)', 'eta(958)', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> pi+ pi-', 'B0 --> K+ pi-', 'B0 --> rho(770)- pi+', 'B+ --> eta(958) K+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011031'],"[""We present preliminary results of several searches for rare charmless hadronic decays of the B meson using data collected by the BABAR detector at the Stanford Linear Accelerator Center's PEP-II storage ring. We search for the decays h^+h^-, h^+h^-h^+, h^+h^-pi^0, X^0h^+, and X^0 K_S^0, where h = pi or K, and X^0 = eta^prime or omega. In a sample of 8.8 million B-anti-B decays we measure the branching fractions: BF(B^0 --> pi^+pi^-) = (9.3^{+2.6}_{-2.3}^{+1.2}_{-1.4}) x 10^{-6}, BF(B^0 --> K^+pi^-) = (12.5^{+3.0}_{-2.6}^{+1.3}_{-1.7}) x 10^{-6}, BF(B^0 --> rho^-pi^+) = (49 +/- 13^{+6}_{-5}) x 10^{-6}$, and BF(B^+ --> eta^prime K^+) = (62 +/- 18 +/- 8) x 10^{-6}$. We calculate upper limits for the modes without a significant signal.""]",['2000-11-13']
491,['eng'],"['Brown, C N', 'Awes, T C', 'Beddo, M E', 'Brooks, M L', 'Bush, J D', 'Carey, T A', 'Chang, T H', 'Cooper, W E', 'Gagliardi, C A', 'Garvey, G T', 'Geesaman, D F', 'Hawker, E A', 'He Xiao Chun', 'Isenhower, L D', 'Kaplan, D M', 'Kaufman, S B', 'Koetke, D D', 'Kyle, G S', 'Lee, W M', 'Leitch, M J', 'Makins, N C R', 'McGaughey, P L', 'Moss, J M', 'Müller, B A', 'Nord, P M', 'Papavassiliou, V', 'Park, B K', 'Peng, J C', 'Petitt, G', 'Reimer, P E', 'Sadler, M E', 'Stankus, P W', 'Towell, R S', 'Tribble, R E', 'Vasilev, M A', 'Webb, J C', 'Willis, J L', 'Wise, D K', 'Young, G R']",['Observation of Polarization in Bottomonium Production at $\\sqrt{s}$=38.8 GeV'],['XX'],"['p nucleus, inclusive reaction', 'copper', 'upsilon mesons, hadroproduction', 'upsilon mesons, leptonic decay', 'Upsilon(9460)', 'Upsilon(10020)', 'Upsilon(10355)', 'muon, pair production', 'mass spectrum, dimuon', 'angular distribution', 'polarization, transverse', 'transverse momentum, dependence', 'x-dependence', 'quantum chromodynamics, nonrelativistic', 'quark antiquark, annihilation', 'gluon gluon, fusion', 'experimental results', 'Batavia TEVATRON PS', 'p copper --> muon+ muon- anything', '38.8 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011030'],[],['2000-11-10']
492,['eng'],"['Thompson, R', 'Dytman, S A', 'Kim, K Y', 'Müller, J', 'Adams, G S', 'Amaryan, M J', 'Anciant, E', 'Anghinolfi, M', 'Asavapibhop, B', 'Auger, T', 'Audit, G', 'Avakian, H', 'Barrow, S', 'Battaglieri, M', 'Beard, K', 'Bektasoglu, M', 'Berman, B L', 'Bertozzi, W', 'Bianchi, N', 'Biselli, A', 'Boiarinov, S', 'Bonner, B E', 'Briscoe, W J', 'Brooks, W', 'Burkert, V D', 'Calarco, J R', 'Capitani, G P', 'Carman, D S', 'Carnahan, B', 'Cetina, C', 'Cole, P L', 'Coleman, A', 'Connelly, J', 'Cords, D', 'Corvisiero, P', 'Crabb, D', 'Crannell, H', 'Cummings, J', 'Day, D', 'Degtyarenko, P V', 'Demirchyan, R A', 'Dennis, L C', 'Deppman, A', 'De Sanctis, E', 'De Vita, R', 'Dhuga, K S', 'Djalali, C', 'Dodge, G E', 'Doughty, D', 'Dragovitsch, P', 'Dugger, M R', 'Eckhause, M', 'Efremenko, Yu V', 'Egiyan, H', 'Egiyan, K S', 'Elouadrhiri, L', 'Farhi, L', 'Feuerbach, R J', 'Ficenec, J', 'Fissum, K', 'Freyberger, A P', 'Funsten, H O', 'Gai, M', 'Gavrilov, V B', 'Gilfoyle, G P', 'Giovanetti, K L', 'Gilad, S', 'Girard, P M', 'Griffioen, K A', 'Guidal, M', 'Guillo, M', 'Gyurjyan, V', 'Hancock, D', 'Hardie, J', 'Heddle, D', 'Heisenberg, J', 'Hersman, F W', 'Hicks, K', 'Hicks, R S', 'Holtrop, M', 'Hyde-Wright, C E', 'Ito, M M', 'Jenkins, D', 'Joo, K K', 'Kane, J', 'Khandaker, M', 'Kim, W', 'Klein, A', 'Klein, F J', 'Klusman, M', 'Kossov, M', 'Kuhn, S E', 'Kuang, Y', 'Laget, J M', 'Lawrence, D', 'Leskin, G A', 'Longhi, A', 'Loukachine, K', 'Lucas, M', 'Magahiz, R', 'Major, R W', 'Manak, J J', 'Marchand, C', 'Matthews, S K', 'Maximon, L', 'McAleer, S', 'McCarthy, J', 'McNabb, J W C', 'Mecking, B A', 'Mestayer, M D', 'Meyer, C A', 'Minehart, R C', 'Mirazita, M', 'Miskimen, R', 'Muccifora, V', 'Murphy, L', 'Mutchler, G S', 'Napolitano, J', 'Niyazov, R A', 'Ohandjanyan, M S', ""O'Brien, J T"", 'Opper, A K', 'Patois, Y', 'Perrot-Kunne, F', 'Peterson, G A', 'Philips, S', 'Pivnyuk, N A', 'Pocanic, D', 'Pogorelko, O I', 'Polli, E', 'Preedom, B M', 'Price, J W', 'Qin, L M', 'Raue, B A', 'Reolon, A R', 'Riccardi, G', 'Ricco, G', 'Ripani, M', 'Ritchie, B G', 'Ronchetti, F', 'Rossi, P', 'Roudot, F', 'Rowntree, D', 'Rubin, P D', 'Salgado, C W', 'Sanzone, M', 'Sapunenko, V', 'Sarty, A', 'Sargsyan, M', 'Schumacher, R A', 'Shafi, A', 'Sharabyan, Yu G', 'Shaw, J', 'Shuvalov, S M', 'Skabelin, A', 'Smith, T', 'Smith, C', 'Smith, E S', 'Sober, D I', 'Spraker, M', 'Stepanyan, S', 'Stoler, P', 'Taiuti, M', 'Taragin, M F', 'Taylor, S', 'Tedeschi, D J', 'Tung, T Y', 'Vineyard, M F', 'Vlasov, A', 'Weller, H', 'Weinstein, L B', 'Welsh, R', 'Weygand, D P', 'Whisnant, S', 'Witkowski, M T', 'Wolin, E', 'Yegneswaran, A', 'Yun, J', 'Zhou, Z', 'Zhao, J']","[""The $ep \\to e'p\\eta$ reaction at and above the $S_{11}(1535)$ baryon resonance""]",['Particle Physics - Experimental Results'],"['electron p, inelastic scattering', 'eta, photoproduction', 'nucleon resonance, photoproduction', 'coupling, (nucleon resonance nucleon eta)', 'N(1535)', 'channel cross section, energy dependence', 'partial wave, interference', 'mass spectrum, missing-mass', 'angular distribution', 'magnetic spectrometer, experimental results', 'Newport News CEBAF Linac', 'electron p --> p eta electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011029'],"['New cross sections for the reaction e p -> ep eta are reported for total center of mass energy W = 1.5--1.86 GeV and invariant momentum transfer Q^2 = 0.25--1.5 GeV^2. This large kinematic range allows extraction of important new information about response functions, photocouplings, and eta N coupling strengths of baryon resonances. Expanded W coverage shows sharp structure at W \\~ 1.7 GeV; this is shown to come from interference between S and P waves and can be interpreted in terms of known resonances. Improved values are derived for the photon coupling amplitude for the S11(1535) resonance.']",['2000-11-10']
493,['eng'],"['Aihara, H']",['The Belle Silicon Vertex Detector'],['Particle Physics - Experimental Results'],"['talk, Hiroshima 2000/03/22', 'semiconductor detector, vertex', 'electronics, readout', 'integrated circuit', 'analog-to-digital converter', 'microprocessor', 'magnetic detector, BELLE', 'KEK TRISTAN Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011028'],['The silicon vertex detector of the Belle experiment has been built to provide the vertex information of $B$ meson decays at the KEKB accelerator. Performance during the initial data taking period and a brief description of the upgrade plan are also presented.'],['2000-11-10']
494,['eng'],"['Scholberg, K']",['Neutrino physics'],['Particle Physics - Experimental Results'],"['review, Columbus 2000/08/09', 'momentum spectrum', 'neutrino, solar', 'neutrino, cosmic radiation', 'neutrino nucleus, interaction', 'neutrino/e', 'neutrino/mu', 'neutrino/tau', 'charged current', 'neutrino, mass difference', 'neutrino, mixing angle', 'neutrino, sterile', 'neutrino, beam', 'neutrino, mass', 'tritium, semileptonic decay', 'double-beta decay', 'neutrino, magnetic moment', 'supernova', 'astrophysics', 'deep underground detector', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011027'],"['The field of neutrino physics is currently very exciting, with several recent results pointing to new physics. I will give an overview of the current experimental situation, focusing primarily on neutrino oscillation results. The data are not entirely consistent however, and puzzles remain. I will then review the new experiments which are poised to solve the outstanding puzzles.']",['2000-11-09']
495,['eng'],"['Akhmetshin, R R', 'Anashkin, E V', 'Arpagaus, M', 'Aulchenko, V M', 'Banzarov, V S', 'Barkov, L M', 'Bashtovoy, N S', 'Bondar, A E', 'Bondarev, D V', 'Bragin, A V', 'Chernyak, D V', 'Eidelman, S I', 'Fedotovich, G V', 'Gabyshev, N I', 'Grebeniuk, A A', 'Grigoriev, D N', 'Hughes, V W', 'Ignatov, F V', 'Ivanov, P M', 'Karpov, S V', 'Kazanin, V F', 'Khazin, B I', 'Koop, I A', 'Krokovnyi, P P', 'Kurdadze, L M', 'Kuzmin, A S', 'Lechner, M', 'Logashenko, I B', 'Lukin, P A', 'Mikhailov, K Yu', 'Nesterenko, I N', 'Okhapkin, V S', 'Otboev, A V', 'Perevedentsev, E A', 'Popov, A S', 'Purlatz, T A', 'Root, N I', 'Ruban, A A', 'Ryskulov, N M', 'Shamov, A G', 'Shatunov, Yu M', 'Shwartz, B A', 'Sibidanov, A L', 'Sidorov, V A', 'Skrinsky, A N', 'Smakhtin, V P', 'Snopkov, I G', 'Solodov, E P', 'Stepanov, P Yu', 'Sukhanov, A Yu', 'Thompson, J A', 'Titov, V M', 'Valishev, A A', 'Yudin, Yu V', 'Zverev, S G']",['Observation of the conversion decay $\\phi \\to \\pi^{0}e^{+}e^{-}$ at CMD-2'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), semileptonic decay', 'Phi(1020), radiative decay', 'Phi(1020), branching ratio', 'magnetic detector, CMD', 'experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> pi0 positron electron', 'pi0 --> 2photon', '1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011026'],"['Using 15.1^{-1} of data collected by CMD-2 in the $\\phi$-meson energy range, the branching ratio of the conversion decay $\\phi\\to\\pi^0e^+e^-$ has been measured for the first time: B(\\phi\\to\\pi^0e^+e^-) = (1.22 \\pm 0.34 \\pm 0.21) \\cdot 10 ^{-5}.']",['2000-11-09']
496,['eng'],"['McDonald, A B']",['First Neutrino Observations from the Sudbury Neutrino Observatory'],['Particle Physics - Experimental Results'],"['talk, Sudbury 2000/06/16', 'neutrino, cosmic radiation', 'neutrino, solar', 'neutrino deuteron, interaction', 'charged current', 'neutrino electron, elastic scattering', 'radioactivity, background', 'deep underground detector, Sudbury', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011025'],"['The first neutrino observations from the Sudbury Neutrino Observatory are presented from preliminary analyses. Based on energy, direction and location, the data in the region of interest appear to be dominated by 8B solar neutrinos, detected by the charged current reaction on deuterium and elastic scattering from electrons, with very little background. Measurements of radioactive backgrounds indicate that the measurement of all active neutrino types via the neutral current reaction on deuterium will be possible with small systematic uncertainties. Quantitative results for the fluxes observed with these reactions will be provided when further calibrations have been completed.']",['2000-11-09']
497,['eng'],"['Lin, C J S']",['$B_s$ Mixing at SLD'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B/s0 anti-B/s0, oscillation', 'B/s0, decay modes', 'B/s0, mass difference', 'particle identification, flavor', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011040'],"['We set a preliminary 95% C.L. exclusion on the oscillation frequency of $B_s^0 - \\bar{B_s^0}$ mixing using a sample of 400,000 hadronic $Z^0$ decays collected by the SLD experiment at the SLC during the 1996-98 run. Three analyses are presented in this paper. The first analysis partially reconstructs the $B_s^0$ by combining a fully reconstructed $D_s$ with the remaining charged B decay tracks. The second analysis selects a sample of events with a partially reconstructed charm vertex and a lepton track. The third analysis reconstructs b-hadrons topologically and exploits the $b \\to c$ cascade charge structure to determine the flavor of the b-hadron at decay. All three analyses take advantage of the large forward-backward asymmetry of the polarized $Z^0 \\to b \\bar{b}$ decays and information in the hemisphere opposite to the reconstructed B vertex to determine the b-hadron flavor at production. The results of the three analyses are combined to exclude the following values of the $B_s^0 - \\bar{B_s^0}$ oscillation frequency: $\\Delta m_s < 7.6 ps^{-1}$ and $11.8 < \\Delta m_s < 14.8 ps^{-1}$ at the 95% confidence level.']",['2000-11-15']
498,['eng'],"['Hitlin, D G']",['First CP Violation Results from BABAR'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'B0, semileptonic decay', 'particle identification, flavor', 'track data analysis, vertex', 'time resolution', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> psi mesons K0(S)', 'B0 --> D*(2010) lepton neutrino', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011024'],"['We present a preliminary measurement of time-dependent CP-violating asymmetries in B^0-->J/psi K_S and B^0-->psi(2S) K_S decays recorded by the BABAR detector at the PEP-II asymmetric B Factory at SLAC. The data sample consists of 9.0 fb-1 collected at the Upsilon(4S) resonance and 0.8 fb-1 off-resonance. One of the neutral B mesons, produced in pairs at the Upsilon(4S), is fully reconstructed. The flavor of the other neutral B meson is tagged at the time of its decay, mainly with the charge of identified leptons and kaons. The time difference between the decays is determined by measuring the distance between the decay vertices. Wrong-tag probabilities and the time resolution function are measured with samples of fully-reconstructed semileptonic and hadronic neutral B final states. The value of the asymmetry amplitude, sin(2*beta), is determined from a maximum likelihood fit to the time distribution of 120 tagged B^0-->J/psi K_S and B^0-->psi(2S) K_S candidates: sin(2*beta) = 0.12+/-0.37(stat)+/-0.09(syst).']",['2000-11-08']
499,['eng'],"['Santoro, A F S']",['The Future of Diffraction at Tevatron'],['Particle Physics - Experimental Results'],"['talk, Cetraro 2000/09/02', 'anti-p p, colliding beams', 'anti-p p, elastic scattering', 'diffraction, structure function', 'momentum transfer, high', 'jet, hadroproduction', 'exchange, (2pomeron)', 'quark, heavy', 'glueball', 'centauro', 'Higgs particle', 'correlation', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'upgrade, proposed', 'proposed experiment, Batavia TEVATRON Coll', '2000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011023'],['This paper summarizes the main current upgrade for Diffractive Physics at Tevatron. We describe both CDF and D0 new devices that are being installed around the CDF and D0 area that will allow to produce new results in Diffractive Physics.'],['2000-11-08']
500,['eng'],"['Abbiendi, G', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anagnostou, G', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Caron, B', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Krop, D', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rabbertz, K', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thomas, J', 'Thomson, M A', 'Tonnesmann, M', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']","['Charged Multiplicities in Z Decays into u, d, and s Quarks']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, hadronization', 'charged particle, multiplicity', 'dependence, flavor', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011022'],"['About 4.4 million hadronic decays of Z bosons, recorded by the OPAL detector at LEP at a centre-of-mass energy of around sqrt(s) = 91.2 GeV, are used to determine the mean charged particle multiplicities for the three light quark flavours. Events from primary u, d, and s quarks are tagged by selecting characteristic particles which carry a large fraction of the beam energy. The charged particle multiplicities are measured in the hemispheres opposite to these particles. An unfolding procedure is applied to obtain these multiplicities for each primary light quark flavour. This yields <n_u> = 17.77 +- 0.51 +0.86 -1.20, <n_d> = 21.44 +- 0.63 +1.46 -1.17, <n_s> = 20.02 +- 0.13 +0.39 -0.37, where statistical and systematic errors are given. The results for <n_u> and <n_d> are almost fully statistically anti-correlated. Within the errors the result is consistent with the flavour independence of the strong interaction for the particle multiplicities in events from the light up, down, and strange quarks.']",['2000-11-07']
501,['eng'],"['Jaffe, D E']",['Search for CP violation at CLEO'],['Particle Physics - Experimental Results'],"['talk, Ferrara 2000/09/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'meson, pair production', 'B, radiative decay', 'tree approximation', 'Feynman graph, penguin', 'B, branching ratio', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'D0 anti-D0, interference', 'invariance, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011021'],['Recent results from CLEO on the search for CP violation in beauty and charm meson decays are reviewed.'],['2000-11-07']
502,['eng'],"['Champion, T J']","['Studies of Charmless Two-Body, Quasi-Two-Body and Three-Body B Decays']",['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'rho(770)', 'K*(892)', 'eta(958)', 'omega(783)', 'B, branching ratio', 'upper limit', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> 2hadron', 'B --> 3hadron', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011018'],"['Preliminary results are presented on a search for several exclusive charmless hadronic B decays, from data collected by the BABAR detector near the Upsilon(4S) resonance. These include two-body decay modes h^{+/-}h^{-/+} three-body decay modes with final states h^{+/-}h^{-/+}h^{+/-} and h^{+/-}h^{-/+}\\pi^0, and quasi-two-body decay modes with final states X^0 h and X^0 K_s^0, where h = pi or K and X^0 = eta^prime or omega. The measurement of branching fractions for four decay modes, and upper limits for nine modes are presented.']",['2000-11-07']
503,['eng'],"['Bandourin, D V', 'Konoplyanikov, V F', 'Skachkov, N B']","['Jet energy scale setting with ""photon+Jet"" events at LHC Energies']",['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'jet, hadroproduction', 'photon, associated production', 'quark gluon, interaction', 'quark antiquark, annihilation', 'background', 'transverse momentum, lower limit', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011017'],"['The possibilities of the background events suppression, based on the QCD subprocesses of qg-,gg-,qq- scattering with big cross sections, to the signal ""photon+Jet"" events are studied. Basing on the introduced selection criteria, the background suppression factors and signal events selection efficiencies and the number of the events, that can be collected at LHC with low luminosity L=10^{33}cm^2 s^{-1} during one month of continuous work, are determined.']",['2000-11-07']
504,['eng'],"['Bandourin, D V', 'Konoplyanikov, V F', 'Skachkov, N B']","['""photon+Jet"" events rate estimation for gluon distribution determination at LHC']",['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'photon, direct production', 'jet, associated production', 'quark gluon, Compton scattering', 'gluon, momentum spectrum', 'background', 'jet, energy', 'numerical calculations, Monte Carlo', 'magnetic detector, CMS', 'CERN LHC Coll', 'p p --> jet photon anything', '14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011015'],"['It is shown that ""photon+Jet"" events, being collected at LHC, would provide us with the data sufficient for an extraction of gluon distribution function in a proton using valence and s quark distributions measured in the same experiment with another physical proces A new region of 10^{-4}< x < 10^{-1} with 1.6x10^3< Q^2<10^5 ~(GeV/c)^2 can be covered. The rates of g c-> photon +Jet events are also given.']",['2000-11-06']
505,['eng'],"['Bandourin, D V', 'Konoplyanikov, V F', 'Skachkov, N B']","['Jet energy scale setting with ""photon + Jet"" events']",['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'jet, hadroproduction', 'photon, associated production', 'jet, energy', 'jet, transverse momentum', 'photon, transverse momentum', 'upper limit', 'lower limit', 'calorimeter, hadronic', 'calibration', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011014'],"['It is shown in the paper that Pt activity limitation (modulus of the vector sum) of all particle beyond ""photon+Jet"" system Pt^{out} lead to the noticeable photon Pt -- jet Pt disbalance decreasing. On simultaneous restricion of the cluster Pt and Pt^{out} from above it is possible to reach an acceptable balance between photon Pt and jet Pt with a sufficient number of the ""photon+Jet"" events for jet energy scale setting and hadron calorimeter calibratiom of CMS detector at LHC.']",['2000-11-06']
506,['eng'],"['Bandourin, D V', 'Konoplyanikov, V F', 'Skachkov, N B']","['Jet energy scale setting with ""photon + Jet"" events']",['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'jet, hadroproduction', 'jet, energy', 'photon, associated production', 'transverse momentum, spectra', 'rapidity dependence', 'angular dependence', 'radiation, initial-state interaction', 'calorimeter, hadronic', 'numerical calculations, Monte Carlo']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011013'],"['In this paper the study of ""photon+Jet"" events is continued, aimed at jet energy scale setting and hadron calorimeter calibration at LHC energies. The event number distribution over photon Pt and eta is presented. The features of ""photon+Jet"" events in the barrel region of CMS detector (|\\eta|<1.4) are exposed. Pt structure of the region in the eta-phi space inside and beyond jet is shown.']",['2000-11-06']
507,['eng'],"['Bandourin, D V', 'Konoplyanikov, V F', 'Skachkov, N B']",['Jet energy scale setting with $\\gamma$ + Jet events'],['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'jet, hadroproduction', 'photon, associated production', 'jet, transverse momentum', 'photon, transverse momentum', 'quark gluon, interaction', 'quark antiquark, annihilation', 'Feynman graph, higher-order', 'radiation, initial-state interaction', 'calorimeter, hadronic', 'calibration', 'numerical calculations, Monte Carlo', 'tables']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011012'],"['The ""direct photon plus Jet"" events, based on the q ~q-> g+photon and qg-> q+photon subprocesses, are proposed for jet energy scale setting and hadron calorimeter calibration at LHC energies. General features and selection criteria of ""direct photon plus Jet"" events that would provide a good photon Pt -- Jet Pt balance are described. CMS detector geometry is taken as the basement.']",['2000-11-06']
508,['eng'],"['Jinnouchi, O', 'Asai, S', 'Kobayashi, T']",['Measurement of Orthopositronium Decay Rate Using SiO2 Powder'],['Particle Physics - Experimental Results'],"['positron nucleus, nuclear reaction', 'silicon, oxygen', 'positronium, production', 'positronium, annihilation', 'positronium, lifetime', 'final state, (3photon)', 'spectra, time', 'photon, energy spectrum', 'quantum electrodynamics, validity test', 'semiconductor detector, germanium', 'scintillation counter, experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011011'],"['The intrinsic decay rate of orthopositronium (o-Ps) formed in SiO_2 powder was measured using a modified method which determined the time dependence of the pick-off annihilation rate using high-energy-resolution germanium detectors. That is, the main systematic error due to thermalization was accounted for and integrated into the time spectrum fitting procedure. The averaged value was found to be lambda_(o-Ps)=7.0399+0.0020-0.0021(stat.) +-0.0015(sys.) mu s^{-1}, which agrees well with the O(alpha^2) QED prediction; varying 2.8-4.2 experimental standard deviations from other measurements.']",['2000-11-06']
509,['eng'],"['Bauer, J M']","[""Kinematic Fit for the Radiative Bhabha Calibration of BaBar's Electromagnetic Calorimeter""]",['Particle Physics - Experimental Results'],"['calorimeter, electromagnetic', 'calibration', 'electron positron, elastic scattering', 'bremsstrahlung', 'statistical analysis', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011019'],"[""For the radiative Bhabha calibration of BaBar's electromagnetic calorimeter, the measured energy of a photon cluster is being compared with the energy obtained via a kinematic fit involving other quantities from that event. The details of the fitting algorithm are described in this note, together with its derivation and checks that ensure that the fitting routine is working properly.""]",['2000-11-07']
510,['eng'],"['Brock, R', 'Erler, J', 'Kim, Y K', 'Marciano, W', 'Members, W G', 'Ashmanskas, W J', 'Baur, Ulrich', 'Ellison, J', 'Lancaster, M', 'Nodulman, L', 'Rha, J', 'Waters, D', 'Womersley, J']",['Report of the Working Group on Precision Measurements'],['Particle Physics - Experimental Results'],"['review, Batavia 1999/03/04', 'electroweak interaction, validity test', 'anti-p p, colliding beams', 'W, hadroproduction', 'W, mass', 'W, width', 'electroweak interaction, radiative correction', 'mass spectrum, transverse', 'transverse momentum, spectra', 'lepton, pair production', 'angular distribution, asymmetry', 'Weinberg angle', 'interference, (Z0 photon)', 'gauge boson, postulated particle', 'search for, composite', 'space-time, higher-dimensional', 'electron positron, colliding beams', 'p p, colliding beams', 'programming, Monte Carlo', 'Z0, width', 'fermion, mass', 'neutrino nucleon, interaction', 'quark, beauty', 'quark, radiative decay', 'quantum chromodynamics, perturbation theory', 'numerical calculations', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'proposed experiment', 'Batavia TEVATRON Coll', '1800, 2000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011009'],"['In the first part of this report, we discuss the prospects for measuring the W mass and width in Run II. The basic techniques used to measure M_W are described and the statistical, theoretical and detector-related uncertainties are discussed in detail. Alternative methods of measuring the W mass at the Tevatron and the prospects for M_W measurements at other colliders are also described. In the second part, we discuss the measurement of the forward backward asymmetry in Drell Yan production in Run II which can be used to determine the effective weak mixing angle. Estimates of the statistical and systematic uncertainties in Run II are given. The third part summarizes the features of the FORTRAN package GAPP which performs a fit to the electroweak observables and extracts the probability distribution function of the Higgs boson mass.']",['2000-11-03']
511,['eng'],"['Cheng, C']",['B lifetime measurements with exclusively reconstructed B decays'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B0, lifetime', 'B+, lifetime', 'lifetime, ratio', 'D', 'D*(2010)', 'J/psi(3100)', 'psi(3685)', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> charmed meson pi', 'B --> charmed meson rho(770)', 'B --> charmed meson a1(1260)', 'B0 --> J/psi(3100) K*(892)', 'B+ --> psi mesons K+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011007'],['Data collected with the BABAR detector at the PEP-II asymmetric B Factory at SLAC are used to study the lifetime of the B0 and B+ mesons. The data sample consists of 7.4 fb-1 collected near the Y(4S) resonance. B0 and B+ mesons are fully reconstructed in several exclusive hadronic decay modes to charm and charmonium final states. The B lifetime are determined from the flight length difference between the two B mesons. The preliminary measurements of the lifetimes are tau_{B0} = 1.506 +/- 0.052 (stat) +/- 0.029 (syst) ps tau_{B+} = 1.602 +/- 0.049 (stat) +/- 0.035 (syst) ps and of their ratio is tau_{B+}/tau_{B0} = 1.065 +/- 0.044 (stat) +/- 0.021 (syst).'],['2000-11-03']
512,['eng'],"['Rahatlou, S']",['A study of $B^{0}-\\overline{B^{0}}$ oscillations with full reconstructed B mesons with the BABAR detector'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0 anti-B0, oscillation', 'time dependence', 'B0, mass difference', 'B0, hadronic decay', 'B0, semileptonic decay', 'D', 'D*(2010)', 'J/psi(3100)', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> charmed meson pi+', 'B0 --> charmed meson rho(770)+', 'B0 --> charmed meson a1(1260)', 'B0 --> J/psi(3100) K*(892)', 'B0 --> D*(2010) lepton+ neutrino', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011006'],"['Time-dependent B0-anti-B0 flavor oscillations are studied in e+e- annihilation data collected with the BABAR detector at center-of-mass energies near the Upsilon(4S) resonance. We report a preliminary result for the time-dependent B0-anti-B0 oscillation frequency, Delta_md = 0.512 +/- 0.017 +/- 0.022 hbar ps^{-1}.']",['2000-11-03']
513,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Baroiant, S', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bell, W H', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Bishai, M', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Caskey, W', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Chung, Y S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', ""D'Auria, S"", 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Fernández, J P', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Furic, I K', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Gorelov, I V', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Grim, G P', 'Gris, P', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hill, C', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirby, M', 'Kirk, M', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, J', 'Lancaster, M', 'Lander, R', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Meyer, A', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Moulik, T', 'Mulhearn, M', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Nelson, T', 'Neu, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Ribon, A', 'Riegler, W', 'Rimondi, F', 'Ristori, L', 'Riveline, M', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Roy, A', 'Safonov, A', 'Saint-Denis, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sánchez, C', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Thompson, A S', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vataga-Pagliarone, E', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Wilkes, T', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Search for the Supersymmetric Partner of the Top-Quark in $p \\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'sparticle, search for', 'squark, truth', 'quark, truth', 'quark, pair production', 'quark, rare decay', 'electroweak interaction, validity test', 'quark, branching ratio', 'upper limit', 'LSP, mass', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'truth --> squark LSP', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011004'],"['We report on a search for the supersymmetric partner of the top quark (stop) produced in $t \\bar{t}$ events using $110 {\\rm pb}^{-1}$ of $p \\bar{p}$ collisions at $\\sqrt{s} = 1.8 {\\rm TeV}$ recorded with the Collider Detector at Fermilab. In the case of a light stop squark, the decay of the top quark into stop plus the lightest supersymmetric particle (LSP) could have a significant branching ratio. The observed events are consistent with Standard Model $t \\bar{t}$ production and decay. Hence, we set limits on the branching ratio of the top quark decaying into stop plus LSP, excluding branching ratios above 45% for a LSP mass up to 40 {\\rm GeV/c}$^{2}$.']",['2000-11-02']
514,['eng'],"['Gao, Y']",['Results on B to Charmonia Decays from CLEO'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'Upsilon(10570), hadronic decay', 'Upsilon(10570), branching ratio', 'B, pair production', 'B, hadronic decay', 'violation, CP', 'quarkonium, charm', 'B, branching ratio', 'psi mesons', 'chi mesons, charm', 'eta/c(2980)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Upsilon(10570) --> B+ B-', 'Upsilon(10570) --> 2B0', 'B --> quarkonium K', 'B --> J/psi(3100) pi0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011003'],"['We review some recent results on B to charmonia decays from CLEO based on 9.7 BBbar pairs collected with the CLEO detector. These include measurements of B^{0} to J\\Psi K^0_s, \\chi_{c1} K^0_s and J/\\Psi \\pi^0 branching fractions, search for direct CP violation in B^{\\pm} to J/\\Psi K^\\pm and \\Psi(2S) K^\\pm, observation of B \\to \\eta_{c} K, study of \\chi_{c1}, \\chi_{c2} production and measurement of the relative branching fraction of \\Upsilon(4S) to charged and neutral B meson pairs.']",['2000-11-02']
515,['eng'],"['Burrows, P N', 'Abe, K', 'Abe, K', 'Abe, T', 'Adam, I', 'Akimoto, H', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Berger, R', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Calcaterra, A', 'Cassell, R', 'Chou, A', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Crawford, G', 'Damerell, C J S', 'Daoudi, M', 'Dasu, S', 'De Groot, N', 'De Sangro, R', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Erofeeva, I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fernández, J P', 'Flood, K', 'Frey, R', 'Hart, E L', 'Hasuko, K', 'Hertzbach, S S', 'Huffer, M E', 'Huynh, X', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Kajikawa, R', 'Kalelkar, M S', 'Kang, H J', 'Kofler, R R', 'Kroeger, R S', 'Langston, M', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'McKemey, A K', 'Messner, R', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Narita, S', 'Nauenberg, U', 'Neal, H', 'Nesom, G', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Ratcliff, B N', 'Reidy, J', 'Reinertsen, P L', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schumm, B A', 'Schwiening, J', 'Serbo, V V', 'Shapiro, G', 'Sinev, N B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, A', 'Swartz, M', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Usher, T', 'Vavra, J', 'Verdier, R', 'Wagner, D L', 'Waite, A P', 'Walston, S', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Wright, T R', 'Yamamoto, R K', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H']",['Studies of hadronic decays of Z0 bosons at SLD'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, fragmentation function', 'model, hadronization', 'dependence, flavor', 'correlation, (2hadron)', 'rapidity, correlation', 'charge correlation', 'correlation, long-range', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011002'],['The latest SLD results on light-quark fragmentation and tests of hadronisation models are presented'],['2000-11-02']
516,['eng'],"['Saltzberg, D', 'Gorham, P W', 'Walz, D', 'Field, C', 'Iverson, R H', 'Odian, A', 'Resch, G', 'Schoessow, P', 'Williams, D']",['Observation of the Askaryan Effect'],['Particle Physics - Experimental Results'],"['electron, beam', 'bremsstrahlung', 'photon nucleus, interaction', 'silicon, oxygen', 'showers, electromagnetic', 'showers, spatial distribution', 'time dependence', 'charge, asymmetry', 'radiation, Cherenkov', 'microwaves, emission', 'coherence', 'electric field', 'polarization', 'experimental results', 'SLAC Lab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011001'],"['We present the first direct experimental evidence for the charge excess in high energy particle showers predicted nearly 40 years ago by Askaryan. We directed bremsstrahlung photons from picosecond pulses of 28.5 GeV electrons at the SLAC Final Focus Test Beam facility into a 3.5 ton silica sand target, producing electromagnetic showers several meters long. A series of antennas spanning 0.3 to 6 GHz were used to detect strong, sub-nanosecond radio frequency pulses produced whenever a shower was present. The measured electric field strengths are consistent with a completely coherent radiation process. The pulses show 100% linear polarization, consistent with the expectations of Cherenkov radiation. The field strength versus depth closely follows the expected particle number density profile of the cascade, consistent with emission from excess charge distributed along the shower. These measurements therefore provide strong support for experiments designed to detect high energy cosmic rays and neutrinos via coherent radio emission from their cascades.']",['2000-11-02']
517,['eng'],"['Wang, Y F']",['A Water Cerenkov Calorimeter as the Next Generation Neutrino Detector'],['Particle Physics - Experimental Results'],"['talk, Honolulu 2000/10/02', 'neutrino, counters and detectors', 'calorimeter', 'Cherenkov counter, water', 'neutrino, oscillation', 'neutrino, cosmic radiation', 'neutrino, beam', 'neutrino, particle source', 'numerical calculations, Monte Carlo', 'deep underground detector, Soudan', 'KEK JHP PS', 'Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010081'],"['We propose here a large homogeneous calorimeter as the next generation neutrino detector for $\\nu$ factories and/or conventional $\\nu$ beams. The active media is chosen to be water for obvious economical reasons. The \\v Cerenkov light produced in water is sufficient to have good energy resolution, and the pattern recognition is realized by a modular water tank structure. Monte Carlo simulations demonstrate that the detector performance is excellent for identifying neutrino CC events while rejecting background events.']",['2000-11-01']
518,['eng'],"['Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Savinov, V', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T']",['Observation of New States Decaying into ${\\Lambda_{c}}^{+}\\pi^{-}\\pi^{+}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, electroproduction', 'charmed baryon, hadronic decay', 'Lambda/c+, excited state', 'final state, (Lambda/c+ pi+ pi-)', 'mass difference, spectra', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010080'],"['Using 13.7 fb^{-1} of data recorded by the CLEO detector at CESR, we investigate the spectrum of charmed baryons which decay into Lambda_c^+ pi^- pi^+ and are more massive than the Lambda_{c1} baryons. We find evidence for two new states: one is broad and has an invariant mass roughly 480 MeV above that of the Lambda_c^+; the other is narrow with an invariant mass of 596 +- 1 +- 2 MeV above the Lambda_c^+ mass. These results are preliminary.']",['2000-11-01']
519,['eng'],"['Tanaka, J']",['Measurement of Charmed Meson Lifetimes with Belle'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, electroproduction', 'charmed meson, hadronic decay', 'charmed meson, lifetime', 'D0', 'D+', 'D/s+', 'lifetime, ratio', 'violation, CP', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'D0 --> K- pi+', 'D+ --> K- 2pi+', 'D+ --> Phi(1020) pi+', 'D/s+ --> Phi(1020) pi+', 'D/s+ --> K*(892) K+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010078'],"['The lifetimes of charmed mesons have been measured using 2.75fb$^{-1}$ of data collected with the Belle detector at KEKB. Each candidate is fully reconstructed to identify the flavor of the charmed meson. The lifetimes are measured to be $\\tau(D^0)=(414.8\\pm3.8\\pm3.4)$ fs, $\\tau(D^+)=(1040^{+23}_{-22}\\pm18)$ fs and $\\tau(D_s^+)=(479^{+17}_{-16}{}^{+6}_{-8})$ fs, where the first error is statistical and the second error is systematic. The mixing parameter $y_{CP}$ is also measured through the lifetime difference of $D^0$ mesons decaying into CP-mixed states and CP eigenstates. We find $y_{CP}=(1.0^{+3.8}_{-3.5}{}^{+1.1}_{-2.1})%$, corresponding to a 95% confidence interval $-7.0%<\\ycp<8.7%$.']",['2000-11-01']
520,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bogdanchikov, A G', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Drozdetsky, A A', 'Druzhinin, V P', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Korol, A A', 'Koshuba, S V', 'Mamutkin, A A', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Skripkin, A G', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Vasilev, A V']",['Recent results from SND detector at VEPP-2M'],['Particle Physics - Experimental Results'],"['talk, Protvino 2000/06/21', 'electron positron, colliding beams', 'electron positron, annihilation', 'vector meson, electroproduction', 'vector meson, radiative decay', 'vector meson, rare decay', 'vector meson, branching ratio', 'Phi(1020)', 'omega(783)', 'rho(770)', 'pi, multiple production', 'channel cross section, energy dependence', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> vector meson', 'vector meson --> 2pi0 photon', 'Phi(1020) --> eta pi0 photon', 'vector meson --> eta photon', 'electron positron --> omega(783) pi0', 'electron positron --> pi+ pi- pi0', 'Phi(1020) --> pi+ pi-', 'Phi(1020) --> omega(783) pi0', '0.36-1.38 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010077'],"['The current status of experiments with SND detector at VEPP-2M $e^+e^-$ collider in the energy range $2E_0=0.4-1.4$ GeV is given. The new results of analysis of $\\phi$ decay into $\\pi^0\\pi^0\\gamma$, $\\eta\\pi^0\\gamma$ are based on the full SND statistics corresponding 20 million of $\\phi$ decay. New measurement of $\\omega\\to\\pi^0\\pi^0\\gamma$ decay and a first observation of $\\rho\\to\\pi^0\\pi^0\\gamma$ are presented. The accuracy of many other rare decays of light vector mesons was improved. In the energy range $2E_0=1.0\\div1.4$ GeV the cross sections of the processes $e^+e^-\\to\\omega\\pi^0$ and $e^+e^-\\to\\pi^+\\pi^-\\pi^0$ were measured. The results of the fitting of data are discussed.']",['2000-11-01']
521,['eng'],"['Parashar, N', 'Bardon, O', 'Goodwin, R', 'Hansen, S', 'Hoeneisen, B', 'Podstavkov, V M', 'Uvarov, S', 'Wood, D']",['Real-Time Data Processing in the Muon System of the D0 Detector'],['Particle Physics - Experimental Results'],"['talk, Santa Fe 1999/06/14']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0105092'],"[""This paper presents a real-time application of the 16-bit fixed point Digital Signal Processors (DSPs), in the Muon System of the D0 detector located at the Fermilab Tevatron, presently the world's highest-energy hadron collider. As part of the Upgrade for a run beginning in the year 2000, the system is required to process data at an input event rate of 10 KHz without incurring significant deadtime in readout. The ADSP21csp01 processor has high I/O bandwidth, single cycle instruction execution and fast task switching support to provide efficient multisignal processing. The processor's internal memory consists of 4K words of Program Memory and 4K words of Data Memory. In addition there is an external memory of 32K words for general event buffering and 16K words of Dual Port Memory for input data queuing. This DSP fulfills the requirement of the Muon subdetector systems for data readout. All error handling, buffering, formatting and transferring of the data to the various trigger levels of the data acquisition system is done in software. The algorithms developed for the system complete these tasks in about 20 microseconds per event.""]",['2001-06-01']
522,['eng'],"['Verderi, M']",['First Year of the BABAR Experiment Data Taking'],['Particle Physics - Experimental Results'],"['talk, Lisbon 2000/06/29', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, semileptonic decay', 'violation, CP', 'J/psi(3100)', 'D*(2010)', 'charge, dilepton', 'semiconductor detector, vertex', 'drift chamber', 'Cherenkov counter', 'calorimeter, electromagnetic', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010076'],"['The BABAR experiment at the PEP-II asymmetric B factory observed its first hadronic events on the 26th of May 1999. We present the progress made so far on the data taking, the BABAR detector performances and the physics analyses.']",['2000-10-31']
523,['eng'],"['Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Park, W', 'Thorndike, E H', 'Jessop, C P', 'Savinov, V']",['Bounds on the CP Asymmetry in $b \\to s\\gamma$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'quark, beauty', 'quark, radiative decay', 'antiquark, radiative decay', 'asymmetry, CP', 'electroweak interaction, validity test', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'beauty --> strangeness photon', 'beauty --> down photon', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010075'],"['We have measured the CP asymmetry A_CP = [BF(b -> s gamma) - BF(bbar -> sbar gamma)]/[BF(b -> s gamma) + BF(bbar -> sbar gamma)] to be A_CP = (-0.079 +/- 0.108 +/- 0.022)(1.0 +/- 0.030), implying that, at 90% confidence level, A_CP lies between -0.27 and +0.10. These limits rule out some extreme non-Standard Model predictions, but are consistent with most, as well as with the Standard Model.']",['2000-10-31']
524,['eng'],"['Appel, J A']",['The Experiment Road to the Heavier Quarks and Other Heavy Objects'],['Particle Physics - Experimental Results'],"['talk, Metepec 2000/08/09', 'particle physics, history', 'quark, charm', 'quark, beauty', 'quark, truth', 'quark, particle identification', 'quark, production', 'quark, decay', 'quark, hadronization', 'violation, CP', 'hadron spectroscopy', 'B0 anti-B0, interference', 'experimental methods', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010074'],"['After a brief history of heavy quarks, I will discuss charm, bottom, and top quarks in turn. For each one, I discuss its first observation, and then what we have learned about production, hadronization, and decays - and what these have taught us about the underlying physics. I will also point out remaining open issues. For this series of lectures, the charm quark will be emphasized. It is the first of the heavy quarks, and its study is where many of the techniques and issues first appeared. Only very brief mention is made of CP violation in the bottom-quark system since that topic is the subject of a separate series of lectures by Gabriel Lopez. As the three quarks are reviewed, a pattern of techniques and lessons emerges. These are identified, and then briefly considered in the context of anticipated physics signals of the future; e.g., for Higgs and SUSY particles.']",['2000-10-31']
525,['eng'],"['Solomey, N']",['Latest Results on Weak Semi-Leptonic Hyperon Decays in KTeV'],['Particle Physics - Experimental Results'],"['talk, Valencia 2000/06/27', 'Xi0, semileptonic decay', 'Xi0, branching ratio', 'muon, final state', 'electron, final state', 'decay, form factor', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010073'],"['The KTeV experiment at Fermilab has finished its $\\Xi^0$ semi-leptonic decay analysis from the 1997 run and presented here are the final numbers for the branching ratio and form factors. A new run with three times the statistics was taken in 1999 and a first look at the data shows the quality and consistency of the results, predicting a similar improvement in these measurements.']",['2000-10-31']
526,['eng'],"['Bai, J Z', 'Ban, Y', 'Bian, J G', 'Blum, I K', 'Chen, G P', 'Chen, H F', 'Chen, J', 'Chen Jia Chao', 'Chen, Y', 'Chen, Y B', 'Chen, Y Q', 'Cheng, B S', 'Cui, X Z', 'Ding, H L', 'Dong, L Y', 'Du, Z Z', 'Dunwoodie, W M', 'Gao, C S', 'Gao, M L', 'Gao, S Q', 'Gratton, P', 'Gu, J H', 'Gu, S D', 'Gu, W X', 'Gu, Y F', 'Guo, Z J', 'Guo, Y N', 'Han, S W', 'Han, Y', 'Harris, F A', 'He, J', 'He, J T', 'He, K L', 'He, M', 'Heng, Y K', 'Hitlin, D G', 'Hu, G Y', 'Hu, H M', 'Hu, J L', 'Hu, Q H', 'Hu, T', 'Hu Xiao Qing', 'Huang, G S', 'Huang, Y Z', 'Izen, J M', 'Jiang, C H', 'Jin, Y', 'Jones, B D', 'Ju, X', 'Ke, Z J', 'Kelsey, M H', 'Kim, B K', 'Kong, D', 'Lai, Y F', 'Lang, P F', 'Lankford, A J', 'Li, C G', 'Li, D', 'Li, H B', 'Li, J', 'Li, J C', 'Li, P Q', 'Li, R B', 'Li, W', 'Li, W G', 'Li, X H', 'Li Xiao Nan', 'Liu, H M', 'Liu, J', 'Liu, R G', 'Liu, Y', 'Lou, X C', 'Lowery, B', 'Lu, F', 'Lu, J G', 'Luo, X L', 'Ma, E C', 'Ma, J M', 'Malchow, R', 'Mao, H S', 'Mao, Z P', 'Meng, X C', 'Nie, J', 'Olsen, S L', 'Oyang, J Y T', 'Paluselli, D', 'Pan, L J', 'Panetta, J', 'Porter, F', 'Qi, N D', 'Qi, X R', 'Qian, C D', 'Qiu, J F', 'Qu, Y H', 'Que, Y K', 'Rong, G', 'Schernau, M', 'Shao, Y Y', 'Shen, B W', 'Shen, D L', 'Shen, H', 'Shen, X Y', 'Sheng, H Y', 'Shi, H Z', 'Song, X F', 'Standifird, J', 'Sun, F', 'Sun, H S', 'Sun, Y', 'Sun, Y Z', 'Tang, S Q', 'Toki, W', 'Tong, G L', 'Varner, G S', 'Wang, F', 'Wang, L S', 'Wang, L Z', 'Wang, M', 'Wang, P', 'Wang, P L', 'Wang, S M', 'Wang, T J', 'Wang, Y Y', 'Weaver, M', 'Wei, C L', 'Wu, J M', 'Wu, N', 'Wu, Y G', 'Xi, D M', 'Xia, X M', 'Xie, P P', 'Xie, Y', 'Xie, Y H', 'Xu, G F', 'Xue, S T', 'Yan, J', 'Yan, W G', 'Yang, C M', 'Yang, C Y', 'Yang, H X', 'Yang, J', 'Yang, W', 'Yang, X F', 'Ye, M H', 'Ye Shu Wei', 'Ye, Y X', 'Yu, C S', 'Yu, C X', 'Yu, G W', 'Yu Yu Hei', 'Yu, Z Q', 'Yuan, C Z', 'Yuan, Y', 'Zhang Bing Yun', 'Zhang, C', 'Zhang, C C', 'Zhang, D H', 'Zhang, H L', 'Zhang, J', 'Zhang, J W', 'Zhang, L', 'Zhang, L S', 'Zhang, P', 'Zhang, Q J', 'Zhang, S Q', 'Zhang, X Y', 'Zhang, Y Y', 'Zhao, D X', 'Zhao, H W', 'Zhao Jia Wei', 'Zhao, M', 'Zhao Wei Ren', 'Zhao, Z G', 'Zheng Jian Ping', 'Zheng Lin Sheng', 'Zheng Zhi Peng', 'Zhou, B Q', 'Zhou, G P', 'Zhou, H S', 'Zhou, L', 'Zhu, K J', 'Zhu, Q M', 'Zhu, Y C', 'Zhu, Y S', 'Zhuang, B A']",['First Measurement of the Branching Fraction of the Decay $\\psi(2S) \\to \\tau\\tau$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), leptonic decay', 'tau, pair production', 'psi(3685), branching ratio', 'psi(3685), width', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'psi(3685) --> tau+ tau-', 'approx. 3.7 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010072'],"['The branching fraction of the psi(2S) decay into tau pair has been measured for the first time using the BES detector at the Beijing Electron-Positron Collider. The result is $B_{\\tau\\tau}=(2.71\\pm 0.43 \\pm 0.55) \\times 10^{-3}$, where the first error is statistical and the second is systematic. This value, along with those for the branching fractions into e+e- and mu+mu of this resonance, satisfy well the relation predicted by the sequential lepton hypothesis. Combining all these values with the leptonic width of the resonance the total width of the psi(2S) is determined to be $(252 \\pm 37)$ keV.']",['2000-10-31']
527,['eng'],"['Gennai, Simone']",['A study of bB production mechanisms in Pythia'],['Particle Physics - Experimental Results'],"['talk, Durham 2000/09/17', 'p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'gluon gluon, fusion', 'quark antiquark, annihilation', 'quark quark, interaction', 'gluon, fragmentation', 'transverse momentum, lower limit', 'cross section', 'angular correlation', 'numerical calculations, Monte Carlo', '14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010069'],"['The influence of the Pt_hat cutoff on the production of bB events in Pythia has been studied. Versions 5.75, 6.125 and 6.152 have been considered.']",['2000-10-30']
528,['eng'],"['Raven, G']",['Measurements of Inclusive and Exclusive B Decays to Charmonium with BABAR'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'energy, asymmetry', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'psi mesons', 'chi mesons, charm', 'B, branching ratio', 'B0, mass', 'B+, mass', 'amplitude analysis, CP', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> quarkonium strange meson', 'B --> quarkonium anything', 'B --> J/psi(3100) K*(892)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010067'],"['Using 8.5M B-anti-B events recorded by the BABAR detector the yield of inclusive J/psi, the branching ratios of psi(2S) and chi_C1 are presented. Combining the charmonium state with either a K+,KS, K*+ or K*0 exclusive B decays are reconstructed and their branching ratios determined. Using the fully reconstructed decays, both the B0 and B+ masses and their difference is measured. Finally the contributions of CP even and odd amplitudes in the decay B to J/psi K* are determined from an angular analysis.']",['2000-10-27']
529,['eng'],"['Çiftçi, A K', 'Sultansoy, S F', 'Yavas, O', 'Yilmaz, M']",['TAC Proposal for Fundamental and Applied Research'],['Particle Physics - Experimental Results'],"['talk, Izmir 2000/10/23', 'accelerator, proposed', 'electron positron, linac-ring collider', 'Phi(1020), particle source', 'synchrotron radiation, particle source', 'free electron laser', 'proton synchrotron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010066'],['Main parameters of linac-ring type $phi$ factory and 1-5 GeV energy proton synchrotron proposed in the framework of the Turkic Accelerator Complex (TAC) Project are discussed'],['2000-10-27']
530,['eng'],"['Haas, R']",['Search for Second and Third Generation Leptoquarks at CDF'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'anti-p p, colliding beams', 'new particle, search for', 'leptoquark, pair production', 'technicolor', 'technipion', 'color, triplet', 'technirho', 'color, octet', 'final state, (2jet missing-energy)', 'transverse energy, missing-energy', 'quark, heavy', 'electroweak interaction, validity test', 'channel cross section, mass', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010064'],"['We report the results of a search for second and third generation leptoquarks using 88 ${pb}^{-1}$ of data recorded by the Collider Detector at Fermilab. Color triplet technipions, which play the role of scalar leptoquarks, are investigated due to their potential production in decays of strongly coupled color octet technirhos. Events with a signature of two heavy flavor jets and missing energy may indicate the decay of a second (third) generation leptoquark to a charm (bottom) quark and a neutrino. As the data is found to be consistent with Standard Model expectations, mass limits are determined.']",['2000-10-26']
531,['eng'],"['Berg, B A']",['Clopper-Pearson Bounds from HEP Data Cuts'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'Higgs particle, search for', 'statistical analysis', 'programming, Monte Carlo', 'numerical calculations, Monte Carlo', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010061'],"['For the measurement of $N_s$ signals in $N$ events rigorous confidence bounds on the true signal probability $p_{\\rm exact}$ were established in a classical paper by Clopper and Pearson [Biometrica 26, 404 (1934)]. Here, their bounds are generalized to the HEP situation where cuts on the data tag signals with probability $P_s$ and background data with likelihood $P_b<P_s$. The Fortran program which, on input of $P_s$, $P_b$, the number of tagged data $N^Y$ and the total number of data $N$, returns the requested confidence bounds as well as bounds on the entire cumulative signal distribution function, is available on the web. In particular, the method is of interest in connection with the statistical analysis part of the ongoing Higgs search at the LEP experiments.']",['2000-10-26']
532,['eng'],"['Csilling, Akos']",['Charm and bottom production in two-photon collisions with OPAL'],['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, inclusive reaction', 'D*(2010), photoproduction', 'D*(2010), hadronic decay', 'quark, charm', 'quark, beauty', 'quark, pair production', 'differential cross section, transverse momentum', 'channel cross section, energy dependence', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> D*(2010) positron electron', 'electron positron --> 2charm positron electron', 'electron positron --> 2beauty positron electron', '192-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010060'],['A preliminary update of the previous OPAL measurement of the inclusive production of D* mesons in anti-tagged photon-photon collisions is presented together with the first preliminary OPAL measurement of bottom production in photon-photon collisions.'],['2000-10-25']
533,['eng'],"['Alavi-Harati, A', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barker, A R', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Fordyce, P M', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hanagaki, K', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jensen, D A', 'Kessler, R', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian R"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Qiao, C', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S R', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Suzuki, I', 'Swallow, E C', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['A Measurement of the Branching Ratio of $K_{L} \\to e^{+}e^{-}\\gamma\\gamma$'],['Particle Physics - Experimental Results'],"['K0(L), radiative decay', 'K0(L), branching ratio', 'decay, form factor', 'mass spectrum, (positron electron)', 'calorimeter, electromagnetic', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> positron electron 2photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010059'],"['We report on a study of the decay $K_L \\to e^+e^-\\gamma\\gamma$ carried out as a part of the KTeV/E799 experiment at Fermilab. The 1997 data yielded a sample of 1543 events, including an expected background of $56 \\pm 8$ events. An effective form factor was determined from the observed distribution of the $e^+e^-$ invariant mass. Using this form factor in the calculation of the detector acceptance, the branching ratio was measured to be ${\\mathcal B}(K_L \\to e^+ e^- \\gamma \\gamma, E^*_\\gamma > 5 {MeV}) = (5.84 \\pm 0.15 {\\rm ~(stat)} \\pm 0.32 {\\rm ~(sys)})\\times 10^{-7}$.']",['2000-10-24']
534,['eng'],"['Meyer, T I']",['PIN Photodiodes for Radiation Monitoring and Protection in the BaBar Silicon Vertex Tracker'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'radiation protection', 'semiconductor detector, vertex', 'semiconductor, optical', 'dosimetry', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010058'],"['We discuss the design, implementation and performance of the radiation monitoring and protection system used by the Silicon Vertex Tracker (SVT) in the BaBar detector. Using 12 reverse-biased PIN photodiodes mounted around the beampipe near the IP, we are able to provide instantaneous radiation dose rates, absorbed dose integrals, and active protection that aborts the circulating beams in the PEP-II storage ring when radiation levels exceed user-defined thresholds. The system has reliably protected the SVT from excessive radiation damage and has also served as a key diagnostic tool in understanding radiation backgrounds at PEP-II.']",['2000-10-24']
535,['eng'],"['Bialkowska, H', 'Retyk, W']",['Kaon and $\\Phi$ production vs Participants in Nuclear Collisions'],['Particle Physics - Experimental Results'],"['talk, Berkeley 2000/07/20', 'scattering, heavy ion', 'p nucleus, nuclear reaction', 'K, hadroproduction', 'yield, (Phi(1020) K)', 'dependence, impact parameter', 'dependence, density', 'numerical calculations, interpretation of experiments', 'Brookhaven PS', 'CERN SPS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010057'],"[""Data on kaon and $\\Phi$ production in nuclear collisions as a function of centrality are analysed both at AGS and SPS energy range. We compare the results of several experiments, looking for common trend in `participant scaling' of production yields. We find a smooth description of scaled kaon and $\\Phi$ yields as a function of participant density. We also show a participant density dependence of kaons and $\\Phi$ produced in the forward hemisphere for proton-nucleus collisions.""]",['2000-10-24']
536,['eng'],"['Kudryavtsev, V A', 'Brook, R A', 'Cartwright, S L', 'McMillan, J E', 'Spooner, N J C', 'Thompson, L F']",['Energy calibration of large underwater detectors using stopping muons'],['Particle Physics - Experimental Results'],"['deep underground detector, water', 'Cherenkov counter, water', 'calibration', 'muon, cosmic radiation', 'deep underground detector, AMANDA', 'deep underground detector, Baikal', 'deep underground detector, ANTARES']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010056'],"['We propose to use stopping cosmic-ray muons in the energy calibration of planned and deployed large underwater detectors. The method is based on the proportionality between the incident muon energy and the length of the muon path before it stops. Simultaneous measurements of the muon path and the amplitude of the signal from the photomultiplier tubes allow a relation between the energy deposited in the sensitive volume of the detector and the observed signal to be derived, and also provide a test of detector simulations. We describe the proposed method and present the results of simulations.']",['2000-10-24']
537,['eng'],"['Giacomelli, Giorgio', 'Margiotta, A']",['Neutrino physics and astrophysics with the MACRO detector'],['Particle Physics - Experimental Results'],"['talk, La Paz 2000/07/23', 'astrophysics', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'WIMP, search for', 'muon, angular distribution', 'antineutrino nucleon, interaction', 'antineutrino/e', 'charged current', 'deep underground detector, MACRO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010055'],"['After a brief presentation of the MACRO detector we discuss the data on atmospheric neutrinos and neutrino oscillations, on high energy (E> 1 GeV) neutrino astronomy, on indirect searches for WIMPs and low energy (E >7 MeV) stellar collapse neutrinos.']",['2000-10-24']
538,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Anthonis, T', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bähr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P D', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coppens, Y R', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Fleming, Y H', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hildebrandt, M', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Koutouev, R', 'Koutov, A', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebailly, E', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'List, B', 'Lobodzinska, E', 'Lobodzinski, B', 'Loginov, A Y', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, A B', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Risler, C', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schmitt, S', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Schwanenberger, C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Tsurin, I', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vasilev, S', 'Vazdik, Ya', 'Vichnevski, A', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Measurement and QCD Analysis of Jet Cross Sections in Deep-Inelastic Positron-Proton Collisions at $\\sqrt{s}$ of 300 GeV'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'jet, pair production', 'kinematics, Breit frame', 'differential cross section, transverse energy', 'momentum transfer, dependence', 'rapidity dependence', 'strong interaction, coupling constant', 'gluon, momentum spectrum', 'quark, momentum spectrum', 'renormalization', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'tables', 'bibliography', 'positron p --> jet positron anything', 'positron p --> 2jet positron anything', 'approx. 300 GeV-Cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010054'],['Jet production is studied in the Breit frame in deep-inelastic positron-proton scattering over a large range of four-momentum transfers 5 < Q^2 < 15000 GeV^2 and transverse jet energies 7 < E_T < 60 GeV. The analysis is based on data corresponding to an integrated luminosity of L_int \\simeq 33 pb^(-1) taken in the years 1995-1997 with the H1 detector at HERA at a center-of-mass energy sqrt(s)=300 GeV. Dijet and inclusive jet cross sections are measured multi-differentially using k_perp and angular ordered jet algorithms. The results are compared to the predictions of perturbative QCD calculations in next-to-leading order in the strong coupling constant alphas.QCD fits are performed in which alphas and the gluon density in the proton are determined separately. The gluon density is found to be in good agreement with results obtained in other analyses using data from different processes. The strong coupling constant is determined to be alphas(MZ)=0.1186+-0.0059. In addition an analysis of the data in which both alphas and the gluon density are determined simultaneously is presented.'],['2000-10-24']
539,['eng'],"['Arsenescu, R', 'Baglin, C', 'Beck, H P', 'Borer, K', 'Bussière, A', 'Elsener, Konrad', 'Gorodetzky, P', 'Guillaud, J P', 'Kabana, S', 'Klingenberg, R', 'Lehmann, G', 'Lindén, T', 'Lohmann, K D', 'Mommsen, R K', 'Moser, U', 'Pretzl, Klaus P', 'Schacher, J', 'Spiwoks, R', 'Tuominiemi, Jorma', 'Weber, M']",['Centrality dependence of K+ produced in Pb+Pb collisions at 158 GeV per nucleon'],['Particle Physics - Experimental Results'],"['talk, Berkeley 2000/07/20', 'scattering, heavy ion', 'lead', 'K+, hadroproduction', 'K+, yield', 'dependence, impact parameter', 'quark gluon, plasma', 'calorimeter, experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010053'],"[""The NA52 collaboration searches for a discontinuous behaviour of charged kaons produced in Pb+Pb collisions at 158 A GeV as a function of the impact parameter, which could reveal a hadron to quark-gluon plasma (QGP) phase transition. The K+ yield is found to grow proportional to the number of participating ('wounded') nucleons N, above N=100. Previous NA52 data agree with the above finding and show a discontinuous behaviour in the kaon centrality dependence near N=100, marking the onset of strangeness enhancement -over e.g. p+A data at the same \\sqrt{s}- in a chemically equilibrated phase.""]",['2000-10-23']
540,['eng'],"['Valls, J A']",['Search for Neutral Supersymmetric Higgs Bosons in $p\\overline{p}$ Collisions at $\\sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Higgs particle, search for', 'Higgs particle, neutral particle', 'supersymmetry', 'Higgs particle, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, associated production', 'squark, truth', 'squark, interference', 'Higgs particle, mass', 'lower limit', 'channel cross section, branching ratio', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> Higgs particle 2beauty anything', 'Higgs particle --> 2beauty', '1800 GeV-ems']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010052'],"['We present the results of a search for neutral Higgs bosons produced in association with $b$ quarks in $p\\bar{p}\\to b\\bar{b} \\phi\\to b\\bar{b}b\\bar{b}$ final states with $91 \\pm 7$ pb$^{-1}$ of $p\\bar{p}$ collisions at $\\sqrt{s}=1.8$ TeV recorded by the Collider Detector at Fermilab. We find no evidence of such a signal and the data is interpreted in the context of the neutral Higgs sector of the Minimal Supersymmetric extension of the Standard Model. With basic parameter choices for the supersymmetric scale and the stop quark mixing, we derive 95% C.L. lower mass limits for neutral Higgs bosons for $\\tb$ values in excess of 35.']",['2000-10-23']
541,['eng'],"['Johnson, M B', 'Kopeliovich, V B', 'Potashnikova, I K', 'McGaughey, P L', 'Moss, J M', 'Peng, J C', 'Garvey, G T', 'Leitch, M J', 'Adams, M R', 'Alde, D M', 'Baer, H W', 'Barlett, M L', 'Brown, C N', 'Cooper, W E', 'Carey, T A', 'Danner, G', 'Hoffmann, G W', 'Hsiung, Y B', 'Kaplan, D M', 'Klein, A', 'Lee, C', 'Lillberg, J W', 'McCarthy, R L', 'Mishra, C S', 'Wang, M J']",['Energy loss of fast quarks in nuclei'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'deuteron', 'carbon', 'calcium', 'iron', 'tungsten', 'muon, pair production', 'Drell-Yan process', 'yield, mass number', 'quark, energy loss', 'shadowing', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'p nucleus --> muon+ muon- anything', '900 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010051'],"[""We report an analysis of the nuclear dependence of the yield of Drell-Yan dimuons from the 800 GeV/c proton bombardment of $^2H$, C, Ca, Fe, and W targets. Employing a new formulation of the Drell-Yan process in the rest frame of the nucleus, this analysis examines the effect of initial-state energy loss and shadowing on the nuclear-dependence ratios versus the incident proton's momentum fraction and dimuon effective mass. The resulting energy loss per unit path length is $-dE/dz = 2.32 \\pm 0.52\\pm 0.5$ GeV/fm. This is the first observation of a nonzero energy loss of partons traveling in nuclear environment.""]",['2000-10-20']
542,['eng'],"['Hochman, D']",['Recent Results on Charm Photoproduction'],['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'D/s, photoproduction', 'D/s, hadronic decay', 'D*(2010), photoproduction', 'channel cross section, ratio', 'charmed meson, excited state', 'quantum chromodynamics, perturbation theory', 'J/psi(3100), photoproduction', 'J/psi(3100), leptonic decay', 'differential cross section, transverse momentum', 'rapidity dependence', 'mass spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010050'],"[""Photoproduction of $D_s^{\\pm}$ mesons has been measured in the ZEUS detector at HERA and compared with predictions of NLO pQCD calculations. The ratio of $D_s^{*\\pm}$ to $D^{*\\pm}$ cross sections has been compared to results from $e^{+}e^{-}$ experiments. Orbitally excited P-wave charm mesons have been observed in the $D^{*\\pm}\\pi^{\\mp}$ final state. The fraction of $D^{*\\pm}$ 's originating from these mesons has been calculated and compared with that from $e^{+}e^{-}$ interactions. No evidence for radially excited mesons decaying to $D^{*\\pm}\\pi^{+}\\pi^{-}$ was found. The inelastic production of J/$\\psi$ mesons has been measured and compared to LO and NLO pQCD predictions.""]",['2000-10-20']
543,['eng'],"['Serin, L']",['Lower limit on the mass of the neutralino (LSP) at LEP with the ALEPH detector'],['Particle Physics - Experimental Results'],"['talk, Heidelberg 2000/07/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'sparticle, pair production', 'chargino', 'slepton', 'neutralino, LSP', 'neutralino, mass', 'lower limit', 'Higgs particle, mass', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '130-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010049'],"['The large amount of data accumulated at LEP2 by the ALEPH experiment has been used to search for supersymmetric particles. No signal has been found therefore limits have been determined. Within the Constrained Minimal Supersymmetric Standard Model, the constraints from direct SUSY searches of charginos, sleptons and neutralinos, are combined to extract a lower limit on the mass of the neutralino considered to be the Lightest Supersymmetric particle. An improved limit is obtained when the limit on the Higgs mass is included. Neutralino masses up to 38 GeV/c^2 are excluded at 95 % confidence level.']",['2000-10-20']
544,['eng'],"['Littenberg, L S']",['Rare Kaon Decays'],['Particle Physics - Experimental Results'],"['review, Les Arcs 2000/03/11', 'K, rare decay', 'K, semileptonic decay', 'K, leptonic decay', 'K+', 'K0(L)', 'K, branching ratio', 'upper limit', 'violation, flavor', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010048'],['The current status of the study of rare kaon decays is reviewed. Future prospects are discussed.'],['2000-10-19']
545,['eng'],"['Savinov, V', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H']",['Search for a Scalar Bottom Quark with Mass 3.5-4.5 GeV/$c^{2}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'squark, beauty', 'squark, mass', 'beautiful meson, sparticle', 'beautiful meson, pair production', 'beautiful meson, semileptonic decay', 'correlation, (charmed meson dilepton)', 'channel cross section, upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.52 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010047'],"['We report on a search for a supersymmetric $\\tilde{B}$ meson with mass between 3.5 and 4.5 GeV/$c^2$ using 4.52 ${\\rm fb}^{-1}$ of integrated luminosity produced at $\\sqrt{s}=10.52$ GeV, just below the $e^+e^-\\to B\\bar{B}$ threshold, and collected with the CLEO detector. We find no evidence for a light scalar bottom quark.']",['2000-10-19']
546,['eng'],"['Martyn, H U']",['Event shape studies at HERA'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, pair production', 'event shape analysis', 'kinematics, Breit frame', 'quantum chromodynamics, perturbation theory', 'correction, higher-order', 'correction, hadronization', 'energy dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010046'],['Recent progress on the study of power corrections applied to event shape variables in deep inelastic ep scattering is discussed.'],['2000-10-19']
547,['eng'],"['Arsenescu, R', 'Beck, H P', 'Borer, K', 'Kabana, S', 'Klingenberg, R', 'Lehmann, G', 'Mommsen, R K', 'Moser, U', 'Pretzl, Klaus P', 'Schacher, J', 'Spiwoks, R', 'Weber, M', 'Elsener, Konrad', 'Lohmann, K D', 'Baglin, C', 'Bussière, A', 'Guillaud, J P', 'Lindén, T', 'Tuominiemi, Jorma', 'Gorodetzky, P']",['Centrality dependence of K+ produced in Pb+Pb collisions at 158 GeV per nucleon'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'scattering, heavy ion', 'lead', 'K+, hadroproduction', 'K+, yield', 'dependence, impact parameter', 'quark gluon, plasma', 'critical phenomena', 'experimental results', 'CERN SPS', 'lead lead --> K+ anything', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010045'],"[""The NA52 collaboration searches for a discontinuous behaviour of charged kaons produced in Pb+Pb collisions at 158 A GeV as a function of the impact parameter, which could reveal a hadron to quark-gluon plasma (QGP) phase transition. The K+ yield is found to grow proportional to the number of participating ('wounded') nucleons N, above N=100. Previous NA52 data agree with the above finding and show a discontinuous behaviour in the kaon centrality dependence near N=100, marking the onset of strangeness enhancement -over e.g. p+A data at the same \\sqrt{s}- in a chemically equilibrated phase.""]",['2000-10-19']
548,['eng'],"['Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Todorova-Nová, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Copty, N K', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Devmal, S C', 'Fernández, A', 'Fox, G F', 'Gagnon, P', 'Gerzon, S', 'Göbel, C', 'Gounder, K', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lichtenstadt, J', 'Lundberg, B', 'May Tal-Beck, S', 'Meadows, B', 'De Mello-Neto, J R T', 'Mihalcea, D', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'De Oliveira, A B', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Dos Reis, A C', 'Rubin, H A', 'Sanders, D A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Slaughter, A J', 'Sokoloff, M D', 'Solano, J M', 'Stanton, N R', 'Stefanski, R J', 'Stenson, K', 'Summers, D J', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yang, S M', 'Yi, D', 'Yoshida, S', 'Zaliznyak, R', 'Zhang, C']",['Observation of color-transparency in diffractive dissociation of pions'],['Particle Physics - Experimental Results'],"['pi- nucleus, coherent interaction', 'carbon', 'platinum', 'diffraction, dissociation', 'jet, pair production', 'color, transparency', 'cross section, parametrization', 'transverse momentum, spectra', 'dependence, mass number', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> nucleus 2jet', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010044'],"['We have studied the diffractive dissociation into di-jets of 500 GeV/c pions scattering coherently from carbon and platinum targets. Extrapolating to asymptotically high energies (where t_{min} approaches 0) we find that when the per-nucleus cross-section for this process is parameterized as $ \\sigma = \\sigma_0 A^{\\alpha} $, $ \\alpha $ has values near 1.6, the exact result depending on jet transverse momentum. These values are in agreement with those predicted by theoretical calculations of color-transparency.']",['2000-10-18']
549,['eng'],"['Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Todorova-Nová, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Copty, N K', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Deval, S', 'Fernández, A', 'Fox, G F', 'Gagnon, P', 'Gerzon, S', 'Göbel, C', 'Gounder, K', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lichtenstadt, J', 'Lundberg, B', 'May Tal-Beck, S', 'Meadows, B', 'De Mello-Neto, J R T', 'Mihalcea, D', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'De Oliveira, A B', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Dos Reis, A C', 'Rubin, H A', 'Sanders, D A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Slaughter, A J', 'Sokoloff, M D', 'Solano, J M', 'Stanton, N R', 'Stefanski, R J', 'Stenson, K', 'Summers, D J', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yang, S M', 'Yi, D', 'Yoshida, S', 'Zaliznyak, R', 'Zhang, C']","['Direct measurement of the pion valence quark momentum distribution, the pion light-cone wave function squared']",['Particle Physics - Experimental Results'],"['pi- nucleus, interaction', 'platinum', 'diffraction, dissociation', 'jet, pair production', 'pi, structure function', 'quark, valence', 'quark, momentum spectrum', 'pi, wave function', 'wave function, light cone', 'transverse momentum, spectra', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> nucleus 2jet', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010043'],"['We present the first direct measurements of the pion valence quark momentum distribution which is related to the square of the pion light-cone wave function. The measurements were carried out using data on diffractive dissociation of 500 GeV/c $\\pi^-$ into di-jets from a platinum target at Fermilab experiment E791. The results show that the $|q\\bar {q}>$ light-cone asymptotic wave function, which was developed using perturbative QCD methods, describes the data well for $Q^2 \\sim 10 ~{\\rm (GeV/c)^2}$ or more. We also measured the transverse momentum distribution of the diffractive di-jets.']",['2000-10-18']
550,['eng'],"['Wing, M']",['Introduction to high$-p_T$ inclusives'],['Particle Physics - Experimental Results'],"['review, Ambleside 2000/08/26', 'positron p, colliding beams', 'anti-p p, colliding beams', 'jet, photoproduction', 'jet, hadroproduction', 'transverse momentum, high', 'rapidity spectrum', 'gluon, momentum spectrum', 'quantum chromodynamics, validity test', 'perturbation theory, higher-order', 'transverse energy, high', 'event shape analysis', 'jet, multiplicity', 'photon, direct production', 'differential cross section', 'experimental results', 'DESY HERA Stor', 'Batavia TEVATRON Coll', '300, 630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010042'],"['A selection of theoretical and experimental results are presented in the broader context of understanding QCD and its relation to photon physics. A phenomenological analysis of HERA data to constrain the gluon content of the proton and photon is discussed. Measurements from the Tevatron and fixed-target experiments are compared to theoretical predictions. Finally, the future of higher order pQCD calculations is addressed.']",['2000-10-18']
551,['eng'],"['Kuhne, R']",['Possible Observation of a Second Kind of Light'],['Particle Physics - Experimental Results'],"['photon nucleus, interaction', 'iron', 'photon, path length', 'spin, rotator', 'photon, magnetic', 'interpretation of experiments', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010040'],"['According to classical electrodynamics, sunlight that is passed through an iron layer can be detected with the naked eye only if the thickness of the layer is less than 170nm. However, in an old experiment, August Kundt was able to see the sunlight with the naked eye even when it had passed an iron layer with thickness greater than 200nm. To explain this observation, we propose a second kind of light which was introduced in a different context by Abdus Salam. A tabletop experiment can verify this possibility.']",['2000-10-18']
552,['eng'],"['Numao, T']",['Rare Kaon Decays'],['Particle Physics - Experimental Results'],"['talk, Adelaide 2000/03/13', 'K, rare decay', 'neutral current, flavor changing', 'Kobayashi-Maskawa angle, unitarity', 'experimental methods', 'experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino', 'K0(L) --> pi0 neutrino antineutrino', 'K0(L) --> pi0 lepton+ lepton-', 'K0(L) --> lepton+ lepton-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010039'],['Rare kaon decays via Flavor Changing Neutral Currents are discussed in the context of the CKM unitarity triangle with a particular interest in the rare kaon decays K^+ --> pi^+ nu nubar and K^0_L --> pi^0 nu nubar. New results and the status of these experiments are reported.'],['2000-10-17']
553,['eng'],"['Purohit, M V']",['Light meson and baryon spectroscopy from charm decays in Fermilab E791'],['Particle Physics - Experimental Results'],"['pi nucleus, inclusive reaction', 'carbon', 'platinum', 'charmed particle, photoproduction', 'charmed particle, decay modes', 'Lambda/c+, polarization', 'transverse momentum, dependence', 'D+', 'D/s+', 'hadron spectroscopy', 'decay, amplitude analysis', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'Lambda/c+ --> p K- pi+', 'D+ --> 2pi+ pi-', 'D/s+ --> 2pi+ pi-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010038'],"['We present results from Fermilab experiment E791. We extracted the fractions of resonant components in the $\\Lambda_c^+\\to p K^- \\pi^+$ decays, and found a significant polarization of the $\\Lambda_c^+$ using a fully 5-dimensional resonant analysis. We also did resonant analyses of $D^+$ and $D^+_s$ decays into $\\pi^+\\pi^-\\pi^+$. We observed an insignificant asymmetry in the Breit Wigner describing the $f_0(980)$ and found good evidence for a light and broad scalar resonance in the $D^+$ decays.']",['2000-10-17']
554,['eng'],"['Sultansoy, S F']","['The ""Golden Mode"" at the Upgraded Tevatron?']",['Particle Physics - Experimental Results'],"['anti-p p, inclusive reaction', 'Higgs particle, search for', 'Higgs particle, decay modes', 'family, >3', 'gluon gluon, fusion', 'final state, (4lepton)', 'channel cross section', 'numerical calculations, Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010037'],"['The exiatence of extra SM families results in essential enhancement of the gluon fusion channel Higgs boson production at hadron colliders. In this case, the SM Higgs boson can be seen at the upgraded Tevatron via the ""golden mode"" (H-->4l) for certain values of its mass.']",['2000-10-17']
555,['eng'],"['Richichi, S', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Nelson, H N', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M']",['Study of $B \\to \\psi (2S)K$ and $B \\to \\psi (2S)K^{*}$(892) Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B+, branching ratio', 'B0, branching ratio', 'helicity, angular dependence', 'polarization, longitudinal', 'psi(3685)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> psi(3685) K*(892)', 'B0 --> psi(3685) K0', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010036'],"['Color-suppressed decays of $B$ mesons to final states with $\\psi(2S)$ mesons have been observed with the CLEO detector. The branching fractions for the decays $B^+ \\to \\psi(2S) K^+$, $B^+ \\to \\psi(2S) K^*(892)^+$, $B^0 \\to \\psi(2S) K^0$, and $B^0 \\to \\psi(2S) K^*(892)^0$ are measured to be (7.8 +- 0.7 +- 0.9) 10^{-4}$, (9.2 +- 1.9 +- 1.2) 10^{-4}$, (5.0 +- 1.1 +- 0.6) 10^{-4}$, and (7.6 +- 1.1 +- 1.0) 10^{-4}$, respectively, where the first uncertainty is statistical and the second is systematic. The first measurement of the longitudinal polarization fraction is extracted from the angular analysis of the $B \\to \\psi(2S) K^*(892)$ candidates: $\\Gamma_L / \\Gamma = 0.45 +- 0.11 +- 0.04 $. Our measurements of the decays $B^0 \\to \\psi(2S) K^0$ and $B^+ \\to \\psi(2S) K^*(892)^+$ are first observations.']",['2000-10-17']
556,['eng'],"['Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Savinov, V', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kandaswamy, J', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V']",['Observation of the $\\Omega_{c}^{0}$ Charmed Baryon at CLEO'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Omega/c0, electroproduction', 'Omega/c0, hadronic decay', 'Omega/c0, mass', 'Omega/c0, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Omega/c0 --> Omega- 2pi+ pi-', 'Omega/c0 --> Omega- pi+ pi0', 'Omega/c0 --> Omega- pi+', 'Omega/c0 --> Xi- K- 2pi+', 'Omega/c0 --> Xi0 K- pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010035'],"['The CLEO experiment at the CESR collider has used 13.7 fb$^{-1}$ of data to search for the production of the $\\Omega_c^0$ (css-ground state) in $e^{+}e^{-}$ collisions at $\\sqrt{s} \\simeq 10.6$ {\\rm GeV}. The modes used to study the $\\Omega_c^0$ are $\\Omega^- \\pi^+$, $\\Omega^- \\pi^+ \\pi^0$, $\\Xi^- K^- pi^+ \\pi^+$, $\\Xi^0 K^- pi^+$, and $\\Omega^- \\pi^+ \\pi^- \\pi^+$. We observe a signal of 40.4$\\pm$9.0(stat) events at a mass of 2694.6$\\pm$2.6(stat)$\\pm$1.9(syst) {\\rm MeV/$c^2$}, for all modes combined.']",['2000-10-17']
557,['eng'],"['Telnov, V I']","['Introduction and recent developments in $\\gamma-\\gamma$, $\\gamma-e$ colliders']",['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'electron positron, linear collider', 'photon electron, colliding beams', 'photon photon, colliding beams', 'new particle, search for', 'Higgs particle', 'charged particle, pair production', 'quantum gravity', 'Compton scattering, backscatter', 'beam emittance', 'laser', 'storage ring, optical', 'DESY TESLA Linac']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010034'],"[""High energy photon colliders (gamma-gamma, gamma-electron) based on backward Compton scattering of laser light is a very natural addition to e+e- linear colliders. In this report we consider mainly this option for the TESLA project. Recent study has shown that the horizontal emittance in the TESLA damping ring can be further decreased by a factor of four. In this case the gamma-gamma luminosity luminosity in the high energy part of spectrum can reach 0.3--0.5 L_e+e-. Typical cross sections of interesting processes in gamma-gamma collisions are higher than those in e+e- collisions by about one order of magnitude, so the number of events in gamma-gamma collisions will be more that in e+e- collisions. The key new element in photon colliders is a very powerful laser system. The most straightforward solution is ``an optical storage ring (optical trap)'' with diode pumped laser injector which is today technically feasible. This paper briefly review the status of a photon collider based at TESLA, its possible parameters.""]",['2000-10-17']
558,['eng'],"['Telnov, V I']",['Photon collider at TESLA'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2000/06/14', 'electron positron, linear collider', 'photon electron, colliding beams', 'photon photon, colliding beams', 'Higgs particle, search for', 'charged particle, pair production', 'quantum gravity', 'luminosity', 'Compton scattering, backscatter', 'beam optics, beta function', 'beam emittance', 'optics, laser', 'storage ring, optical', 'RF system, optical', 'free electron laser', 'DESY TESLA Linac', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010033'],"[""High energy photon colliders (gamma-gamma, gamma-electron) based on backward Compton scattering of laser light is a very natural addition to e+e- linear colliders. In this report we consider this option for the TESLA project. Recent study has shown that the horizontal emittance in the TESLA damping ring can be further decreased by a factor of four. In this case the gamma-gamma luminosity luminosity in the high energy part of spectrum can reach 0.3--0.5 L_{e+e-}. Typical cross sections of interesting processes in gamma-gamma collisions are higher than those in e+e- collisions by about one order of magnitude, so the number of events in gamma-gamma collisions will be more that in e+e- collisions. Photon colliders can, certainly, give additional information and they are the best for the study of many phenomena. The main question is now the technical feasibility. The key new element in photon colliders is a very powerful laser system. An external optical cavity is a promising approach for the TESLA project. A free electron laser is another option. However, a more straightforward solution is ``an optical storage ring (optical trap)'' with diode pumped laser injector which is today technically feasible. This paper briefly review the status of a photon collider based at TESLA, its possible parameters and existing problems.""]",['2000-10-16']
559,['eng'],"['Elvira, V D']",['QCD at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Lisbon 2000/06/29', 'anti-p p, colliding beams', 'quantum chromodynamics, validity test', 'jet, hadroproduction', 'jet, fragmentation', 'channel cross section, energy dependence', 'transverse energy, spectra', 'cross section, ratio', 'production, small-angle', 'rapidity dependence', 'mass spectrum, (2jet)', 'jet, multiplicity', 'hadron, multiplicity', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010032'],"['At the Fermilab Tevatron energies, ($\\sqrt{s}$=1800 GeV and $\\sqrt{s}$=630 GeV), jet production is the dominant process. During the period 1992-1996, the D0 and CDF experiments accumulated almost 100 pb**-1 of data and performed the most accurate jet production measurements up to this date. These measurements and the NLO-QCD theoretical predictions calculated during the last decade, have improved our understanding of QCD, our knowledge of the proton structure, and pushed the limit to the scale associated with quark compositeness to 2.4-2.7 TeV. In this paper, we present the most recent published and preliminary measurements on jet production and fragmentation by the D0 and CDF collaborations.']",['2000-10-16']
560,['eng'],"['Abbiendi, G', 'Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Investigation of the Decay of Orbitally-Excited B Mesons and First Measurement of the Branching Ratio $BR(B*_{J} \\to B*\\pi(X))$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'beautiful meson, excited state', 'beautiful meson, hadronic decay', 'beautiful meson, radiative decay', 'beautiful meson, branching ratio', 'mass spectrum, (B*(5320) pi)', 'mass, width', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010031'],"['From about 4 million hadronic Z decays recorded by the OPAL detector on and near to the Z resonance, we select a sample of more than 570000 inclusively reconstructed B mesons. Orbitally-excited mesons B*J are reconstructed using Bpi+- combinations. Independently, B* mesons are reconstructed using the decay B* -> Bgamma. The selected B* candidates are used to obtain samples enriched or depleted in the decay B*J -> B*pi+-(X), where (X) refers to decay modes with or without additional accompanying decay particles. From the number of signal candidates in the Bpi+- mass spectra of these two samples, we perform the first measurement of the branching ratio of orbitally-excited B mesons decaying into B*pi(X): BR(B*J ->B*pi(X)) = 0.85 +0.36-0.37 +- 0.12, where the first error is statistical and the second systematic. If B*J decay modes other than single pion transitions can be neglected the measured ratio corresponds to the branching ratio BR(B*J->B*pi). In the framework of Heavy Quark Symmetry, a simultaneous fit to the Bpi+- mass spectra of the samples enriched or depleted in B*J->B*pi+-(X) decays yields the mass and the width of the B1(3/2) state, as well as the branching ratio of B*J mesons decaying into B*pi: M(B1(3/2)) = (5.738 +0.005-0.006 +-0.007) GeV/c2 G(B1(3/2)) = (18 +15-13 +29-23) MeV/c BR(B*J->B*pi) = 0.74 +0.12-0.10 +0.21-0.15, where the uncertainties are statistical and systematic, respectively.']",['2000-10-16']
561,['eng'],"['Braccini, S']",['K0sK0s Final State and Glueball Searches and $\\Lambda-\\overline{\\Lambda}$ Production in Two-Photon Collisions in L3 at LEP'],['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, inclusive reaction', 'K0(S), pair production', 'Lambda, pair production', 'glueball, search for', 'mass spectrum', 'f2(1525)', 'interference, (a2(1320) f2(1270))', 'meson resonance, (1750)', 'f4(2220)', 'width, branching ratio', 'upper limit', 'quark, diquark', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2K0(S) positron electron anything', 'electron positron --> Lambda Antilambda positron electron anything', '91-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010030'],"[""The K0sK0s final state in two-photon collisions is studied with the L3 detector at LEP using data collected at centre-of-mass energies from 91 GeV to 202 GeV. The mass spectrum is dominated by the formation of the f_2'(1525) tensor meson in the helicity two state. The two-photon width times the branching ratio is measured to be Gamma_{gamma gamma}(f_2'(1525))Br(f_2'(1525)->KKbar) = 0.076 +- 0.006 +- 0.011 keV. Clear evidence for destructive f_2(1270)-a_2(1320) interference is observed. In addition a clear signal for f_J(1750) is observed. The study of the decay angular distribution in the 1750 MeV mass region shows that the spin two helicity two wave is dominant. No signal is observed in the region around 2.2 GeV. The upper limit for the two-photon partial width of the \\xi(2230) tensor glueball candidate of Gamma_{gamma gamma}(\\xi(2230))Br(\\xi(2230)->K0sK0s)<1.4 eV at 95% C.L. is derived. The production of Lambda-Lambdabar pairs in two-photon collisions is also studied. The cross section is compared to quark-diquark model predictions.""]",['2000-10-16']
562,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Production rate of $b\\overline{b}$ quark pairs from gluons and $b\\overline{b}b\\overline{b}$ events in hadronic Z decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'gluon, fragmentation', 'quark, beauty', 'quark, pair production', 'final state, (4beauty)', 'track data analysis, vertex', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'Z0 --> 4beauty', 'gluon --> 2beauty', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010029'],"['The rates are measured per hadronic Z decay for gluon splitting to bb(bar) quark pairs, g_bb, and of events containing two bb(bar) quark pairs, g_4b, using a sample of four-jet events selected from data collected with the OPAL detector. Events with an enhanced signal of gluon splitting to bb(bar) quarks are selected if two of the jets are close in phase-space and contain detached secondary vertices. For the event sample containing two bb(bar) quark pairs, three of the four jets are required to have a significantly detached secondary vertex. Information from the event topology is combined in a likelihood fit to extract the values of g_bb and g_4b, namely g_bb = (3.07 +- 0.53(stat) +- 0.97(syst))x10^-3 g_4b = (0.36 +- 0.17(stat) +- 0.27(syst))x10^-3']",['2000-10-16']
563,['eng'],"['Wadhwa, M']",['Double Tag Events in Two-Photon Collisions at LEP'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'hadron, multiple production', 'cross section, energy dependence', 'quantum chromodynamics, perturbation theory', 'model, quark parton', 'Lipatov equation', 'experimental results', 'CERN LEP Stor', 'electron positron --> (n)hadron positron electron', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010028'],"['Double tag events in two photon collisions are studied using the L3 detector at the LEP center of mass energies $\\sqrt{s} \\simeq 189-202$ GeV. The cross-section of $\\gamma ^* \\gamma ^*$ collisions is measured at an average photon virtuality $<Q^2 > = 15 \\rm{GeV}^2$. The results are in agreement with Monte Carlo predictions based on perturbative QCD, while the Quark Parton Model alone is insufficient to describe the data. The measurements are compared to the LO and the NLO BFKL calculations']",['2000-10-16']
564,['eng'],"['Abe, T']",['The final SLD results for ALR and Alepton'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, leptonic decay', 'lepton, pair production', 'polarization, asymmetry', 'coupling, (Z0 lepton)', 'coupling, asymmetry', 'lepton, universality', 'Weinberg angle', 'Higgs particle, mass', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102021'],"['We present the final measurements of the left-right cross-section asymmetry (ALR) for Z boson production by e+e- collisions and Z boson-lepton coupling asymmetry parameters Ae, Amu, and Atau in leptonic Z decays with the SLD detector at the SLAC Linear Collider. Using the complete sample of polarized Z bosons collected at SLD, we get ALR = 0.15056 +- 0.00239, Ae = 0.1544 +- 0.0060, Amu = 0.142 +- 0.015, and Atau = 0.136 +- 0.015. The ALR=Ae and Ae results are combined and we find Ae = 0.1516 +- 0.0021. Assuming lepton universality, we obtain a combined effective weak mixing angle of sin 2 theta eff W = 0.23098 +- 0.00026. Within the context of the SM, our result prefers a light Higgs mass.']",['2001-02-12']
565,['eng'],"['Abott, B', 'Abdesselam, A', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Bacon, T C', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Todorova-Nová, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bauer, D', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Beuselinck, R', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Duflot, L', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gao, M', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grudberg, P M', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Illingworth, R', 'Ito, A S', 'Jaffré, M', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Leggett, C', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Luo, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Papageorgiou, K', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Petroff, P', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Ridel, M', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Differential cross section for W boson production as a function of transverse momentum in proton-antiproton collisions at 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'differential cross section, transverse momentum', 'quantum chromodynamics, perturbation theory', 'validity test', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010026'],['We report a measurement of the differential cross section for W boson production as a function of its transverse momentum in proton-antiproton collisions at sqrt{s} = 1.8 TeV. The data were collected by the D0 experiment at the Fermilab Tevatron Collider during 1994-1995 and correspond to an integrated luminosity of 85 pb^{-1}. The results are in good agreement with quantum chromodynamics over the entire range of transverse momentum.'],['2000-10-13']
566,['eng'],"['Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Savinov, V', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F']",['Study of $\\tau$ Decays to Six Pions and Neutrino'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'pi, multiple production', 'final state, (6pi)', 'eta, intermediate state', 'omega(783), intermediate state', 'CVC model', 'tau-, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> pi+ 2pi- 3pi0 neutrino/tau', 'tau- --> 2pi+ 3pi- pi0 neutrino/tau', 'tau- --> omega(783) pi+ 2pi- neutrino/tau', 'tau- --> eta pi+ 2pi- neutrino/tau', 'tau- --> eta pi- 2pi0 neutrino/tau', '189-200 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010025'],['The $\\tau$ decays to six-pion final states have been studied with the CLEO detector at the Cornell Electron Storage Ring. The measured branching fractions are ${\\cal B}(\\tau^-\\to 2\\pi^-\\pi^+3\\pi^0\\nu_{\\tau })=(2.2 \\pm 0.3 \\pm 0.4)\\times 10^{-4}$ and ${\\cal B}(\\tau^-\\to 3\\pi^-2\\pi^+\\pi^0\\nu_{\\ tau})=(1.7 \\pm 0.2 \\pm 0.2)\\times 10^{-4}$. A search for substructure in these decays shows that they are saturated by intermediate states with $\\eta$ or $\\omega$ mesons. We present the first observation of the decay $\\tau^-\\to 2\\pi^-\\pi^+\\omega\\nu_{\\tau}$ and the branching fraction is measured to be $(1.2 \\pm 0.2 \\pm 0.1) \\times 10^{-4}$. The measured branching fractions are in good agreement with the isospin expectations but somewhat below the Conserved-Vector-Current predictions.'],['2000-10-13']
567,['eng'],"['Achard, P']",['Inclusive $\\pi0$ and K0s in $\\gamma-\\gamma$ at L3'],['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, inclusive reaction', 'pi0, photoproduction', 'K0(S), photoproduction', 'differential cross section, transverse momentum', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> pi0 positron electron anything', 'electron positron --> K0(S) positron electron anything', '189-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010024'],"['The ee -> ee+pi0+X and ee -> ee+K0s+X reactions are studied at LEP using data collected with the L3 detector at sqrt{s}=189-202 GeV. Preliminary results for the differential cross section dsigma/dpt in the transverse momentum range 0.2 GeV < pt < 7.5 GeV at central values of pseudo-rapidity, |eta| < 0.5 or |eta| < 1.5, and the differential cross section dsigma/d|eta| for different values of pt are presented. For pt le 1 GeV, the pt -dependence of the data are well described by an exponential fit. For pt > 1 GeV the cross sections are compared to NLO QCD calculations and to LO Monte Carlo predictions.']",['2000-10-13']
568,['eng'],"['Lai, W P', 'Cheng, K C', 'Li, H B', 'Sheng, H Y', 'Zhuang, B A', 'Chang, C Y', 'Chen, C P', 'Chen, Y P', 'Hsu, H C', 'Li, J', 'Liang, C Y', 'Liu, Y', 'Liu, Z S', 'Luo, C S', 'Shi, F', 'Su, R F', 'Teng, P K', 'Wang, P L', 'Wong, H T', 'Zhang, Z Y', 'Zhao, D X', 'Zhao Jia Wei', 'Zhao, P P', 'Zhou, Z Y']",['The Electronics and Data Acquisition Systems of a CsI(Tl) Scintillating Crystal Detector for Low Energy Neutrino Experiment'],['Particle Physics - Experimental Results'],"['neutrino, interaction', 'scintillation counter, crystal', 'cesium, iodine', 'photoelectron, amplifier', 'electronics', 'data acquisition', 'trigger', 'signal processing', 'programming']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010021'],"['A 500 kg CsI(Tl) scintillating crystal detector is under construction for the studies of low-energy neutrino physics. The requirements, design, realization and the performance of the associated electronics, trigger, data acquisition and software control systems are described. Possibilities for future extensions are discussed.']",['2000-10-12']
569,['eng'],"['Nisius, R']","['First Measurement of the Photon Structure Function $F_{2},c^{\\gamma}$']",['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'quark, charm', 'quark, pair production', 'photon, structure function', 'structure function, charm', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010020'],"['The first measurement of F_2,c^gamma is presented. At low x the measurement indicates a non-zero hadron-like component to F_2,c^gamma. At large x the measurement constitutes a test of perturbative QCD at next-to-leading order, with only m_c and alpha_s as free parameters, with a precision of O(40%).']",['2000-10-12']
570,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Bornheim, A', 'Brock, I', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Rautenberg, J', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Foster, B', 'Heath, G P', 'Heath, H F', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Suszycki, L', 'Szuba, D', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Borras, K', 'Chiochia, V', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Goers, S', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hebbel, K', 'Hillert, S', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Labes, H', 'Löhr, B', 'Mankel, R', 'Martens, J', 'Martínez, M', 'Milite, M', 'Moritz, M', 'Notz, D', 'Petrucci, M C', 'Polini, A', 'Rohde, M', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Parenti, A', 'Pelfer, P G', 'Bamberger, Andreas', 'Benen, A', 'Coppola, N', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Bell, M', 'Doyle, A T', 'Glasman, C', 'Lee, S W', 'Lupi, A', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Carli, T', 'Garfagnini, A', 'Gialas, I', 'Gladilin, L K', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Son, D', 'Barreiro, F', 'García, G', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Vázquez, M E', 'Barbi, M S', 'Corriveau, F', 'Hanna, D S', 'Ochs, A', 'Padhi, S', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Antonov, A', 'Bashkirov, V', 'Danilov, M V', 'Dolgoshein, B A', 'Gladkov, D', 'Sosnovtsev, V V', 'Suchkov, S', 'Dementev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Shcheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tassi, E', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dusini, S', 'Limentani, S', 'Longhin, A', 'Posocco, M', 'Stanco, L', 'Turcato, M', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Saull, P R B', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C']",['Measurement of dijet cross sections for events with a leading neutron in photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'jet, pair production', 'n, leading particle', 'differential cross section, transverse energy', 'rapidity spectrum', 'n, energy spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet n positron anything']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010019'],"['Differential cross sections for dijet photoproduction in association with a leading neutron using the reaction e^+ + p --> e^+ + n + jet + jet + X_r have been measured with the ZEUS detector at HERA using an integrated luminosity of 6.4 pb^{-1}. The fraction of dijet events with a leading neutron in the final state was studied as a function of the jet kinematic variables. The cross sections were measured for jet transverse energies E^{jet}_T > 6 GeV, neutron energy E_n > 400 GeV, and neutron production angle theta_n < 0.8 mrad. The data are broadly consistent with factorization of the lepton and hadron vertices and with a simple one-pion-exchange model.']",['2000-10-11']
571,['eng'],"['Akhmetshin, R R', 'Anashkin, E V', 'Arpagaus, M', 'Aulchenko, V M', 'Banzarov, V S', 'Barkov, L M', 'Bashtovoy, N S', 'Bondar, A E', 'Bondarev, D V', 'Bragin, A V', 'Chernyak, D V', 'Eidelman, S I', 'Fedotovich, G V', 'Gabyshev, N I', 'Grebeniuk, A A', 'Grigoriev, D N', 'Hughes, V W', 'Ignatov, F V', 'Ivanov, P M', 'Karpov, S V', 'Kazanin, V F', 'Khazin, B I', 'Koop, I A', 'Korostelev, M S', 'Krokovnyi, P P', 'Kurdadze, L M', 'Kuzmin, A S', 'Logashenko, I B', 'Lukin, P A', 'Mikhailov, K Yu', 'Nesterenko, I N', 'Okhapkin, V S', 'Otboev, A V', 'Perevedentsev, E A', 'Popov, A S', 'Purlatz, T A', 'Redin, S I', 'Root, N I', 'Ruban, A A', 'Ryskulov, N M', 'Shamov, A G', 'Shatunov, Yu M', 'Shwartz, B A', 'Sibidanov, A L', 'Sidorov, V A', 'Skrinsky, A N', 'Smakhtin, V P', 'Snopkov, I G', 'Solodov, E P', 'Stepanov, P Yu', 'Sukhanov, A Yu', 'Thompson, J A', 'Titov, V M', 'Valishev, A A', 'Yudin, Yu V', 'Zverev, S G']","[""Observation of the $\\phi \\to \\eta' \\gamma$ decay with four charged particles and photons in the final state""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'eta(958), hadronic decay', 'Phi(1020), branching ratio', 'magnetic detector, CMD', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> eta(958) photon', 'eta(958) --> eta pi+ pi-', 'eta --> pi+ pi- pi0', 'eta --> pi+ pi- photon', '10.2 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010018'],"[""Using 11.6 1/pb of data collected in the energy range 0.864-1.06 GeV by CMD-2 at VEPP-2M, the rare decay mode phi to eta' gamma was observed via the decay chain eta' to pi+pi- eta, eta to pi+pi-pi0 or eta to pi+pi- gamma. The following branching ratio was obtained: Br(phi to eta' gamma) = (4.9^{+2.2}_{-1.8} +- 0.6) \\cdot 10^{-5}.""]",['2000-10-10']
572,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bähr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Borras, K', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P D', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Kaufmann, O', 'Kausch, M', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krücker, D', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Kutuev, R K', 'Lachnit, W A', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'List, B', 'Lobodzinska, E', 'Lobodzinski, B', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vazdik, Ya', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J']",['Dijet Production in Charged and Neutral Current $e^{+}p$ Interactions at High $Q^{2}$'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'jet, electroproduction', 'mass spectrum, (2jet)', 'neutral current', 'charged current', 'angular distribution', 'transverse energy, energy spectrum', 'momentum spectrum, parton', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet anything', 'approx. 300 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010016', 'http://www-h1.desy.de/h1/www/publications/htmlsplit/H1prelim-00-035.long.html']","['Jet production in charged and neutral current events in the kinematic range of Q^2 from 640 to 35000 GeV^2 is studied in deep-inelastic positron-proton scattering at HERA. The measured rate of multi-jet events and distributions of jet polar angle, transverse energy, dijet mass, and other dijet variables are presented. Using parton densities derived from inclusive DIS cross sections, perturbative QCD calculations in NLO are found to give a consistent description of both the neutral and charged current dijet production. A direct, model independent comparison of the jet distributions in charged and neutral current events confirms that the QCD dynamics of the hadronic final state is independent of the underlying electroweak scattering process.']",['2000-10-10']
573,['eng'],"['Abe, K', 'Adam, I', 'Akimoto, H', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Berger, R', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Cassell, R', 'Chou, A', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Crawford, G', 'Damerell, C J S', 'Daoudi, M', 'De Groot, N', 'De Sangro, R', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Erofeeva, I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fernández, J P', 'Flood, K', 'Frey, R', 'Hart, E L', 'Hasuko, K', 'Hertzbach, S S', 'Huffer, M E', 'Huynh, X', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Kajikawa, R', 'Kalelkar, M S', 'Kang, H J', 'Kofler, R R', 'Kroeger, R S', 'Langston, M', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'McKemey, A K', 'Messner, R', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Narita, S', 'Nauenberg, U', 'Neal, H', 'Nesom, G', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Ratcliff, B N', 'Reidy, J', 'Reinertsen, P L', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schumm, B A', 'Schwiening, J', 'Serbo, V V', 'Shapiro, G', 'Sinev, N B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Usher, T', 'Vavra, J', 'Verdier, R', 'Wagner, D L', 'Waite, A P', 'Walston, S', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Wright, T R', 'Yamamoto, R K', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H']",['An improved direct measurement of leptonic coupling asymmetries with polarized Z bosons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, leptonic decay', 'electron, pair production', 'muon, pair production', 'tau, pair production', 'Z0, polarization', 'coupling, (Z0 lepton)', 'coupling, asymmetry', 'lepton, universality', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010015'],"['We present final measurements of the Z boson-lepton coupling asymmetry parameters Ae, Amu, and Atau with the complete sample of polarized Z bosons collected by the SLD detector at the SLAC Linear Collider. From the left-right production and decay polar angle asymmetries in leptonic Z decays we measure Ae = 0.1544 +- 0.0060, Amu = 0.142 +- 0.015, and Atau = 0.136 +- 0.015. Combined with our left-right asymmetry measured from hadronic decays, we find Ae = 0.1516 +- 0.0021. Assuming lepton universality, we obtain a combined effective weak mixing angle of sin**2 theta^{eff}_W = 0.23098 +- 0.00026.']",['2000-10-10']
574,['eng'],"['Kushnirenko, A', 'Alkhazov, G', 'Atamanchuk, A G', 'Balatz, M Y', 'Bondar, N F', 'Cooper, P S', 'Dauwe, L J', 'Davidenko, G V', 'Dersch, U', 'Dolgolenko, A G', 'Dzyubenko, G B', 'Edelstein, R M', 'Emediato, L', 'Endler, A M F', 'Engelfried, J', 'Eschrich, I', 'Escobar, C O', 'Evdokimov, A V', 'Filimonov, I S', 'García, F G', 'Gaspero, M', 'Giller, I', 'Golovtsov, V L', 'Gouffon, P', 'Gülmez, E', 'He Kang Ling', 'Iori, M', 'Jun, S Y', 'Kaya, M', 'Kilmer, J', 'Kim, V T', 'Kochenda, L M', 'Konorov, I', 'Kozhevnikov, A P', 'Krivshich, A G', 'Krüger, H', 'Kubantsev, M A', 'Kubarovsky, A V', 'Kulyavtsev, A I', 'Kuropatkin, N P', 'Kurshetsov, V F', 'Kwan, S', 'Lach, J', 'Lamberto, A', 'Landsberg, G L', 'Larin, I', 'Leikin, E M', 'Li Yun Shan', 'Luksys, M', 'Lungov, T', 'Maleev, V P', 'Mao, D', 'Mao Chen Sheng', 'Mathew, P', 'Mattson, M E', 'Matveev, V', 'McCliment, E', 'Moinester, M A', 'Molchanov, V V', 'Morelos, A', 'Nelson, K D', 'Nemitkin, A V', 'Neoustroev, P V', 'Newsom, C R', 'Nilov, A P', 'Nurushev, S B', 'Ocherashvili, A I', 'Önel, Y M', 'Ozel, E', 'Ozkorucuklu, S', 'Penzo, Aldo L', 'Petrenko, S I', 'Pogodin, P I', 'Procario, M', 'Prutskoi, V A', 'Ramberg, E', 'Rappazzo, G F', 'Razmyslovich, B V', 'Rud, V I', 'Russ, J', 'Schiavon, R P', 'Simón, J', 'Sitnikov, A I', 'Skow, D', 'Smith, V J', 'Srivastava, M', 'Steiner, V', 'Stepanov, V', 'Stutte, L', 'Svoiski, M', 'Terentyev, N K', 'Thomas, G P', 'Uvarov, L N', 'Vasilev, A N', 'Vavilov, D V', 'Verebryusov, V S', 'Victorov, V A', 'Vishnyakov, V E', 'Vorobyov, A A', 'Vorwalter, K', 'You, J']",['Precision measurements of the $Lambda_{c}+$ and D0 lifetimes'],['Particle Physics - Experimental Results'],"['hadron nucleus, inclusive reaction', 'pi-', 'p', 'Xi-', 'carbon', 'copper', 'charmed particle, hadroproduction', 'charmed particle, hadronic decay', 'Lambda/c+, lifetime', 'D0, lifetime', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '600 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010014'],"['We report new precision measurements of the lifetimes of the Lambda_c+ and D0 from SELEX, the charm hadro-production experiment at Fermilab. Based upon 1630 Lambda_c+ and 10210 D0 decays we observe lifetimes of tau[Lambda_c+] = 198.1 +- 7.0 +- 5.6 fs and tau[D0] = 407.9 +- 6.0 +- 4.3 fs']",['2000-10-09']
575,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the $B^0$ Lifetime and Oscillation Frequency using $\\overline{B}^{0} \\to D^{*+}l^{-}\\overline{\\nu}$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'anti-B0, semileptonic decay', 'B0, lifetime', 'B0 anti-B0, interference', 'oscillation, time', 'B0, mass difference', 'D*(2010), hadronic decay', 'particle identification, flavor', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'anti-B0 --> D*(2010) lepton- antineutrino', 'D*(2010) --> D0 pi+', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010013'],"['The lifetime and oscillation frequency of the B0 meson has been measured using B0->D*+l-v decays recorded on the Z0 peak with the OPAL detector at LEP. The D*+ -> D0pi+ decays were reconstructed using an inclusive technique and the production flavour of the B0 mesons was determined using a combination of tags from the rest of the event. The results t_B0 = 1.541 +- 0.028 +- 0.023 ps, Dm_d = 0.497 +- 0.024 +- 0.025 ps-1 were obtained, where in each case the first error is statistical and the second systematic.']",['2000-10-09']
576,['eng'],"['Söldner-Rembold, S']",['Photon Structure'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'photon, structure function', 'quantum electrodynamics', 'muon, pair production', 'hadron, multiple production', 'structure function, charm', 'photon, off-shell', 'x-dependence', 'momentum transfer, dependence', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010012'],['The LEP experiments measure the QED and QCD structure of the photon in deep-inelastic electron-photon scattering. The status of these measurements is discussed in this short review.'],['2000-10-09']
577,['eng'],"['Schwiening, J', 'Adam, I', 'Aleksan, R', 'Aston, D', 'Benkebil, M', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Brown, D N', 'Bourgeois, P', 'Chauveau, J', 'Cohen-Tanugi, J', 'Convery, M', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Ferrag, S', 'Gaidot, A', 'Geld, T L', 'Hamel de Monchenault, G', 'Hast, C', 'Höcker, A', 'Kadel, R W', 'Kadyk, J A', 'Lacker, H', 'London, G W', 'Lu, A', 'Lutz, A M', 'Lynch, G', 'Mancinelli, G', 'Martínez-Vidal, F', 'Mayer, N', 'Meadows, B T', 'Müller, D', 'Plaszczynski, S', 'Pripstein, M', 'Ratcliff, B N', 'Roos, L', 'Roussot, E', 'Schune, M H', 'Shelkov, V', 'Sokoloff, M D', 'Spanier, S M', 'Stark, J', 'Telnov, A V', 'Thiebaux, C', 'Vasileiadis, G', 'Vasseur, G', 'Vavra, J', 'Verderi, M', 'Wenzel, W A', 'Wilson, R J', 'Wormser, G', 'Yéche, C', 'Yellin, S', 'Zito, M']","['DIRC, the Particle Identification System for BABAR']",['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'performance', 'silicon, glass', 'optics, reflection', 'photoelectron, amplifier', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010068'],"['The DIRC, a novel type of Cherenkov ring imaging device, is the primary hadronic particle identification system for the BABAR detector at the asymmetric B-factory, PEP-II at SLAC. BABAR began taking data with colliding beams mode in late spring 1999. This paper describes the performance of the DIRC during the first 16 months of operation.']",['2000-10-27']
578,['eng'],"['Russ, J']",['Recent Results from SELEX'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'hadron nucleus, inclusive reaction', 'pi-', 'p', 'Xi-', 'carbon', 'copper', 'charmed particle, hadroproduction', 'charmed particle, hadronic decay', 'charmed particle, lifetime', 'Lambda/c+', 'D0', 'D/s', 'yield, (particle antiparticle)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '600 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010011'],"['The SELEX experiment (E781) is 3-stage magnetic spectrometer for the study of charm hadroproduction at large xF using 600 Gev Sigma-, pi- and p beams. New precise measurements of the Lambda_c, D0, and Ds lifetimes are presented. We also report results on Lambda_c and Ds production by Sigma-, pi- and p beams at xF>0.2. The data agree with expectations from color-drag models to explain charm particle/antiparticle production asymmetries.']",['2000-10-06']
579,['eng'],"['Taylor, R J']",['A high-$Q^{2}$ measurement of the photon structure function $F^{\\gamma}_{2}$ at LEP2'],['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'momentum transfer, high', 'photon, structure function', 'structure function, momentum transfer', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '183-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010010'],"['The photon structure function F_2^gamma has been measured at <Q^2> of 706 GeV^2, using a sample of two-photon events with a scattered electron observed in the OPAL electromagnetic endcap calorimeter. The data were taken during the years 1997-1999, when LEP operated at e+e- centre-of-mass energies ranging from 183 to 202 GeV, and correspond to an integrated luminosity of 424 pb^-1. This analysis represents the highest <Q^2> measurement of F_2^gamma made to date.']",['2000-10-06']
580,['eng'],"['Glasman, C']",['Jet Substructure at HERA'],['Particle Physics - Experimental Results'],"['talk, Ambleside 2000/08/26', 'positron p, colliding beams', 'photon p, interaction', 'jet, photoproduction', 'photon, resolved', 'event shape analysis', 'jet, multiplicity', 'quark, jet', 'gluon, jet', 'leading logarithm approximation', 'showers, parton', 'angular distribution', 'quantum chromodynamics, radiative correction', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010009'],['Measurements of jet shapes and subjet multiplicities in photoproduction performed by ZEUS are presented and compared to leading-logarithm parton-shower Monte Carlo models. The predicted differences on the size of gluon- and quark-initiated jets are used to select samples to study the dynamics of the subprocesses.'],['2000-10-05']
581,['eng'],"['Aihara, H']",['A Measurement of CP Violation in B0 Meson Decays with Belle'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'energy, asymmetry', 'B0, hadronic decay', 'quarkonium, charm', 'K0', 'pi0', 'particle identification, flavor', 'track data analysis, vertex', 'asymmetry, time dependence', 'violation, CP', 'magnetic detector, BELLE', 'experimental results', 'KEK TRISTAN Stor', 'B0 --> quarkonium K0', 'B0 --> J/psi(3100) pi0', '10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010008'],['We present a preliminary measurement of the Standard Model CP violation parameter $\\sin 2\\phi_1$ using the Belle detector. A $6.2~{\\rm fb}^{-1}$ sample of events produced by the KEKB asymmetric $e^+e^-$ collider operating at the $\\Upsilon(4S)$ resonance is used. We report a preliminary result of'],['2000-10-05']
582,['eng'],"['Zeller, G P']",['Electroweak Physics at NuTeV'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'iron', 'charged current', 'neutral current', 'cross section, ratio', 'Weinberg angle', 'electroweak interaction, validity test', ""Z', mass"", 'lower limit', 'scintillation counter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010007'],"['The NuTeV experiment at Fermilab presents a determination of the electroweak mixing angle. High purity, large statistics samples of muon-neutrino and muon-antineutrino events allow the use of the Paschos-Wolfenstein relation, a technique which considerably reduces systematic errors associated with charm production and other sources. Within the Standard Model, this measurement of sin2thw indirectly determines the W boson mass to a precision comparable to direct measurements from high energy e+e- and ppbar colliders. NuTeV measures sin2thw(on-shell)=0.2253+/-0.0019(stat)+/-0.0010(syst), which implies M_W=80.26+/-0.11 GeV. Outside the Standard Model, this result can be used to explore the possibility of new physics; in particular, we present limits on both neutrino oscillations and the presence of extra neutral vector gauge bosons.']",['2000-10-04']
583,['eng'],"['Campanelli, M']",['The experimental future of Neutrino Oscillations'],['Particle Physics - Experimental Results'],"['talk, Hanoi 2000/07/19', 'neutrino, oscillation', 'neutrino, astrophysics', 'neutrino, cosmic radiation', 'neutrino, beam', 'neutrino, mass difference', 'neutrino, mixing angle', 'flavor, 3', 'neutrino, sterile', 'experimental methods', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010006'],"['After the recent experimental results on neutrino oscillations, some shape starts to emerge from the puzzle. However, the situation is still far from being clarified. First of all, accommodating all experimental results in a single and simple framework is not possible, and the possibility of sterile neutrinos entering the oscillation process has not been ruled out. Moreover, new questions arise that the presently-available data, nor those that will be available in a near future, will be able to answer. In this paper some of these problems will be discussed, as well as the experimental guidelines for their clarification.']",['2000-10-04']
584,['eng'],"['Dissertori, G']",['Measurements of the bottom quark mass'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, beauty', 'Z0, branching ratio', 'mass, beauty', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010005'],"['I will review new measurements of the b quark mass, presented at this conference by ALEPH and DELPHI. A large set of observables has been used and detailed studies on jet algorithms have been performed. These measurements at the Z peak are consistent with the results obtained at the Upsilon scale when assuming the running of the b quark mass as predicted by perturbative QCD.']",['2000-10-04']
585,['eng'],"['Iwasaki, M', 'Abe, T', 'Adam, I', 'Akimoto, H', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Berger, R', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Cassell, R', 'Chou, A', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Crawford, G', 'Damerell, C J S', 'Daoudi, M', 'Dasu, S', 'De Groot, N', 'De Sangro, R', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Erofeeva, I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fernández, J P', 'Flood, K', 'Frey, R', 'Hart, E L', 'Hasuko, K', 'Hertzbach, S S', 'Huffer, M E', 'Huynh, X', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Kajikawa, R', 'Kalelkar, M S', 'Kang, H J', 'Kofler, R R', 'Kroeger, R S', 'Langston, M', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'McKemey, A K', 'Messner, R', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Narita, S', 'Nauenberg, U', 'Neal, H', 'Nesom, G', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Ratcliff, B N', 'Reidy, J', 'Reinertsen, P L', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schumm, B A', 'Schwiening, J', 'Serbo, V V', 'Shapiro, G', 'Sinev, N B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Usher, T', 'Vavra, J', 'Verdier, R', 'Wagner, D L', 'Waite, A P', 'Walston, S', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Wright, T R', 'Yamamoto, R K', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H']",['Measurements of Parity-Violation Parameters at SLD'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, beauty', 'quark, charm', 'quark, strangeness', 'coupling, (Z0 quark)', 'violation, CP', 'angular distribution, asymmetry', 'polarization, asymmetry', 'magnetic detector, SLD', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010003'],"['We present direct measurements of the parity-violation parameters $A_b$, $A_c$, and $A_s$ at the $Z^0$ resonance with the SLD detector. The measurements are based on approximately 530k hadronic $Z^0$ events collected in 1993-98. Obtained results are $A_b = 0.914\\pm0.024$ (SLD combined: preliminary), $A_c = 0.635\\pm0.027$ (SLD combined: preliminary), and $A_s = 0.895\\pm0.066(stat.)\\pm 0.062(sys.)$.']",['2000-10-03']
586,['eng'],"['Summers, D J', 'Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Banerjee, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Copty, N K', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Devmal, S C', 'Fernández, A', 'Fox, G F', 'Gagnon, P', 'Göbel, C', 'Gounder, K', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lundberg, B', 'Magnin, J', 'May Tal-Beck, S', 'Meadows, B', 'De Mello-Neto, J R T', 'Neto', 'Mihalcea, D', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'de Oliveira, A', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Dos Reis, A C', 'Rubin, H A', 'Sanders, D A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Slaughter, A J', 'Sokoloff, M D', 'Solano, J M', 'Stanton, N R', 'Stefanski, R J', 'Stenson, K', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yang, S M', 'Yi, D', 'Yoshida, S', 'Zaliznyak, R', 'Zhang, C A']",['Search for Rare and Forbidden Charm Meson Decays at Fermilab E791'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/11', 'hadron nucleus, inclusive reaction', 'charmed meson, hadroproduction', 'charmed meson, rare decay', 'neutral current, flavor changing', 'violation, flavor', 'lepton number, violation', 'D+, semileptonic decay', 'D/s+, semileptonic decay', 'D0, leptonic decay', 'charmed meson, branching ratio', 'upper limit', 'mass spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'charmed meson --> K lepton+ lepton-', 'charmed meson --> pi lepton+ lepton-', 'charmed meson --> meson 2lepton+', 'D0 --> lepton+ lepton-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010002'],"['We report the results of a blind search for flavor-changing neutral current, lepton-flavor violating, and lepton-number violating decays of D+, D(s)+, and D0 mesons (and their antiparticles) into modes containing muons and electrons. Using data from Fermilab charm hadroproduction experiment E791, we examine the pi l l and K l l decay modes of D+ and D(s)+ and the l+ l- decay modes of D0. No evidence for any of these decays is found. Therefore, we present branching-fraction upper limits at 90% confidence level for the 24 decay modes examined. Eight of these modes have no previously reported limits, and fourteen are reported with significant improvements over previously published results.']",['2000-10-03']
587,['eng'],"['Yang, U K', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie']",['Recent structure function results from neutrino scattering at Fermilab'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'iron', 'charged current', 'nucleon, structure function', 'structure function, longitudinal', 'x-dependence', 'momentum transfer, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010001'],"['We report on the extraction of the structure functions F_2 and Delta xF_3 = xF_3(nu)-xF_3(nubar) from CCFR nu_mu-Fe and nubar_mu-Fe different ial cross sections. The extraction is performed in a physics model independent (PMI) way. This first measurement of Delta xF_3, which is useful in testing models of heavy charm production, is higher than current theoretical predictios. The ratio of the F_2 (PMI) values measured in nu_mu and mu scattering is in agreement (within 5%) with the NLO predictions using massive charm production schemes, thus resolving the long-standing discrepancy between the two sets of data. In addition, measurements of F_L (or, equivalently, R) and 2xF_1 are reported in the kinematic region where anomalous nuclear effects in R are observed at HERMES.']",['2000-10-03']
588,['eng'],"['Bodek, Arie']",['Measurement of $d\\sigma/dy$ for high mass Drell-Yan $e^{+}e^{-}$ Pairs at CDF'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electron, pair production', 'Drell-Yan process', 'quantum chromodynamics', 'perturbation theory, higher-order', 'differential cross section, rapidity dependence', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> positron electron anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009067'],['We report on the first measurement of the rapidity distribution dsigma/dy over nearly the entire kinematic region of rapidity for e+e- pairs in the Z-boson region of 66<M_ee<116 GeV/c2 and at higher mass M_ee>116 GeV/c2. The data sample consists of 108 pb-1 of pbar-p collisions at sqrt{s}=1.8 TeV taken by the Collider Detector at Fermilab during 1992--1995. The total cross section in the Z-boson region is measured to be 252 +- 11 pb. The measured total cross section and dsigma/dy are compared with quantum chromodynamics calculations in leading and higher orders.'],['2000-10-02']
589,['eng'],"['Kluth, S']",['Power correction analyses in $e^{+}e^{-}$ annihilation'],['Particle Physics - Experimental Results'],"['talk, Montpellier 2000/07/06', 'electron positron, annihilation', 'hadron, multiple production', 'quantum chromodynamics, correction', 'event shape analysis', 'strong interaction, coupling constant', 'infrared problem', 'renormalon', 'factorization', 'color']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009066'],['The current status of theoretical work and experimental analyses on power corrections in QCD for e+e- annihilation will be reviewed. Measurements of the number of active quark flavours n_f and the QCD colour factors C_A and C_F derived from QCD fits to event shape distributions at lower energies and LEP energies will be presented. The fits are based on O(alpha_s^2)+NLLA QCD predictions with power corrections to model hadronisation.'],['2000-10-02']
590,['eng'],"['Piotrzkowski, K']",['Tagging Two-Photon Production at the LHC'],['Particle Physics - Experimental Results'],"['p p, interaction', 'exchange, two-photon', 'photon photon, luminosity', 'exchange, (2pomeron)', 'transverse momentum, spectra', 'photon photon, interaction', 'Higgs particle, photoproduction', 'quark, truth', 'quark, pair production', 'W, pair production', 'numerical calculations, CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009065'],['Tagging two-photon production offers a significant extension of the LHC physics programme. Effective luminosity of high-energy gamma-gamma collisions reaches 1% of the proton-proton luminosity and the standard detector techniques used for measuring very forward proton scattering should allow for a reliable extraction of interesting two-photon interactions. Particularly exciting is a possibility of detecting two-photon exclusive Higgs boson production at the LHC.'],['2000-10-02']
591,['eng'],"['Abe, T', 'Adam, I', 'Akimoto, H', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Berger, R', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Cassell, R', 'Chou, A', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Crawford, G', 'Damerell, C J S', 'Daoudi, M', 'Dasu, S', 'De Groot, N', 'De Sangro, R', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Erofeeva, I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fernández, J P', 'Flood, K', 'Frey, R', 'Hart, E L', 'Hasuko, K', 'Hertzbach, S S', 'Huffer, M E', 'Huynh, X', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Kajikawa, R', 'Kalelkar, M S', 'Kang, H J', 'Kofler, R R', 'Kroeger, R S', 'Langston, M', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'McKemey, A K', 'Messner, R', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Narita, S', 'Nauenberg, U', 'Neal, H', 'Nesom, G', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Ratcliff, B N', 'Reidy, J', 'Reinertsen, P L', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schumm, B A', 'Schwiening, J', 'Serbo, V V', 'Shapiro, G', 'Sinev, N B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, A', 'Swartz, M', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Usher, T', 'Vavra, J', 'Verdier, R', 'Wagner, D L', 'Waite, A P', 'Walston, S', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Wright, T R', 'Yamamoto, R K', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H']",['Direct measurement of Ab at the Z0 pole using a lepton tag'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'angular distribution, asymmetry', 'quark, semileptonic decay', 'lepton, particle identification', 'polarization, asymmetry', 'coupling, (Z0 beauty)', 'violation, CP', 'differential cross section', 'track data analysis, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009064'],"['We present a direct measurement of the parity violation parameter Ab, derived from the left-right forward-backward asymmetry of b quarks tagged via leptons from semileptonic decays. The lepton identification algorithm combines information from tracking, calorimetry and from the SLD Cherenkov Ring Imaging Detector. The value of Ab is extracted using a maximum likelihood fit to the differential cross section for fermion production. Vertexing information and decay kinematics have been used to discriminate among the different sources of tagged leptons. A new treatment of mixing effects and of background contamination has been introduced and a new vertexing algorithm has been used in the muon analysis. Based on the 1993-1998 SLD sample of 550K hadronic Z0 decays with highly polarized electron beams, we have measured Ab with a ~3% statistical error.']",['2000-10-02']
592,['eng'],"['Collar, J I', 'Giomataris, Yu']",['Low-background applications of MICROMEGAS detector technology'],['Particle Physics - Experimental Results'],"['talk, Lyon 2000/10/15', 'talk, Stockholm 2000/06/28', 'drift chamber, avalanche', 'drift chamber, gas', 'helium, organic compounds', 'electrode, microstrip', 'search for, axion', 'axion, solar', 'astrophysics, missing-mass', 'postulated particle, WIMP', 'neutrino, counters and detectors', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009063'],"['The MICROMEGAS detector concept, generally optimized for use in accelerator experiments, displays a peculiar combination of features that can be advantageous in several astroparticle and neutrino physics applications. Their sub-keV ionization energy threshold, excellent energy and space resolution, and a simplicity of design that allows the use of radioclean materials in their construction are some of these characteristics. We envision tackling experimental challenges such as the measurement of neutral-current neutrino-nucleus coherent scattering or Weakly Interacting Massive Particle (WIMP) detectors with directional sensitivity. The large physics potential of a compact (total volume O(1)m$^{3}$), multi-purpose array of low-background MICROMEGAS is made evident.']",['2000-09-29']
593,['eng'],"['Peters, C', 'Elliott, B', 'Yu, S', 'Eylon, S', 'Henestroza, E']",['Design and Construction of the 3.2 Mev High Voltage Column for Darht II'],['Particle Physics - Experimental Results'],"['talk, Monterey 2000/08/21', 'electron, linear accelerator', 'synchrotron radiation, particle source', 'injection', 'vacuum system', 'electric field, stability', 'Los Alamos Lab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009062'],"['A 3.2 MeV injector has been designed and built for the Darht II Project at Los Alamos Lab. The installation of the complete injector system is nearing completion at this time. The requirements for the injector are to produce a 3.2 MeV, 2000 ampere electron pulse with a flattop width of at least 2-microseconds and emittance of less than 0.15 p cm-rad normalized. A large high voltage column has been built and installed. The column is vertically oriented, is 4.4 meters long, 1.2 meters in diameter, and weights 5700 kilograms. A novel method of construction has been employed which utilizes bonded mycalex insulating rings. This paper will describe the design, construction, and testing completed during construction. Mechanical aspects of the design will be emphasized.']",['2000-09-29']
594,['eng'],"['Bodek, Arie', 'Yang, U K', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Fleming, B T', 'Formaggio, J A', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McFarland, K S']",['New Measurements of Nucleon Structure Functions from CCFR/NuTeV'],['Particle Physics - Experimental Results'],"['talk, Columbus 2000/08/09', 'neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'iron', 'charged current', 'nucleon, structure function', 'x-dependence', 'momentum transfer, dependence', 'differential cross section', 'production, charm', 'scintillation counter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009061'],"['We report on the extraction of the structure functions F_2 and Delta xF_3 = xF_3nu-xF_3nub from CCFR neutrino-Fe and antineutrino-Fe differential cross sections. The extraction is performed in a physics model independent (PMI) way. This first measurement for Delta xF_3, which is useful in testing models of heavy charm production, is higher than current theoretical predictions. Within 5% the F_2 (PMI) values measured in neutrino and muon scattering are in agreement with the predictions of Next-to-Leading-Order PDFs (using massive charm production schemes), thus resolving the long-standing discrepancy between the two measurements.']",['2000-09-29']
595,['eng'],"['Geiser, A']",['Future Atmospheric Neutrino Detectors'],['Particle Physics - Experimental Results'],"['talk, Sudbury 2000/06/16', 'neutrino, oscillation', 'neutrino, mass', 'cosmic radiation', 'showers, air', 'Cherenkov counter, ring imaging', 'Cherenkov counter, water', 'calorimeter, magnetic', 'iron', 'drift chamber, liquid argon', 'drift chamber, time projection', 'deep underground detector, Soudan', 'deep underground detector, Gran Sasso', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009060'],"['Future experiments focusing on atmospheric neutrino detection are reviewed. One of the main goals of these experiments is the detection of an unambiguous oscillation pattern (nu_mu reappearance) to prove the oscillation hypothesis. Further goals include the discrimination of nu_mu - nu_tau and nu_mu - nu_sterile oscillations, and the detection of a potential small nu_mu - nu_e contribution. The search for matter effects in three or more flavour oscillations can be used to constrain hybrid oscillation models and potentially measure the sign of delta m^2. The detectors and measurement techniques proposed to achieve these goals are described, and their physics reach is discussed.']",['2000-09-28']
596,['eng'],"['Breitweg, J']",['A search for resonance decays to antineutrino-jet in $e^{+}p$ scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'narrow resonance, search for', 'jet, electroproduction', 'antineutrino, associated production', 'mass spectrum', 'resonance, scalar', 'resonance, vector', 'squark', 'R parity, violation', 'leptoquark, coupling', 'channel cross section, branching ratio', 'upper limit', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> jet antineutrino anything', 'positron p --> positron anything', 'approx. 300 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009059', 'http://www-zeus.desy.de/~schlenst/conf/osaka_paper.html']","['A study of the antineutrino-jet mass spectrum in e^+p -> antineutrino+X events at center-of-mass energy 300 GeV has been performed with the ZEUS detector at HERA using an integrated luminosity of 47.7 pb^-1. The mass spectrum is in good agreement with that expected from Standard Model processes over the antineutrino -jet mass range studied. No significant excess attributable to the decay of a narrow resonance is observed. By using both e^+p -> e^+ X and e^+p -> antineutrino X data, mass-dependent limits are set on the s-channel production of scalar and vector resonant states. Couplings to first-generation quarks are considered and limits are presented as a function of the e^+q and antineutrino-q branching ratios. These limits are used to constrain the production of leptoquarks and R-parity violating squarks.']",['2000-09-28']
597,['eng'],"['Nelson, H N']",['CLEO Results on Heavy Meson Mixing'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0 anti-B0, interference', 'D0 anti-D0, interference', 'violation, CP', 'anti-B0, semileptonic decay', 'anti-B0, hadronic decay', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> lepton neutrino', 'B0 --> D*(2010) hadron', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K+ pi-', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009057'],"[""We discuss recent CLEO results on D0-D0bar and B0d-B0dbar mixing. The principal results are that for the D0 system, allowing for CP violations, the mixing amplitude x'<2.9% (95% C.L.), and for the B0d system, chi=0.198+-0.013+-0.014. We make projections for future sensistivity to D0-D0bar mixing, and to sin(2*beta+gamma).""]",['2000-09-27']
598,['eng'],"['Bazarko, A']",['MiniBooNE'],['Particle Physics - Experimental Results'],"['talk, Sudbury 2000/06/16', 'neutrino, oscillation', 'neutrino/mu, secondary beam', 'neutrino/e, search for', 'Cherenkov counter', 'organic compounds', 'scintillation counter, hodoscope', 'photoelectron, amplifier', 'electronics, readout', 'beam transport', 'buildings', 'proposed experiment', 'deep underground detector', 'Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009056'],"[""MiniBooNE is preparing to search for nu_mu to nu_e oscillations at Fermilab. The experiment is designed to make a conclusive statement about LSND's neutrino oscillation evidence. We give a status report on the preparation of the experiment and outline the experimental prospects.""]",['2000-09-27']
599,['eng'],"['Adler, Stephen Louis', 'Aoki, M', 'Ardebili, M', 'Atiya, M S', 'Bergbusch, P C', 'Blackmore, E W', 'Bryman, D A', 'Chiang, I H', 'Convery, M R', 'Diwan, M V', 'Frank, J S', 'Haggerty, J S', 'Inagaki, T', 'Ito, M M', 'Kabe, S', 'Kettell, S H', 'Kishi, Y', 'Kitching, P', 'Kobayashi, M', 'Komatsubara, T K', 'Konaka, A', 'Kuno, Y', 'Kuriki, M', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'MacDonald, J A', 'McPherson, R A', 'Meyers, P D', 'Mildenberger, J L', 'Muramatsu, N', 'Nakano, T', 'Ng, C', 'Numao, T', 'Poutissou, J M', 'Poutissou, R', 'Redlinger, G', 'Sato, T', 'Shinkawa, T', 'Shoemaker, F C', 'Soluk, R', 'Stone, J R', 'Strand, R C', 'Sugimoto, S', 'Witzig, C', 'Yoshimura, Y']",['Search for the Decay $K^{+} \\to \\pi^{+} \\pi^{0} \\nu \\overline{\\nu}$'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'K+, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ pi0 neutrino antineutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009055'],"['The first search for the decay K^+ -> pi^+ pi^0 nu nubar has been performed with the E787 detector at BNL. Based on zero events observed in the kinematical search region defined by 90 MeV/c < P_{pi^+} < 188 MeV/c and 135 MeV < E_{pi^0} < 180 MeV, an upper limit B(K^+ -> pi^+ pi^0 nu nubar) < 4.3 x 10^{-5} at 90% confidence level is established.']",['2000-09-27']
600,['eng'],"['Palla, Fabrizio']",['$m_{b}$ from ALEPH and comparison with other LEP experiments'],['Particle Physics - Experimental Results'],"['talk, Montpellier 2000/07/06', 'talk, Villefranche-sur-Mer 2000/01/03', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'quark, beauty', 'quark, pair production', 'mass, beauty', 'quantum chromodynamics, perturbation theory', 'correction, hadronization', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009054'],"['I will review the measurements of the $b$-quark mass performed by ALEPH and DELPHI. A large set of observables has been used together with detailed studies on jet algorithms. Very clear effects due to the $b$-quark mass running are observed. Comparing with the determinations at the $\\Upsilon(4S)$ threshold, the measurements of the running $b$-quark mass at the $Z$ pole are consistent with the predicted evolution from QCD.']",['2000-09-27']
601,['eng'],"['Afanasiev, S V', 'Anticic, T', 'Bächler, J', 'Barna, D', 'Barnby, L S', 'Bartke, J', 'Barton, R A', 'Betev, L', 'Bialkowska, H', 'Billmeier, A', 'Blume, C', 'Blyth, C O', 'Boimska, B', 'Botje, M', 'Bracinik, J', 'Brady, F P', 'Bramm, R', 'Brun, R', 'Buncic, P', 'Carr, L', 'Cebra, D', 'Cooper, G E', 'Cramer, J G', 'Csató, P', 'Eckardt, V', 'Eckhardt, F', 'Ferenc, D', 'Filip, P', 'Fischer, H G', 'Fodor, Zoltán', 'Foka, P Y', 'Freund, P', 'Friese, V', 'Ftácnik, J', 'Gál, J', 'Gazdzicki, M', 'Georgopoulos, G', 'Gladysz-Dziadus, E', 'Harris, J W', 'Hegyi, S', 'Hlinka, V', 'Höhne, C', 'Igo, G', 'Ivanov, M', 'Jacobs, P', 'Janik, R', 'Jones, P G', 'Kadija, K', 'Kolesnikov, V I', 'Kollegger, T', 'Kowalski, M', 'Lasiuk, B', 'Van Leeuwen, M', 'Lévai, P', 'Malakhov, A I', 'Margetis, S', 'Markert, C', 'Mayes, B', 'Melkumov, G L', 'Mischke, A', 'Molnár, J', 'Nelson, J M', 'Odyniec, G J', 'Pálla, G', 'Panagiotou, A D', 'Petridis, A', 'Pikna, M', 'Pinsky, L', 'Poskanzer, A M', 'Prindle, D J', 'Pühlhofer, F', 'Reid, J G', 'Renfordt, R E', 'Retyk, W', 'Ritter, H G', 'Röhrich, D', 'Roland, C', 'Roland, G', 'Rybicki, A', 'Sammer, T', 'Sandoval, A', 'Sann, H', 'Schäfer, E', 'Schmitz, N', 'Seyboth, P', 'Sikler, F', 'Sitar, B', 'Skrzypczak, E', 'Snellings, R', 'Squier, G T A', 'Stock, Reinhard', 'Strmen, P', 'Ströbele, H', 'Susa, T', 'Szarka, I', 'Szentpétery, I', 'Sziklai, J', 'Toy, M', 'Trainor, T A', 'Trentalange, S', 'Ullrich, T S', 'Varga, D', 'Vassiliou, M', 'Veres, G I', 'Vesztergombi, György', 'Voloshin, S A', 'Vranic, D', 'Wang, F', 'Weerasundara, D D', 'Wenig, S', 'Wetzler, A', 'Whitten, C', 'Xu, N', 'Yates, T A', 'Yoo, I K', 'Zimányi, J']",['Event-by-event fluctuations of the kaon to pion ratio in central Pb+Pb collisions at 158 GeV per Nucleon'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'lead', 'central region', 'charged particle, multiple production', 'yield, (K pi)', 'fluctuation, upper limit', 'magnetic spectrometer, experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009053'],"['We present the first measurement of fluctuations from event to event in the production of strange particles in collisions of heavy nuclei. The ratio of charged kaons to charged pions is determined for individual central Pb+Pb collisions. After accounting for the fluctuations due to detector resolution and finite number statistics we derive an upper limit on genuine non-statistical fluctuations, perhaps related to a first or second order QCD phase transition. Such fluctuations are shown to be very small.']",['2000-09-26']
602,['eng'],"['Martínez-Vidal, F']",['Measurement of B0 and B+ lifetimes and B0-antiB0 mixing with fully reconstructed B decays in BaBar'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B0, semileptonic decay', 'B+, lifetime', 'B0, lifetime', 'B0 anti-B0, interference', 'time dependence', 'B0, mass difference', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009051'],"['Time-dependent B0-antiB0 flavor oscillations and B0 and B+ lifetimes are studied in a sample of fully reconstructed B mesons collected with the BaBar detector, running at the PEP-II asymmetric e+e- B Factory with center-of-mass energies near the Upsilon(4S) resonance. This is the first time that time-dependent mixing and lifetime measurements have been performed at Upsilon(4S) energies.']",['2000-09-26']
603,['eng'],"['Pagliarone, C']",['Beyond the Standard Model at Tevatron'],['Particle Physics - Experimental Results'],"['talk, Yalta 2000/05/27', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electroweak interaction, validity test', 'new particle, search for', 'squark, truth', 'gluino', 'final state, (beauty lepton missing-energy)', 'final state, ((n)lepton)', 'R parity, violation', 'leptoquark', 'particle, technicolor', 'final state, (jet missing-energy)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011005'],"['This article presents recent results of searches for physics beyond the Standard Model using the CDF and the D$\\not$O detector at the Fermilab Tevatron Collider. All results shown correspond to analysis performed using the past 1992-1996 Fermilab Tevatron run I data (roughly $100$ $pb^{-1}$ per each experiment). In particular we describe recent Tevatron searches for scalar top in the $b+\\ell+$missing-$E_{T}$ channel, for squark and gluinos using like-sign dileptons (LS), for large extra space-time dimensions and the search for leptoquarks and technicolor in the missing-$E_{T}$+heavy flavour jet events. Tight limits on the existence of such models have been set.']",['2000-11-02']
604,['eng'],"['Iori, M']",['Recent results from SELEX'],['Particle Physics - Experimental Results'],"['talk, Valencia 2000/06/27', 'hadron nucleus, inclusive reaction', 'Sigma-', 'pi-', 'p', 'carbon', 'copper', 'charmed particle, hadroproduction', 'charmed particle, hadronic decay', 'Lambda/c+, lifetime', 'D0, lifetime', 'D/s, lifetime', 'yield, x-dependence', 'asymmetry', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'hadron nucleus --> charmed particle anything', 'Lambda/c+ --> p K- pi+', 'D0 --> K- (n)pi', 'D/s --> K*(892) K', 'D/s --> Phi(1020) pi', '600 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009049'],"['Preliminary results on asymmetry for Lc produced by Sigma-,pi- and p beams at xf>0.2 and precise measurements of the Lc,D0 and Ds lifetimes are presented.']",['2000-09-25']
605,['eng'],"['Achasov, M N', 'Baru, S E', 'Beloborodov, K I', 'Berdyugin, A V', 'Bogdanchikov, A G', 'Bozhenok, A V', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Kukartsev, G A', 'Pakhtusova, E V', 'Polunin, A A', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Shary, V V', 'Shatunov, Yu M', 'Vasilev, A V']",['Search for direct production of a2(1320) and f2(1270) mesons in $e^{+}e^{-}$ annihilation'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tensor meson, electroproduction', 'a2(1320), width', 'f2(1270), width', 'upper limit', 'channel cross section, energy dependence', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> f2(1270)', 'electron positron --> a2(1320)', 'f2(1270) --> 2pi0', 'a2(1320) --> eta pi0', '1.0-1.4 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009048'],"['A search for direct production of C-even resonances a2(1320) and f2(1270) in e+e- annihilation was performed with SND detector at VEPP-2M e+e- collider. The upper limits of electronic widths of these mesons were obtained at 90% confidence level: Gamma(a2(1320) \\to e+e-) < 0.56 eV, Gamma(f2(1270) \\to e+e-) < 0.11 eV.']",['2000-09-25']
606,['eng'],"['Komatsubara, T K']",['Recent Results from the BNL E787 Experiment'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'K+, rare decay', 'K+, radiative decay', 'K+, semileptonic decay', 'neutral current, flavor changing', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino', 'K+ --> muon+ neutrino photon', 'K+ --> pi+ pi0 photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009047'],"['Recent results from a rare kaon decay experiment E787 at the BNL-AGS on K^+ \\to \\pi^+ \\nu \\bar\\nu, K^+ \\to \\mu^+ \\nu \\gamma, and K^+ \\to \\pi^+ \\pi^0 \\gamma decays are reported.']",['2000-09-22']
607,['eng'],"['Milstene, C', 'Frank, J', 'Kettell, S H', 'Strand, R C', 'Bellantoni, L', 'Coleman, R', 'Cooper, P S', 'Crisler, M', 'Nguyen, H', 'Ramberg, E', 'Tschirhart, R S', 'Britvich, G V', 'Kubarovskii, V P', 'Molchanov, L', 'Landsberg, V', 'Obraztsov, V F', 'Petrenko, S V', 'Polyakov, V', 'Vavilov, D V', 'Yushchenko, O P', 'Engelfried, J', 'Morelos, A', 'Campbell, M', 'Lang, K', 'Dukes, C', 'Nelson, K']",['Charged Kaons at the Main Injector (CKM)'],['Particle Physics - Experimental Results'],"['talk, Valencia 2000/06/27', 'K+, semileptonic decay', 'K+, branching ratio', 'background', 'K+, secondary beam', 'Cherenkov counter, ring imaging', 'magnetic spectrometer', 'proposed experiment, Fermilab', 'K+ --> pi+ neutrino antineutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009046'],"['The CKM collaboration is proposing to measure the branching ratio of the rare K decay (K+ --> pi+ nu nubar) at the Main Injector at Fermilab. Our goal is to be able to observe about 100 events, for a Standard Model branching ratio of about 1.0E-10. This implies that we must be able to reduce the background to a few events.']",['2000-09-22']
608,['eng'],"['Cinabro, D']",['New Results from CLEO'],['Particle Physics - Experimental Results'],"['review, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, rare decay', 'B, hadronic decay', 'B, semileptonic decay', 'B, leptonic decay', 'B, branching ratio', 'final state, (0charm)', 'charm, production', 'Kobayashi-Maskawa angle', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009045'],['The latest results from the CLEO collaboration are summarized. An update on the status of the upgraded CLEO III detector is also included.'],['2000-09-21']
609,['eng'],"['Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Savinov, V', 'Coan, T E', 'Fadeev, V', 'Gao, Y S', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Kostin, M A', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Xu, Z', 'Godang, R', 'Bonvicini, G', 'Cinabro, D', 'Dubrovin, M', 'McGee, S', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Gritsan, A', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Drell, P S', 'Duboscq, J E', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Hsu, L', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Palmer, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Romano, A', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Viehhauser, G', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Stöck, H', 'Yelton, J', 'Brandenburg, G', 'Ershov, A', 'Kim, D Y J', 'Wilson, R', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A']",['Study of $\\chi_{c1}$ and $\\chi_{c2}$ Meson Production in B Meson Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'quarkonium, production', 'quarkonium, radiative decay', 'chi/c1(3510)', 'chi/c2(3555)', 'psi(3685)', 'strangeness, production', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> chi mesons anything', 'B --> chi mesons strangeness anything', 'psi(3685) --> chi mesons photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009044'],"['Using a sample of 9.7 million B meson pairs collected with the CLEO detector, we study B decays to the chi_c1 and chi_c2 charmonia states, which are reconstructed via their radiative decays to J/psi. We first measure the branching fraction for inclusive chi_c1 production in B decays to be Br(B->chi_c1 X)=(4.14+-0.31+-0.40)*10^-3, where the first uncertainty is statistical and the second one is systematic. We derive the branching fractions for direct chi_c1 and chi_c2 production in B decays by subtracting the known contribution of the decay chain B->psi(2S)X with psi(2S)->chi_c1,2 gamma. We obtain Br[B->chi_c1(direct) X]=(3.83+-0.31+-0.40)*10^-3. No statistically significant signal for chi_c2 production is observed in either case. Using the Feldman-Cousins approach, we determine the 95% confidence intervals to be [0.2, 2.0]*10^-3 for Br(B->chi_c2 X), [0.0,1.7]*10^-3 for Br[B->chi_c2(direct) X], and [0.00,0.44] for the ratio Br[B->chi_c2(direct) X]/Br[B->chi_c1(direct) X]. We also measure the branching ratio Br[B->chi_c2(direct) X_s]/Br[B->chi_c1(dir ect) X_s] for different X_s configurations by reconstructing B decays into exclusive final states with J/psi, a photon, a kaon, and up to four pions. For all the X_s configurations we observe a strong chi_c1 signal yet no statistically significant chi_c2 signal. We discuss how our results compare with theoretical predictions in different models of charmonium production.']",['2000-09-21']
610,['eng'],"['Frlez, E', 'Pocanic, D', 'Ritt, S']",['ADC common noise correction and zero suppression in the PIBETA detector'],['Particle Physics - Experimental Results'],"['calorimeter, electromagnetic', 'scintillation counter, crystal', 'cesium, iodine', 'scintillation counter, plastics', 'scintillation counter, hodoscope', 'plastics, target', 'proportional chamber, wire', 'electronics, background', 'analog-to-digital converter', 'PSI Cycl']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009042'],"[""We describe a simple procedure for reducing ADC common noise in modular detectors that does not require additional hardware. A method using detector noise groups should work well for modular particle detectors such as segmented electromagnetic calorimeters, plastic scintillator hodoscopes, cathode strip wire chambers, segmented active targets, and the like. We demonstrate a ``second pedestal noise correction'' method by comparing representative ADC pedestal spectra for various elements of the PIBETA detector before and after the applied correction.""]",['2000-09-20']
611,['eng'],"['Yang, U K', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Fleming, B T', 'Formaggio, J A', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McFarland, K S', 'McNulty, C', 'Mishra, S R', 'Naples, D', 'Suwonjandee, N', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Sciulli, F J', 'Seligman, W G', 'Shaevitz, M H', 'Smith, W H', 'Spentzouris, P', 'Stern, E G', 'Vaitaitis, A G', 'Vakili, M', 'Yu, J', 'Zeller, G P', 'Zimmerman, E D']",['Measurements of $F_{2}$ and $xF_{3}^{\\nu}-xF_{3}^{\\overline{\\nu}}$ from CCFR $\\nu_{\\mu}-Fe$ and $\\overline{\\nu}_{\\mu}$-Fe data in a physics model independent way'],['Particle Physics - Experimental Results'],"['neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'neutrino/mu', 'iron', 'nucleon, structure function', 'charm, production', 'differential cross section', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009041'],"['We report on the extraction of the structure functions F_2 and Delta xF_3 = xF_3(nu)-xF_3(nubar) from CCFR nu_mu-Fe and nubar_mu-Fe differential cross sections. The extraction is performed in a physics model independent (PMI) way. This first measurement of Delta xF_3, which is useful in testingmodels of heavy charm production, is higher than current theoretical predictions. The ratio of the F_2(PMI) values measured in nu_mu and nubar_mu scattering is in agreement (within 5%) with the predictions of NLO PDFS using massive charm production schemes, thus resolvin long-standing discrepancy between the two sets of data.']",['2000-09-19']
612,['eng'],"['Warburton, A']","['First Observation of the $\\Sigma_{c}^{*+}$ Charmed Baryon, and New Measurements of the $\\Sigma_{c}^{0}$, $\\Sigma_{c}^{+}$, $\\Sigma_{c}^{++}$, and $\\Omega_{c}^{0}$ Charmed Baryons']",['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, electroproduction', 'charmed baryon, mass', 'charmed baryon, width', 'Sigma/c+', 'Sigma/c++', 'Sigma/c0', 'Omega/c0, hadronic decay', 'postulated particle, Sigma/c*', 'Sigma/c, hadronic decay', 'final state, (Lambda/c+ pi)', 'mass spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009040'],"[""Using ~13.7 fb^{-1} of e^+e^- collision data recorded at near the Upsilon(4S) resonance by the CLEO II and CLEO II.V detector configurations on the Cornell Electron Storage Ring, we present the world's most precise measurements of the Sigma_c^0, Sigma_c^+, and Sigma_c^{++} charmed-baryon masses as well as the first measurements of the intrinsic widths of the Sigma_c^0 and Sigma_c^{++} baryons. We also report on the first observation and mass measurement of the Sigma_c^{*+} charmed baryon, M(Sigma_c^{*+}) - M(Lambda_c^+) = (231.0 +- 1.1[stat] +- 2.0[syst]) MeV/c^2, and the first CLEO observation of the Omega_c^0 baryon, for which we measure a mass M(Omega_c^0) = (2694.6 +- 2.6[stat] +- 2.4[syst]) MeV/c^2 from a sample of (40.4 +- 9.0[stat]) candidate events. All new results are preliminary.""]",['2000-09-18']
613,['eng'],"['Valassi, A']",['Bose-Einstein Correlations in W-pair events at LEP'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'correlation, two-pion', 'boson, statistics', 'charge, two-pion', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', 'W --> quark antiquark', 'W --> lepton neutrino', '172-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009039'],"[""An overview of measurements of Bose-Einstein correlations in W-pair events at LEP is given. The results presented are based on data collected at centre-of-mass energies between 172 and 202GeV. The review concentrates on the search for Bose-Einstein correlations between pions from different W's in e+e- -> W+W- -> qqbarqqbar events. No agreement is reached in the results of the four experiments.""]",['2000-09-18']
614,['eng'],"['Landsberg, G L']",['Mini-Review on Extra Dimensions'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'dimension, >4', 'search for', 'graviton, emission', 'graviton, exchange', 'interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009038'],"['One of the most stimulating recent ideas in particle physics involves a possibility that our universe has additional compactified spatial dimensions, perhaps as large as 1 mm. In this mini-review, we discuss the results of recent experimental searches for such large extra dimensions.']",['2000-09-18']
615,['eng'],"['Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, H N', 'Nelson, T K', 'Roberts, D', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Boisvert, V', 'Cassel, David G', 'Crowcroft, D S', 'Dickson, M', 'Von Dombrowski, S', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Ogg, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Soffer, A', 'Valant-Spaight, B L', 'Warburton, A', 'Ward, C', 'Athanas, M', 'Avery, P', 'Jones, C D', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Briere, R A', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Selen, M', 'Thaler, J J', 'Edwards, K W', 'Bellerive, A', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Coppage, D', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhou, L', 'Anderson, S', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Alam, M S', 'Athar, S B', 'Ling, Z', 'Mahmood, A H', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lee, J', 'Lorenc, J', 'Schwarthoff, H', 'Wolf, A', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Glenn, S', 'Kwon, Y', 'Lyon, A L', 'Roberts, S', 'Thorndike, E H', 'Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Dambasuren, E', 'Kopp, S E', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Csorna, S E', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chan, S', 'Eigen, G', 'Lipeles, E', 'Miller, J S', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F']",['Search for Direct CP Violation in $\\Xi$ Hyperon Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, pair production', 'quark, strangeness', 'Xi-, hadronic decay', 'Antixi-, hadronic decay', 'decay, asymmetry', 'mass spectrum', 'angular distribution', 'CP, invariance', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Xi- --> Lambda pi-', 'Antixi- --> Antilambda pi+', 'Lambda --> p pi-', 'Antilambda --> anti-p pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009037'],"['Using data collected with the CLEO II detector we have performed a search for direct CP violation in the $\\Xi$ hyperon system. CP violation gives rise to an asymmetry, A, between the parity-violating angular distributions of the decay chains $\\Xi^- \\To \\Lambda pi^-$, $\\Lambda \\To p \\pi^-$ and $\\bar{\\Xi}^+ \\To \\bar{\\Lambda} \\pi^+$, $\\bar{\\Lambda} \\To \\bar{p} \\pi^+$. In the Standard Model, A is expected to be in the range $10^{-4}$ to $10^{-5}$. If CP violation were found at a higher level it could indicate the presence of new physics. We find no evidence for CP violation: A = -0.057 +- 0.064 +- 0.039. We also obtain $A_{\\Xi} = -0.070 +- 0.064 +- 0.045$ and $\\alpha_{\\bar{\\Xi}}= 0.49^{+0.06}_{-0.05} +- 0.10$.']",['2000-09-17']
616,['eng'],"['Achasov, M N', 'Beloborodov, K I', 'Berdyugin, A V', 'Bogdanchikov, A G', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Pakhtusova, E V', 'Polunin, A A', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V', 'Vasilev, A V', 'Velikzhanin, Yu S']","['Processes $e^+e^- \\to K^+K^-$, $K_SK_L$ and $\\pi^+\\pi^-\\pi^0$ at the $\\phi(1020)$ resonance energy region']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), mass', 'Phi(1020), width', 'Phi(1020), hadronic decay', 'K, pair production', 'pi, multiple production', 'channel cross section, branching ratio', 'amplitude analysis', 'vector dominance', 'energy dependence', 'magnetic detector, SND', 'experimental results', 'Novosibirsk Stor2', 'tables', 'electron positron --> K+ K-', 'electron positron --> K0(L) K0(S)', 'electron positron --> pi+ pi- pi0', 'approx. 1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009036'],"['The cross sections of the processes $e^+e^- \\to K^+K^-$, $e^+e^- \\to K_SK_L$ and $e^+e^- \\to \\pi^+\\pi^-\\pi^0$ were measured in the SND experiment at the VEPP-2M collider in the energy region near the $\\phi(1020)$ meson. The measured cross sections had been analyzed in the framework of the vector meson dominance model and the main parameters of the $\\phi$-resonance were obtained, such as its mass, width, the production cross section and branching ratios of the main decay modes. The measured value of the $\\phi$ meson total width $\\Gamma_{\\phi} = 4.21 \\pm 0.04$ is lower then the present world average $4.43 \\pm 0.05$ MeV. Additional contribution, besides the conventional vector meson dominance model, was found in the $e^+e^- \\to \\pi^+\\pi^-\\pi^0$ reaction cross section.']",['2000-09-17']
617,['eng'],"['Abe, K']",['Measurement of $A_c$ with Charmed Mesons at SLD'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, charm', 'quark, pair production', 'particle identification, charm', 'D*(2010), hadronic decay', 'D, hadronic decay', 'D0, semileptonic decay', 'coupling, (Z0 charm)', 'parity, violation', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009035'],"['We present a direct measurement of the parity-violation parameter $A_c$ in the coupling of the $Z^0$ to $c$-quarks with the SLD detector. The measurement is based on a sample of 530k hadronic $Z^0$ decays, produced with a mean electron-beam polarization of $|P_e| = 73 %$. The tagging of $c$-quark events is performed using two methods: the exclusive reconstruction of $D^{\\ast+}$, $D^+$, and $D^0$ mesons, and the soft-pions ($\\pi_s$) produced in the decay of $D^{\\ast+}\\to D^0 \\pi_s^+$. The large background from $D$ mesons produced in $B$ hadron decays is separated efficiently from the signal using precision vertex information. The combination of these two methods yields $A_c = 0.688 \\pm 0.041.$']",['2000-09-17']
618,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grudberg, P M', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Scully, J R', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Measurement of the Angular Distribution of Electrons from $W \\to e\\nu$ Decays Observed in $p\\overline{p}$ Collisions at $\\sqrt{s}$=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'electron, angular distribution', 'parametrization', 'W, transverse momentum', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009034'],"['We present the first measurement of the electron angular distribution parameter alpha_2 in W to e nu events produced in proton-antiproton collisions as a function of the W boson transverse momentum. Our analysis is based on data collected using the D0 detector during the 1994--1995 Fermilab Tevatron run. We compare our results with next-to-leading order perturbative QCD, which predicts an angular distribution of (1 +/- alpha_1 cos theta* + alpha_2 cos^2 theta*), where theta* is the polar angle of the electron in the Collins-Soper frame. In the presence of QCD corrections, the parameters alpha_1 and alpha_2 become functions of p_T^W, the W boson transverse momentum. This measurement provides a test of next-to-leading order QCD corrections which are a non-negligible contribution to the W boson mass measurement.']",['2000-09-17']
619,['eng'],"['Dainton, J B']",['Photon Structure and Quantum Fluctuation'],['Particle Physics - Experimental Results'],"['review, London 2000/05/24', 'electron positron, colliding beams', 'photon electron, interaction', 'photon photon, interaction', 'positron p, colliding beams', 'photon p, interaction', 'jet, photoproduction', 'final state, (2jet)', 'hadron, multiple production', 'photon, structure function', 'photon, resolved', 'quantum electrodynamics', 'quantum chromodynamics', 'momentum transfer, dependence', 'differential cross section, transverse energy', 'factorization', 'rapidity dependence', 'transverse momentum, dependence', 'experimental results', 'bibliography', 'photon electron --> muon+ muon- electron', 'electron positron --> positron electron anything', 'positron p --> jet positron anything']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009033'],"['Photon structure derives from quantum fluctuation in quantum field theory to fermion and anti-fermion, and has been an experimentally established feature of electrodynamics since the discovery of the positron. In hadronic physics, the observation of factorisable photon structure is similarly a fundamental test of the quantum field theory Quantum Chromodynamics (QCD). An overview of measurements of hadronic photon structure in e+e- and ep interactions is presented, and comparison made with theoretical expectation, drawing on the essential features of photon fluctuation into quark and anti-quark in QCD.']",['2000-09-14']
620,['eng'],"['Bergman, D R']",['A New Measurement of the Radiative Ke3 Branching Ratio and Photon Spectrum'],['Particle Physics - Experimental Results'],"['talk, Cracow 2000/05/19', 'K0(L), secondary beam', 'K0(L), radiative decay', 'K0(L), branching ratio', 'photon, energy spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi+ electron neutrino/e photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009032'],"['We present a preliminary report on a new measurement of the radiative neutral Ke3 branching ratio and the first study of the photon spectrum in this decay. We find BR(Ke3g, E*_g>30 GeV, Th*_eg>20 deg)/BR(Ke3) = 0.911+-0.009(stat)+0.021-0.010(syst)%. Our measurement of the spectrum is consistent with inner bremsstrahlung only as the source of photons at the 2 sigma level.']",['2000-09-14']
621,['eng'],"['Besuglov, M P', 'Bobchenko, B M', 'Byistritskaya, E V', 'Vasenko, A A', 'Vishnevsky, M E', 'Galanina, N D', 'Gusev, K E', 'Demidov, V S', 'Demidova, E V', 'Zchurkin, V V', 'Kirpichnikov, I V', 'Kuznetsov, V A', 'Markizov, V N', 'Martemyanov, A N', 'Nedosekin, A A', 'Pavlov, B N', 'Sadyukov, V A', 'Sokolov, A Y', 'Starostin, A S', 'Khaldeeva, N A']",['Quasi-coherent interaction of protons with $^{28}Si$ at $T_{p}=1GeV$'],['Particle Physics - Experimental Results'],"['p nucleus, coherent interaction', 'silicon', 'excited nucleus, transition', 'photon, energy spectrum', 'momentum transfer, spectra', 'angular distribution', 'pi, hadroproduction', 'pi, pair production', 'intranuclear cascade', 'cross section', 'Delta(1232)', 'magnetic spectrometer, experimental results', 'Serpukhov PS', '1 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009031'],"['The total, elastic and inelastic cross-sections for quasi-coherent interactions of protons with Si28 have been measured using hadron-gamma coincidence method at the energy 1 GeV. The limits for the existence of long-lived excited states of the Si28 nucleus have been obtained in the range of energies from 0 to 0.8 GeV.']",['2000-09-13']
622,['eng'],"['Alavi-Harati, A', 'Albuquerque, I F M', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barker, A R', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Fordyce, P M', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hanagaki, K', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jennings, J', 'Jensen, D A', 'Kessler, R S', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'McManus, A P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian R"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Qiao, C', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S R', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Suzuki, I', 'Swallow, E C', 'Swanson, R A', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['Search for the Decay $K_{L} \\to \\pi^{0}e^{+}e^{-}$'],['Particle Physics - Experimental Results'],"['K0(L), semileptonic decay', 'violation, CP', 'Kobayashi-Maskawa angle', 'mass spectrum, (positron electron 2photon)', 'K0(L), branching ratio', 'upper limit', 'calorimeter, electromagnetic', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi0 positron electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009030'],"['We report on a search for the decay Kl -> pi0 e+ e- carried out by the KTeV/E799 experiment at Fermilab. This decay is expected to have a significant CP violating contribution and the measurement of its branching ratio could support the CKM mechanism for CP violation or could point to new physics. Two events were observed in the 1997 data with an expected background of 1.06 +-0.41 events, and we set an upper limit Br(Kl -> pi0 e+ e-) < 5.1 x 10^-10 at the 90% confidence level.']",['2000-09-13']
623,['eng'],"['Brown, H N', 'Bunce, G M', 'Carey, R M', 'Cushman, P B', 'Danby, G T', 'Debevec, P T', 'Deng, H', 'Deninger, W J', 'Dhawan, S K', 'Druzhinin, V P', 'Duong, L', 'Earle, W', 'Efstathiadis, E F', 'Fedotovich, G V', 'Farley, Francis J M', 'Giron, S', 'Gray, F', 'Grosse-Perdekamp, M', 'Grossmann, A', 'Haeberlen, U', 'Hare, M F', 'Hazen, E S', 'Hertzog, D W', 'Hughes, V W', 'Iwasaki, M', 'Jungmann, K', 'Kawall, D', 'Kawamura, M', 'Khazin, B I', 'Kindem, J', 'Krienen, F', 'Kronkvist, I J', 'Larsen, R', 'Lee, Y Y', 'Logashenko, I B', 'McNabb, R', 'Meng, W', 'Mi, J', 'Miller, J P', 'Morse, W M', 'Onderwater, C J G', 'Orlov, Y', 'Ozben, C', 'Polly, C', 'Pai, C', 'Paley, J M', 'Pretz, J', 'Prigl, R', 'zu Putlitz, G', 'Redin, S I', 'Rind, O', 'Roberts, B L', 'Ryskulov, N', 'Sedykh, S N', 'Semertzidis, Y K', 'Shatunov, Yu M', 'Solodov, E P', 'Sossong, M', 'Steinmetz, A', 'Sulak, Lawrence R', 'Timmermans, C', 'Trofimov, A V', 'Urner, D', 'Von Walter, P', 'Warburton, D', 'Winn, D', 'Yamamoto, A', 'Zimmerman, D']",['Improved Measurement of the Positive Muon Anomalous Magnetic Moment'],['Particle Physics - Experimental Results'],"['muon, storage ring', 'muon+, magnetic moment', 'muon, polarized beam', 'injection', 'magnetic field', 'resonance, magnetic', 'experimental results', 'Brookhaven PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009029'],"[""A new measurement of the positive muon's anomalous magnetic moment has been made at the Brookhaven Alternating Gradient Synchrotron using the direct injection of polarized muons into the superferric storage ring. The angular frequency difference omega_{a} between the angular spin precession frequency omega_{s} and the angular orbital frequency omega_{c} is measured as well as the free proton NMR frequency omega_{p}. These determine R = omega_{a} / omega_{p} = 3.707~201(19) times 10^{-3}. With mu_{mu} / mu_{p} = 3.183~345~39(10) this gives a_{mu^+} = 11~659~191(59) times 10^{-10} (pm 5 ppm), in good agreement with the previous CERN and BNL measurements for mu^+ and mu^-, and with the standard model prediction.""]",['2000-09-13']
624,['eng'],"['Sanders, D A']",['Review of Recent Searches for Rare and Forbidden Dilepton Decays of Charmed Mesons'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'charmed meson, hadroproduction', 'charmed meson, semileptonic decay', 'charmed meson, leptonic decay', 'charmed meson, rare decay', 'final state, dilepton', 'D+', 'D/s+', 'D0', 'neutral current, flavor changing', 'flavor, violation', 'charmed meson, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009027'],"['I briefly review the results of recent searches for flavor-changing neutral current and lepton-flavor and lepton-number violating decays of D+, Ds, and D0 mesons (and their antiparticles) into modes containing muons and electrons. The primary focus is the results from Fermilab charm hadroproduction experiment E791. E791 examined 24 pi,l,l and K,l,l decay modes of D+ and Ds and l+l- decay modes of D0. Limits presented by E791 for 22 rare and forbidden dilepton decays of D mesons were more stringent than those obtained from previous searches, or else were the first reported.']",['2000-09-11']
625,['eng'],"['Battaglia, M']",['Experimental Status of Semileptonic B Decays'],['Particle Physics - Experimental Results'],"['talk, Montpellier 2000/07/06', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'quark, branching ratio', 'Kobayashi-Maskawa angle', 'charm, production', 'final state, (0charm)', 'B, semileptonic decay', 'charmed meson, excited state', 'experimental results', 'CERN LEP Stor', 'Cornell CESR Stor', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009026'],"['Recent analyses of the LEP and Y(4S) data have better outlined the picture of semileptonic B decays. Results on inclusive and exclusive decay branching fractions and on the extraction of the Vub and Vcb elements of the CKM mixing matrix are discussed, together with some of the still open questions and the sources of model systematics.']",['2000-09-11']
626,['eng'],"['Söldner-Rembold, S']",['Photon Structure'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'electron p, colliding beams', 'photon p, interaction', 'hadron, multiple production', 'vector dominance', 'photon, structure function', 'x-dependence', 'differential cross section, transverse momentum', 'charm, production', 'model, quark parton', 'gluon, exchange', 'Lipatov equation', 'experimental results', 'CERN LEP Stor', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009025'],['The structure of the photon is probed in photon-photon interactions at LEP and in photon-proton interactions at HERA.'],['2000-09-11']
627,['eng'],"['Barker, A R', 'Kettell, S H']",['Developments in Rare Kaon Decay Physics'],['Particle Physics - Experimental Results'],"['review, experimental results', 'K, rare decay', 'K, branching ratio', 'upper limit', 'K0(L), leptonic decay', 'K, semileptonic decay', 'K, radiative decay', 'decay, form factor', 'violation, CP', 'Kobayashi-Maskawa angle', 'flavor, violation', 'Brookhaven PS', 'Fermilab', 'CERN SPS', 'Frascati Stor', 'Serpukhov PS', 'KEK PS', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009024'],"['We review the current status of the field of rare kaon decays. The study of rare kaon decays has played a key role in the development of the standard model, and the field continues to have significant impact. The two areas of greatest import are the search for physics beyond the standard model and the determination of fundamental standard-model parameters. Due to the exquisite sensitivity of rare kaon decay experiments, searches for new physics can probe very high mass scales. Studies of the k->pnn modes in particular, where the first event has recently been seen, will permit tests of the standard-model picture of quark mixing and CP violation.']",['2000-09-11']
628,['eng'],"['Chiodini, G', 'Appel, J A', 'Artuso, M', 'Butler, J N', 'Cardoso, G', 'Cheung, H', 'Christian, D C', 'Colautti, A', 'Coluccia, R', 'Corato, M D', 'Gottschalk, E E', 'Hall, B K', 'Hoff, J R', 'Kasper, P A', 'Kutschke, R', 'Kwan, S W', 'Mekkaoui, A', 'Menasce, D', 'Newsom, C R', 'Sala, S', 'Yarema, R J', 'Wang, J C', 'Zimmermann, S']",['Beam Test Results of the BTeV Silicon Pixel Detector'],['Particle Physics - Experimental Results'],"['talk, Genova 2000/06/05', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'spatial resolution', 'electronics, readout', 'integrated circuit', 'magnetic spectrometer, BTeV', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009023'],"['The results of the BTeV silicon pixel detector beam test carried out at Fermilab in 1999-2000 are reported. The pixel detector spatial resolution has been studied as a function of track inclination, sensor bias, and readout threshold.']",['2000-09-08']
629,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of triple gauge boson couplings from $W^{+}W^{-}$ production at LEP energies up to 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'coupling, (3gauge boson)', 'W, hadronic decay', 'W, leptonic decay', 'event shape analysis', 'angular distribution', 'electroweak interaction, validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', '189 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009022', 'http://alephwww.cern.ch/ALPUB/oldconf/osaka00/abs_324/abs_324.ps']","['A measurement of triple gauge boson couplings is presented, based on W-pair data recorded by the OPAL detector at LEP during 1998 at a centre-of-mass energy of 189 GeV with an integrated luminosity of 183 pb^-1. After combining with our previous measurements at centre-of-mass energies of 161-183 GeV we obtain k_g=0.97 +0.20 -0.16, g_1^z=0.991 +0.060 -0.057 and lambda_g=-0.110 +0.058 -0.055, where the errors include both statistical and systematic uncertainties and each coupling is determined by setting the other two couplings to their SM values. These results are consistent with the Standard Model expectations.']",['2000-09-08']
630,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A Measurement of the Rate of Charm Production in W Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'production, charm', 'W, branching ratio', 'coupling, (W charm)', 'Kobayashi-Maskawa angle', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W- anything', 'W --> charm anything', 'W --> (n)hadron', '183-189 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009020'],"['Using data recorded at centre-of-mass energies around 183 GeV and 189 GeV with the OPAL detector at LEP, the fundamental coupling of the charm quark to the W boson has been studied. The ratio Rc^W = Gamma(W -> cX)/Gamma(W -> hadrons) has been measured from jet properties, lifetime information, and leptons produced in charm decays. A value compatible with the Standard Model expectation of 0.5 is obtained: Rc^W = 0.481 +- 0.042(stat.) +- 0.032(syst.). By combining this result with measurements of the W boson total width and hadronic branching ratio, the magnitude of the CKM matrix element Vcs is determined to be |Vcs| = 0.969 +- 0.058.']",['2000-09-08']
631,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['$W^{+}W^{-}$ Production Cross Section and W Branching Fractions in $e^{+}e^{-}$ Collisions at 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, leptonic decay', 'W, hadronic decay', 'W, branching ratio', 'channel cross section', 'lepton, universality', 'electroweak interaction, validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', 'electron positron --> W+ W-', 'W --> quark antiquark', '189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009019'],"['From a data sample of 183 pb^-1 recorded at a center-of-mass energy of roots = 189 GeV with the OPAL detector at LEP, 3068 W-pair candidate events are selected. Assuming Standard Model W boson decay branching fractions, the W-pair production cross section is measured to be sigmaWW = 16.30 +- 0.34(stat.) +- 0.18(syst.) pb. When combined with previous OPAL measurements, the W boson branching fraction to hadrons is determined to be 68.32 +- 0.61(stat.) +- 0.28(syst.) % assuming lepton universality. These results are consistent with Standard Model expectations.']",['2000-09-08']
632,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the Mass and Width of the W Boson in $e^{+}e^{-}$ Collisions at 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'W, mass', 'W, width', 'electroweak interaction, validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009018'],"['The mass and width of the W boson are determined in e+e- collisions at LEP using 183 pb^-1 of data recorded at a centre-of-mass energy roots=189 GeV with the OPAL detector. The invariant mass distributions from 970 WW->qqqq and 1118 WW->qqln candidate events are used to measure the mass of the W boson, Mw = 80.451 +- 0.076(stat.) +- 0.049(syst.) GeV. A direct measurement of the width of the W boson gives Gw=2.09 +- 0.18(stat.) +- 0.09(syst.) GeV. The results are combined with previous OPAL results from 78 pb^-1 of data recorded with roots from 161 to 183 GeV, to obtain: Mw = 80.432 +- 0.066(stat.) +- 0.045(syst.) GeV, Gw = 2.04 +- 0.16(stat.) +- 0.09(syst.) GeV. The consistency of the direct measurement of Mw with that inferred from other measurements of electroweak parameters provides an important test of the Standard Model of electroweak interactions.']",['2000-09-08']
633,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A Study of One-Prong Tau Decays with a Charged Kaon'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'tau, branching ratio', 'charged particle, energy loss', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau- --> K- neutrino/tau', 'tau- --> K- (n)neutral particle neutrino/tau', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009017'],"['From an analysis of the ionisation energy loss of charged particles selected from 110326 e+e- -> tau+tau- candidates recorded by the OPAL detector at e+e- centre-of-mass energies near the Z0 resonance, we determine the one-prong tau decay branching ratios: Br(tau- -> nu_tau K- >=0h0) = 1.528 +- 0.039 +- 0.040 % Br(tau- -> nu_tau K-) = 0.658 +- 0.024 +- 0.029 % where the h0 notation refers to a pi0, an eta, a K^0_S, or a K^0_L, and where the first uncertainty is statistical and the second is systematic.']",['2000-09-08']
634,['eng'],"['Aitala, E M']","['Asymmetries in the production of lambda zero, cascade minus, and omega minus hyperons in 500 GeV/c pi minus-Nucleon Interactions']",['Particle Physics - Experimental Results'],"['pi- nucleon, inclusive reaction', 'Lambda, hadroproduction', 'Xi-, hadroproduction', 'Omega-, hadroproduction', 'hyperon antihyperon, asymmetry', 'x-dependence', 'transverse momentum, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleon --> hyperon anything', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009016'],"['Using data from Fermilab fixed-target experiment E791, we have measured particle-antiparticle production asymmetries for lambda zero, cascade minus, and omega minus hyperons in pi minus-nucleon interactions at 500 GeV/c. The asymmetries are measured as functions of Feynman-x (x_F) and pt^2 over the ranges of -0.12 GE x_F LE 0.12 and 0 GE pt^2 LE 4 (GeV/c)^2. We find substantial asymmetries, even at x_F = 0. We also observe leading-particle- type asymmetries which qualitatively agree with theoretical predictions.']",['2000-09-07']
635,['eng'],"['Wang Shui Cai', 'Wong, H T', 'Fujiwara, M']",['Intrinsic Radioactivity in a GSO Crystal and Limits on Double Beta Decay of Gd-160'],['Particle Physics - Experimental Results'],"['scintillation counter, crystal', 'crystal, radioactivity', 'double-beta decay, (0neutrino)', 'gadolinium, lifetime', 'lower limit', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009014'],"['Scintillating crystal detector offers potential advantages in low-energy low-background experiments for particle physics and astrophysics. The GSO crystal is an interesting detector to explore for future neutrino physics experiments. The contributions to background due to the various channels of intrinsic radio-isotopes from the Th-232 and U-238 series are identified and studied with time-correlation analysis and detailed fits to the spectral shape. Good agreement is achieved between measured and simulated spectra, indicating background suppression factors to the 10^{-2} - 10^{-3} level are possible. The procedures can be adopted for background understanding and suppression in other low-count-rate experiments where the dominant source of background is from internal radioactivity. Based on 1656 hours of data taking, limits on the double beta decay half-life for the various channels in Gd-160 are presented. The limit for the neutrinoless mode is T^{0 \\nu \\beta \\beta}_{{1/2}} > 2.0(0.8) X 10^{20} y at 68(90)% confidence level.']",['2000-09-07']
636,['eng'],[],['Study of the process e+e- to pi+pi-pi+pi-pi0 with CMD-2 detector'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'pi, multiple production', 'eta, intermediate state', 'omega(783), intermediate state', 'mass spectrum, (pi+ pi- pi0)', 'omega(1600), electron p', 'rho(1450), electron p', 'channel cross section, energy dependence', 'magnetic detector, CMD', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> 2pi+ 2pi- pi0', 'electron positron --> omega(783) pi+ pi-', 'electron positron --> eta pi+ pi-', '1.28-1.38 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009013'],['The process e+e- to pi+ pi- pi+ pi- pi0 has been studied in the center of mass energy range 1280 -- 1380 MeV using 3.0 1/pb of data collected with the CMD-2 detector in Novosibirsk. Analysis shows that the cross section of the five pion production is dominated by the contributions of the eta pi+pi- and omega pi+pi- intermediate states.'],['2000-09-07']
637,['eng'],"['Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S A', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X']",['First Observation of the Decays $B^{0}\\to D^{*-}p\\overline {p}\\pi^{+}$ and $B ^{0}\\to D^{*-}p\\overline {n}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'D*(2010)', 'B0, branching ratio', 'B0 --> D*(2010) anti-n p', 'B0 --> D*(2010) p anti-p pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009011'],"['We report the first observation of exclusive decays of the type B to D^* N anti-N X, where N is a nucleon. Using a sample of 9.7 times 10^{6} B-Bbar pairs collected with the CLEO detector operating at the Cornell Electron Storage Ring, we measure the branching fractions B(B^0 \\to D^{*-} proton antiproton \\pi^+) = ({6.5}^{+1.3}_{-1.2} +- 1.0) \\times 10^{-4} and B(B^0 \\to D^{*-} proton antineutron) = ({14.5}^{+3.4}_{-3.0} +- 2.7) times 10^{-4}. Antineutrons are identified by their annihilation in the CsI electromagnetic calorimeter.']",['2000-09-06']
638,['eng'],"['Acciarri, M', 'Achard, P', 'Adriani, O', 'Aguilar-Benítez de Lugo, M', 'Alcaraz, J', 'Alemanni, G', 'Allaby, James V', 'Aloisio, A', 'Alviggi, M G', 'Ambrosi, G', 'Anderhub, H', 'Andreev, V P', 'Angelescu, T', 'Anselmo, F', 'Arefev, A', 'Azemoon, T', 'Aziz, T', 'Bagnaia, P', 'Bajo, A', 'Baksay, L', 'Balandras, A', 'Baldew, S V', 'Banerjee, S', 'Banerjee, Sw', 'Barczyk, A', 'Barillère, R', 'Bartalini, P', 'Basile, M', 'Battiston, R', 'Bay, A', 'Becattini, F', 'Becker, U', 'Behner, F', 'Bellucci, L', 'Berbeco, R', 'Berdugo, J', 'Berges, P', 'Bertucci, B', 'Betev, B L', 'Bhattacharya, S', 'Biasini, M', 'Biland, A', 'Blaising, J J', 'Blyth, S C', 'Bobbink, Gerjan J', 'Böhm, A', 'Boldizsar, L', 'Borgia, B', 'Bourilkov, D', 'Bourquin, Maurice', 'Braccini, S', 'Branson, J G', 'Brochu, F', 'Buffini, A', 'Buijs, A', 'Burger, J D', 'Burger, W J', 'Cai, X D', 'Capell, M', 'Cara Romeo, G', 'Carlino, G', 'Cartacci, A M', 'Casaus, J', 'Castellini, G', 'Cavallari, F', 'Cavallo, N', 'Cecchi, C', 'Cerrada-Canales, M', 'Cesaroni, F', 'Chamizo-Llatas, M', 'Chang, Y H', 'Chaturvedi, U K', 'Chemarin, M', 'Chen, A', 'Chen, G', 'Chen, G M', 'Chen, H F', 'Chen, H S', 'Chiefari, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Civinini, C', 'Clare, I', 'Clare, R', 'Coignet, G', 'Colino, N', 'Costantini, S', 'Cotorobai, F', 'de la Cruz, B', 'Csilling, Akos', 'Cucciarelli, S', 'Dai, T S', 'van Dalen, J A', ""D'Alessandro, R"", 'De Asmundis, R', 'Déglon, P L', 'Degré, A', 'Deiters, K', 'Della Volpe, D', 'Delmeire, E', 'Denes, P', 'De Notaristefani, F', 'De Salvo, A', 'Diemoz, Marcella.', 'Dierckxsens, M', 'Van Dierendonck, D N', 'Dionisi, C', 'Dittmar, Michael', 'Dominguez, A', 'Doria, A', 'Dova, M T', 'Duchesneau, D', 'Dufournaud, D', 'Duinker, P', 'Durán, I', 'El-Mamouni, H', 'Engler, A', 'Eppling, F J', 'Erné, Frits C', 'Extermann, Pierre', 'Fabre, M', 'Falagán, M A', 'Falciano, S', 'Favara, A', 'Fay, J', 'Fedin, O', 'Felcini, Marta', 'Ferguson, T', 'Fesefeldt, H S', 'Fiandrini, E', 'Field, J H', 'Filthaut, F', 'Fisher, P H', 'Fisk, I', 'Forconi, G', 'Freudenreich, Klaus', 'Furetta, C', 'Galaktionov, Yu', 'Ganguli, S N', 'García-Abia, P', 'Gataullin, M', 'Gau, S S', 'Gentile, S', 'Gheordanescu, N', 'Giagu, S', 'Gong, Z F', 'Grenier, G', 'Grimm, O', 'Grünewald, M W', 'Guida, M', 'van Gulik, R', 'Gupta, V K', 'Gurtu, A', 'Gutay, L J', 'Haas, D', 'Hasan, A', 'Hatzifotiadou, D', 'Hebbeker, T', 'Hervé, Alain', 'Hidas, P', 'Hirschfelder, J', 'Hofer, H', 'Holzner, G', 'Hoorani, H', 'Hou, S R', 'Hu, Y', 'Iashvili, I', 'Jin, B N', 'Jones, L W', 'de Jong, P', 'Josa-Mutuberria, I', 'Khan, R A', 'Kaur, M', 'Kienzle-Focacci, M N', 'Kim, D', 'Kim, J K', 'Kirkby, Jasper', 'Kiss, D', 'Kittel, E Wolfram', 'Klimentov, A', 'König, A C', 'Kopp, A', 'Koutsenko, V F', 'Kräber, M H', 'Krämer, R W', 'Krenz, W', 'Krüger, A', 'Kunin, A', 'Ladrón de Guevara, P', 'Laktineh, I', 'Landi, G', 'Lebeau, M', 'Lebedev, A', 'Lebrun, Philippe.', 'Lecomte, P', 'Lecoq, P', 'Le Coultre, P', 'Lee, H J', 'Le Goff, J M', 'Leiste, R', 'Levchenko, P M', 'Li Chuan', 'Likhoded, S A', 'Lin, C H', 'Lin, W T', 'Linde, F L', 'Lista, L', 'Liu, Z A', 'Lohmann, W', 'Longo, E', 'Lü, Y S', 'Lübelsmeyer, K', 'Luci, C', 'Luckey, D', 'Lugnier, L', 'Luminari, L', 'Lustermann, W', 'Ma, W G', 'Maity, M', 'Malgeri, L', 'Malinin, A', 'Maña, C', 'Mangeol, D J', 'Mans, J', 'Marian, G', 'Martin, J P', 'Marzano, F', 'Mazumdar, K', 'McNeil, R R', 'Mele, S', 'Merola, L', 'Meschini, M', 'Metzger, W J', 'Von der Mey, M', 'Mihul, A', 'Milcent, H', 'Mirabelli, G', 'Mnich, J', 'Mohanty, G B', 'Moulik, T', 'Muanza, G S', 'Muijs, A J M', 'Musicar, B', 'Musy, M', 'Napolitano, M', 'Nessi-Tedaldi, F', 'Newman, H', 'Niessen, T', 'Nisati, A', 'Nowak, H', 'Ofierzynski, R A', 'Organtini, G', 'Oulianov, A', 'Palomares, C', 'Pandoulas, D', 'Paoletti, S', 'Paolucci, P', 'Paramatti, R', 'Park, H K', 'Park, I H', 'Passaleva, G', 'Patricelli, S', 'Paul, T', 'Pauluzzi, M', 'Paus, C', 'Pauss, Felicitas', 'Pedace, M', 'Pensotti, S', 'Perret-Gallix, D', 'Petersen, B', 'Piccolo, D', 'Pierella, F', 'Pieri, M', 'Piroué, P A', 'Pistolesi, E', 'Plyaskin, V', 'Pohl, M', 'Pozhidaev, V', 'Postema, H', 'Pothier, J', 'Prokofiev, D O', 'Prokofev, D', 'Quartieri, J', 'Rahal-Callot, G', 'Rahaman, M A', 'Raics, P', 'Raja, N', 'Ramelli, R', 'Rancoita, P G', 'Ranieri, R', 'Raspereza, A V', 'Raven, G', 'Razis, P A', 'Ren, D', 'Rescigno, M', 'Reucroft, S', 'Riemann, S', 'Riles, K', 'Rodin, J', 'Roe, B P', 'Romero, L', 'Rosca, A', 'Rosier-Lees, S', 'Rubio, Juan Antonio', 'Ruggiero, G', 'Rykaczewski, H', 'Saremi, S', 'Sarkar, S', 'Salicio, J', 'Sánchez, E', 'Sanders, M P', 'Sarakinos, M E', 'Schäfer, C', 'Shchegelskii, V', 'Schmidt-Kärst, S', 'Schmitz, D', 'Schopper, Herwig Franz', 'Schotanus, D J', 'Schwering, G', 'Sciacca, C', 'Seganti, A', 'Servoli, L', 'Shevchenko, S', 'Shivarov, N', 'Shoutko, V', 'Shumilov, E', 'Shvorob, A V', 'Siedenburg, T', 'Son, D', 'Smith, B', 'Spillantini, P', 'Steuer, M', 'Stickland, D P', 'Stone, A', 'Stoyanov, B', 'Strässner, A', 'Sudhakar, K', 'Sultanov, G G', 'Sun, L Z', 'Suter, H', 'Swain, J D', 'Szillasi, Z', 'Sztaricskai, T', 'Tang, X W', 'Tauscher, Ludwig', 'Taylor, L', 'Tellili, B', 'Timmermans, C', 'Ting, S C C', 'Ting, S M', 'Tonwar, S C', 'Tóth, J', 'Tully, C', 'Tung, K L', 'Uchida, Y', 'Ulbricht, J', 'Valente, E', 'Vesztergombi, György', 'Vetlitskii, I', 'Vicinanza, D', 'Viertel, Gert M', 'Villa, S', 'Vivargent, M', 'Vlachos, S', 'Vodopyanov, I', 'Vogel, H', 'Vogt, H', 'Vorobev, I', 'Vorobyov, A A', 'Vorvolakos, A', 'Wadhwa, M', 'Wallraff, W', 'Wang, M', 'Wang, X L', 'Wang, Z M', 'Weber, A', 'Weber, M', 'Wienemann, P', 'Wilkens, H', 'Wu, S X', 'Wynhoff, S', 'Xia, L', 'Xu, Z Z', 'Yamamoto, J', 'Yang, B Z', 'Yang, C G', 'Yang, H J', 'Yang, M', 'Ye, J B', 'Yeh, S C', 'Zalite, A', 'Zalite, Yu', 'Zhang, Z P', 'Zhu, G Y', 'Zhu, R Y', 'Zichichi, Antonino', 'Zilizi, G', 'Zimmermann, B', 'Zöller, M']",['Search for Charged Higgs Bosons in $e^{+}e^{-}$ Collisions at Centre-of-Mass Energies up to 202 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, charged particle', 'Higgs particle, pair production', 'Higgs particle, decay modes', 'Higgs particle, mass', 'lower limit', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2Higgs particle', 'Higgs particle --> charm strangeness', 'Higgs particle --> tau neutrino/tau', '192-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009010'],"['A search for pair-produced charged Higgs bosons is performed with the L3 detector at LEP using data collected at centre-of-mass energies between 192 and 202 GeV, corresponding to an integrated luminosity of 233.2 pb^-1. Decays into a charm and a strange quark or into a tau lepton and its neutrino are considered. The observed events are consistent with the expectations from Standard Model background processes. Including data taken at lower centre-of-mass energies, lower limits on the charged Higgs mass are derived at the 95% confidence level. They vary from 67.4 to 79.9GeV as a function of the H^+/- --> tau nu branching ratio.']",['2000-09-06']
639,['eng'],"['Erdmann, M']",['Hadronic Structure Functions'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'electron p, colliding beams', 'electron p, deep inelastic scattering', 'p, structure function', 'neutral current', 'charged current', 'differential cross section, momentum transfer', 'quark, momentum spectrum', 'gluon, momentum spectrum', 'photon, structure function', 'color, singlet', 'exchange, singlet', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009009'],['Experimental results on hadronic structures are discussed in view of our physics understanding. Achievements and challenges are noted.'],['2000-09-06']
640,['eng'],"['Zimmerman, E D']",['Recent Results Addressing the KARMEN Timing Anomaly'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'pi+, rare decay', 'new particle, search for', 'neutral particle, electromagnetic decay', 'neutral particle, lifetime', 'experimental results', 'PSI Cycl', 'Rutherford ISIS PS', 'pi+ --> muon+ neutral particle']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009008'],['Recent resuls from experiments at Fermilab and the Paul Scherrer Institute have constrained the parameter space available for a hypothetical particle $Q^0$ produced in the decay $\\pi^+ \\to \\mu^+ Q^0$. This decay has been invoked to explain a peculiar feature of an event arrival time distribution observed in the KARMEN neutrino experiment.'],['2000-09-05']
641,['eng'],"['Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Fleming, B T', 'Frey, R', 'Formaggio, J A', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McDonald, J', 'McNulty, C', 'McFarland, K S', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Suwonjandee, N', 'Vakili, M', 'Vaitaitis, A G', 'Yang, U K', 'Yu, J', 'Zeller, G P', 'Zimmerman, E D']",['Observation of Anomalous Dimuon Events in the NuTeV Decay Detector'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'beryllium', 'new particle, search for', 'neutralino', 'heavy lepton', 'neutral particle, decay', 'muon, pair production', 'mass, transverse', 'mass spectrum, dimuon', 'energy, asymmetry', 'drift chamber, experimental results', 'Batavia TEVATRON PS', '800 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009007'],"['A search for long-lived neutral particles (N^0) which decay into at least one muon has been performed using an instrumented decay channel at the E815 (NuTeV) experiment at Fermilab. The decay channel was composed of helium bags interspersed with drift chambers, and was used in conjunction with the NuTeV neutrino detector to search for N^0 decays. The data were examined for particles decaying into the muonic final states mu mu, mu e, and mu pi. Three mu mu events were observed over an expected background of 0.040 +/- 0.009 events; no events were observed in the other modes. Although the observed events share some characteristics with neutrino interactions, the observed rate is a factor of 75 greater than expected. No Standard Model process appears to be consistent with this observation.']",['2000-09-05']
642,['eng'],"['Lu, C', 'McDonald, K T']",['The Charge Distribution on the Cathode of a Straw Tube Chamber'],['Particle Physics - Experimental Results'],"['proportional chamber, drift tube', 'electric field, time dependence', 'charge, yield']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009006'],"[""We use Green's reciprocation theorem and the method of weighting fields to deduce the charge distribution on the cathode of a straw tube proportional chamber. The time dependence of the associated current is also discussed.""]",['2000-09-05']
643,['eng'],"['Fujiwara, M C', 'Adamczak, A', 'Bailey, J M', 'Beer, G A', 'Beveridge, J L', 'Faifman, M P', 'Huber, T M', 'Kammel, P', 'Kim, S K', 'Knowles, P E', 'Kunselman, A R', 'Markushin, V E', 'Marshall, G M', 'Martoff, C J', 'Mason, G R', 'Mulhauser, F', 'Olin, A', 'Petitjean, C', 'Porcelli, T A', 'Zmeskal, J']",['Using Thin Film Targets for Muonic Atoms and Muon Catalyzed Fusion Studies'],['Particle Physics - Experimental Results'],"['talk, Tsukuba 1999/12/01', 'muonic atom', 'fusion', 'target, proposed']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009005'],"['Studies of muonic atoms and muon catalyzed fusion have been conventionally done in a bulk target of gas, liquid or solid hydrogen isotopes. The use of thin film targets developed at TRIUMF have notable advantages in tackling some of the most important questions in the field, which could be further exploited at future high intensity muon sources. We review the technique of the thin film method with emphasis on recent results and a future proposal.']",['2000-09-05']
644,['eng'],"['Mele, S']",['ZZ Cross Section Measurements'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, pair production', 'Z0, decay modes', 'final state, (4fermion)', 'channel cross section', 'quark, beauty', 'quark, pair production', 'experimental results', 'CERN LEP Stor', '183-208 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009004'],['Results on the cross section measurement of Z boson pair-production at LEP are presented. The more general case of neutral-current four-fermion production and the particular case of ZZ events enriched in b quarks are also discussed. All the results agree with the Standard Model predictions.'],['2000-09-04']
645,['eng'],"['Milton, K A', 'Kalbfleisch, G R', 'Strauss, M G', 'Gamberg, L P', 'Luo, W', 'Smith, E H']",['New Limits on the Production of Magnetic Monopoles at Fermilab'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'anti-p p, colliding beams', 'magnetic monopole, search for', 'magnetic monopole, pair production', 'Drell-Yan process', 'bound state, (nucleus magnetic monopole)', 'beryllium', 'aluminum', 'channel cross section, upper limit', 'magnetic field', 'superconducting, interference', 'charge, magnetic', 'experimental results', 'Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009003'],"['First results from an experiment (Fermilab E882) searching for magnetically charged particles bound to elements from the CDF and D{\\O}detectors are reported. The experiment is described, and limits on magnetic monopole pair production cross sections for magnetic charges 1, 2, 3, and 6 times the Dirac pole strength are presented. These limits ($\\sim1$ pb), hundreds of times smaller than those found in previous direct accelerator-based searches, use simple model assumptions for the photonic production of monopoles, as does the extraction of mass limits in the hundreds of GeV range.']",['2000-09-04']
646,['eng'],"['Ambrosio, M', 'Antolini, R', 'Auriemma, G', 'Bakari, D', 'Baldini, A', 'Barbarino, G C', 'Barish, B C', 'Battistoni, G', 'Bellotti, R', 'Bemporad, C', 'Bernardini, P', 'Bilokon, H', 'Bisi, V', 'Bloise, C', 'Bower, C', 'Brigida, M', 'Bussino, S', 'Cafagna, F', 'Calicchio, M', 'Campana, D', 'Carboni, M', 'Cecchini, S', 'Cei, F', 'Chiarella, V', 'Choudhary, B C', 'Coutu, S', 'De Cataldo, G', 'Dekhissi, H', 'De Marzo, C', 'De Mitri, I', 'Antolini, R', 'Auriemma, G', 'Bakari, D', 'Baldini, A', 'Barbarino, G C', 'Barish, B C', 'Battistoni, G', 'Bellotti, R', 'Bemporad, C', 'Bernardini, P', 'Bilokon, H', 'Bisi, V', 'Bloise, C', 'Bower, C', 'Brigida, M', 'Bussino, S', 'Cafagna, F', 'Calicchio, M', 'Campana, D', 'Carboni, M', 'Cecchini, S', 'Cei, F', 'Chiarella, V', 'Choudhary, B C', 'Coutu, S', 'De Cataldo, G', 'Dekhissi, H', 'De Marzo, C', 'De Mitri, I', 'Derkaoui, J E', 'De Vincenzi, M', 'Di Credico, A', 'Erriquez, O', 'Favuzzi, C', 'Forti, C', 'Fusco, P', 'Giacomelli, Giorgio', 'Giannini, G', 'Giglietto, N', 'Giorgini, M', 'Grassi, M', 'Gray, L', 'Grillo, A', 'Guarino, F', 'Gustavino, C', 'Habig, A', 'Hanson, K', 'Heinz, R', 'Iarocci, Enzo', 'Katsavounidis, E', 'Katsavounidis, I', 'Kearns, E T', 'Kim, H', 'Kyriazopoulou, S', 'Lamanna, E', 'Lane, C', 'Levin, D S', 'Lipari, P', 'Longley, N P', 'Longo, M J', 'Loparco, F', 'Maaroufi, F', 'Mancarella, G', 'Mandrioli, G', 'Manzoor, S', 'Margiotta, A', 'Marini, A', 'Martello, D', 'Marzari-Chiesa, A', 'Mazziotta, M N', 'Michael, D G', 'Mikheyev, S P', 'Miller, L', 'Monacelli, P', 'Montaruli, T', 'Monteno, M', 'Mufson, S L', 'Musser, J', 'Nicolo, D', 'Nolty, R', 'Okada, C', 'Orth, C', 'Osteria, G', 'Ouchrif, M', 'Palamara, O', 'Patera, V', 'Patrizii, L', 'Pazzi, R', 'Peck, C W', 'Perrone, L', 'Petrera, S', 'Pistilli, P', 'Popa, V', 'Rainó, A', 'Reynoldson, J', 'Ronga, F', 'Rrhioua, A', 'Satriano, C', 'Satta, L', 'Scapparone, E', 'Scholberg, K', 'Sciubba, A', 'Serra, P', 'Sioli, M', 'Sirri, G', 'Sitta, M', 'Spinelli, P', 'Spinetti, M', 'Spurio, M', 'Steinberg, R', 'Stone, J L', 'Sulak, Lawrence R', 'Surdo, A', 'Tarle, G', 'Togo, V', 'Vakili, M', 'Vilela, E', 'Walter, C W', 'Webb, R']",['Search for massive rare particles with MACRO'],['Particle Physics - Experimental Results'],"['new particle, search for', 'magnetic monopole', 'strangelet', 'Q-ball', 'flux, upper limit', 'streamer chamber, drift tube', 'deep underground detector, MACRO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009002'],"['Massive rare particles have been searched for in the penetrating cosmic radiation using the MACRO apparatus at the Gran Sasso National Laboratories. Liquid scintillators, streamer tubes and nuclear track detectors have been used to search for magnetic monopoles (MMs). Based on no observation of such signals, stringent flux limits are established for MMs as slow as a few 10^(-5)c. The methods based on the scintillator and on the nuclear track subdetectors were also applied to search for nuclearites. Preliminary results of the searches for charged Q-balls are also presented.']",['2000-09-04']
647,['eng'],"['Fukuda, S', 'Fukuda, Y', 'Ishitsuka, M', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kobayashi, K', 'Koshio, Y', 'Miura, M', 'Moriyama, S', 'Nakahata, M', 'Nakayama, S', 'Obayashi, Y', 'Okada, A', 'Okumura, K', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, H', 'Takeuchi, Y', 'Toshito, T', 'Totsuka, Y', 'Yamada, S', 'Earl, M A', 'Habig, A', 'Kearns, E T', 'Messier, M D', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Goldhaber, M', 'Barszczak, T', 'Fukuda, Y', 'Ishitsuka, M', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kobayashi, K', 'Koshio, Y', 'Miura, M', 'Moriyama, S', 'Nakahata, M', 'Nakayama, S', 'Obayashi, Y', 'Okada, A', 'Okumura, K', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, H', 'Takeuchi, Y', 'Toshito, T', 'Totsuka, Y', 'Yamada, S', 'Earl, M A', 'Habig, A', 'Kearns, E T', 'Messier, M D', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Goldhaber, M', 'Barszczak, T', 'Casper, David William', 'Gajewski, W', 'Kropp, W R', 'Mine, S', 'Price, L R AU Fukuda, S', 'Fukuda, Y', 'Ishitsuka, M', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kobayashi, K', 'Koshio, Y', 'Miura, M', 'Moriyama, S', 'Nakahata, M', 'Nakayama, S', 'Obayashi, Y', 'Okada, A', 'Okumura, K', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, H', 'Takeuchi, Y', 'Toshito, T', 'Totsuka, Y', 'Yamada, S', 'Earl, M A', 'Habig, A', 'Kearns, E T', 'Messier, M D', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Goldhaber, M', 'Barszczak, T', 'Smy, M B', 'Sobel, H W', 'Vagins, M R', 'Ganezer, K S', 'Keig, W E', 'Ellsworth, R W', 'Tasaka, S', 'Kibayashi, A', 'Learned, J G', 'Matsuno, S', 'Takemori, D', 'Hayato, Y', 'Ishii, T', 'Kobayashi, T', 'Nakamura, K', 'Oyama, Y', 'Sakai, A', 'Sakuda, M', 'Sasaki, O', 'Kohama, M', 'Suzuki, A T', 'Inagaki, T', 'Nishikawa, K', 'Haines, T J', 'Blaufuss, E', 'Kim, B K', 'Sanford, R', 'Svoboda, R', 'Chen, M L', 'Goodman, J A', 'Guillian, G', 'Sullivan, G W', 'Hill, J', 'Jung, C K', 'Martens, K', 'Malek, M', 'Mauger, C', 'McGrew, C', 'Sharkey, E', 'Viren, B M', 'Yanagisawa, C', 'Kirisawa, M', 'Inaba, S', 'Mitsuda, C', 'Miyano, K', 'Okazawa, H', 'Saji, C', 'Takahashi, M', 'Takahata, M', 'Nagashima, Y', 'Nitta, K', 'Takita, M', 'Yoshida, M', 'Kim, S B', 'Ishizuka, T', 'Etoh, M', 'Gando, Y', 'Hasegawa, T', 'Inoue, K', 'Ishihara, K', 'Maruyama, T', 'Shirai, J', 'Suzuki, A', 'Koshiba, M', 'Hatakeyama, Y', 'Ichikawa, Y', 'Koike, M', 'Nishijima, K', 'Fujiyasu, H', 'Ishino, H', 'Morii, M', 'Watanabe, Y', 'Golebiewska, U', 'Kielczewska, D', 'Boyd, S C', 'Stachyra, A L', 'Wilkes, R J', 'Young, K K']",['Tau Neutrinos Favored over Sterile Neutrinos in Atmospheric Muon Neutrino Oscillations'],['Particle Physics - Experimental Results'],"['neutrino/mu, cosmic radiation', 'neutrino, oscillation', 'neutrino/tau', 'neutrino, sterile', 'matter, effect', 'angular distribution', 'neutrino, mass difference', 'neutrino, mixing angle', 'Cherenkov counter, water', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009001'],"['The previously published atmospheric neutrino data did not distinguish whether muon neutrinos were oscillating into tau neutrinos or sterile neutrinos, as both hypotheses fit the data. Using data recorded in 1100 live-days of the Super-Kamiokande detector, we use three complementary data samples to study the difference in zenith angle distribution due to neutral currents and matter effects. We find no evidence favoring sterile neutrinos, and reject the hypothesis at the 99% confidence level. On the other hand, we find that oscillation between muon and tau neutrinos suffices to explain all the results in hand.']",['2000-09-04']
648,['eng'],"['Kettell, S H']",['Future Kaon Programs at BNL and FNAL'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'K0(L), semileptonic decay', 'K+, semileptonic decay', 'neutrino, pair production', 'K, branching ratio', 'Kobayashi-Maskawa angle', 'proposed experiment', 'Batavia TEVATRON PS', 'Brookhaven PS', 'K0(L) --> pi0 neutrino antineutrino', 'K+ --> pi+ pi0 neutrino antineutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008078'],"['Future kaon decay programs at BNL and FNAL are discussed. The primary focus of these programs is the measurement of the golden modes, the neutral and charged kaon decays to a pion and two neutrinos. The observation of the charged mode by E787 at BNL is the first step in a series of measurements which will completely determine the unitarity triangle within the kaon system.']",['2000-09-03']
649,['eng'],"['Kettell, S H']",['Measurement of $B(K^{+} \\to \\pi^{+} \\nu\\overline{\\nu})^{1}$'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'K+, semileptonic decay', 'neutrino, pair production', 'K+, radiative decay', 'K+, branching ratio', 'upper limit', 'Kobayashi-Maskawa angle', 'experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino', 'K+ --> pi+ pi0 photon', 'K+ --> muon+ neutrino/mu photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008077'],"['The experimental measurement of positive kaons decaying to a positive pion and a neutrino, anti-neutrino pair (pnn) is reviewed. Recent results from experiment E787 at BNL are presented: with data from 1995--97 the branching ratio has been measured to be B(pnn) = (1.5^{+3.4}_{-1.2}) \\times10^{-10}. The future prospects for additional data in this mode are examined.']",['2000-09-03']
650,['eng'],"['Benvenuti, Alberto C', 'Denegri, D', 'Genchev, V', 'Khanov, A I', 'Stepanov, N', 'Vankov, P']",['Muon Track Matching'],['Particle Physics - Experimental Results'],"['muon, tracks', 'track data analysis', 'statistical analysis', 'quark, jet', 'quark, beauty', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008075'],"['For most physical processes the tracks observed in the muon stations must be matched with the corresponding tracks in the inner tracker, the external muon system providing muon identification and triggering but the tracker points giving the precise momentum measurement at lower momenta. For high momenta the momentum resolution is much improved by the interconnection of inner and outer measurements. The matching of outer and inner measurements is more delicate in case of muons embedded in jets. A study of the matching procedure was carried out using samples of (b, anti b) jets at high Pt, requiring (b, anti b) -> mu decays.']",['2000-08-31']
651,['eng'],"['Adarkar, H', 'Dugad, S R', 'Krishnaswamy, M R', 'Menon, M G K', 'Sreekantan, B V', 'Hayashi, Y', 'Ito, N', 'Kawakami, S', 'Miyake, S', 'Uchihori, Y']",['Experimental evidence for G.U.T. Proton Decay'],['Particle Physics - Experimental Results'],"['p, semileptonic decay', 'grand unified theory, SU(5)', 'p, lifetime', 'n, oscillation', 'deep underground detector, Kolar Gold Fields', 'experimental results', 'p --> pi0 lepton+', 'p --> K+ neutrino', 'p --> K0 lepton+', 'p --> pi+ neutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008074'],"['Deep underground in Kolar Gold Fields, in southern India, an experiment to detect proton decay had been carried out since the end of 1980. Analysis of data yielded the following results; (l) the life time of proton is about 1 x 1031 years, (2) it decays into wide spectrum of decay modes, p -> e+ + pai0, p ->anti-nutrino + K+ and so on, and (3) the life time and the distribution of decay modes are close to the predictions of SU(5) SUSY GUT. Four events representing possibly neutron oscillation are also seen.']",['2000-08-31']
652,['eng'],"['Rubbia, André']",['ICANOE and OPERA experiments at the LNGS/CNGS'],['Particle Physics - Experimental Results'],"['talk, Sudbury 2000/06/16', 'neutrino, beam', 'neutrino, oscillation', 'neutrino, cosmic radiation', 'flavor, 3', 'neutrino, mass difference', 'neutrino, mixing angle', 'p, semileptonic decay', 'numerical calculations', 'deep underground detector, Gran Sasso', 'proposed experiment', 'p --> K+ antineutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008071'],['We discuss two experiments ICANOE and OPERA that have been proposed within the context of long-baseline and atmospheric neutrino experiments in Europe. The joint ICANOE/OPERA program aims at further improving our understanding of the effect seen in atmospheric neutrinos. This program is based on (1) a continuation of the observation of atmospheric neutrinos with the improved technique of ICANOE/ICARUS (2) a sensitive numu->nue and numu->nutau appearance program with the accelerator neutrinos coming from CERN (CNGS) from a distance of 730~km.'],['2000-08-30']
653,['eng'],"['Foster, B']",['Low-x Physics'],['Particle Physics - Experimental Results'],"['review, London 2000/05/24', 'lepton nucleon, deep inelastic scattering', 'anti-p p, interaction', 'nucleon, structure function', 'small-x', 'momentum spectrum, parton', 'Altarelli-Parisi equation', 'Lipatov equation', 'momentum transfer, dependence', 'structure function, charm', 'structure function, longitudinal', 'jet, electroproduction', 'pi0, electroproduction', 'small-angle', 'cross section, ratio', 'rapidity, gap', 'Regge poles', 'quantum chromodynamics, perturbation theory', 'parametrization', 'model, dipole', 'shadowing', 'experimental results', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008069'],"['Low-x physics is reviewed, with particular emphasis on searches for deviations from GLAP evolution of the parton densities. Although there are several intriguing indications, both in HERA and Tevatron data, as yet there is no unambiguous evidence for other than standard next-to-leading-order GLAP evolution. The framework of dipole models and saturation of parton densities is examined and confronted with the data. Although such models give a good qualitative description of the data, so do other, more conventional, explanations.']",['2000-08-29']
654,['eng'],"['Alton, A']",['Observation of neutral current charm production in $\\nu_{\\mu}Fe$ scattering at the Tevatron'],['Particle Physics - Experimental Results'],"['neutrino nucleus, deep inelastic scattering', 'antineutrino/mu', 'neutrino/mu', 'neutral current', 'quark, charm', 'quark, pair production', 'fusion, Z0 gluon', 'mass, charm', 'quark, semileptonic decay', 'lepton, charge', 'channel cross section', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008068'],"['We report on the first observation of open charm production in neutral current deep inelastic neutrino scattering as seen in the NuTeV detector at Fermilab. The production rate is shown to be consistent with a pure gluon-$% Z^{0}$ boson production model, and the observed level of charm production is used to determine the effective charm mass. As part of our analysis, we also obtain a new measurement for the proton-nucleon charm production cross section at $\\sqrt{s}=38.8$ GeV.']",['2000-08-29']
655,['eng'],"['Geiser, A']",['The MONOLITH project'],['Particle Physics - Experimental Results'],"['talk, Monterey 2000/05/22', 'neutrino, oscillation', 'neutrino/mu', 'showers, air', 'calorimeter, magnetic detector', 'iron', 'spark chamber, glass', 'deep underground detector, Gran Sasso']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008067'],"['MONOLITH is a proposed massive (34 kt) magnetized tracking calorimeter at the Gran Sasso laboratory in Italy, optimized for the detection of atmospheric muon neutrinos. The main goal is to establish (or reject) the neutrino oscillation hypothesis through an explicit observation of the full first oscillation swing. The Delta m^2 sensitivity range for this measurement comfortably covers the complete Super-Kamiokande allowed region. Other measurements include studies of matter effects and the NC/CC and anti-nu/nu ratio, the study of cosmic ray muons in the multi-TeV range, and auxiliary measurements from the CERN to Gran Sasso neutrino beam. Depending on approval, data taking with part of the detector could start in 2004. The detector and its performance are described, and its potential later use as a neutrino factory detector is addressed.']",['2000-08-29']
656,['eng'],"['Battaglia, M']",['Determinations of |Vub| with inclusive techniques at LEP'],['Particle Physics - Experimental Results'],"['talk, Valencia 2000/06/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'final state, (0charm)', 'Kobayashi-Maskawa angle, (up beauty)', 'operator product expansion', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008066'],"['The charmless semileptonic decay branching fraction has been measured, using inclusive techniques, by the Aleph, Delphi and L3 experiments at LEP. The average of their results is 1.74 +/- 0.37 +/- 0.38 +/- 0.21 10-3. From this result the value of the |Vub| element in the CKM mixing matrix has been derived, using OPE predictions, obtaining: |Vub| = (4.13 +0.42/-0.47 (stat.+det.) +0.43/-0.48 (b->c syst.) +0.24/-0.25 (b->u syst.) +/- 0.02 (taub) +/- 0.20 (HQE)) 10-3.']",['2000-08-29']
657,['eng'],"['Albright, Carl H']",['Physics at a Neutrino Factory'],['Particle Physics - Experimental Results'],"['neutrino, particle source', 'muon, storage ring', 'neutrino, beam', 'neutrino/mu', 'neutrino/e', 'neutrino, flux', 'neutrino, oscillation', 'neutrino, sterile', 'neutrino, mass', 'neutrino, mixing angle', 'neutrino/tau', 'counters and detectors, proposed', 'lepton, particle identification', 'violation, CP', 'neutrino nucleon, deep inelastic scattering', 'charged current', 'polarization', 'nucleon, structure function', 'total cross section', 'neutrino nucleus, deep inelastic scattering', 'nucleon, spin', 'quark, charm', 'D0 anti-D0, interference', 'electroweak interaction, validity test', 'heavy lepton, mixing angle', 'neutrino, magnetic moment', 'supersymmetry', 'R parity, violation', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008064'],"['In response to the growing interest in building a Neutrino Factory to produce high intensity beams of electron- and muon-neutrinos and antineutrinos, in October 1999 the Fermilab Directorate initiated two six-month studies. The first study, organized by N. Holtkamp and D. Finley, was to investigate the technical feasibility of an intense neutrino source based on a muon storage ring. This design study has produced a report in which the basic conclusion is that a Neutrino Factory is technically feasible, although it requires an aggressive R&D program. The second study, which is the subject of this report, was to explore the physics potential of a Neutrino Factory as a function of the muon beam energy and intensity, and for oscillation physics, the potential as a function of baseline.']",['2000-08-28']
658,['eng'],"['Mikaelyan, L A']",['Present and Future Oscillation Experiments at Reactors'],['Particle Physics - Experimental Results'],"['talk, Dubna 2000/07/19', 'neutrino, oscillation', 'fission, particle source', 'antineutrino p, interaction', 'charged current', 'positron, energy spectrum', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, experimental results', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008063'],"[""This is a report on recent progress and developments since the NANP'99 Conference in current and future long baseline (~1 km) and very long baseline (~100 - 800 km) oscillation experiments at reactors. These experiments, under certain assumptions, can fully reconstruct the internal mass structure of the electron neutrino and provide laboratory test of solar and atmospheric neutrino problems.""]",['2000-08-28']
659,['eng'],"['Cormack, C M']",['Structure Functions at Very High $Q^{2}$ From HERA'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'electron p, colliding beams', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'neutral current', 'charged current', 'differential cross section', 'momentum transfer, high', 'p, structure function', 'x-dependence', 'momentum transfer, dependence', 'W, mass', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008062'],['Measurements of Deep-Inelastic Neutral and Charged current interactions are presented in lepton proton scattering at HERA. The measurements are obtained from taken during 1996 to 1999 and consists of $30 \\rm{pb^{-1}}$ of $e^+p$ and $16 \\rm{pb^{-1}}$ of $e^-p$ data. The addition of the new high statistics electron data with the positron data allows the first extraction of the parity violating structure function $xF_3$ and tests of high-$Q^2$ electroweak effects of the heavy bosons $Z^0$ and $W$ are observed and found to be consistent with the Standard Model expectation.'],['2000-08-25']
660,['eng'],"['Aubert, Bernard']",['Search for $B^{+}1^{+}1^{-}$ and $B^{0} \\to K^{(*0)}1^{+}1^{-}$'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'K*(892)', 'B+, branching ratio', 'B0, branching ratio', 'upper limit', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B+ --> K+ lepton+ lepton-', 'B0 --> K*(892) lepton+ lepton-', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008059'],"['Using a sample of 3.7 x 10^{6} Y(4S) --> B-anti-B events collected with the BABAR detector at the PEP-II storage ring, we search for the electroweak penguin decays B^+ --> K^+e^+e^-, B^+ --> K^+mu^+mu^-, B^0 --> K^{*0)e^+e^-, and B^0 --> K^{*0)mu^+mu^-. We observe no significant signals for these modes and set preliminary 90% C.L. upper limits of B(B^+ --> K^+e^+e^-) < 12.5 x 10^{-6}, B(B^+ --> K^+mu^+mu^-) < 8.3 x 10^{-6}, B(B^0 --> K^{*0)e^+e^-) < 24.1 x 10^{-6}, B(B^0 --> K^{*0)mu^+mu^-) < 24.5 x 10^{-6}.']",['2000-08-25']
661,['eng'],"['Aubert, Bernard']",['Measurements of charmless three-body and quasi-two-body B decays'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'eta(958)', 'omega(783)', 'final state, (0charm)', 'B0, branching ratio', 'B+, branching ratio', 'upper limit', 'meson, pair production', 'final state, (3meson)', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008058'],"[""We present preliminary results of a search for several exclusive charmless hadronic B decays from electron-positron annihilation data collected by the BABAR detector near the Y(4S) resonance. These include three-body decay modes with final states h^{+/-}h^{-/+}h^{+/-} and h^{+/-}h^{-/+}pi^0, and quasi-two-body decay modes with final states X^0 h and X^0 K0S, where h = pi or K and X^0 = eta^' or omega. We find B(B^0 --> rho^(-/+)pi^(+/-)) = (49+/-13^{+6}_{-5}) x 10^{-6} and B(B^+ --> eta^' K^+) = (62+/-18+/-8) x 10^{-6} and present upper limits for eight other decays.""]",['2000-08-25']
662,['eng'],"['Aubert, Bernard']",['Measurement of branching fractions for two-body charmless B decays to charged pions and kaons at BABAR'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'final state, (0charm)', 'B0, branching ratio', 'upper limit', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> pi+ pi-', 'B0 --> K+ pi-', 'B0 --> K+ K-', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008057'],"[""We present preliminary results of a search for charmless two-body B decays to charged pions and kaons using data collected by the BABAR detector at the Stanford Linear Accelerator Center's PEP-II storage ring. In a sample of 8.8 million produced B-anti-B pairs we measure the branching fractions B(B^0 --> pi^+pi^-) = (9.3^{+2.6}_{-2.3}^{+1.2}_{-1.4}) x 10^{-6} and B(B^0 --> K^+\\pi^-) = (12.5^{+3.0}_{-2.6}^{+1.3}_{-1.7}) x 10^{-6}, where the first uncertainty is statistical and the second is systematic. For the decay B^0 --> K^+K^- we find no significant signal and set an upper limit of B(B^0 --> K^+K^-) < 6.6 x 10^{-6} at the 90% confidence level.""]",['2000-08-25']
663,['eng'],"['Aubert, Bernard']",['Study of inclusive $D_{S}^{((*)+/-)}$ production in B decays and measurement of $B^{0} \\to D^{(*-)}D_{S}^{((*)+)}$ decays using a partial reconstruction technique'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'B0, branching ratio', 'charmed meson, pair production', 'charmed meson, yield', 'D/s', 'D/s*(2110)', 'D*(2010)', 'momentum spectrum', 'particle identification', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> D/s(2110) D*(2010)', 'B0 --> D*(2010) D/s', 'D/s --> Phi(1020) pi', 'approx. 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008056'],"['Electron-positron annihilation data collected by the BABAR detector near the Y(4S) resonance are used to study the inclusive decay of B mesons to D_S^(+/-) and D_S^(*+/-) mesons, where the D_S^(+/-) is reconstructed using the decay D_S^(+/-) --> phi pi^(+/-). The production fraction of inclusive D_S^((*)+/-) and the corresponding momentum spectra have been determined. The exclusive decays B^0 --> D^(*-)D_S^((*)+) are observed with a partial reconstruction technique which uses the soft pion from the D^(*+/-) decay in association with the reconstructed D_S^((*)+/-). The beam energy constraint is used to determine the missing mass recoiling against the D_S^(+/-) system, showing a clear signal for this process. From the observed rates, preliminary results for the corresponding branching fractions have been obtained.']",['2000-08-25']
664,['eng'],"['Aubert, Bernard', 'Boucham, A', 'Boutigny, D', 'De Bonis, I', 'Favier, J', 'Gaillard, Jean-Marc', 'Galeazzi, F', 'Jérémie, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Zachariadou, K', 'Palano, A', 'Chen, G P', 'Chen Jia Chao', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Fan, Q', 'Gill, M S', 'Gowdy, S J', 'Groysman, Y', 'Jacobsen, R G', 'Kadel, R W', 'Kadyk, J A', 'Kerth, L T', 'Kluth, S', 'Kral, J F', 'Leclerc, C', 'Levi, M E', 'Liu, T', 'Lynch, G', 'Meyer, A B', 'Momayezi, M', 'Oddone, P J', 'Perazzo, A', 'Pripstein, M', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Strother, P', 'Telnov, A V', 'Wenzel, W A', 'Champion, T J', 'Hawkes, C M', 'Kirk, A', ""O'Neale, S W"", 'Watson, A T', 'Watson, N K', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Chevalier, N', 'Clark, P J', 'Cottingham, N', 'De Groot, N', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M A', 'Stoker, D P', 'Ahsan, A', 'Arisaka, K', 'Buchanan, C D', 'Chun, S', 'Branson, J G', 'Faccini, R', 'MacFarlane, D B', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Campagnari, C', 'Dahmes, B', 'Hart, P A', 'Kuznetsova, N P', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Turri, M', 'Williams, D C', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoredsky, A P', 'Hitlin, D G', 'Kolomensky, Yu G', 'Metzler, S', 'Oyang, J Y T', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Aleksan, R', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Hamel de Monchenault, G', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S M', 'Jayatilleke, S M', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Wilson, R J', 'Zhang, J', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J D', 'Sen, S', 'Smith, J G', 'Wagner, D L', 'Brandt, T', 'Brose, J', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Kocian, M L', 'Müller-Pfefferkorn, R', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Roussot, E', 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di Lodovico, F', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E A', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Fabbricatore, P', 'Farinon, S', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Musenich, R', 'Parodi, R', 'Passaggio, S', 'Pastore, F', 'Patrignani, C', 'Pia, M G', 'Priano, C', 'Robutti, E', 'Santroni, A', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'Meyer, W T', 'Rosenberg, E I', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Morganti, M', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Benkebil, M', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', 'Shi, X', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'McMahon, S', 'McMahon, T R', 'Payne, D J', 'Touramanis, C', 'Aspinwall, M L', 'Dauncey, P D', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R D', 'Nash, J A', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Vidal, P B', 'Williams, M I', 'Cowan, G D', 'Green, M G', 'Kurup, A', 'McGrath, P', 'Scott, I', 'Brown, D', 'Davis, C L', 'Li, Y', 'Pavlovich, J', 'Trunov, A G', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Fullwood, J', 'Khan, A', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Thompson, R J', 'Weatherall, J H', 'Dallapiccola, C', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Brau, B', 'Cowan, R', 'Taylor, F', 'Yamamoto, R K', 'Blaylock, G', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R R', 'Lin, C S', 'Willocq, S', 'Wittlin, J', 'Bloom, P', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Kroeger, R A', 'Reidy, J', 'Sanders, D', 'Summers, D J', 'Arguin, J F', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Woch, A', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cavallo, N', 'De Nardo, G', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Piccolo, D', 'Sciacca, C', 'Falbo, M', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Colecchia, F', 'Dal Corso, F', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Hamon, O', 'Le Diberder, F', 'Leruste, P J', 'Lory, J', 'Martínez-Vidal, F', 'Roos, L', 'Stark, J', 'Versille, S', 'Manfredi, P F', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Kelsey, M H', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Cavoto, G', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M S', 'Plano, R J', 'Adye, T', 'Egede, U', 'Franek, B J', 'Geddes, N I', 'Gopal, Gian P', 'Copty, N K', 'Purohit, M V', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Anulli, F', 'Aston, D', 'Baird, K', 'Bloom, Elliott D', 'Boyarski, A M', 'Bulos, F', 'Calderini, G', 'Convery, M R', 'Coupal, D P', 'Coward, D H', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Hewett, J L', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kim, P', 'Langenegger, U', 'Leith, D W G S', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'Manzin, G', 'Marsiske, H', 'Menke, S', 'Messner, R', 'Moffeit, K C', 'Morii, M', 'Mount, R', 'Müller, D R', ""O'Grady, C P"", 'Paolucci, P', 'Petrak, S', 'Quinn, Helen R', 'Ratcliff, B N', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Sciolla, G', 'Serbo, V V', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'Wisniewski, W J', 'Young, C C', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'De Silva, A', 'Henderson, R', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Prest, M', 'Vallazza, E', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'Jackson, P D', 'Kowalewski, R V', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Johnson, J R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Walsh, J', 'Wu, S L', 'Yu, Z', 'Zobernig, H G']",['A measurement of the branching fraction of the exclusive decay $B^{0} \\to K^{*0}\\gamma$'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), hadroproduction', 'B, pair production', 'B0, radiative decay', 'B0, branching ratio', 'K*(892), hadronic decay', 'mass spectrum, (K+ pi-)', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> K*(892) photon', 'K*(892) --> K+ pi-', 'approx 10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008055'],"[""The b --> s gamma transition proceeds by a loop ``penguin'' diagram. It may be used to measure precisely the couplings of the top quark and to search for the effects of any new particles appearing in the loop. We present a preliminary measurement of the branching fraction of the exclusive decay, B^0 --> K^{*0}gamma. We use 8.6 x 10^6 B-anti-B decays to measure B(B^0 --> K^{*0}gamma) = (5.4+/-0.8+/-0.5) x 10^{-5}.""]",['2000-08-24']
665,['eng'],"['Aubert, Bernard', 'Boucham, A', 'Boutigny, D', 'De Bonis, I', 'Favier, J', 'Gaillard, Jean-Marc', 'Galeazzi, F', 'Jérémie, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Zachariadou, K', 'Palano, A', 'Chen, G P', 'Chen Jia Chao', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Fan, Q', 'Gill, M S', 'Gowdy, S J', 'Groysman, Y', 'Jacobsen, R G', 'Kadel, R W', 'Kadyk, J A', 'Kerth, L T', 'Kluth, S', 'Kral, J F', 'Leclerc, C', 'Levi, M E', 'Liu, T', 'Lynch, G', 'Meyer, A B', 'Momayezi, M', 'Oddone, P J', 'Perazzo, A', 'Pripstein, M', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Strother, P', 'Telnov, A V', 'Wenzel, W A', 'Champion, T J', 'Hawkes, C M', 'Kirk, A', ""O'Neale, S W"", 'Watson, A T', 'Watson, N K', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Chevalier, N', 'Clark, P J', 'Cottingham, N', 'De Groot, N', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M A', 'Stoker, D P', 'Ahsan, A', 'Arisaka, K', 'Buchanan, C D', 'Chun, S', 'Branson, J G', 'Faccini, R', 'MacFarlane, D B', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Campagnari, C', 'Dahmes, B', 'Hart, P A', 'Kuznetsova, N P', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Turri, M', 'Williams, D C', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoredsky, A P', 'Hitlin, D G', 'Kolomensky, Yu G', 'Metzler, S', 'Oyang, J Y T', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Aleksan, R', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Hamel de Monchenault, G', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S M', 'Jayatilleke, S M', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Wilson, R J', 'Zhang, J', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J D', 'Sen, S', 'Smith, J G', 'Wagner, D L', 'Brandt, T', 'Brose, J', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Kocian, M L', 'Müller-Pfefferkorn, R', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Roussot, E', 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di Lodovico, F', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E A', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Fabbricatore, P', 'Farinon, S', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Musenich, R', 'Parodi, R', 'Passaggio, S', 'Pastore, F', 'Patrignani, C', 'Pia, M G', 'Priano, C', 'Robutti, E', 'Santroni, A', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'Meyer, W T', 'Rosenberg, E I', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Morganti, M', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Benkebil, M', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', 'Shi, X', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'McMahon, S', 'McMahon, T R', 'Payne, D J', 'Touramanis, C', 'Aspinwall, M L', 'Dauncey, P D', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R D', 'Nash, J A', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Vidal, P B', 'Williams, M I', 'Cowan, G D', 'Green, M G', 'Kurup, A', 'McGrath, P', 'Scott, I', 'Brown, D', 'Davis, C L', 'Li, Y', 'Pavlovich, J', 'Trunov, A G', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Fullwood, J', 'Khan, A', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Thompson, R J', 'Weatherall, J H', 'Dallapiccola, C', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Brau, B', 'Cowan, R', 'Taylor, F', 'Yamamoto, R K', 'Blaylock, G', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R R', 'Lin, C S', 'Willocq, S', 'Wittlin, J', 'Bloom, P', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Kroeger, R A', 'Reidy, J', 'Sanders, D', 'Summers, D J', 'Arguin, J F', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Woch, A', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cavallo, N', 'De Nardo, G', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Piccolo, D', 'Sciacca, C', 'Falbo, M', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Colecchia, F', 'Dal Corso, F', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Hamon, O', 'Le Diberder, F', 'Leruste, P J', 'Lory, J', 'Martínez-Vidal, F', 'Roos, L', 'Stark, J', 'Versille, S', 'Manfredi, P F', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Kelsey, M H', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Cavoto, G', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M S', 'Plano, R J', 'Adye, T', 'Egede, U', 'Franek, B J', 'Geddes, N I', 'Gopal, Gian P', 'Copty, N K', 'Purohit, M V', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Anulli, F', 'Aston, D', 'Baird, K', 'Bloom, Elliott D', 'Boyarski, A M', 'Bulos, F', 'Calderini, G', 'Convery, M R', 'Coupal, D P', 'Coward, D H', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Hewett, J L', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kim, P', 'Langenegger, U', 'Leith, D W G S', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'Manzin, G', 'Marsiske, H', 'Menke, S', 'Messner, R', 'Moffeit, K C', 'Morii, M', 'Mount, R', 'Müller, D R', ""O'Grady, C P"", 'Paolucci, P', 'Petrak, S', 'Quinn, Helen R', 'Ratcliff, B N', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Sciolla, G', 'Serbo, V V', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'Wisniewski, W J', 'Young, C C', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'De Silva, A', 'Henderson, R', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Prest, M', 'Vallazza, E', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'Jackson, P D', 'Kowalewski, R V', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Johnson, J R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Walsh, J', 'Wu, S L', 'Yu, Z', 'Zobernig, H G']",['Measurement of the time dependence of $B^{0}-anti-B^{0}$ oscillations using inclusive dilepton events'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0 anti-B0, oscillation', 'time dependence', 'B0, mass difference', 'particle identification, flavor', 'charge, dilepton', 'neural network', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008054'],"['A preliminary study of time dependence of B^0-anti-B^0 oscillations using dilepton events is presented. The flavor of the B meson is determined by the charge sign of the lepton. To separate signal leptons from cascade and fake leptons we have used a method which combines several discriminating variables in a neural network. The time evolution of the oscillations is studied by reconstructing the time difference between the decays of the B mesons produced by the Y(4S) decay. With an integrated luminosity of 7.7 fb-1 collected on resonance by BABAR at the PEP-II asymmetric B Factory, we measure the difference in mass of the neutral B eigenstates, Delta_mB0 to be (0.507+/-0.015+/-0.022) x 10^{12} hbar-s^{-1}.']",['2000-08-24']
666,['eng'],"['Aubert, Bernard', 'Boucham, A', 'Boutigny, D', 'De Bonis, I', 'Favier, J', 'Gaillard, Jean-Marc', 'Galeazzi, F', 'Jérémie, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Zachariadou, K', 'Palano, A', 'Chen, G P', 'Chen Jia Chao', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Fan, Q', 'Gill, M S', 'Gowdy, S J', 'Groysman, Y', 'Jacobsen, R G', 'Kadel, R W', 'Kadyk, J A', 'Kerth, L T', 'Kluth, S', 'Kral, J F', 'Leclerc, C', 'Levi, M E', 'Liu, T', 'Lynch, G', 'Meyer, A B', 'Momayezi, M', 'Oddone, P J', 'Perazzo, A', 'Pripstein, M', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Strother, P', 'Telnov, A V', 'Wenzel, W A', 'Champion, T J', 'Hawkes, C M', 'Kirk, A', ""O'Neale, S W"", 'Watson, A T', 'Watson, N K', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Chevalier, N', 'Clark, P J', 'Cottingham, N', 'De Groot, N', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M A', 'Stoker, D P', 'Ahsan, A', 'Arisaka, K', 'Buchanan, C D', 'Chun, S', 'Branson, J G', 'Faccini, R', 'MacFarlane, D B', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Campagnari, C', 'Dahmes, B', 'Hart, P A', 'Kuznetsova, N P', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Turri, M', 'Williams, D C', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoredsky, A P', 'Hitlin, D G', 'Kolomensky, Yu G', 'Metzler, S', 'Oyang, J Y T', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Aleksan, R', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Hamel de Monchenault, G', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S M', 'Jayatilleke, S M', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Wilson, R J', 'Zhang, J', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J D', 'Sen, S', 'Smith, J G', 'Wagner, D L', 'Brandt, T', 'Brose, J', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Kocian, M L', 'Müller-Pfefferkorn, R', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Roussot, E', 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di Lodovico, F', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E A', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Fabbricatore, P', 'Farinon, S', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Musenich, R', 'Parodi, R', 'Passaggio, S', 'Pastore, F', 'Patrignani, C', 'Pia, M G', 'Priano, C', 'Robutti, E', 'Santroni, A', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'Meyer, W T', 'Rosenberg, E I', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Morganti, M', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Benkebil, M', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', 'Shi, X', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'McMahon, S', 'McMahon, T R', 'Payne, D J', 'Touramanis, C', 'Aspinwall, M L', 'Dauncey, P D', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R D', 'Nash, J A', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Vidal, P B', 'Williams, M I', 'Cowan, G D', 'Green, M G', 'Kurup, A', 'McGrath, P', 'Scott, I', 'Brown, D', 'Davis, C L', 'Li, Y', 'Pavlovich, J', 'Trunov, A G', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Fullwood, J', 'Khan, A', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Thompson, R J', 'Weatherall, J H', 'Dallapiccola, C', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Brau, B', 'Cowan, R', 'Taylor, F', 'Yamamoto, R K', 'Blaylock, G', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R R', 'Lin, C S', 'Willocq, S', 'Wittlin, J', 'Bloom, P', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Kroeger, R A', 'Reidy, J', 'Sanders, D', 'Summers, D J', 'Arguin, J F', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Woch, A', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cavallo, N', 'De Nardo, G', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Piccolo, D', 'Sciacca, C', 'Falbo, M', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Colecchia, F', 'Dal Corso, F', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Hamon, O', 'Le Diberder, F', 'Leruste, P J', 'Lory, J', 'Martínez-Vidal, F', 'Roos, L', 'Stark, J', 'Versille, S', 'Manfredi, P F', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Kelsey, M H', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Cavoto, G', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M S', 'Plano, R J', 'Adye, T', 'Egede, U', 'Franek, B J', 'Geddes, N I', 'Gopal, Gian P', 'Copty, N K', 'Purohit, M V', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Anulli, F', 'Aston, D', 'Baird, K', 'Bloom, Elliott D', 'Boyarski, A M', 'Bulos, F', 'Calderini, G', 'Convery, M R', 'Coupal, D P', 'Coward, D H', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Hewett, J L', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kim, P', 'Langenegger, U', 'Leith, D W G S', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'Manzin, G', 'Marsiske, H', 'Menke, S', 'Messner, R', 'Moffeit, K C', 'Morii, M', 'Mount, R', 'Müller, D R', ""O'Grady, C P"", 'Paolucci, P', 'Petrak, S', 'Quinn, Helen R', 'Ratcliff, B N', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Sciolla, G', 'Serbo, V V', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'Wisniewski, W J', 'Young, C C', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'De Silva, A', 'Henderson, R', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Prest, M', 'Vallazza, E', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'Jackson, P D', 'Kowalewski, R V', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Johnson, J R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Walsh, J', 'Wu, S L', 'Yu, Z', 'Zobernig, H G']",['Measurement of the $B^{0}$ meson properties using partially reconstructed $B^{0} \\to D^{*-}\\pi^{+}$ and $B^{0} \\to D^{*-}l^{+}\\nu$ decay with the BABAR detector'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'B0, semileptonic decay', 'D*(2010)', 'B0, lifetime', 'track data analysis, vertex', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> D*(2010) pi+', 'B0 --> D*(2010) lepton+ neutrino', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008053'],"['The two B^0 decay processes B^0 --> D^{*-}pi^+ and B^0 --> D^{*-}l^+nu have been studied by means of a partial reconstruction technique using a data sample collected with the BABAR detector at the PEP-II storage ring. To increase statistics, only the soft pi^- from the decay D^{*-} --> pi^-D^0 was used in association with either an oppositely-charged high-momentum pion or lepton. Events were then identified by exploiting the constraints from the simple kinematics of Y(4S) decays. A clear signature is obtained in each case. The position of the B^0 decay point was obtained from the reconstructed pi^+(l^+)pi^- vertex. The position of the other anti-B^0 in the event was also determined. Taking advantage of the boost given to the Y(4S) system by the asymmetric beam energies of PEP-II, the lifetime of the B^0 meson has been measured from the separation distance between the two vertices along the beam direction. The preliminary results are tau_B0 = 1.55+/-0.05+/-0.07 ps, tau_B0 = 1.62+/-0.02+/-0.09 ps, respectively for the B^0 --> D^{*-}pi^+ and B^0 --> D^{*-}l^+nu channels.']",['2000-08-24']
667,['eng'],"['Aubert, Bernard', 'Boucham, A', 'Boutigny, D', 'De Bonis, I', 'Favier, J', 'Gaillard, Jean-Marc', 'Galeazzi, F', 'Jérémie, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Zachariadou, K', 'Palano, A', 'Chen, G P', 'Chen Jia Chao', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Fan, Q', 'Gill, M S', 'Gowdy, S J', 'Groysman, Y', 'Jacobsen, R G', 'Kadel, R W', 'Kadyk, J A', 'Kerth, L T', 'Kluth, S', 'Kral, J F', 'Leclerc, C', 'Levi, M E', 'Liu, T', 'Lynch, G', 'Meyer, A B', 'Momayezi, M', 'Oddone, P J', 'Perazzo, A', 'Pripstein, M', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Strother, P', 'Telnov, A V', 'Wenzel, W A', 'Champion, T J', 'Hawkes, C M', 'Kirk, A', ""O'Neale, S W"", 'Watson, A T', 'Watson, N K', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Chevalier, N', 'Clark, P J', 'Cottingham, N', 'De Groot, N', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M A', 'Stoker, D P', 'Ahsan, A', 'Arisaka, K', 'Buchanan, C D', 'Chun, S', 'Branson, J G', 'Faccini, R', 'MacFarlane, D B', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Campagnari, C', 'Dahmes, B', 'Hart, P A', 'Kuznetsova, N P', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Turri, M', 'Williams, D C', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoredsky, A P', 'Hitlin, D G', 'Kolomensky, Yu G', 'Metzler, S', 'Oyang, J Y T', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Aleksan, R', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Hamel de Monchenault, G', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S M', 'Jayatilleke, S M', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Wilson, R J', 'Zhang, J', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J D', 'Sen, S', 'Smith, J G', 'Wagner, D L', 'Brandt, T', 'Brose, J', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Kocian, M L', 'Müller-Pfefferkorn, R', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Roussot, E', 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di Lodovico, F', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E A', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Fabbricatore, P', 'Farinon, S', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Musenich, R', 'Parodi, R', 'Passaggio, S', 'Pastore, F', 'Patrignani, C', 'Pia, M G', 'Priano, C', 'Robutti, E', 'Santroni, A', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'Meyer, W T', 'Rosenberg, E I', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Morganti, M', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Benkebil, M', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', 'Shi, X', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'McMahon, S', 'McMahon, T R', 'Payne, D J', 'Touramanis, C', 'Aspinwall, M L', 'Dauncey, P D', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R D', 'Nash, J A', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Vidal, P B', 'Williams, M I', 'Cowan, G D', 'Green, M G', 'Kurup, A', 'McGrath, P', 'Scott, I', 'Brown, D', 'Davis, C L', 'Li, Y', 'Pavlovich, J', 'Trunov, A G', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Fullwood, J', 'Khan, A', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Thompson, R J', 'Weatherall, J H', 'Dallapiccola, C', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Brau, B', 'Cowan, R', 'Taylor, F', 'Yamamoto, R K', 'Blaylock, G', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R R', 'Lin, C S', 'Willocq, S', 'Wittlin, J', 'Bloom, P', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Kroeger, R A', 'Reidy, J', 'Sanders, D', 'Summers, D J', 'Arguin, J F', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Woch, A', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cavallo, N', 'De Nardo, G', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Piccolo, D', 'Sciacca, C', 'Falbo, M', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Colecchia, F', 'Dal Corso, F', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Hamon, O', 'Le Diberder, F', 'Leruste, P J', 'Lory, J', 'Martínez-Vidal, F', 'Roos, L', 'Stark, J', 'Versille, S', 'Manfredi, P F', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Kelsey, M H', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Cavoto, G', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M S', 'Plano, R J', 'Adye, T', 'Egede, U', 'Franek, B J', 'Geddes, N I', 'Gopal, Gian P', 'Copty, N K', 'Purohit, M V', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Anulli, F', 'Aston, D', 'Baird, K', 'Bloom, Elliott D', 'Boyarski, A M', 'Bulos, F', 'Calderini, G', 'Convery, M R', 'Coupal, D P', 'Coward, D H', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Hewett, J L', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kim, P', 'Langenegger, U', 'Leith, D W G S', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'Manzin, G', 'Marsiske, H', 'Menke, S', 'Messner, R', 'Moffeit, K C', 'Morii, M', 'Mount, R', 'Müller, D R', ""O'Grady, C P"", 'Paolucci, P', 'Petrak, S', 'Quinn, Helen R', 'Ratcliff, B N', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Sciolla, G', 'Serbo, V V', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'Wisniewski, W J', 'Young, C C', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'De Silva, A', 'Henderson, R', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Prest, M', 'Vallazza, E', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'Jackson, P D', 'Kowalewski, R V', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Johnson, J R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Walsh, J', 'Wu, S L', 'Yu, Z', 'Zobernig, H G']",['Measurement of the branching fractions for $B^{0}\\to D^{*-}\\pi^{+}$ and $B^{0} \\to D^{*-}\\rho^{+}$'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'B0, branching ratio', 'D*(2010)', 'rho(770)+', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B0 --> D*(2010) pi+', 'B0 --> D*(2010) rho(770)+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008051'],"['Using 5.2 fb-1 of e^+e^- annihilation data recorded with the BABAR detector at the PEP-II storage ring while operating on the Y(4S) resonance, a sample of fully reconstructed B^0 decays in the hadronic modes B^0 -> D^{*-}pi^+ and B^0 -> D^{*-}rho^+ have been reconstructed. In this paper, a study of these events is reported, including preliminary measurements of the absolute branching fractions for these modes, which are found to be B(B^0 -> D^{*-}pi^+) = (2.9+/-0.3+/-0.3) x 10^{-3} and B(B^0 -> D^{*-}rho^+) = (11.2+/-1.1+/-2.5) x 10^{-3}.']",['2000-08-24']
668,['eng'],"['Aubert, Bernard', 'Boucham, A', 'Boutigny, D', 'De Bonis, I', 'Favier, J', 'Gaillard, Jean-Marc', 'Galeazzi, F', 'Jérémie, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Zachariadou, K', 'Palano, A', 'Chen, G P', 'Chen Jia Chao', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Fan, Q', 'Gill, M S', 'Gowdy, S J', 'Groysman, Y', 'Jacobsen, R G', 'Kadel, R W', 'Kadyk, J A', 'Kerth, L T', 'Kluth, S', 'Kral, J F', 'Leclerc, C', 'Levi, M E', 'Liu, T', 'Lynch, G', 'Meyer, A B', 'Momayezi, M', 'Oddone, P J', 'Perazzo, A', 'Pripstein, M', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Strother, P', 'Telnov, A V', 'Wenzel, W A', 'Champion, T J', 'Hawkes, C M', 'Kirk, A', ""O'Neale, S W"", 'Watson, A T', 'Watson, N K', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Chevalier, N', 'Clark, P J', 'Cottingham, N', 'De Groot, N', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M A', 'Stoker, D P', 'Ahsan, A', 'Arisaka, K', 'Buchanan, C D', 'Chun, S', 'Branson, J G', 'Faccini, R', 'MacFarlane, D B', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Campagnari, C', 'Dahmes, B', 'Hart, P A', 'Kuznetsova, N P', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Turri, M', 'Williams, D C', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoredsky, A P', 'Hitlin, D G', 'Kolomensky, Yu G', 'Metzler, S', 'Oyang, J Y T', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Aleksan, R', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Hamel de Monchenault, G', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S M', 'Jayatilleke, S M', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Wilson, R J', 'Zhang, J', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J D', 'Sen, S', 'Smith, J G', 'Wagner, D L', 'Brandt, T', 'Brose, J', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Kocian, M L', 'Müller-Pfefferkorn, R', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Roussot, E', 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di Lodovico, F', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E A', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Fabbricatore, P', 'Farinon, S', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Musenich, R', 'Parodi, R', 'Passaggio, S', 'Pastore, F', 'Patrignani, C', 'Pia, M G', 'Priano, C', 'Robutti, E', 'Santroni, A', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'Meyer, W T', 'Rosenberg, E I', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Morganti, M', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Benkebil, M', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', 'Shi, X', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'McMahon, S', 'McMahon, T R', 'Payne, D J', 'Touramanis, C', 'Aspinwall, M L', 'Dauncey, P D', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R D', 'Nash, J A', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Vidal, P B', 'Williams, M I', 'Cowan, G D', 'Green, M G', 'Kurup, A', 'McGrath, P', 'Scott, I', 'Brown, D', 'Davis, C L', 'Li, Y', 'Pavlovich, J', 'Trunov, A G', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Fullwood, J', 'Khan, A', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Thompson, R J', 'Weatherall, J H', 'Dallapiccola, C', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Brau, B', 'Cowan, R', 'Taylor, F', 'Yamamoto, R K', 'Blaylock, G', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R R', 'Lin, C S', 'Willocq, S', 'Wittlin, J', 'Bloom, P', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Kroeger, R A', 'Reidy, J', 'Sanders, D', 'Summers, D J', 'Arguin, J F', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Woch, A', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cavallo, N', 'De Nardo, G', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Piccolo, D', 'Sciacca, C', 'Falbo, M', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Colecchia, F', 'Dal Corso, F', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Hamon, O', 'Le Diberder, F', 'Leruste, P J', 'Lory, J', 'Martínez-Vidal, F', 'Roos, L', 'Stark, J', 'Versille, S', 'Manfredi, P F', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Kelsey, M H', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Cavoto, G', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M S', 'Plano, R J', 'Adye, T', 'Egede, U', 'Franek, B J', 'Geddes, N I', 'Gopal, Gian P', 'Copty, N K', 'Purohit, M V', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Anulli, F', 'Aston, D', 'Baird, K', 'Bloom, Elliott D', 'Boyarski, A M', 'Bulos, F', 'Calderini, G', 'Convery, M R', 'Coupal, D P', 'Coward, D H', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Hewett, J L', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kim, P', 'Langenegger, U', 'Leith, D W G S', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'Manzin, G', 'Marsiske, H', 'Menke, S', 'Messner, R', 'Moffeit, K C', 'Morii, M', 'Mount, R', 'Müller, D R', ""O'Grady, C P"", 'Paolucci, P', 'Petrak, S', 'Quinn, Helen R', 'Ratcliff, B N', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Sciolla, G', 'Serbo, V V', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'Wisniewski, W J', 'Young, C C', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'De Silva, A', 'Henderson, R', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Prest, M', 'Vallazza, E', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'Jackson, P D', 'Kowalewski, R V', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Johnson, J R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Walsh, J', 'Wu, S L', 'Yu, Z', 'Zobernig, H G']",['Exclusive B decays to charmonium final states'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B0, branching ratio', 'B+, branching ratio', 'quarkonium, charm', 'J/psi(3100), leptonic decay', 'psi(3685), leptonic decay', 'chi/c1(3510), radiative decay', 'B, mass', 'mass difference, (B0 B+)', 'helicity, amplitude analysis', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> J/psi(3100) K', 'B --> J/psi(3100) K*(892)', 'B --> psi(3685) K', 'B+ --> chi/c1(3510) K+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008050'],"['We report on exclusive decays of B mesons into final states containing charmonium using data collected with the BABAR detector at the PEP-II storage rings. The charmonium states considered here are J/psi, psi(2S), and chi_C1. Branching fractions for several exclusive final states, a measurement of the decay amplitudes for the B0 --> J/psi K* decay, and measurements of the B0 and B+ masses are presented. All of the results we present here are preliminary.']",['2000-08-24']
669,['eng'],"['Aubert, Bernard', 'Boucham, A', 'Boutigny, D', 'De Bonis, I', 'Favier, J', 'Gaillard, Jean-Marc', 'Galeazzi, F', 'Jérémie, A', 'Karyotakis, Yu', 'Lees, J P', 'Robbe, P', 'Tisserand, V', 'Zachariadou, K', 'Palano, A', 'Chen, G P', 'Chen Jia Chao', 'Qi, N D', 'Rong, G', 'Wang, P', 'Zhu, Y S', 'Eigen, G', 'Reinertsen, P L', 'Stugu, B', 'Abbott, B', 'Abrams, G S', 'Borgland, A W', 'Breon, A B', 'Brown, D N', 'Button-Shafer, J', 'Cahn, R N', 'Clark, A R', 'Fan, Q', 'Gill, M S', 'Gowdy, S J', 'Groysman, Y', 'Jacobsen, R G', 'Kadel, R W', 'Kadyk, J A', 'Kerth, L T', 'Kluth, S', 'Kral, J F', 'Leclerc, C', 'Levi, M E', 'Liu, T', 'Lynch, G', 'Meyer, A B', 'Momayezi, M', 'Oddone, P J', 'Perazzo, A', 'Pripstein, M', 'Roe, N A', 'Romosan, A', 'Ronan, M T', 'Shelkov, V G', 'Strother, P', 'Telnov, A V', 'Wenzel, W A', 'Champion, T J', 'Hawkes, C M', 'Kirk, A', ""O'Neale, S W"", 'Watson, A T', 'Watson, N K', 'Koch, H', 'Krug, J', 'Kunze, M', 'Lewandowski, B', 'Peters, K', 'Schmücker, H', 'Steinke, M', 'Andress, J C', 'Chevalier, N', 'Clark, P J', 'Cottingham, N', 'De Groot, N', 'Dyce, N', 'Foster, B', 'Mass, A', 'McFall, J D', 'Wallom, D', 'Wilson, F F', 'Abe, K', 'Hearty, C', 'Mattison, T S', 'McKenna, J A', 'Thiessen, D', 'Camanzi, B', 'McKemey, A K', 'Tinslay, J', 'Blinov, V E', 'Bukin, A D', 'Bukin, D A', 'Buzykaev, A R', 'Dubrovin, M S', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Kravchenko, E A', 'Onuchin, A P', 'Salnikov, A A', 'Serednyakov, S I', 'Skovpen, Yu I', 'Yushkov, A N', 'Lankford, A J', 'Mandelkern, M A', 'Stoker, D P', 'Ahsan, A', 'Arisaka, K', 'Buchanan, C D', 'Chun, S', 'Branson, J G', 'Faccini, R', 'MacFarlane, D B', 'Rahatlou, S', 'Raven, G', 'Sharma, V', 'Campagnari, C', 'Dahmes, B', 'Hart, P A', 'Kuznetsova, N P', 'Levy, S L', 'Long, O', 'Lu, A', 'Richman, J D', 'Verkerke, W', 'Witherell, M', 'Yellin, S', 'Beringer, J', 'Dorfan, D E', 'Eisner, A M', 'Frey, A', 'Grillo, A A', 'Grothe, M', 'Heusch, C A', 'Johnson, R P', 'Kröger, W', 'Lockman, W S', 'Pulliam, T', 'Sadrozinski, H F W', 'Schalk, T L', 'Schmitz, R E', 'Schumm, B A', 'Seiden, A', 'Turri, M', 'Williams, D C', 'Chen, E', 'Dubois-Felsmann, G P', 'Dvoredsky, A P', 'Hitlin, D G', 'Kolomensky, Yu G', 'Metzler, S', 'Oyang, J Y T', 'Porter, F C', 'Ryd, A', 'Samuel, A', 'Weaver, M', 'Yang, S', 'Zhu, R Y', 'Aleksan, R', 'De Domenico, G', 'de Lesquen, A', 'Emery, S', 'Gaidot, A', 'Ganzhur, S F', 'Hamel de Monchenault, G', 'Hamel de Monchenault, G', 'Kozanecki, Witold', 'Langer, M', 'London, G W', 'Mayer, B', 'Serfass, B', 'Vasseur, G', 'Yéche, C', 'Zito, M', 'Devmal, S C', 'Geld, T L', 'Jayatilleke, S M', 'Jayatilleke, S M', 'Mancinelli, G', 'Meadows, B T', 'Sokoloff, M D', 'Blouw, J', 'Harton, J L', 'Krishnamurthy, M', 'Soffer, A', 'Toki, W H', 'Wilson, R J', 'Zhang, J', 'Fahey, S', 'Ford, W T', 'Gaede, F', 'Johnson, D R', 'Michael, A K', 'Nauenberg, U', 'Olivas, A', 'Park, H', 'Rankin, P', 'Roy, J D', 'Sen, S', 'Smith, J G', 'Wagner, D L', 'Brandt, T', 'Brose, J', 'Dahlinger, G', 'Dickopp, M', 'Dubitzky, R S', 'Kocian, M L', 'Müller-Pfefferkorn, R', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Wilden, L', 'Behr, L', 'Bernard, D', 'Bonneaud, G R', 'Brochard, F', 'Cohen-Tanugi, J', 'Ferrag, S', 'Roussot, E', 'Thiebaux, C', 'Vasileiadis, G', 'Verderi, M', 'Anjomshoaa, A', 'Bernet, R', 'Di Lodovico, F', 'Muheim, F', 'Playfer, S', 'Swain, J E', 'Bozzi, C', 'Dittongo, S', 'Folegani, M', 'Piemontese, L', 'Treadwell, E A', 'Baldini-Ferroli, R', 'Calcaterra, A', 'De Sangro, R', 'Falciai, D', 'Finocchiaro, G', 'Patteri, P', 'Peruzzi, I M', 'Piccolo, M', 'Zallo, A', 'Bagnasco, S', 'Buzzo, A', 'Contri, R', 'Crosetti, G', 'Fabbricatore, P', 'Farinon, S', 'Lo Vetere, M', 'Macri, M', 'Monge, M R', 'Musenich, R', 'Parodi, R', 'Passaggio, S', 'Pastore, F', 'Patrignani, C', 'Pia, M G', 'Priano, C', 'Robutti, E', 'Santroni, A', 'Cochran, J', 'Crawley, H B', 'Fischer, P A', 'Lamsa, J', 'Meyer, W T', 'Rosenberg, E I', 'Bartoldus, R', 'Dignan, T', 'Hamilton, R', 'Mallik, U', 'Angelini, C', 'Batignani, G', 'Bettarini, S', 'Bondioli, M', 'Carpinelli, M', 'Forti, F', 'Giorgi, M A', 'Lusiani, A', 'Morganti, M', 'Paoloni, E', 'Rama, M', 'Rizzo, G', 'Sandrelli, F', 'Simi, G', 'Triggiani, G', 'Benkebil, M', 'Grosdidier, G', 'Hast, C', 'Höcker, A', 'Le Peltier, V', 'Lutz, A M', 'Plaszczynski, S', 'Schune, M H', 'Trincaz-Duvoid, S', 'Valassi, A', 'Wormser, G', 'Bionta, R M', 'Brigljevic, V', 'Fackler, O', 'Fujino, D', 'Lange, D J', 'Mugge, M', 'Shi, X', 'Wenaus, T J', 'Wright, D M', 'Wuest, C R', 'Carroll, M', 'Fry, J R', 'Gabathuler, Erwin', 'Gamet, R', 'George, M', 'Kay, M', 'McMahon, S', 'McMahon, T R', 'Payne, D J', 'Touramanis, C', 'Aspinwall, M L', 'Dauncey, P D', 'Eschrich, I', 'Gunawardane, N J W', 'Martin, R D', 'Nash, J A', 'Sanders, P', 'Smith, D', 'Azzopardi, D E', 'Back, J J', 'Dixon, P', 'Harrison, P F', 'Vidal, P B', 'Williams, M I', 'Cowan, G D', 'Green, M G', 'Kurup, A', 'McGrath, P', 'Scott, I', 'Brown, D', 'Davis, C L', 'Li, Y', 'Pavlovich, J', 'Trunov, A G', 'Allison, J', 'Barlow, R J', 'Boyd, J T', 'Fullwood, J', 'Khan, A', 'Lafferty, G D', 'Savvas, N', 'Simopoulos, E T', 'Thompson, R J', 'Weatherall, J H', 'Dallapiccola, C', 'Farbin, A', 'Jawahery, A', 'Lillard, V', 'Olsen, J', 'Roberts, D A', 'Brau, B', 'Cowan, R', 'Taylor, F', 'Yamamoto, R K', 'Blaylock, G', 'Flood, K T', 'Hertzbach, S S', 'Kofler, R R', 'Lin, C S', 'Willocq, S', 'Wittlin, J', 'Bloom, P', 'Britton, D I', 'Milek, M', 'Patel, P M', 'Trischuk, J', 'Lanni, F', 'Palombo, F', 'Bauer, J M', 'Booke, M', 'Cremaldi, L', 'Kroeger, R A', 'Reidy, J', 'Sanders, D', 'Summers, D J', 'Arguin, J F', 'Martin, J P', 'Nief, J Y', 'Seitz, R', 'Taras, P', 'Woch, A', 'Zacek, V', 'Nicholson, H', 'Sutton, C S', 'Cavallo, N', 'De Nardo, G', 'Fabozzi, F', 'Gatto, C', 'Lista, L', 'Piccolo, D', 'Sciacca, C', 'Falbo, M', 'LoSecco, J M', 'Alsmiller, J R G', 'Gabriel, T A', 'Handler, T', 'Colecchia, F', 'Dal Corso, F', 'Michelon, G', 'Morandin, M', 'Posocco, M', 'Stroili, R', 'Torassa, E', 'Voci, C', 'Benayoun, M', 'Briand, H', 'Chauveau, J', 'David, P', 'La Vaissière, C de', 'Del Buono, L', 'Hamon, O', 'Le Diberder, F', 'Leruste, P J', 'Lory, J', 'Martínez-Vidal, F', 'Roos, L', 'Stark, J', 'Versille, S', 'Manfredi, P F', 'Re, V', 'Speziali, V', 'Frank, E D', 'Gladney, L', 'Guo, Q H', 'Panetta, J H', 'Haire, M J', 'Judd, D', 'Paick, K', 'Turnbull, L', 'Wagoner, D E', 'Albert, J', 'Bula, C', 'Kelsey, M H', 'Lu, C', 'McDonald, K T', 'Miftakov, V', 'Schaffner, S F', 'Smith, A J S', 'Tumanov, A', 'Varnes, E W', 'Cavoto, G', 'Ferrarotto, F', 'Ferroni, F', 'Fratini, K', 'Lamanna, E', 'Leonardi, E', 'Mazzoni, M A', 'Morganti, S', 'Piredda, G', 'Safai-Tehrani, F', 'Serra, M', 'Waldi, R', 'Jacques, P F', 'Kalelkar, M S', 'Plano, R J', 'Adye, T', 'Egede, U', 'Franek, B J', 'Geddes, N I', 'Gopal, Gian P', 'Copty, N K', 'Purohit, M V', 'Yumiceva, F X', 'Adam, I', 'Anthony, P L', 'Anulli, F', 'Aston, D', 'Baird, K', 'Bloom, Elliott D', 'Boyarski, A M', 'Bulos, F', 'Calderini, G', 'Convery, M R', 'Coupal, D P', 'Coward, D H', 'Dorfan, J', 'Doser, M', 'Dunwoodie, W M', 'Glanzman, T', 'Godfrey, G L', 'Grosso, P', 'Hewett, J L', 'Himel, Thomas M', 'Huffer, M E', 'Innes, W R', 'Jessop, C P', 'Kim, P', 'Langenegger, U', 'Leith, D W G S', 'Luitz, S', 'Lüth, V', 'Lynch, H L', 'Manzin, G', 'Marsiske, H', 'Menke, S', 'Messner, R', 'Moffeit, K C', 'Morii, M', 'Mount, R', 'Müller, D R', ""O'Grady, C P"", 'Paolucci, P', 'Petrak, S', 'Quinn, Helen R', 'Ratcliff, B N', 'Robertson, S H', 'Rochester, L S', 'Roodman, A', 'Schietinger, T', 'Schindler, R H', 'Schwiening, J', 'Sciolla, G', 'Serbo, V V', 'Snyder, A', 'Soha, A', 'Spanier, S M', 'Stahl, A', 'Su, D', 'Sullivan, M K', 'Talby, M', 'Tanaka, H A', 'Vavra, J', 'Wagner, S R', 'Weinstein, A J', 'Wisniewski, W J', 'Young, C C', 'Burchat, P R', 'Cheng, C H', 'Kirkby, D', 'Meyer, T I', 'Roat, C', 'De Silva, A', 'Henderson, R', 'Bugg, W', 'Cohn, H', 'Hart, E', 'Weidemann, A W', 'Benninger, T', 'Izen, J M', 'Kitayama, I', 'Lou, X C', 'Turcotte, M', 'Bianchi, F', 'Bóna, M', 'Di Girolamo, B', 'Gamba, D', 'Smol, A V', 'Zanin, D', 'Bosisio, L', 'Della Ricca, G', 'Lanceri, L', 'Pompili, A', 'Poropat, P', 'Prest, M', 'Vallazza, E', 'Vuagnin, G', 'Panvini, R S', 'Brown, C M', 'Jackson, P D', 'Kowalewski, R V', 'Roney, J M', 'Band, H R', 'Charles, E', 'Dasu, S', 'Elmer, P', 'Johnson, J R', 'Nielsen, J', 'Orejudos, W', 'Pan, Y', 'Prepost, R', 'Scott, I J', 'Walsh, J', 'Wu, S L', 'Yu, Z', 'Zobernig, H G']",['Measurement of inclusive production of charmonium states in B meson decays'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'quarkonium, charm', 'J/psi(3100), leptonic decay', 'psi(3685), hadronic decay', 'chi/c1(3510), radiative decay', 'chi/c2(3555), radiative decay', 'B, branching ratio', 'mass spectrum', 'magnetic detector, BaBar', 'experimental results', 'SLAC PEP Stor', 'B --> quarkonium anything', 'psi mesons --> lepton+ lepton-', 'psi(3685) --> J/psi(3100) pi+ pi-', 'chi mesons --> J/psi(3100) photon', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008049'],"['We reconstruct the charmonium mesons J/psi, psi(2S) and chi_C1 using a sample of 8.46 x 10^6 B-anti-B events collected by the BABAR detector operating at e^+e^- center of mass energies near the Y(4S) resonance. By measuring rates relative to the branching fraction of the J/psi, we obtain preliminary inclusive B branching fractions of (0.25+/-0.02+/-0.02)% to the psi(2S) and (0.39+/-0.04+/-0.04)% to the chi_C1, and set a 90% confidence level limit of 0.24% on decays through the chi_C2.']",['2000-08-24']
670,['eng'],"['Ishida, T']",['The First Results of K2K long-baseline Neutrino Oscillation Experiment'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'neutrino, oscillation', 'neutrino/mu, beam', 'neutrino/tau, search for', 'deep underground detector, KAMIOKANDE', 'experimental results', 'KEK PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008047'],['The first results of the K2K(KEK to Kamioka) long-baseline neutrino oscillation experiment are presented in this talk. In 1999 7.2x10^18 protons on target were delivered to the experiment. During this period of running there were 3 events fully contained in the Super-Kamiokande inner detector fiducial area which occurred during the beam spill timing window. In the case of no oscillations the expected number of events during this period was 12.3+1.7-1.9. The near detectors located at KEK also have begun detailed measurements of neutrino interactions in water at around 1 GeV.'],['2000-08-24']
671,['eng'],"['Mikaelyan, L A']",['Future Reactor Neutrino Oscillation Experiments at Krasnoyarsk'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'fission, particle source', 'antineutrino nucleon, interaction', 'antineutrino/e', 'charged current', 'correlation, (n positron)', 'scintillation counter, liquid', 'calibration']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008046'],"['Recent studies of atmospheric neutrinos and the results from CHOOZ and Palo-Verde experiment call for new and more sensitive searches for neutrino oscillations at reactors. The main goal of the project considered here is to look for very small mixing angle oscillations of electron neutrinos in the atmospheric neutrino mass parameter region around \\Delta m^2 ~3 10^-3 eV^2 and to define the element U_{e3} of the neutrino mixing matrix (U_{e3}is the contribution of the mass-3 state to the electron neutrino flavor state). The practical goal of the project is to decrease, relative to the CHOOZ, the statistic and systematic errors as much as possible. To achieve this we plan to use two identical antineutrino detectors each with a ~50-ton liquid scintillator target located at ~1100 m and ~250 m from the underground reactor (~600 mwe). Much attention is given to the detector calibration and monitoring procedures. As a first step we consider two much smaller pilot detectors each of ~ a 3 ton target mass stationed at ~20 m and 35-60 m from the reactor. The goals of this first stage are: (i) to accumulate necessary experience and (ii) to investigate with electron neutrinos the LSND mass parameter region.']",['2000-08-24']
672,['eng'],"['Alavi-Harati, A', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barker, A R', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hanagaki, K', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jensen, D A', 'Kessler, R S', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian R"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Qiao, C', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S R', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Suzuki, I', 'Swallow, E C', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['Study of the $K^{0}_{L} \\to \\pi^{+}\\pi^{-}\\gamma$ Direct Emission Vertex'],['Particle Physics - Experimental Results'],"['K0(L), secondary beam', 'K0(L), radiative decay', 'K0(L), hadronic decay', 'K0(L), branching ratio', 'photon, direct production', 'bremsstrahlung, internal', 'decay, form factor', 'parametrization', 'rho(770), propagator', 'photon, energy spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi+ pi- photon', 'K0(L) --> pi+ pi-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008045'],"['We have perfomed studies of the KL to PI+PI-GAMMA Direct Emission (DE) and Inner Bremsstrahlung (IB) vertices, based on data collected by KTeV during the 1996 Fermilab fixed target run. We find a1/a2 = -0.737 +- 0.034 GeV^2 for the DE form-factor parameter in the rho-propagator parametrization, and report on fits of the form-factor to linear and quadratic functions as well. We concurrently measure B.R.(KL to PI+PI-GAMMA, E_gamma >20 MeV)/(KL to PI+PI-) = (20.8 +- 0.3)*10^-3, and a KL to PI+PI-GAMMA DE/(DE + IB) branching ratio of 0.683 +- 0.011.']",['2000-08-23']
673,['eng'],"['Scholberg, K']",['Supernova Neutrino Detection'],['Particle Physics - Experimental Results'],"['talk, Sudbury 2000/06/16', 'neutrino, astrophysics', 'supernova', 'neutrino, counters and detectors', 'scintillation counter', 'Cherenkov counter, deuterium', 'neutrino nucleon, interaction', 'charged current', 'particle identification']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008044'],"['World-wide, several detectors currently running or nearing completion are sensitive to a core collapse supernova neutrino signal in the Galaxy. I will briefly describe the nature of the neutrino signal and then survey current and future detection techniques. I will also explore what physics and astrophysics we can learn from the next Galactic core collapse.']",['2000-08-23']
674,['eng'],"['Andreev, V P', 'Belousov, A S', 'Fomenko, A M', 'Gorbov, L A', 'Greenshaw, T', 'Levonian, S V', 'Malinovskii, E I', 'Maxfield, S J', 'Shevyakov, I', 'Smirnov, P A', 'Soloviev, Yu V', 'Winter, G G']",['A New High Energy Photon Tagger for the H1 - Detector at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'luminosity', 'exchange, one-photon', 'photon, energy', 'calorimeter, performance', 'radiation, damage', 'optics, absorption', 'calibration', 'charged particle, multiplicity', 'energy dependence', 'magnetic detector, H1', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008042'],"['The H1 detector at HERA has been upgraded by the addition of a new electromagnetic calorimeter. This is installed in the HERA tunnel close to the electron beam line at a position 8m from the interaction point in the electron beam direction. The new calorimeter extends the acceptance for tagged photoproduction events to the high y range, 0.85 < y < 0.95, and thus significantly improves the capability of H1 to study high energy gamma-p processes. The calorimeter design, performance and first results obtained during the 1996-1999 HERA running are described.']",['2000-08-23']
675,['eng'],"['Gary, J W']",['Jet Structure Studies at LEP and HERA'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'positron p, colliding beams', 'jet, electroproduction', 'positron, photoproduction', 'leading particle', 'quark, jet', 'gluon, jet', 'quantum chromodynamics', 'perturbation theory, higher-order', 'hadron, multiplicity', 'jet, pair production', 'quark, heavy', 'experimental results', 'CERN LEP Stor', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008041'],"['A summary of some recent studies in jet physics is given. Topics include leading particle production in light flavor events in e+e- annihilations, an analytical treatment of gluon and quark jets at the next-to-next-to-next-to-leading order (3NLO), and various studies performed at LEP and HERA involving separated gluon and quark jets.']",['2000-08-22']
676,['eng'],"['Ramm, C A']","['Unexplained Structure in $(\\mu,\\pi)$ Invariant Mass Distributions']",['Particle Physics - Experimental Results'],"['review', 'mass spectrum, (pi muon)', 'neutrino nucleon, inclusive reaction', 'antineutrino nucleon, inclusive reaction', 'neutrino/mu', 'charged current', 'pi, neutrinoproduction', 'K, decay', 'mass enhancement, (429)', 'bubble chamber, experimental results', 'spark chamber, experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008040'],"['Structures in invariant mass distributions from (mu,pi) combinations in the range 0.380<mupi<0.470 GeV from neutrino and kaon experiments are presented in comparable formats. No artifacts have been found to account for any part of the structure. Hypotheses that the similarities are due to recurrent statistical fluctuations are beyond credibility. My conclusion is that the similarities are overwhelming evidence that the structure is of an unexplained physical origin. It includes an enhancement which would accord with the decay of a narrow (mu,pi) state of mass 0.429 GeV. The purpose of this report is to request and enable every experimenter with precise mupi distributions to investigate their degree of correspondence with these analyses.']",['2000-08-22']
677,['eng'],"['Tokumoto, S', 'Chin, Y H', 'Mizuno, H', 'Ohya, K', 'Yamaguchi, S', 'Kazakov, J S', 'Loewen, R R', 'Fowkes, R', 'Menegat, A', 'Vlieks, A E']",['High Power Testing Results of the X-Band Mixed-Mode RF Windows for Linear Colliders'],['Particle Physics - Experimental Results'],"['talk, Monterey 2000/08/21', 'electron positron, linear collider', 'linear collider, proposed', 'RF system, power supply', 'ceramics']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008039', 'http://www.slac.stanford.edu/econf/C000821/THA02.shtml']","['In this paper, we summarize the high power testing results of the X-band mixed-mode RF windows at KEK and SLAC for linear colliders. The main feature of these windows is that the combination of modes on the surface of the ceramic significantly decreases the electric and magnetic fields in the junction between the ceramic and the metal. So far two types of high power windows (with the diameter of 53 mm and 64 mm) have been fabricated. A high power model of the smaller type window was fabricated and tested in a resonant ring at KEK. A maximum circulating power of 81 MW with 300 ns duration or 66 MW with 700 ns duration was achieved. Light emission was observed for a power level of over 10 MW. Later, both windows were shipped to SLAC for even higher power testing using combined power from two klystrons. The first window (53 mm diameter) achieved a transmitted power of 80 MW with 1.5 microsec duration at 30 Hz repetition. It was not destroyed during the testing. The testing of the second window was carried out next to the small type and achieved 62 MW with 1.5 maicrosec duration with 10 Hz repetition. The final results of both windows are presented in this report.']",['2000-08-22']
678,['eng'],"['Airapetian, A', 'Akopov, N Z', 'Akushevich, I V', 'Amarian, M', 'Arrington, J', 'Aschenauer, E C', 'Avakian, H', 'Avakian, R', 'Avetisian, A', 'Avetissian, E', 'Bailey, P', 'Bains, B', 'Baumgarten, C', 'Beckmann, M', 'Belostotskii, S', 'Bernreuther, S', 'Bianchi, N', 'Böttcher, H', 'Borisov, A', 'Bouwhuis, M', 'Brack, J', 'Brauksiepe, S', 'Brauniu, B', 'Brückner, W', 'Brüll, A', 'Budz, P', 'Bulten, H J', 'Capitani, G P', 'Carter, P', 'Chumney, P', 'Cisbani, E', 'Court, G R', 'Dalpiaz, P F', 'De Leo, R', 'De Nardo, L', 'De Sanctis, E', 'De Schepper, D', 'Devitsin, E G', 'De Witt-Huberts, P K A', 'Di Nezza, P', 'Dzhordzhadze, V', 'Düren, M', 'Dvoredsky, A P', 'Elbakian, G M', 'Ely, J', 'Fantoni, A', 'Feshchenko, A', 'Ferro-Luzziwad, M', 'Fiedler, K', 'Filippone, B W', 'Fischer, H', 'Fox, B', 'Franzl, J', 'Frullani, S', 'Gärber, Y', 'Garibaldi, F', 'Garutti, E', 'Gavrilov, G E', 'Karibian, V', 'Golendukhin, A', 'Graw, G', 'Grebenyuk, O', 'Green, P W', 'Greeniaus, L G', 'Gute, A', 'Haeberli, W', 'Hartig, M', 'Hasch, D', 'Heesbeen, D', 'Heinsius, F H', 'Henoch, M', 'Hertenberger, R', 'Hesselink, W H A', 'Hoffmann-Rothe, P', 'Hofman, G J', 'Holler, Y', 'Holto, R J', 'Hommez, B', 'Iarygin, G', 'Iodice, M', 'Izotov, A A', 'Jackson, H E', 'Jgoun, A', 'Jung, P', 'Kaiser, R', 'Kanesakaac, J', 'Kinney, E R', 'Kiselev, A', 'Kitching, P', 'Kobayashi, H', 'Koch, N', 'Königsmann, Kay C', 'Kolster, H', 'Korotkov, V A', 'Kotik, E', 'Kozlov, V', 'Krivokhizhin, V G', 'Kyle, G S', 'Lagamba, L', 'Laziev, A', 'Lenisa, P', 'Lindemann, T', 'Lorenzon, W', 'Makins, N C R', 'Martin, J W', 'Marukyan, H O', 'Masolij, F', 'McAndrew, M', 'McIlhany, K', 'McKeown, R D', 'Menden, F', 'Metzu, A', 'Meyners, N', 'Miklukho, O', 'Miller, C A', 'Milner, R', 'Mitsyn, V', 'Muccifora, V', 'Mussa, R', 'Nagaitsev, A P', 'Nappi, E', 'Naryshkin, Yu', 'Nass, A', 'Negodaevag, K', 'Nowak, W D', ""O'Neill, T G"", 'Openshaw, R', 'Ouyang, J', 'Owen, B R', 'Pate, S F', 'Potashov, S Yu', 'Potterveld, D H', 'Rakness, G', 'Rappoport, V', 'Redwine, R P', 'Reggiani, D', 'Reolon, A R', 'Ristinen, R', 'Rith, K', 'Robinson, D', 'Ruh, M', 'Ryckbosch, D', 'Sakemi, Y', 'Savin, I A', 'Scarlett, C', 'Schäfer, A', 'Schill, C', 'Schmidt, F', 'Schnell, G', 'Schulerf, K P', 'Schwind, A', 'Seibert, J', 'Seitz, B', 'Shibata, T A', 'Shin, T', 'Shutov, V', 'Simani, C', 'Simon, A', 'Sinram, K', 'Steffens, E', 'Steijger, J J M', 'Stewart, J', 'Stösslein, U', 'Suetsugu, K', 'Sutter, M F', 'Tallini, H A', 'Taroiana, S P', 'Terkulov, A R', 'Tessarin, S', 'Thomas, E', 'Tipton, B', 'Tytgat, M', 'Urciuoli, G M', 'Van den Brand, J F J', 'van der Steenhoven, G', 'Van de Vyver, R', 'Van Hunen, J J', 'Vetterli, M C', 'Vikhrov, V V', 'Vincter, M G', 'Visser, J', 'Volk, E', 'Weiskopf, C', 'Wendland, J', 'Wilbert, J', 'Wiseq, T', 'Yen, S', 'Yoneyama, S', 'Zohrabyan, H G']",['The $Q^{2}$-dependence of the Generalised Gerasimov-Drell-Hearn Integral for the Proton'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron, polarized beam', 'p, polarized target', 'polarization, longitudinal', 'cross section, spin', 'sum rule, Drell-Hearn-Gerasimov', 'momentum transfer, dependence', 'nucleon resonance', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', '27.6 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008037'],"['The dependence on Q^2 (the negative square of the 4-momentum of the exchanged virtual photon) of the generalised Gerasimov-Drell-Hearn integral for the proton has been measured in the range 1.2 GeV^2 < Q^2 < 12 GeV^2 by scattering longitudinally polarised positrons on a longitudinally polarised hydrogen gas target. The contributions of the nucleon-resonance and deep-inelastic regions to this integral have been evaluated separately. The latter has been found to dominate for Q^2 > 3 GeV^2, while both contributions are important at low Q^2. The total integral shows no significant deviation from a 1/Q^2 behaviour in the measured Q^2 range, and thus no sign of large effects due to either nucleon-resonance excitations or non-leading twist.']",['2000-08-21']
679,['eng'],"['Ashery, D']",['Measurement of Light-Cone Wave Functions by Diffractive Dissociation'],['Particle Physics - Experimental Results'],"['talk, Heidelberg 2000/06/12', 'pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'diffraction, dissociation', 'jet, pair production', 'yield, (2jet)', 'wave function, light cone', 'pi, wave function', 'photon, wave function', 'color, transparency', 'dependence, mass number', 'experimental results', 'Batavia TEVATRON PS', '500 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008036'],['Diffractive dissociation of particles can be used to study their light-cone wave function. Results from Fermilab experiment E791 for diffractive dissociation of 500 GeV/c $\\pi^-$ mesons into di-jets are presented. The results show that the $|q\\bar {q}>$ light-cone asymptotic wave function describes the data well for $Q^2 \\sim 10 ~{\\rm (GeV/c)^2}$ or more. Evidence for color transparency comes from a measurement of the $A$-dependence of the yield of the diffractive di-jets. It is proposed to carry out similar studies for the light-cone wave function of the photon.'],['2000-08-21']
680,['eng'],"['Higo, T', 'Funahashi, Y', 'Higashi, Y', 'Hitomi, N', 'Suzuki, T', 'Takata, K', 'Takatomi, T', 'Toge, N', 'Watanabe, Y', 'Li, Z', 'Miller, R H', 'Wang, J W']",['Meeting Tight Frequency Requirement of Rounded Damped Detuned Structure'],['Particle Physics - Experimental Results'],"['talk, Monterey 2000/08/21', 'electron positron, linear collider', 'linear collider, proposed', 'wake field', 'microwaves, absorption', 'vacuum system, impedance', 'vacuum system, fabrication']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008035', 'http://www.slac.stanford.edu/econf/C000821/TUA02.shtml']","['Following successful design and fabrication of damped detuned structures, the R&D for the accelerating structures of the NLC/JLC linear collider project proceeded to studies of Rounded Damped Detuned Structure with curved cross section of the cavity shape for increased shunt impedance. The important features of the structure are the accurately tuned accelerating mode frequency and the distribution of the first dipole modes smooth and close to the design distribution. These requirements were met based on the high-accuracy diamond turning with its capability to realize the periphery tolerance of two microns. The lowest dipole mode frequencies scattered by 0.6 MHz RMS. The error in the accelerating mode frequency averaged over a structure was 0.1 MHz by applying a feed-forward method.']",['2000-08-21']
681,['eng'],"['Hitomi, N', 'Funahashi, Y', 'Higashi, Y', 'Higo, T', 'Koike, S', 'Suzuki, T', 'Takata, K', 'Takatomi, T', 'Toge, T', 'Watanabe, Y']",['Fabrication Process of Rounded Damped Detuned Structure'],['Particle Physics - Experimental Results'],"['electron positron, linear collider', 'linear collider, proposed', 'wake field', 'microwaves, absorption', 'vacuum system, impedance', 'vacuum system, fabrication']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008034'],"['Following the successful design and fabrication of Damped Detuned Structures (DDS), the JLC/NLC linear collider project advanced to Rounded Damped Detuned Structures (RDDS) with curved cross section of the cavity shape for increased shunt impedance. Various advanced techniques for fabricating RDDS1 disks comparing to those for DDS were established to satisfy the dimension accuracy of +-1 micron over the entire surface made by ultra-precision turning. These disks were assembled with almost the same stacking and bonding jigs and processes as those of DDS3 assembly. In consequence, the assembly showed little disk-to-disk misalignment within 1 micron before and after the process. Though, it had 200 micron smooth bowing, which was subsequently corrected as DDS3, and flares at both ends.']",['2000-08-21']
682,['eng'],"['Naito, T', 'Ebihara, K', 'Hayano, H', 'Urakawa, J']",['Development of rf reference line for the linear collider'],['Particle Physics - Experimental Results'],"['talk, Monterey 2000/08/21', 'electron positron, linear collider', 'linear collider, proposed', 'RF system, control system', 'control system, time', 'optics, fibre']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008033', 'http://www.slac.stanford.edu/econf/C000821/THA04.shtml']","['The rf distribution system for the linear collider requires stable x-band(11.424GHz) rf phase signal over 25km length. In order to realize the distribution system, a fiber optic link using a phase stabilized optical fiber was tested. The phase stabilized optical fiber has been employed at LEP, KEKB, etc.. This paper describes the hardware system and result of the preliminary test of the feed back system for stabilization of the phase change.']",['2000-08-21']
683,['eng'],"['Bai, J Z', 'Ban, Y', 'Bian, J G', 'Blum, I K', 'Chen, A D', 'Chen, G P', 'Chen, H F', 'Chen, H S', 'Chen, J', 'Chen Jia Chao', 'Chen, X D', 'Chen, Y', 'Chen, Y B', 'Cheng, B S', 'Choi, J B', 'Cui, X Z', 'Ding, H L', 'Dong, L Y', 'Du, Z Z', 'Dunwoodie, W M', 'Gao, C S', 'Gao, M L', 'Gao, S Q', 'Gratton, P', 'Gu, J H', 'Gu, S D', 'Gu, W X', 'Guo, Y N', 'Guo, Z J', 'Han, S W', 'Han, Y', 'Harris, F A', 'He, J', 'He, J T', 'He, K L', 'He, M', 'Heng, Y K', 'Hitlin, D G', 'Hu, G Y', 'Hu, H M', 'Hu, J L', 'Hu, Q H', 'Hu, T', 'Huang, G S', 'Huang, X P', 'Huang, Y Z', 'Izen, J M', 'Jiang, C H', 'Jin, Y', 'Jones, B D', 'Ju, X', 'Kang, J S', 'Ke, Z J', 'Kelsey, M H', 'Kim, B K', 'Kim, H J', 'Kim, S K', 'Kim, T Y', 'Kong, D', 'Lai, Y F', 'Lang, P F', 'Lankford, A J', 'Li, C G', 'Li, D', 'Li, H B', 'Li, J', 'Li, J C', 'Li, P Q', 'Li, W', 'Li, W G', 'Li, X H', 'Li Xiao Nan', 'Li Xue Qian', 'Li Zhong Chao', 'Liu, B', 'Liu, F', 'Liu Feng', 'Liu, H M', 'Liu, J', 'Liu, J P', 'Liu, R G', 'Liu, Y', 'Liu, Z X', 'Lou, X C', 'Lowery, B', 'Lu, G R', 'Lu, F', 'Lu, J G', 'Luo, X L', 'Ma, E C', 'Ma, J M', 'Malchow, R L', 'Mao, H S', 'Mao, Z P', 'Meng, X C', 'Mo, X H', 'Nie, J', 'Olsen, S L', 'Oyang, J Y T', 'Paluselli, D', 'Pan, L J', 'Panetta, J', 'Park, H', 'Porter, F', 'Qi, N D', 'Qi, X R', 'Qian, C D', 'Qiu, J F', 'Qu, Y H', 'Que, Y K', 'Rong, G', 'Schernau, M', 'Shao, Y Y', 'Shen, B W', 'Shen, D L', 'Shen, H', 'Shen, H Y', 'Shen, X Y', 'Shi, F', 'Shi, H Z', 'Song, X F', 'Standifird, J', 'Suh, J Y', 'Sun, H S', 'Sun, L F', 'Sun, Y Z', 'Tang, S Q', 'Toki, W', 'Tong, G L', 'Varner, G S', 'Wang, F', 'Wang, L', 'Wang, L S', 'Wang, L Z', 'Wang, P', 'Wang, P L', 'Wang, S M', 'Wang, Y Y', 'Wang, Z Y', 'Weaver, M', 'Wei, C L', 'Wu, N', 'Wu, Y G', 'Xi, D M', 'Xia, X M', 'Xie, Y', 'Xie, Y H', 'Xu, G F', 'Xue, S T', 'Yan, J', 'Yan, W G', 'Yang, C M', 'Yang, C Y', 'Yang, H X', 'Yang, W', 'Yang, X F', 'Ye, M H', 'Ye Shu Wei', 'Ye, Y X', 'Yu, C S', 'Yu, C X', 'Yu, G W', 'Yu Yu Hei', 'Yu, Z Q', 'Yuan, C Z', 'Yuan, Y', 'Zhang Bing Yun', 'Zhang, C', 'Zhang, C C', 'Zhang, D H', 'De Hong Zhang', 'Zhang, H L', 'Zhang, J', 'Zhang, J W', 'Zhang, L', 'Zhang Lei', 'Zhang, L S', 'Zhang, P', 'Zhang, Q J', 'Zhang, S Q', 'Zhang, X Y', 'Zhang, Y Y', 'Zhao, D X', 'Zhao, H W', 'Jia Wei Zhao', 'Zhao Jia Wei', 'Zhao, M', 'Zhao Wei Ren', 'Zhao, Z G', 'Zheng Jian Ping', 'Zheng Lin Sheng', 'Zheng Zhi Peng', 'Zhou, B Q', 'Zhou, L', 'Zhu, K J', 'Zhu, Q M', 'Zhu, Y C', 'Zhu, Y S', 'Zhu, Z A', 'Zhuang, B A']",['Measurement of $\\psi(2S)$ decays to baryon pairs'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), hadronic decay', 'baryon, pair production', 'p', 'Lambda', 'Sigma', 'Delta(1232)', 'Xi(1530)', 'Omega-', 'psi(3685), branching ratio', 'symmetry, SU(3)', 'factorization', 'quantum chromodynamics, perturbation theory', 'mass spectrum', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> psi(3685)', 'psi(3685) --> baryon antibaryon', '3.685 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008031'],"['A sample of 3.95M $\\psi(2S)$ decays registered in the BES detector are used to study final states containing pairs of octet and decuplet baryons. We report branching fractions for $\\psi(2S)\\to p\\bar{p}$, $\\Lambda\\bar{\\Lambda}$, $\\Sigma^0\\bar{\\Sigma}{}^0$, $\\Xi^-\\bar{\\Xi}{}^+$, $\\Delta^{++}\\bar{\\Delta}{}^{--}$, $\\Sigma^+(1385)\\bar{\\Sigma}{}^-(1385 )$, $\\Xi^0(1530)\\bar{\\Xi}{}^0(1530)$, and $\\Omega^-\\bar{\\Omega}{}^+$. These results are compared to expectations based on the SU(3)-flavor symmetry, factorization, and perturbative QCD.']",['2000-08-21']
684,['eng'],"['Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Banerjee, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Copty, N K', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Devmal, S C', 'Fernández, A', 'Fox, G F', 'Gagnon, P', 'Göbel, C', 'Gounder, K', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lundberg, B', 'Magnin, J', 'May Tal-Beck, S', 'Meadows, B', 'De Mello-Neto, J R T', 'Mihalcea, D', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'de Oliveira, A', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Dos Reis, A C', 'Rubin, H A', 'Sanders, D A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Simão, F R A', 'Slaughter, A J', 'Sokoloff, M D', 'Solano, J M', 'Stanton, N R', 'Stefanski, R J', 'Stenson, K', 'Summers, D J', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yang, S M', 'Yi, D', 'Yoshida, S', 'Zaliznyak, R', 'Zhang, C']",['Asymmetries in the Production of $\\Lambda_{c}^{+}$ and $\\Lambda_{c}^{-}$ Baryons in 500 GeV/c $\\pi^{-}$ Nucleon Interactions'],['Particle Physics - Experimental Results'],"['pi- nucleon, interaction', 'Lambda/c+, hadroproduction', 'Lambda/c+, hadronic decay', 'charge, asymmetry', 'x-dependence', 'transverse momentum, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleon --> Lambda/c+ anything', 'Lambda/c+ --> p K- pi+', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008029'],"[""We present a measurement of asymmetries in the production of $\\Lambda_c^+$ and $\\Lambda_c^-$ baryons in 500 GeV/c $\\pi^-$--nucleon interactions from the E791 experiment at Fermilab. The asymmetries were measured as functions of Feynman x ($x_F$) and transverse momentum squared ($p_T^2$) using a sample of $1819 \\pm 62$ $\\Lambda_c$'s observed in the decay channel $\\Lambda_c \\to pK^-\\pi^+$. We observe more $\\Lambda_c^+$ than $\\Lambda_c^-$ baryons, with an asymmetry of $(12.7\\pm3.4\\pm1.3) %$ independent of $x_F$ and $p_T^2$ in our kinematical range $(-0.1 < x_F < 0.6$ and $0.0 < p_T^2 < 8.0 (GeV/c)^2$). This $\\Lambda_c$ asymmetry measurement is the first with data in both the positive and negative $x_F$ regions.""]",['2000-08-17']
685,['eng'],"['Hadig, T']",['Inclusive Hadron Production and Dijets at HERA'],['Particle Physics - Experimental Results'],"['talk, Providence 1999/08/09', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'jet, photoproduction', 'hadron, multiple production', 'jet, multiplicity', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'channel cross section, rapidity dependence', 'photon, structure function', 'gluon, momentum spectrum', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008028'],['This article summarizes a talk given at the International Symposium on Multiparticle Dynamics 1999 in Providence/USA. It provides an overview on the variety of measurements of the hadronic final state in jet production for deep-inelastic scattering and photoproduction at HERA.'],['2000-08-16']
686,['eng'],"['Hadig, T']",['The strong coupling and the gluon density from jets in DIS'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'electron p, deep inelastic scattering', 'jet, electroproduction', 'jet, pair production', 'quantum chromodynamics, perturbation theory', 'strong interaction, coupling constant', 'gluon, momentum spectrum', 'magnetic detector, ZEUS', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008027'],"['The extraction of the parameters of perturbative QCD is one of the main tasks for the HERA experiments. Studies on the structure of the hadronic final states with jet algorithms give a direct handle on the parton density functions and the strong coupling strength over a wide kinematic range. In this article, new results of the H1 and ZEUS collaborations for the strong coupling and the gluon density in the proton are presented.']",['2000-08-16']
687,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Boos, E E', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D K', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grudberg, P M', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Scully, J R', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Search for Electroweak Production of Single Top Quarks in $pbar{p}$ Collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, hadroproduction', 'quark, semileptonic decay', 'final state, ((n)jet lepton)', 'channel cross section, upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> truth beauty anything', 'anti-p p --> truth beauty quark anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008024'],"['We present a search for electroweak production of single top quarks in the electron+jets and muon+jets decay channels. The measurements use ~90 pb^-1 of data from Run 1 of the Fermilab Tevatron collider, collected at 1.8 TeV with the DZero detector between 1992 and 1995. We use events that include a tagging muon, implying the presence of a b jet, to set an upper limit at the 95% confidence level on the cross section for the s-channel process ppbar->tb+X of 39 pb. The upper limit for the t-channel process ppbar->tqb+X is 58 pb.']",['2000-08-16']
688,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Balm, P W', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Desai, S V', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Duensing, S', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D K', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Graham, G', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Groer, L S', 'Grudberg, P M', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hou, S', 'Huang, Y', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V E', 'Landsberg, G L', 'Leflat, A', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Moore, R W', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Peters, O', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Rapidis, P A', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Scully, J R', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Tripathi, S M', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Wijngaarden, D A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Cross Section for b Jet Production in $p\\overline{p}$ Collisions at $\\sqrt(s) = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'quark, beauty', 'quark, semileptonic decay', 'rapidity, central region', 'differential cross section, transverse energy', 'channel cross section, transverse momentum', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> beauty anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008021'],"['Bottom quark production in pbar-p collisions at sqrt(s)=1.8 TeV is studied with 5 inverse picobarns of data collected in 1995 by the DO detector at the Fermilab Tevatron Collider. The differential production cross section for b jets in the central rapidity region (|y(b)| < 1) as a function of jet transverse energy is extracted from a muon-tagged jet sample. Within experimental and theoretical uncertainties, DO results are found to be higher than, but compatible with, next-to-leading-order QCD predictions.']",['2000-08-15']
689,['eng'],"['Akhmetshin, R R', 'Anashkin, E V', 'Arpagaus, M', 'Aulchenko, V M', 'Banzarov, V S', 'Barkov, L M', 'Bashtovoy, N S', 'Bondar, A E', 'Bondarev, D V', 'Bragin, A V', 'Chernyak, D V', 'Eidelman, S I', 'Fedotovich, G V', 'Gabyshev, N I', 'Grebeniuk, A A', 'Grigoriev, D N', 'Hughes, V W', 'Ignatov, F V', 'Ivanov, P M', 'Karpov, S V', 'Kazanin, V F', 'Khazin, B I', 'Koop, I A', 'Korostelev, M S', 'Krokovnyi, P P', 'Kurdadze, L M', 'Kuzmin, A S', 'Logashenko, I B', 'Lukin, P A', 'Mikhailov, K Yu', 'Milshtein, A I', 'Nesterenko, I N', 'Okhapkin, V S', 'Otboev, A V', 'Perevedentsev, E A', 'Popov, A S', 'Purlatz, T A', 'Redin, S I', 'Root, N I', 'Ruban, A A', 'Ryskulov, N M', 'Shamov, A G', 'Shatunov, Yu M', 'Shwartz, B A', 'Sibidanov, A L', 'Sidorov, V A', 'Skrinsky, A N', 'Smakhtin, V P', 'Snopkov, I G', 'Solodov, E P', 'Stepanov, P Yu', 'Sukhanov, A Yu', 'Thompson, J A', 'Titov, V M', 'Valishev, A A', 'Yudin, Yu V', 'Zverev, S G']",['Observation of the $\\phi \\to \\pi^{+}pi^{-}pi^{+} \\pi^{-}$ Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), hadronic decay', 'pi, multiple production', 'cross section, energy dependence', 'Phi(1020), branching ratio', 'upper limit', 'Iizuka-Okubo-Zweig rule', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> 2pi+ 2pi-', 'Phi(1020) --> 2pi+ 2pi- pi0', 'Phi(1020) --> eta pi+ pi-', '0.984-1.060 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008019'],"['Using 11.6 pb^{-1} of data collected in the energy range 0.984--1.06 GeV by CMD-2 at VEPP-2M, the cross section of the reaction e+e- to pi+pi-pi+pi- has been studied. For the first time an interference pattern was observed in the energy dependence of the cross section near the phi meson. The branching ratio of the phi to pi+pi-pi+pi- decay double suppressed by the G-parity and OZI rule is measured Br(phi to pi+pi-pi+pi-) = (3.93 +- 1.74 +- 2.14) \\cdot 10^{-6} The upper limits have been placed for the decays phi to pi+pi-pi+pi-pi0 and phi to eta pi+pi- Br(phi to pi+pi-pi+pi-pi0) < 4.6 \\cdot 10^{-6} 90% CL Br(phi to eta pi+pi-) < 1.8 \\cdot 10^{-5} 90% CL']",['2000-08-15']
690,['eng'],"['Kalelkar, M S']",['Light Quark Fragmentation in Polarized Z0 Decays at SLD'],['Particle Physics - Experimental Results'],"['talk, Montpellier 2000/07/06', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, fragmentation', 'rapidity, correlation', 'quark, strangeness', 'coupling, (Z0 strangeness)', 'angular distribution, asymmetry', 'polarization, asymmetry', 'magnetic detector, SLD', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008032'],"['We report results on two physics topics from the SLD experiment at the SLAC Linear Collider, using our full sample of 550,000 events of the type e+e- --> Z0 --> q-q(bar). The electron beam was polarized, enabling the quark and antiquark hemispheres to be tagged in each event. One physics topic is the first study of rapidities signed such that positive rapidity is along the quark rather than antiquark direction. Distributions of ordered differences in signed rapidity between pairs of particles are analyzed, providing the first direct observation of baryon number ordering along the q-q(bar) axis. The other topic is the first direct measurement of A_s, the parity-violating coupling of the Z0 to strange quarks, by measuring the left-right forward-backward production asymmetry in polar angle of the tagged s-quark. We obtain A_s = 0.895 +- 0.066(stat.) +- 0.062(syst.), which is consistent with the Standard Model and is currently the most precise measurement of this quantity.']",['2000-08-21']
691,['eng'],"['Aggarwal, M M', 'Agnihotri, A', 'Ahammed, Z', 'Angelis, Aris L S', 'Antonenko, V G', 'Arefev, V', 'Astakhov, V A', 'Avdeichikov, V', 'Awes, T C', 'Baba, P V K S', 'Badyal, S K', 'Barlag, C', 'Bathe, S', 'Batyunya, B', 'Bernier, T', 'Bhalla, K B', 'Bhatia, V S', 'Blume, C', 'Bock, R', 'Bohne, E M', 'Böröcz, Z K', 'Bucher, D', 'Buijs, A', 'Büsching, H', 'Carlén, L', 'Chalyshev, V', 'Chattopadhyay, S', 'Cherbachev, R', 'Chujo, T', 'Claussen, A', 'Das, A C', 'Decowski, M P', 'Delagrange, H', 'Dzhordzhadze, V', 'Dönni, P', 'Dubovik, I', 'Dutt, S K', 'Dutta-Majumdar, M R', 'El-Chenawi, K F', 'Eliseev, S', 'Enosawa, K', 'Foka, P Y', 'Fokin, S', 'Ganti, M S', 'Garpman, S I A', 'Gavrishchuk, O P', 'Geurts, F J M', 'Ghosh, T K', 'Glasow, R', 'Sen-Gupta, S K', 'Guskov, B', 'Gustafsson, H Å', 'Gutbrod, H H', 'Higuchi, R', 'Hrivnacova, I', 'Ippolitov, M S', 'Kalechofsky, H', 'Kamermans, R', 'Kampert, K H', 'Karadzhev, K', 'Karpio, K', 'Kato, S', 'Kees, S', 'Klein-Bösing, C', 'Knoche, S', 'Kolb, B W', 'Kosarev, I', 'Kucheryaev, I', 'Krümpel, T', 'Kugler, A', 'Kulinich, P A', 'Kurata, M', 'Kurita, K', 'Kuzmin, N A', 'Langbein, I', 'Lebedev, A', 'Lee, Y Y', 'Löhner, H', 'Luquin, L', 'Mahapatra, D P', ""Man'ko, V I"", 'Martin, M', 'Martínez, G', 'Maksimov, A', 'Mgebrishvili, G', 'Miake, Y', 'Mir, M F', 'Mishra, G C', 'Miyamoto, Y', 'Mohanty, B', 'Mora, M J', 'Morrison, D', 'Mukhopadhyay, D S', 'Naef, H', 'Nandi, B K', 'Nayak, S K', 'Nayak, T K', 'Neumaier, S', 'Nyanin, A', 'Nikitin, V A', 'Nikolaev, S', 'Nilsson, P', 'Nishimura, S', 'Nomokonov, V P', 'Nystrand, J', 'Obenshain, F E', 'Oskarsson, A', 'Otterlund, I', 'Pachr, M', 'Pavlyuk, S', 'Peitzmann, T', 'Petracek, V', 'Pinganaud, W', 'Plasil, F', 'Von Poblotzki, U', 'Purschke, M L', 'Rak, J', 'Raniwala, R', 'Raniwala, S', 'Ramamurthy, V S', 'Rao, N K', 'Retière, F', 'Reygers, K', 'Roland, G', 'Rosselet, L', 'Rufanov, I A', 'Roy, C', 'Rubio, J M', 'Sako, H', 'Sambyal, S S', 'Santo, R', 'Sato, S', 'Schlagheck, H', 'Schmidt, H R', 'Schutz, Y', 'Shabratova, G', 'Shah, T H', 'Sibiryak, Yu', 'Siemiarczuk, T', 'Silvermyr, D', 'Sinha, B C', 'Slavin, N', 'Söderström, K', 'Solomey, N', 'Sørensen, S P', 'Stankus, P', 'Stefanek, G', 'Steinberg, P', 'Stenlund, E', 'Stüken, D', 'Sumbera, M', 'Svensson, T', 'Trivedi, M D', 'Tsvetkov, A A', 'Tykarski, L', 'Urbahn, J', 'Van den Pijll, E C', 'van Eijndhoven, N', 'van Nieuwenhuizen, G J', 'Vinogradov, A', 'Viyogi, Y P', 'Vodopyanov, A S', 'Vörös, S', 'Wyslouch, B', 'Yagi, K', 'Yokota, Y', 'Young, G R']",['Three-Pion Interferometry Results from Central Pb+Pb Collisions at 158 A GeV/c'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'lead', 'hadron, multiple production', 'correlation, (3pi-)', 'boson, statistics', 'correlation function, (2pi-)', 'magnetic spectrometer, experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008018'],['Three-particle correlations have been measured for identified negative pions from central 158 A GeV Pb+Pb collisions by the WA98 experiment at CERN. A substantial contribution of the genuine three-body correlation has been found as expected for a mainly chaotic and symmetric source.'],['2000-08-11']
692,['eng'],"['Schwarz, J H']",['Introduction to Superstring Theory'],['Particle Physics - Experimental Results'],"['lectures, St. Croix 2000/06/15', 'string model', 'supersymmetry', 'gauge field theory', 'particle, spectra', 'quantization', 'perturbation theory', 'space-time, higher-dimensional', 'boundary condition', 'gauge fixing', 'anomaly', 'duality, T-duality', 'membrane model', 'M-theory', 'vacuum state']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008017'],"['These four lectures, addressed to an audience of graduate students in experimental high energy physics, survey some of the basic concepts in string theory. The purpose is to convey a general sense of what string theory is and what it has achieved. Since the characteristic scale of string theory is expected to be close to the Planck scale, the structure of strings probably cannot be probed directly in accelerator experiments. The most accessible experimental implication of superstring theory is supersymmetry at or below the TeV scale.']",['2000-08-11']
693,['eng'],"['Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S A', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Nelson, H N', 'Richman, J D', 'Witherell, M S', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J']",['Measurements of $B \\to D_{s^{(*)+}} D^{*(*)}$ Branching Fractions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'charmed meson, pair production', 'charmed meson, excited state', 'D/s', 'D*(2010)', 'D*(2110)', 'D1(2420)', 'D*2(2460)', 'B0, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008015'],"['This article describes improved measurements by CLEO of the $B^0 \\to D_s^+ D^{*-}$ and $B^0 \\to D_s^{*+} D^{*-}$ branching fractions, and first evidence for the decay $B^+ \\to D_s^{(*)+} \\bar{D}^{**0}$, where $\\bar{D}^{**0}$ represents the sum of the $\\bar{D}_1(2420)^0$, $\\bar{D}_2^*(2460)^0 $, and $\\bar{D}_1(j=1/2)^0$ L=1 charm meson states. Also reported is the first measurement of the $D_s^{*+}$ polarization in the decay $B^0 \\to D_s^{*+} D^{*-}$. A partial reconstruction technique, employing only the fully reconstructed $D_s^+$ and slow pion $\\pi_s^-$ from the $D^{*-} \\to \\bar{D}^0 \\pi^-_s$ decay, enhances sensitivity. The observed branching fractions are $ {\\mathcal B} (B^0 \\to D_s^+ D^{*-}) = (1.10 \\pm 0.18 \\pm 0.10 \\pm 0.28)%$, $ {\\mathcal B} (B^0 \\to D_s^{*+} D^{*-}) = (1.82 \\pm 0.37 \\pm 0.24 \\pm 0.46)%$, and $ {\\mathcal B} (B^+ \\to D_s^{(*)+} \\bar{D}^{**0}) = (2.73 \\pm 0.78 \\pm 0.48 \\pm 0.68)%$, where the first error is statistical, the second systematic, and the third is due to the uncertainty in the $D_s^+ \\to \\phi \\pi^+$ branching fraction. The measured $D_s^{*+}$ longitudinal polarization, $\\Gamma_L/\\Gamma = (50.6 \\pm 13.9 \\pm 3.6)%$, is consistent with the factorization prediction of 54%.']",['2000-08-09']
694,['eng'],"['Uvarov, V']",['Inclusive Particle Production at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, jet', 'gluon, jet', 'baryon, yield', 'Sigma-', 'Lambda(1520)', 'meson, yield', 'yield, ratio', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011058'],"['New results on inclusive production of Sigma^- and Lambda(1520) and on proton production in quark and gluon jets are presented. These results are based on 2 million hadronic Z decays collected with the DELPHI detector at LEP. They are compared with the results of other LEP experiments and with models. It has been shown that the total production rates of all light-flavour hadrons measured so far at LEP 1 follow phenomenological laws related to the spin, isospin, strangeness and mass of the particles. A significant proton enhancement in gluon jets is observed, indicating that baryon production proceeds directly from colour objects.']",['2000-11-21']
695,['eng'],"['Kettell, S H']",['Rare Kaon Decay Experiments'],['Particle Physics - Experimental Results'],"['review, Athens 2000/05/12', 'K, rare decay', 'K, semileptonic decay', 'K, leptonic decay', 'violation, flavor', 'K0(L), branching ratio', 'K+, branching ratio', 'upper limit', 'Kobayashi-Maskawa angle', 'experimental results', 'K0(L) --> muon electron', 'K0(L) --> muon+ muon-', 'K --> pi neutrino antineutrino', 'K --> pi lepton+ lepton-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008012'],"['The status of rare kaon decay experiments is reviewed. With the current generation of experiments now finishing, several exciting new results are available. New limits in the search for Lepton Flavor Violation (LFV) will be discussed, as will new limits and measurements of the CKM matrix parameters. The next generation of rare kaon decay experiments and their contribution to determination of CKM parameters is also briefly discussed.']",['2000-08-08']
696,['eng'],"['Lee, S W']",['Prompt Photons in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'photon, photoproduction', 'photon, direct production', 'differential cross section, rapidity dependence', 'transverse energy, dependence', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008011'],"['First inclusive measurements of isolated prompt photons in photoproduction at HERA have been made with the ZEUS detector. Cross sections are given as a function of the pseudorapidity and the transverse energy of the photon, for E_T^gamma > 5 GeV in the gamma-p centre-of-mass energy range 134-285 GeV. Comparisons are made with predictions from LO Monte Carlo models and NLO QCD calculations. For forward eta^gamma (proton direction) good agreement is found, but in the rear direction all predictions fall below the data.']",['2000-08-08']
697,['eng'],"['Chikovani, L', 'Djobava, T']",['Study of ATLAS Sensitivity to FCNC TOP Quark Decay $t \\to Zq$'],['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, rare decay', 'neutral current, flavor changing', 'intermediate boson, leptonic decay', 'W, hadronic decay', 'background', 'magnetic detector, ATLAS', 'efficiency', 'numerical calculations, CERN LHC Coll', 'p p --> 2truth anything', 'truth --> Z0 charm', 'truth --> Z0 up', 'truth --> W beauty', '14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008010'],"['The sensitivity of ATLAS experiment to the top-quark rare decay via flavor- changing neutral currents t \\to Zq (q represents c and u quarks) have been studied at \\sqrt{s}= 14 TeV in two decay modes: 1. The pure leptonic decay of gauge bosons: t\\bar{t} \\to ZqWb \\to l^{+} l^{-} j l^{+-} nu j_{b} (l=e, mu) 2. The leptonic decay of Z bosons and hadronic decay of W bosons t\\bar{t} \\to ZqWb \\to l^{+} l^{-} jjjj_{b} (l=e, mu) The dominant backgrounds Z-jets, Zw and t\\bar{t} has been analysed. The signal and backgrounds were generated via PYTHIA 5.7, simulated and analysed using ATLFAST 2.14. A branching ratio for t \\to Zq as low as 1.1x1-^{4} for the leptonic mode and 2.3x10^{4} for hadronic mode could be discovered at the 5\\sigma level with an integrated luminosity of 10^{5} pb^{-1}.']",['2000-08-08']
698,['eng'],"['McCance, G J']",['Event Shapes and Power Correction Results from HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'event shape analysis', 'kinematics, Breit frame', 'final state, (2jet)', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'parametrization', 'correction, hadronization', 'strong interaction, coupling constant', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008009'],"['Inclusive event shape variables have been measured in the Breit Frame for neutral current deep-inelastic positron-proton scattering using the H1 and ZEUS detectors at HERA. The variables thrust, jet broadening, C-parameter, jet mass and two kinds of differential two-jet rate have been studied in the kinematic range 7 < Q < 100 GeV. The Q dependence of the shape variables have been compared with QCD applying power corrections proportional to 1/Q^p to account for hadronisation effects. The concept of power corrections is tested by fitting the strong coupling constant alpha_s and a non-perturbative parameter alpha(p-1)_bar.']",['2000-08-07']
699,['eng'],"['Paschke, K', 'Quinn, B']",['Spin Observables in Antilambda-Lambda Production from Antiproton-Proton Annihilation with a Transverse Inital State Polarization'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'Lambda, pair production', 'p, polarized target', 'polarization, transverse', 'polarization, measurement', 'spin, amplitude analysis', 'parametrization', 'Lambda, decay', 'angular distribution']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008008'],"['The formalism describing the scattering of two spin-1/2 objects is reviewed for the case of antilambda-lambda production from antiproton-proton annihilation. It is shown that an experiment utilizing a transverse target polarization can, in principle, completely determine the spin structure of the reaction. Additional measurements, even those using both beam and target polarizations, would not be sensitive to any additional spin dynamics. Thus, the transverse target polarization allows access to the complete set of spin observables, not just the subset upon which the literature has previously focused. This discussion is especially relevant in light of the data collected by PS185/3 at LEAR.']",['2000-08-07']
700,['eng'],"['Artuso, M', 'Ayad, R', 'Efimov, A', 'Kopp, S E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J', 'Anderson, S', 'Kubota, Y', 'Smith, A', 'Coan, T E', 'Fadeev, V', 'Ye, J']",['The Cleo III Ring Imaging Cherenkov Detector'],['Particle Physics - Experimental Results'],"['talk, La Biodola 2000/05/21', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'Cherenkov counter, crystal', 'lithium, fluorine', 'drift chamber, gas', 'organic compounds', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008007'],"['The CLEO detector has been upgraded to include a state of the art particle identification system, based on the Ring Imaging Cherenkov Detector (RICH) technology, in order to take data at the upgraded CESR electron positron collider. The expected performance is reviewed, as well as the preliminary results from an engineering run during the first few months of operation of the CLEO III detector.']",['2000-08-07']
701,['eng'],"['Rabbertz, K', 'Wollmer, U']",['Event Shapes and Power Corrections in ep DIS at HERA'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'event shape analysis', 'kinematics, Breit frame', 'final state, (2jet)', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'correction, hadronization', 'strong interaction, coupling constant', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008006'],"['Deep-inelastic ep scattering data, taken with the H1 and ZEUS detectors at HERA, are used to study the means and distributions of the event shape variables thrust, jet broadening, jet mass, C-parameter and two kinds of differential two-jet rate. The data cover a range of the four-momentum transfer Q, taken to be the relevant energy scale, between 7 GeV and 141 GeV. The Q dependences are compared with second-order calculations of perturbative QCD. Power law corrections are applied to account for hadronization effects.']",['2000-08-04']
702,['eng'],"['Bodek, Arie', 'Yang, U K', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bolton, T', 'Brau, J E', 'Buchholz, D', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Fleming, B T', 'Formaggio, J A', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McFarland, K S']",['New Measurements of Nucleon Structure Functions from the CCFR/NuTeV Collaboration'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'neutrino nucleus, interaction', 'antineutrino nucleus, interaction', 'neutrino/mu', 'iron', 'nucleon, structure function', 'momentum spectrum, parton', 'quark, charm', 'differential cross section, momentum transfer', 'quantum chromodynamics, perturbation theory', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008003'],"['We report on the extraction of the structure functions F_2 and Delta xF_3 = xF_3nu-xF_3nubar from CCFR neutrino-Fe and antineutrino-Fe differential cross sections. The extraction is performed in a physics model independent (PMI) way. This first measurement for Delta xF_3, which is useful in testing models of heavy charm production, is higher than current theoretical predictions. The F_2 (PMI) values measured in neutrino and muon scattering are in good agreement with the predictions of Next to Leading Order PDFs (using massive charm production schemes), thus resolving the long-standing discrepancy between the two sets of data.']",['2000-08-03']
703,['eng'],"['Price, P B', 'Woschnagg, K']",['Role of Group and Phase Velocity in High-Energy Neutrino Observatories'],['Particle Physics - Experimental Results'],"['muon, radiation', 'water, solids', 'radiation, Cherenkov', 'radiation, laser', 'laser, pulsed', 'radiation, velocity', 'track data analysis, error', 'dependence, density', 'temperature, dependence', 'numerical calculations', 'deep underground detector']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008001'],"['Kuzmichev recently showed that use of phase velocity rather than group velocity for Cherenkov light signals and pulses from calibration lasers in high-energy neutrino telescopes leads to errors in track reconstruction and distance measurement. We amplify on his remarks and show that errors for four cases of interest to AMANDA, IceCube, and RICE (radio Cherenkov detector) are negligibly small.']",['2000-08-02']
704,['eng'],"['Alton, A']",['Search for light-to-heavy quark flavor changing neutral currents in $\\nu _{\\mu}N$ and $\\overline{\\nu}_{\\mu}N$ scattering at the Tevatron'],['Particle Physics - Experimental Results'],"['neutrino nucleus, inclusive reaction', 'antineutrino nucleus, inclusive reaction', 'iron', 'quark, charm', 'quark, beauty', 'quark, neutrinoproduction', 'neutral current, flavor changing', 'search for', 'quark, semileptonic decay', 'lepton, charge', 'Kobayashi-Maskawa angle', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007059'],"['We report on a search for flavor-changing neutral-currents (FCNC) in the production of heavy quarks in deep inelastic $\\nu_{\\mu}N$ and $\\bar{\\nu}% _{\\mu}N$ scattering by the NuTeV experiment at the Fermilab Tevatron. This measurement, made possible by the high-purity NuTeV sign-selected beams, probes for FCNC in heavy flavors at the quark level and is uniquely sensitive to neutrino couplings of potential FCNC mediators. All searches are consistent with zero, and limits on the effective mixing strengths $% | V_{uc}| ^{2}$, $| V_{db}| ^{2}$, and $| V_{sb}| ^{2}$ are obtained.']",['2000-08-01']
705,['eng'],"['Erdmann, M']","['On the Structure of the Proton, the Photon, and Colour Singlet Exchange']",['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'p, structure function', 'photon, structure function', 'momentum transfer, dependence', 'x-dependence', 'parametrization', 'color, singlet', 'diffraction', 'experimental results', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007058'],"['Structure function measurements of the proton, the photon, and of colour singlet exchange are analysed using fits based on logarithmic Q**2-dependence. The fits reveal the x-dependencies of the hadronic structures and the interaction dynamics as directed by the data.']",['2000-08-01']
706,['eng'],"['Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Ferguson, T', 'Vogel, H', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R']",['A Search for $B\\to \\tau\\nu$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, leptonic decay', 'B, semileptonic decay', 'tau, leptonic decay', 'tau, semileptonic decay', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> tau neutrino', 'B --> K neutrino antineutrino', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007057'],"['We report results of a search for $B\\to\\tau\\nu$ in a sample of 9.7 million charged $B$ meson decays. The search uses both $\\pi\\nu$ and $\\ell\\nu\\bar\\nu$ decay modes of the $\\tau$, and demands exclusive reconstruction of the companion $\\bar B$ decay to suppress background. We set an upper limit on the branching fraction ${\\cal B}(B\\to \\tau\\nu) < 8.4\\times 10^{-4}$ at 90% confidence level. With slight modification to the analysis we also establish ${\\cal B}(B^\\pm\\to K^\\pm\\nu\\bar\\nu) < 2.4\\times 10^{-4}$ at 90% confidence level.']",['2000-07-28']
707,['eng'],"['Learned, J G']",['The Atmospheric Neutrino Anomaly'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'neutrino, flux', 'ratio, (neutrino/mu neutrino/e)', 'energy dependence', 'pi, leptonic decay', 'muon, leptonic decay', 'decay, path length', 'neutrino, oscillation', 'magnetic field, geophysics', 'angular distribution', 'neutrino, mass difference', 'neutrino, mixing angle', 'neutrino, beam', 'astrophysics', 'deep underground detector, KAMIOKANDE', 'experimental results', 'proposed experiment', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007056'],"['With the 1998 announcement of new evidence for muon neutrino disappearance observed by the Super-Kamiokande experiment, the more than a decade old atmospheric neutrino anomaly moved from a possible indication for neutrino oscillations to an almost inescapable implication. The evidence from all experiments is reviewed, and indications are presented that the oscillations are probably between muon and tau neutrinos with nearly maximal mixing. Implications and future directions in neutrino oscillations research are discussed.']",['2000-07-28']
708,['eng'],"['Brooijmans, G']",['Determination of Scanning Efficiencies in Experiments Using Nuclear Emulsion Sheets'],['Particle Physics - Experimental Results'],"['nuclear emulsion', 'track data analysis', 'efficiency', 'statistical analysis', 'neutrino, counters and detectors']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007055'],"['During their exposure, nuclear emulsion sheets detect both tracks from experiment-related particles, as well as a considerable amount of background tracks, mainly due to cosmic rays. Unless the exposure has been fairly short, it is therefore fairly likely that a fraction of the tracks that have been identified as belonging to the particles the experiment is interested in, are really due to background. A method, which allows to measure this fraction reliably directly from the data, is described.']",['2000-07-27']
709,['eng'],"['Artuso, M', 'Wang, J']",['Study of the spatial resolution achievable with the BTeV pixel sensors'],['Particle Physics - Experimental Results'],"['talk, Genova 2000/06/05', 'semiconductor detector, pixel', 'spatial resolution', 'magnetic field', 'electronics, readout', 'numerical calculations, Monte Carlo', 'magnetic spectrometer, BTeV', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007054'],"['A Monte Carlo simulation has been developed to predict the spatial resolution of silicon pixel detectors. The results discussed in this paper focus on the unit cell geometry of 50 $\\mu$m x 400 $\\mu$m, as chosen for BTeV. Effects taken into account include energy deposition fluctuations along the charged particle path, diffusion, magnetic field and response of the front end electronics. We compare our predictions with measurements from a recent test beam study performed at Fermilab.']",['2000-07-27']
710,['eng'],"['Roche, J', 'Friedrich, J M', 'Lhuillier, D', 'Bartsch, P', 'Baumann, D', 'Berthot, J', 'Bertin, P Y', 'Breton, V', 'Böglin, W', 'Böhm, R', ""D'Hose, N"", 'Derber, S', 'Degrande, N', 'Ding, M', 'Distler, M O', 'Ducret, J E', 'Ewald, I', 'Fonvieille, H', 'Friedrich, J M', 'Guichon, P A M', 'Holvoet, H', 'Hyde-Wright, C E', 'Jennewein, P', 'Kahrau, M', 'Kerhoas, S', 'Krygier, K W', 'Lannoy, B', 'Liesenfeld, A', 'Marchand, C', 'Marchand, D', 'Marroncle, J', 'Martino, J', 'Merkel, H', 'Merle, P', 'De Meyer, G', 'Mougey, J', 'Müller, U', 'Neuhausen, R', 'Pospischil, T', 'Quéméner, G', 'Ravel, O', 'Roblin, Y', 'Rohe, D', 'Rosner, G', 'Ryckbosch, D', 'Schmieden, H', 'Tamas, G', 'Tytgat, M', 'Vanderhaeghen, M', 'Van Hoorebeke, L', 'Van de Vyver, R', 'Van de Wiele, J', 'Vernin, P', 'Wagner, A', 'Walcher, T', 'Weiss, M']",['The first determination of Generalized Polarizabilities of the proton by a Virtual Compton Scattering experiment'],['Particle Physics - Experimental Results'],"['electron p, inelastic scattering', 'photon p, Compton scattering', 'photon, off-shell', 'p, polarizability', 'polarizability, electric', 'polarizability, magnetic', 'differential cross section, angular dependence', 'momentum transfer, dependence', 'Mainz Linac', 'electron p --> p electron photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007053'],"['Absolute differential cross sections for the reaction (e+p -> e+p+gamma) have been measured at a four-momentum transfer with virtuality Q^2=0.33 GeV^2 and polarization \\epsilon = 0.62 in the range 33.6 to 111.5 MeV/c for the momentum of the outgoing photon in the photon-proton center of mass frame. The experiment has been performed with the high resolution spectrometers at the Mainz Microtron MAMI. From the photon angular distributions, two structure functions which are a linear combination of the generalized polarizabilities have been determined for the first time.']",['2000-07-27']
711,['eng'],"['Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G']",['Determination of the $B \\to D^{*}+l-\\nu$ Decay Width and $|V_{cb}|$'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'D*(2010)', 'Kobayashi-Maskawa angle', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D*(2010) lepton neutrino', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007052'],"['We determine the CKM matrix element |Vcb| using a sample of 3.33 million BBbar events in the CLEO detector at CESR. We determine the yield of reconstructed B --> D*+ l nu decays as a function of w = v_B . v_D*, and from this we obtain the differential decay rate d\\Gamma/dw. By extrapolating the differential decay rate to w=1, the kinematic point at which the D* is at rest relative to the B, we extract the product |Vcb| F(1), where F(1) is the form factor at w=1 and is predicted accurately by theory. We find |Vcb| F(1) = 0.0424 +- 0.0018(stat.) +- 0.0019(syst.). We also integrate the differential decay rate over w to obtain B(B --> D*+ l nu) = (5.66 +- 0.29 +- 0.33)%. All results are preliminary.']",['2000-07-26']
712,['eng'],"['Abe, K']",['First symmetry tests in polarized Z0 decays$\\to b\\overline{b}g$'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, polarization', 'Z0, hadronic decay', 'final state, (3jet)', 'quark, jet', 'gluon, jet', 'angular distribution, asymmetry', 'electroweak interaction, validity test', 'parity, violation', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty gluon', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007051'],"['We have made the first direct symmetry tests in the decays of polarized Z0 bosons into fully-identified b bbar g states, collected in the SLD experiment at SLAC. We searched for evidence of parity violation at the b bbar g vertex by studying the asymmetries in the b-quark polar- and azimuthal-angle distributions, and for evidence of T-odd, CP-even or odd, final-state interactions by measuring angular correlations between the three-jet plane and the Z0 polarization. We found results consistent with Standard Model expectations, and set 95% C.L. limits on anomalous contributions.']",['2000-07-26']
713,['eng'],"['Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A']","[""Evidence of New States Decaying into $\\Xi_c^{'}\\pi$""]",['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, excited state', 'charmed baryon, hadronic decay', 'charmed baryon, cascade decay', 'final state, (Xi/c+ pi- photon)', 'final state, (Xi/c0 pi+ photon)', 'Xi/c+, hadronic decay', 'Xi/c0, hadronic decay', 'mass difference, spectra', 'postulated particle, Xi/c1', 'spin, parity', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007050'],"['Using 13.7 fb^{-1} of data recorded by the CLEO detector at CESR, we report preliminary evidence for two new charmed baryons; one decaying into Xi_c^{0\\prime} pi^+ with the subsequent decay Xi_c^{0\\prime} to Xi_c^0 gamma, and its isospin partner decaying into Xi_c^{+\\prime} pi^- followed by Xi_c^{+\\prime} to Xi_c^+ gamma. We measure the following mass differences for the two states: M(Xi_c^0 gamma pi^+)-M(\\Xi_c^0)=318.4+ -1.5+-2.9 MeV, and M(Xi_c^+ gamma pi^-)-M(Xi_c^+)=323.9+-pm1.4+-pm3.0 MeV. We interpret these new states as the J^P = (1/2)^-1 Xi_{c1} particles, the charmed-strange analogues of the Lambda_{c1}^+(2593).']",['2000-07-25']
714,['eng'],"['Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A']",['Observation of New States Decaying into $\\Lambda_{c}^{+}\\pi^{-}\\pi^{+}$'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, excited state', 'charmed baryon, hadronic decay', 'charmed baryon, mass', 'final state, (Lambda/c+ pi+ pi-)', 'mass difference, spectra', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> charmed baryon anything', 'charmed baryon --> Lambda/c+ pi+ pi-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007049'],"['Using 13.7 fb^{-1} of data recorded by the CLEO detector at CESR, we investigate the spectrum of charmed baryons which decay into Lambda_c^+ pi^- pi^+ and are more massive than the Lambda_{c1} baryons. We find evidence for two new states: one is broad and has an invariant mass roughly 480 MeV above that of the Lambda_c^+; the other is narrow with an invariant mass of 596 +- 1 +- 2 MeV above the Lambda_c^+ mass. These results are preliminary.']",['2000-07-25']
715,['eng'],"['Roe, B P', 'Woodroofe, M B']",['Setting Confidence Belts'],['Particle Physics - Experimental Results'],['statistical analysis'],['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007048'],['We propose using a Bayes procedure with uniform improper prior to determine the credible belts for the Poisson distribution in the presence of background and for the continuous problem of measuring a quantity theta >= 0 with a normally distributed measurement error. The credible limits are then examined from a frequentist point of view and found to have good frequentist and conditional frequentist properties and some optimality properties.'],['2000-07-25']
716,['eng'],"['Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J']",['Observation of the $Omega_{c}$ Charmed Baryon at CLEO'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Omega/c0, electroproduction', 'Omega/c0, hadronic decay', 'channel cross section, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Omega/c0 anything', 'Omega/c0 --> Omega- pi+', 'Omega/c0 --> Omega- pi+ pi0', 'Omega/c0 --> Omega- 2pi+ pi-', 'Omega/c0 --> Xi- K- 2pi+', 'Omega/c0 --> Xi0 K- pi+', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007047'],"['The CLEO detector at the CESR collider has used 13.7 fb^{-1} to search for the production of Omega_c (css-ground state) in e^{+}e^{-} collisions at sqrt{s} = 10.6 GeV The modes used to study the Omega_c are Omega- pi+, Omega- pi+ pi0, Xi- K- pi+ pi+, Xi0 K- pi+, and Omega- pi+ pi+ pi-. We observe 40.4 +- 9.0(stat) combined events at a mass of 2694.6 +- 2.6(stat) +- 2.4(syst) MeV. We have also measured the \\sigma * Br of the above modes for xp > 0.5 to be 11.3 +- 3.9 +- 2.3 fb, 47.6 +- 18.0 +- 2.8 fb, 45.1 +- 23.2 +- 4.1 fb, 18.2 +- 10.6 +- 3.8 fb, and <5.1 fb @ 90 % CL, respectively.']",['2000-07-25']
717,['eng'],"['Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J']",['Study of $\\chi_{c1}$ and $\\chi_{c2}$ meson production in B meson decays'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'chi/c1(3510), direct production', 'chi/c2(3555), direct production', 'psi(3685), radiative decay', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> chi mesons anything', 'B --> psi(3685) anything', 'psi(3685) --> chi mesons photon', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007046'],"['Using a sample of 9.7 million B meson pairs collected with the CLEO detector, we study inclusive B meson decays to the chi_c1 and chi_c2 charmonia states. We measure the branching fraction for the inclusive chi_c1 production in B decays to be Br(B->chi_c1 X)=(4.14+-0.31+-0.40)*10^-3, where the first uncertainty is statistical and the second one is systematic. We obtain the branching fractions for direct chi_c1 and chi_c2 production in B decays by subtracting the contribution from the decay chain B->psi(2S)X with psi(2S)->chi_c1,2 gamma. We measure Br(B->chi_c1[direct] X)=(3.83+-0.31+-0.40)*10^-3. No statistically significant signal for chi_c2 production is observed in either case. We determine the 95% C.L. upper limits to be Br(B->chi_c2 X)<2.0*10^-3 Br(B->chi_c2[direct] X)<1.7*10^-3, and Br(B->chi_c2[direct] X)/Br(B->chi_c1[direct] X)<0.44. All quoted results are preliminary.']",['2000-07-25']
718,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Chung, Y S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Furic, I K', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kirby, M', 'Kirk, M', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Meyer, A', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mulhearn, M', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Riveline, M', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Safonov, A', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Measurement of the W Boson Mass with the Collider Detector at Fermilab'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'muon, angular distribution', 'muon, momentum', 'electron, energy', 'background', 'W, mass', 'mass spectrum, transverse', 'momentum spectrum, parton', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', 'W --> electron neutrino/e', 'W --> muon neutrino/mu', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007044'],"['We present a measurement of the W boson mass using data collected with the CDF detector during the 1994-95 collider run at the Fermilab Tevatron. A fit to the transverse mass spectrum of a sample of 30,115 W -> enu events recorded in an integrated luminosity of 84 pb^(-1) gives a mass Mw = 80.473 +- 0.065(stat.) +- 0.092(syst.) GeV/c^2. A fit to the transverse mass spectrum of a sample of 14,740 W -> munu events from 80 pb^(-1) gives a mass Mw = 80.465 +- 0.100(stat.) +- 0.103(syst.) GeV/c^2. The dominant contributions to the systematic uncertainties are the uncertainties in the electron energy scale and the muon momentum scale, 0.075 GeV/c^2 and 0.085 GeV/c^2, respectively. The combined value for the electron and muon channel is Mw = 80.470 +- 0.089 GeV/c^2. When combined with previously published CDF measurements, we obtain Mw = 80.433 +- 0.079 GeV/c^2.']",['2000-07-24']
719,['eng'],"['Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H']",['Search for Decays of $B^{0}$ Mesons into Pairs of Leptons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, leptonic decay', 'flavor, violation', 'B0, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> positron electron', 'B0 --> muon+ muon-', 'B0 --> muon electron', '10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007042'],"['We search for the decays of the $B^0$ meson into $e^+e^-$, $\\mu^+\\mu^-$ $e^{\\pm}\\mu^{\\mp}$ pairs in a sample of $9.7\\times 10^6$ $B{\\bar B}$ pairs recorded by CLEO detector. No signal is found, and the following upper limits on the corresponding branching fractions are established: $<8.3\\times 10^{-7}$, $<6.1\\times 10^{-7}$, $< 15\\times 10^{-7}$ at 90% confidence level. A new lower limit on the Pati-Salam leptoquark mass $M_{LQ}>27$ TeV is established at 90% confidence level.']",['2000-07-21']
720,['eng'],"['Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J']",['First Observation of the $\\Sigma_{c}^{*+}$ Baryon and a New Measurement of the $\\Sigma_{c}^{+}$ Mass'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, electroproduction', 'charmed baryon, hadronic decay', 'Sigma/c+', 'Sigma/c(2530)', 'mass difference, (Sigma/c(2530) Lambda/c+)', 'mass difference, (Sigma/c+ Lambda/c+)', 'Lambda/c+, decay modes', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007041'],"['Using data recorded with the CLEO II and CLEO II.V detector configurations at the Cornell Electron Storage Rings, we report the first observation and mass measurement of the $\\Sigma_c^{*+}$ charmed baryon, and an updated measurement of the mass of the $\\Sigma_c^+$ baryon. We find $M(\\Sigma_c^{*+})-M(\\Lambda_c^+)$= 231.0 +- 1.1 +- 2.0 MeV, and $M(\\Sigma_c^{+})-M(\\Lambda_c^+)$= 166.4 +- 0.2 +- 0.3 MeV, where the errors are statistical and systematic respectively.']",['2000-07-21']
721,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Benelli, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Boeriu, O', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Csilling, Akos', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'De Wolf, E', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menges, W', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Renkel, P', 'Rick, Hartmut', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Toya, D', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Two Higgs Doublet Model and Model Independent Interpretation of Neutral Higgs Boson Searches'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, neutral particle', 'Higgs particle, multiplet', 'doublet, 2', 'Higgs particle, electroproduction', 'Z0, associated production', 'Z0, decay modes', 'Higgs particle, pair production', 'Higgs particle, decay modes', 'Higgs particle, mass', 'quark, pair production', 'tau, pair production', 'gluon, pair production', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'electron positron --> 2Higgs particle', 'Higgs particle --> quark antiquark', 'Higgs particle --> 2gluon', 'Higgs particle --> tau+ tau-', 'Higgs particle --> 2Higgs particle', '183, 189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007040'],"['Searches for the neutral Higgs bosons h0 and A0, are used to obtain limits on the Type II Two Higgs Doublet Model (2HDM(II)) with no CP-violation in the Higgs sector and no additional particles besides the five Higgs bosons. The analysis combines approximately 170 pb-1 of data collected with the OPAL detector at sqrt{s} ~ 189 GeV with previous runs at sqrt{s} ~ mZ and sqrt{s} ~ 183 GeV. The searches are sensitive to the h0, A0 -> qq, gg, tau+tau- and h0 -> A0A0 decay modes of the Higgs bosons. For the first time, the 2HDM(II) parameter space is explored in a detailed scan, and new flavour independent analyses are applied to examine regions in which the neutral Higgs bosons decay predominantly into light quarks or gluons. Model-independent limits are also given.']",['2000-07-21']
722,['eng'],"['Pohl, M']",['Experimentation and Physics at a Future Electron-Positron Linear Collider'],['Particle Physics - Experimental Results'],"['talk, Sanlucar de Barrameda 2000/02/14', 'electron positron, linear collider', 'linear collider, proposed', 'colliding beam detector, proposed', 'electron positron, interaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'W, pair production', 'Z0, pair production', 'coupling, (3gauge boson)', 'new particle, search for', 'Higgs particle, electroproduction', 'Higgs particle, decay modes', 'supersymmetry', 'sparticle, decay modes', 'leptoquark', 'cross section, energy dependence', 'numerical calculations', 'DESY TESLA Linac', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007039'],"['I summarise the physics opportunities and experimental challenges at future Linear Colliders, using material from the recent ECFA/DESY workshop on the subject as well as contributions to the series of worldwide studies. For reasons of economy, the discussion is restricted to the European Tesla project and to its electron-positron mode only.']",['2000-07-21']
723,['eng'],"['Scott, J P']",['Structure Functions at Low x and Q2 at ZEUS'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'p, structure function', 'small-x', 'momentum transfer, low', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007038'],"['Using 3.9 $pb^{-1}$ of data from ep $\\ra$ eX interactions recorded using the ZEUS detector in 1997,the proton structure function, F$_2$, has been measured in the range 0.015 GeV$^2$ $<$ Q$^2 <$ 0.65 GeV$^2$ and $6 \\times 10^{-7} < x < 1 \\times 10^{-3}$. The analysis is based on data taken incorporating new detector components. Compared with the previous analysis, these components allow improved background suppression and better control of systematic uncertainties, extending the accessible kinematic region towards lower Q$^2$.']",['2000-07-21']
724,['eng'],"['Safonov, A']",['Jet Fragmentation and Mlla'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'anti-p p, annihilation', 'anti-p p, inclusive reaction', 'multiple production', 'jet, hadroproduction', 'jet, fragmentation', 'leading logarithm approximation', 'final state, (2jet)', 'charged particle, momentum spectrum', 'charged particle, multiplicity', 'angular dependence', 'quark, jet', 'gluon, jet', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007037'],['Recent CDF results on inclusive momentum distributions and multiplicities of particles in restricted cones around jets are compared to predictions using the Modified Leading Log Approximation. We found that MLLA gives a very reasonable description of jet fragmentation for a wide range of energies. Model parameters are extracted separately from the multiplicity and from the shape of the momentum distributions and are found to agree. The ratio of charged particle multiplicities in gluon and quark jets measured in the context of MLLA is compared to the model-independent result and also found to agree.'],['2000-07-20']
725,['eng'],"['Back, B B', 'Baker, M D', 'Barton, D S', 'Basilev, S', 'Baum, R', 'Betts, R R', 'Bialas, A', 'Bindel, R', 'Bogucki, W', 'Budzanowski, A', 'Busza, W', 'Carroll, A S', 'Ceglia, M', 'Chang, Y H', 'Chen, A E', 'Coghen, T', 'Conner, C', 'Czyz, W', 'Dabrowski, B', 'Decowski, M P', 'Despet, M', 'Fita, P', 'Fitch, J', 'Friedl, M', 'Galuszka, K', 'Ganz, R E', 'García-Solis, E', 'George, N', 'Godlewski, J', 'Gomes, C', 'Griesmayer, E', 'Gulbrandsen, K H', 'Gushue, S', 'Halik, J', 'Halliwell, C', 'Haridas, P', 'Hayes, A', 'Heintzelman, G A', 'Henderson, C', 'Hollis, R', 'Holynski, R', 'Holzman, B', 'Johnson, E', 'Kane, J', 'Katzy, J M', 'Kita, W', 'Kotula, J', 'Kraner, H W', 'Kucewicz, W', 'Kulinich, P A', 'Law, C', 'Lemler, M A', 'Ligocki, T J', 'Lin, W T', 'Manly, S L', 'McLeod, D', 'Michalowski, J', 'Mignerey, A C', 'Mülmenstädt, J', 'Neal, M', 'Nouicer, R', 'Olszewski, A', 'Pak, R', 'Park, I C', 'Patel, M', 'Pernegger, H', 'Plesko, M', 'Reed, C', 'Remsberg, L P', 'Reuter, M', 'Roland, C', 'Roland, G', 'Ross, D', 'Rosenberg, L J', 'Ryan, J', 'Sanzgiri, A', 'Sarin, P', 'Sawicki, P', 'Scaduto, J', 'Shea, J', 'Sinacore, J', 'Skulski, W', 'Steadman, S G', 'Stephans, G S F', 'Steinberg, P', 'Straczek, A', 'Stodulski, M', 'Strek, M', 'Stopa, Z', 'Sukhanov, A', 'Surowiecka, K', 'Tang, J L', 'Teng, R', 'Trzupek, A', 'Vale, C J', 'van Nieuwenhuizen, G J', 'Verdier, R', 'Wadsworth, B', 'Wolfs, F L H', 'Wosiek, B', 'Wozniak, K', 'Wuosmaa, A H', 'Wyslouch, B', 'Zalewski, Kasper']",['Charged particle multiplicity near mid-rapidity in central Au+Au collisions at $\\sqrt{s}$ = 56 and 130 AGeV'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'gold', 'central region', 'charged particle, multiplicity', 'rapidity, density', 'magnetic detector, PHOBOS', 'experimental results', 'Brookhaven RHIC Coll', '56-130 GeV-cms/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007036'],"['We present the first measurement of pseudorapidity densities of primary charged particles near mid-rapidity in Au+Au collisions at $\\sqrt{s} =$ 56 and 130 AGeV. For the most central collisions, we find the charged particle pseudorapidity density to be $dN/d\\eta |_{|\\eta|<1} = 408 \\pm 12 {(stat)} \\pm 30 {(syst)}$ at 56 AGeV and $555 \\pm 12 {(stat)} \\pm 35 {(syst)}$ at 130 AGeV, values that are higher than any previously observed in nuclear collisions. Compared to proton-antiproton collisions, our data show an increase in the pseudorapidity density per participant by more than 40% at the higher energy.']",['2000-07-20']
726,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bähr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Borras, K', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P D', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Kaufmann, O', 'Kausch, M', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Kutuev, R K', 'Lachnit, W A', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebailly, E', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'Lobodzinska, E', 'Lobodzinski, B', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Negri, I', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schmitt, S', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vazdik, Ya', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['A Search for Excited Fermions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'new particle, search for', 'lepton, excited state', 'quark, excited state', 'model, composite', 'excited state, decay modes', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'fermion* --> fermion photon', 'fermion* --> intermediate boson fermion', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007035'],"['A search for excited fermions f^* of the first generation in e^+p scattering at the collider HERA is presented using H1 data with an integrated luminosity of 37 pb^(-1). All electroweak decays of excited fermions, f^* -> f gamma, f W, f Z are considered and all possible final states resulting from the Z or W hadronic decays or decays into leptons of the first two generations are taken into account. No evidence for f^* production is found. Mass dependent exclusion limits on cross-sections and on the ratio of coupling constants to the compositeness scale are derived.']",['2000-07-20']
727,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Chung, Y S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Furic, I K', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kirby, M', 'Kirk, M', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Meyer, A', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mulhearn, M', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Riveline, M', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Safonov, A', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Measurement of the Decay Amplitudes of $B0 \\to J/\\psi K*$ and $B0s \\to J/\\psi\\phi$ Decays'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0, hadronic decay', 'B/s0, hadronic decay', 'J/psi(3100), leptonic decay', 'K*(892), hadronic decay', 'Phi(1020), hadronic decay', 'decay, amplitude analysis', 'parity', 'polarization, longitudinal', 'polarization, transverse', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B0 --> J/psi(3100) K*(892)', 'B/s0 --> J/psi(3100) Phi(1020)', 'J/psi(3100) --> muon+ muon-', 'K*(892) --> K pi', 'Phi(1020) --> K+ K-', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007034'],"['A full angular analysis has been performed for the pseudo-scalar to vector-vector decays, B0 --> J/psi K* and B_s --> J/psi phi, to determine the amplitudes for decays with parity-even longitudinal and transverse polarization and parity-odd transverse polarization. The measurements are based on 190 B0 candidates and 40 B_s candidates collected from a data set corresponding to 89 inverse pb of pbarp collisions at root(s) = 1.8 TeV at the Fermilab Tevatron. In both decays the decay amplitude for longitudinal polarization dominates and the parity-odd amplitude is found to be small.']",['2000-07-19']
728,['eng'],"['Glenzinski, D A', 'Heintz, U']",['Precision Measurements of the W-Boson Mass'],['Particle Physics - Experimental Results'],"['review, experimental results', 'anti-p p, colliding beams', 'W, hadroproduction', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, electroproduction', 'W, pair production', 'threshold', 'W, mass', 'W, hadronic decay', 'W, leptonic decay', 'mass spectrum, transverse', 'electron, transverse momentum', 'W, transverse momentum', 'charge, asymmetry', 'channel cross section, energy dependence', 'electroweak interaction, validity test', 'mass, truth', 'Higgs particle, mass', 'CERN LEP Stor', 'Batavia TEVATRON PS', 'bibliography']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007033', 'http://fnalpubs.fnal.gov/archive/2000/pub/Pub-00-166-E.html']","['The Standard Model of electroweak interactions has had great success in describing the observed data over the last three decades. The precision of experimental measurements affords tests of the Standard Model at the quantum loop level beyond leading order. Despite this great success it is important to continue confronting experimental measurements with the Standard Model predictions as any deviation would signal new physics. As a fundamental parameter of the Standard Model, the mass of the W-boson, M_W, is of particular importance. Aside from being an important test of the SM itself, a precision measurement of M_W can be used to constrain the mass of the Higgs boson, M_H. In this article we review the principal experimental techniques for determining M_W and discuss their combination into a single precision M_W measurement, which is then used to yield constraints on M_H. We conclude by briefly discussing future prospects for precision measurements of the W-boson mass.']",['2000-07-19']
729,['eng'],"['Mann, W A']",['New results on atmospheric neutrinos from Soudan 2'],['Particle Physics - Experimental Results'],"['talk, Sudbury 2000/06/16', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/e', 'flux, ratio', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, mixing angle', 'neutrino nucleon, interaction', 'charged current', 'deep underground detector, Soudan', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007031'],"['Neutrino interactions recorded in a 5.1 fiducial kiloton-year exposure of the Soudan-2 iron tracking calorimeter are analyzed for effects of neutrino oscillations. Using contained single track and single shower events, we update our measurement of the atmospheric nu_mu/nu_e ratio-of-ratios and find R = 0.68 \\pm 0.11 \\pm 0.06. Assuming this anomalously low R-value is the result of nu_mu flavor disappearance via nu_mu to nu_tau oscillation, we select samples of charged current events which offer good resolution, event-by-event, for L/Enu reconstruction. Oscillation-weighted Monte Carlo events are fitted to these data events using a chisq function summed over bins of log(L/E_nu). The region allowed in the (sin^2 2\\theta, \\Delta m^2) plane at 90% CL is obtained using the Feldman-Cousins procedure: 0.46 < sin^2 2\\theta < 1.0 and 2.2x10^-4 < \\Delta m^2 < 2.2x10^-2 ev^2. A small but relatively energetic sample of partially contained nu_mu events has also been isolated. Their distribution in log(L/E_vis) relative to null oscillation Monte Carlo is compatible with nu_mu to nu_tau oscillation scenarios within the parameter region allowed by our contained events.']",['2000-07-18']
730,['eng'],"['Luk, K B', 'Diehl, H T', 'Duryea, J', 'Guglielmo, G', 'Heller, K', 'Ho, P M', 'James, C', 'Johns, K', 'Longo, M J', 'Rameika, R', 'Teige, S', 'Thomson, G B']",['Search for Direct CP Violation in Non-Leptonic Decays of Charged $\\Xi$ and $\\Lambda$ Hyperons'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'beryllium', 'hyperon, hadroproduction', 'hyperon, hadronic decay', 'Xi-', 'Antixi-', 'Lambda', 'decay, asymmetry', 'CP, invariance', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'p beryllium --> Xi- anything', 'Xi- --> Lambda p', 'Lambda --> p pi-', '800 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007030'],"['A search for direct CP violation in the non-leptonic decays of hyperons has been performed. In comparing the product of the decay parameters, $\\alpha_{\\Xi}\\alpha_{\\Lambda}$, in terms of an asymmetry parameter, $A_{\\Xi\\Lambda}$, between hyperons and anti-hyperons in the charged $\\Xi \\to \\Lambda \\pi$ and $\\Lambda \\to p \\pi$ decay sequence, we found no evidence of direct CP violations. The parameter $A_{\\Xi\\Lambda}$ was measured to be $0.012 \\pm 0.014$.']",['2000-07-18']
731,['eng'],"['Thomas, A W']",['HiX2000'],['Particle Physics - Experimental Results'],"['talk, Philadelphia 2000/03/30', 'lepton nucleus, deep inelastic scattering', 'tritium', 'helium, nuclide', 'nucleon, model', 'quark, momentum spectrum', 'quark, valence', 'nucleon, structure function', 'dependence, mass number', 'polarization', 'structure function, spin', 'quantum chromodynamics', 'effect, higher-twist', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007029'],"[""We summarize the theoretical consensus of the HiX workshop concerning those measurements which seem most appropriate for inclusion in the ``white paper'' being prepared to justify the proposed 12 GeV upgrade at Jefferson Lab. The criteria for inclusion are that such measurements should be decisive, not possible elsewhere and should answer crucial physics questions with broad implications.""]",['2000-07-18']
732,['eng'],"['Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Banerjee, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Copty, N K', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Devmal, S C', 'Fernández, A', 'Fox, G F', 'Gagnon, P', 'Göbel, C', 'Gounder, K', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lundberg, B', 'Magnin, J', 'Massafferri, A', 'May Tal-Beck, S', 'Meadows, B', 'De Mello-Neto, J R T', 'Mihalcea, D', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'De Oliveira, A B', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Dos Reis, A C', 'Rubin, H A', 'Sanders, D A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Slaughter, A J', 'Sokoloff, M D', 'Solano, J M', 'Stanton, N R', 'Stefanski, R J', 'Stenson, K', 'Summers, D J', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yang, S M', 'Yi, D', 'Yoshida, S', 'Zaliznyak, R', 'Zhang, C']",['Experimental evidence for a light and broad scalar resonance in $D^{+} \\to \\pi^{-}\\pi^{+}\\pi^{+}$ decay'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D+, hadroproduction', 'D+, hadronic decay', 'Dalitz plot', 'amplitude analysis', 'sigma meson, mass', 'sigma meson, width', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> 2pi+ pi-', 'D+ --> K- 2pi+', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007028'],"['From a sample of $ 1172 \\pm 61 $ $ D^+ \\to \\pi^- \\pi^+ \\pi^+ $ decay, we find $ \\Gamma (D^+ \\to \\pi^- \\pi^+ \\pi^+) / \\Gamma (D^+ \\to K^- \\pi^+ \\pi^+) = 0.0311 \\pm 0.0018 ^{+0.0016}_{-0.0026} $. Using a coherent amplitude analysis to fit the Dalitz plot of this decays, we find strong evidence that a scalar resonance of mass $478^{+24}_{-23} \\pm 17 $ MeV/$c^2$ and width $324^{+42}_{-40} \\pm 21 $ MeV/$c^2$ accounts for approximately half of all decays.']",['2000-07-17']
733,['eng'],"['Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Banerjee, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Copty, N K', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Devmal, S C', 'Fernández, A', 'Fox, G F', 'Gagnon, P', 'Göbel, C', 'Gounder, K', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lundberg, B', 'Magnin, J', 'Massafferri, A', 'May Tal-Beck, S', 'Meadows, B', 'De Mello-Neto, J R T', 'Mihalcea, D', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'De Oliveira, A B', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Dos Reis, A C', 'Rubin, H A', 'Sanders, D A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Slaughter, A J', 'Sokoloff, M D', 'Solano, J M', 'Stanton, N R', 'Stefanski, R J', 'Stenson, K', 'Summers, D J', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yang, S M', 'Yi, D', 'Yoshida, S', 'Zaliznyak, R', 'Zhang, C']",['Study of the $D^{+}_{s} \\to \\pi^{-} \\pi^{+} \\pi^{+}$ decay and measurement of $f_{0}$ masses and widths'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D/s+, hadroproduction', 'D/s+, hadronic decay', 'mass spectrum, (pi+ pi- pi0)', 'Dalitz plot', 'amplitude analysis', 'rho(770)0', 'f0(975)', 'f2(1270)', 'f0(1370)', 'scalar meson, mass', 'scalar meson, width', 'D/s+, branching ratio', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D/s+ --> 2pi+ pi-', 'D/s+ --> Phi(1020) pi+', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007027'],"['From a sample of 848 $\\pm$ 44 $D_s^+ \\to \\pi^- \\pi^+ \\pi^+$ decays, we find $\\Gamma(D_s^+ \\to \\pi^- \\pi^+ \\pi^+) / \\Gamma(D_s^+ \\to \\phi \\pi^+) = 0.245 \\pm 0.028^{+0.019}_{-0.012} $. Using a Dalitz plot analysis of this three body decay, we find significant contributions from the channels $\\rho^0(770)\\pi^+$, $\\rho^0(1450)\\pi^+$, $f_0(980)\\pi^+$, $f_2(1270)\\pi^+$, and $f_0(1370)\\pi^+$. We present also the values obtained for masses and widths of the resonances $f_0(980)$ and $f_0(1370)$.']",['2000-07-17']
734,['eng'],"['Baringer, P', 'Bross, A', 'Büscher, V', 'Canelli, F', 'Davis, G', 'Del Signore, K', 'Desai, S V', 'Estrada, J K', 'Ginther, G', 'Gordeev, A', 'Grannis, P D', 'Grünendahl, S', 'Hou, S', 'Kotcher, J', 'Lincoln, D', 'Liu, M', 'Mayorov, A A', 'Neal, H A', 'Nunnemann, T', 'Patwa, A', 'Qian, J', 'Rijssenbeek, M', 'Rubinov, P M', 'Sawyer, L', 'Talalaevskii, A', 'Turcot, A S', 'Van Kooten, R', 'Wang, Z M', 'Warchol, J', 'Wayne, M', 'Yamin, P', 'Yip, K', 'Zhou, B']",['Cosmic ray tests of the D0 preshower detector'],['Particle Physics - Experimental Results'],"['shower detector', 'scintillation counter, plastics', 'radiation, yield', 'spatial resolution', 'efficiency', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007026'],"['The D0 preshower detector consists of scintillator strips with embedded wavelength-shifting fibers, and a readout using Visible Light Photon Counters. The response to minimum ionizing particles has been tested with cosmic ray muons. We report results on the gain calibration and light-yield distributions. The spatial resolution is investigated taking into account the light sharing between strips, the effects of multiple scattering and various systematic uncertainties. The detection efficiency and noise contamination are also investigated.']",['2000-07-17']
735,['eng'],"['Evans, H G']",['Higgs Searches at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, La Thuile 2000/02/27', 'anti-p p, colliding beams', 'Higgs particle, search for', 'electroweak interaction', 'supersymmetry', 'Higgs particle, hadroproduction', 'intermediate boson, associated production', 'Higgs particle, decay modes', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'upgrade, proposed', 'efficiency', 'proposed experiment', 'Batavia TEVATRON Coll', '1800, 2000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007024'],"['Higgs hunting is a world-wide sport and the Tevatron is set to become the next field of play when Run II starts in March 2001. To set the stage, we summarize results of searches for standard and non-standard Higgs bosons by CDF and Dzero in Run I at the Tevatron. Progress has been made in quantifying the requirements on the Tevatron Collider and on the upgraded experiments in Run II for extending the excellent work done at LEP. Armed with parameterizations of expected detector performance, the Tevatron Higgs Working group has made predictions of the sensitivity of CDF and Dzero to Higgs bosons in the Standard Model and in its Minimal Supersymmetric extension as a function of integrated luminosity. These predictions are presented to underscore the excitement being generated by Run II, and to highlight the need for the highest possible luminosity.']",['2000-07-14']
736,['eng'],"['Brook, N H']",['The Measurement of Azimuthal Asymmetries in Deep Inelastic Scattering'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'neutral current', 'charged particle, multiple production', 'hadron, angular distribution', 'angular distribution, moment', 'angular distribution, asymmetry', 'transverse momentum, dependence', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007023'],['The distribution of the azimuthal angle for the charged hadrons has been studied in the hadronic centre-of-mass system for neutral current deep inelastic positron-proton scattering at HERA. Measurements of the dependence of the moments of this distribution on the transverse momenta of the charged hadrons are presented. Asymmetries that can be unambiguously attributed to perturbative QCD processes have been observed for the first time.'],['2000-07-14']
737,['eng'],"['Jongewaard, E', 'Caryotakis, G', 'Pearson, C', 'Phillips, R M', 'Sprehn, D', 'Vlieks, A E']",['The Next Linear Collider Klystron Development Program'],['Particle Physics - Experimental Results'],"['talk, Vienna 2000/06/26', 'electron positron, linear collider', 'linear collider, proposed', 'RF system, power supply', 'microwaves, amplifier']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008038', 'http://accelconf.web.cern.ch/accelconf/e00/PAPERS/TUP3A06.pdf', 'http://www.slac.stanford.edu/econf/C000821/THA03.shtml']","['Klystrons capable of 75 MW output power at 11.4 GHz have been under development at SLAC for the last decade. The work has been part of the program to realize all the components necessary for the construction of the Next Linear Collider (NLC). The effort has produced a family of solenoid-focused 50 MW klystrons, which are currently powering a 0.5 GeV test accelerator at SLAC and several test stands, where high power components are evaluated and fundamental research is performed studying rf breakdown and dark current production. Continuing development has resulted in a Periodic Permanent Magnet (PPM) focused 50 MW klystron, tested at SLAC and subsequently contracted for manufacture by industry in England and Japan. A 75 MW version of that PPM klystron was built at SLAC and reached 75 MW, with 2.8 microsecond pulses. Based on this design, a prototype 75 MW klystron, designed for low-cost manufacture, is currently under development at SLAC, and will eventually be procured from industry in modest quantities for advanced NLC tests. Beyond these developments, the design of Multiple Beam Klystrons (MBKs) is under study at SLAC. MBKs offer the possibility of considerably lower modulator costs by producing comparable power to the klystrons now available, at much lower voltages. * This work supported by the Department of Energy under contract DE-AC03-76SF00515']",['2000-08-22']
738,['eng'],[],['Search for $\\gamma\\gamma$ decays of a Higgs boson produced in association with a fermion pair in $e^{+}e^{-}$ collisions at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'fermion, pair production', 'Higgs particle, radiative decay', 'channel cross section, branching ratio', 'mass, dependence', 'Higgs particle, mass', 'lower limit', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle fermion antifermion', 'Higgs particle --> 2photon', '88-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008004'],"['A search for gamma gamma decays of Higgs boson is performed in the data sample collected at LEP with the ALEPH detector between 1991 and 1999. This corresponds to an integrated luminosity of 672 pb-1 centre-of-mass energies ranging from 88 to 202 GeV. The search is based on topologies arising from a Higgs boson produced in association with a fermion pair via the Higgs-strahlung process e+e- -> Hffbar, with ffbar = nunubar, e+e-, mu+mu-, tau+tau- or qqbar... (CERN)']",['2000-08-04']
739,['eng'],"['Bagger, Jonathan A']",['The Case for a 500 GeV $e^{+}e^{-}$ Linear Collider'],['Particle Physics - Experimental Results'],"['electron positron, linear collider', 'linear collider, proposed', 'electron positron, annihilation', 'new particle, search for', 'Higgs particle, composite', 'supersymmetry', 'Higgs particle, mass', 'Higgs particle, decay modes', 'Higgs particle, branching ratio', 'sparticle, mass', 'slepton', 'chargino', ""Z'"", 'quark, truth', 'W, coupling', 'electroweak interaction, validity test', 'quantum gravity, higher-dimensional', 'numerical calculations', 'proposed experiment', 'bibliography', '500 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007022'],"['Several proposals are being developed around the world for an e+e- linear collider with an initial center of mass energy of 500 GeV. In this paper, we will discuss why a project of this type deserves priority as the next major initiative in high energy physics.']",['2000-07-13']
740,['eng'],"['Adler, Stephen Louis', 'Aoki, M', 'Ardebili, M', 'Atiya, M S', 'Bergbusch, P C', 'Blackmore, E W', 'Bryman, D A', 'Chiang, I H', 'Convery, M R', 'Diwan, M V', 'Frank, J S', 'Haggerty, J S', 'Inagaki, T', 'Ito, M M', 'Kabe, S', 'Kettell, S H', 'Kishi, Y', 'Kitching, P', 'Kobayashi, M', 'Komatsubara, T K', 'Konaka, A', 'Kuno, Y', 'Kuriki, M', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'MacDonald, J A', 'McPherson, R A', 'Meyers, P D', 'Mildenberger, J L', 'Muramatsu, N', 'Nakano, T', 'Numao, T', 'Poutissou, J M', 'Poutissou, R', 'Redlinger, G', 'Sato, T', 'Shinkawa, T', 'Shoemaker, F C', 'Soluk, R', 'Stone, J R', 'Strand, R C', 'Sugimoto, S', 'Witzig, C', 'Yoshimura, Y']",['Measurement of Direct Photon Emission in $K^{+} \\to \\pi^{+}pi^{0} \\gamma$ Decay'],['Particle Physics - Experimental Results'],"['K+, radiative decay', 'at rest', 'photon, direct production', 'pi+, momentum spectrum', 'energy spectrum', 'K+, branching ratio', 'amplitude analysis', 'transition, magnetic', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ pi0 photon', '0 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007021'],['We have performed a measurement of the K^+ -> pi^+ pi^0 gamma decay and have observed 2 X 10^4 events. The best fit to the decay spectrum gives a branching ratio for direct photon emission of (4.7\\pm0.8\\pm0.3) X 10^{-6} in the pi^+ kinetic energy region of 55 to 90 MeV and requires no component due to interference with inner bremsstrahlung.'],['2000-07-13']
741,['eng'],"['Arik, E', 'Mailov, A A', 'Sultansoy, S F']",['New limit for $nu_{(e)} \\to \\nu_{(tau)}$ oscillations'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'neutrino/e', 'neutrino/tau', 'neutrino, mixing angle', 'numerical calculations', 'interpretation of experiments, CERN SPS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007020'],['We present a calculation for a new limit on nu_(e)->nu_(tau) oscillations based on the recent data from CHORUS experiment'],['2000-07-12']
742,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Kolosov, V N', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the centrally produced $\\eta \\pi^{0}$ and $\\eta \\pi^{-}$ systems in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'central region', 'eta, hadroproduction', 'pi, associated production', 'mass spectrum, (eta pi0)', 'mass spectrum, (eta pi-)', 'partial wave analysis', 'a0(980)', 'a2(1320)', 'transverse momentum, dependence', 'angular dependence', 'momentum transfer, dependence', 'magnetic detector, OMEGA', 'experimental results', 'CERN LEP Stor', 'p p --> 2p eta pi0', 'p p --> Delta(1232)++ eta pi-', '450 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007019'],"['A partial wave analysis of the centrally produced eta pi0 and eta pi- channels has been performed in pp collisions using an incident beam momentum of 450 GeV/c. Clear a0(980) and a2(1320) signals have been observed in S and D+ waves respectively. The dPT, phi and |t| distributions of these resonances are presented.']",['2000-07-12']
743,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Ward, J J', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the Low-x Behaviour of the Photon Structure Function $F2-\\gamma$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'hadron, multiple production', 'photon, structure function', 'structure function, parametrization', 'small-x', 'x-dependence', 'momentum transfer, dependence', 'mass, hadronic', 'numerical calculations, Monte Carlo', 'statistical analysis', 'tables', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '91, 183 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007018'],"['The photon structure function F2-gamma(x,Q**2) has been measured using data taken by the OPAL detector at centre-of-mass energies of 91Gev, 183Gev and 189Gev, in Q**2 ranges of 1.5 to 30.0 GeV**2 (LEP1), and 7.0 to 30.0 GeV**2 (LEP2), probing lower values of x than ever before. Since previous OPAL analyses, new Monte Carlo models and new methods, such as multi-variable unfolding, have been introduced, reducing significantly the model dependent systematic errors in the measurement.']",['2000-07-12']
744,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']","['Multiplicities of $\\pi^{0}$, $\\eta$, $K^{0}$ and of charged particles in quark and gluon jets']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'quark, jet', 'gluon, jet', 'hadron, multiplicity', 'charged particle', 'pi0', 'eta', 'K0', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007017'],"['We compared the multiplicities of pizero, eta, Kzero and of charged particles in quark and gluon jets in 3-jet events, as measured by the OPAL experiment at LEP. The comparisons were performed for distributions unfolded to 100% pure quark and gluon jets, at an effective scale Qjet which took into account topological dependences of the 3-jet environment. The ratio of particle multiplicity in gluon jets to that in quark jets as a function of Qjet for pizero, eta and Kzero was found to be independent of the particle species. This is consistent with the QCD prediction that the observed enhancement in the mean particle rate in gluon jets with respect to quark jets should be independent of particle species. In contrast to some theoretical predictions and previous observations, we observed no evidence for an enhancement of eta meson production in gluon jets with respect to quark jets, beyond that observed for charged particles. We measured the ratio of the slope of the average charged particle multiplicity in gluon jets to that in quark jets, C, and we compared it to a next-to-next-to-next-to leading order calculation. Our result, C=2.27+-0.20(stat+syst),is about one standard deviation higher than the perturbative prediction.']",['2000-07-12']
745,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for Trilinear Neutral Gauge Boson Couplings in $Z-\\gamma$ production at $\\sqrt{s}$=189 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'photon, associated production', 'coupling, (3gauge boson)', 'Z0, hadronic decay', 'Z0, leptonic decay', 'neutrino, pair production', 'channel cross section', 'photon, energy spectrum', 'photon, angular distribution', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007016'],"['The data recorded at a centre-of-mass energy of 189GeV by the OPAL detector at LEP are used to search for trilinear couplings of the neutral gauge bosons in the process e+e- --> Z-gamma. The cross-sections are measured for multihadronic events with an energetic isolated photon and for events with a high energy photon accompanied by missing energy. These cross-sections and the photon energy, polar angle and isolation angle distributions are compared to the Standard Model predictions and to the theoretical expectations of a model allowing for Z-gamma-Z and Z-gamma-gamma vertices. Since no significant deviations with respect to the Standard Model expectations are found, constraints are derived on the strength of neutral trilinear gauge couplings.']",['2000-07-12']
746,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['First Measurement of the Inclusive Branching Ratio of b Hadrons $\\to \\phi$ Mesons in $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'beautiful meson, cascade decay', 'B, branching ratio', 'upper limit', 'B/s', 'Phi(1020), yield', 'Phi(1020), hadronic decay', 'mass spectrum, (K+ K-)', 'Phi(1020), momentum spectrum', 'quark, fragmentation', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'beautiful meson --> Phi(1020) anything', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007015'],"['The inclusive production rate of phi mesons from the decay of b hadrons produced in Z0 decays was measured to be Br(b->phi+X) = 0.0282+-0.0013(stat.)+-0.0019(syst.), using data collected by the OPAL detector at LEP.']",['2000-07-12']
747,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Searches for prompt light gravitino signatures in $e^{+}e^{-}$ Collisions at $\\sqrt{s}$ = 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'gravitino, LSP', 'supersymmetry, symmetry breaking', 'sparticle, mass', 'lower limit', 'sparticle, pair production', 'sparticle, decay', 'slepton', 'chargino', 'neutralino', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007014'],"['Searches for final states expected in models with light gravitinos have been performed, including experimental topologies with multi-leptons with missing energy, leptons and photons with missing energy, and jets and photons with missing energy. No excess over the expectations from the Standard Model has been observed. Limits are placed on production cross-sections in the different experimental topologies. Additionally, combining with searches for the anomalous production of lepton and photon pairs with missing energy results are interpreted in the context of minimal models of gauge mediated SUSY breaking. Exclusion limits are established at the 95% confidence level on the supersymmetric particle masses; m-slepton > 70GeV and m-neutralino > 85GeV for tan(beta)=2, m-stau > 76GeV, m-selectron,-smu > 93GeV and m-neutralino > 76GeV for tan(beta)=20.']",['2000-07-10']
748,['eng'],"['Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J']",['Study of B Decays to Charmonium States $B \\to \\eta_{c}K$ and $B \\to \\chi_{c0}K$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'quarkonium, charm', 'eta/c(2980)', 'chi/c0(3415)', 'B+, branching ratio', 'B0, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> eta/c(2980) K', 'B --> chi/c0(3415) K', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007012'],"['In a sample of $9.66\\times 10^6 B\\bar{B}$ pairs collected with the CLEO detector we make the first observation of B decays to an $\\eta_c$ and a kaon. We measure branching fractions $BR(B^+\\to\\eta_c K^+) = (0.69 + 0.26 - 0.21 +- 0.08 +- 0.20)\\times 10^{-3}$ and $BR(B^0\\to\\eta_c K^0) = (1.09 + 0.55 - 0.42 +- 0.12 +- 0.31)\\times 10^{-3}$, where the first error is statistical, the second is systematic and the third is from the $\\eta_c$ branching fraction uncertainty. From these we extract the $\\eta_c$ decay constant in the factorization approximation, $f_{\\eta_c} = 335 +- 75$ MeV. We also search for B decays to a $\\chi_{c0}$ and a kaon. No evidence for a signal is found and we set 90% CL upper limits: $BR(B^+\\to\\chi_{c0} K^+) < 4.8\\times 10^{-4}$ and $BR(B^0\\to\\chi_{c0} K^0) < 5.0\\times 10^{-4}$.']",['2000-07-10']
749,['eng'],"['Wing, M']",['High $E_{T}$ photoproduction and the photon strucure'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'final state, (2jet)', 'transverse energy, high', 'channel cross section, transverse momentum', 'angular distribution', 'quantum chromodynamics, perturbation theory', 'photon, structure function', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007011'],['Dijet photoproduction results are presented from the H1 and ZEUS collaborations and compared to next-to-leading order pQCD calculations.'],['2000-07-07']
750,['eng'],"['Braccini, S']",['Resonance Formation in Two-Photon Collisions'],['Particle Physics - Experimental Results'],"['talk, Cracow 2000/05/19', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, exclusive reaction', 'meson resonance, photoproduction', 'meson resonance, width', 'mass spectrum', 'pseudoscalar meson, form factor', 'glueball, search for', 'f2(1525)', 'f4(2220)', 'f0(1500)', 'f2(1270)', 'f0(1710)', 'quarkonium, charm', 'experimental results', 'CERN LEP Stor', 'Cornell CESR Stor', 'electron positron --> pi+ pi- pi0 positron electron', 'electron positron --> K0(S) K pi positron electron', 'electron positron --> pi+ pi- photon positron electron', 'electron positron --> eta pi+ pi- positron electron', 'electron positron --> 2K0(S) positron electron', 'electron positron --> pi+ pi- positron electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007010'],['Two-photon collisions at the e$^+$e$^-$ colliders allow to investigate the formation and the properties of resonant states in a very clean experimental environment. A remarkable number of new results have been recently obtained giving important contributions to meson spectroscopy and glueball searches. The most recent results from the LEP collider at CERN and CESR at Cornell are reviewed here.'],['2000-07-07']
751,['eng'],"['Çiftçi, A K', 'Sultansoy, S F', 'Yavas, O']",['TESLA*HERA Based $\\gamma-p$ and $\\gamma-A$ Colliders'],['Particle Physics - Experimental Results'],"['talk, Hamburg 2000/06/14', 'electron positron, linear collider', 'linear collider, proposed', 'proton synchrotron', 'photon p, colliding beams', 'photon nucleus, colliding beams', 'luminosity', 'p, polarized beam', 'nucleus, polarized beam', 'DESY HERA Stor', 'DESY Lab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007009'],"['Main parameters and physics search potential of gamma-p and gamma-A colliders, which will be available due to constructing the TESLA linear electron-positron collider tangentially to the HERA proton ring, are discussed.']",['2000-07-06']
752,['eng'],"['Mikocki, S']",['Search for QCD Instanton-Induced Processes in Deep-Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'quantum chromodynamics', 'instanton, effect', 'jet, transverse energy', 'charged particle, multiplicity', 'sphericity', 'momentum transfer, spectra', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007008'],"['Preliminary H1 results on dedicated searches for QCD instanton induced processes in DIS are presented. The investigations are based on the expected characteristics of their hadronic final state. Searches were performed in the kinematical region x > 0.001, 0.1 < y < 0.6 and the polar angle of scattered positron greater than 156 degrees.']",['2000-07-06']
753,['eng'],"['Ziegler, M', 'Sievers, P', 'Straumann, U']",['A triple GEM detector with two dimensional readout'],['Particle Physics - Experimental Results'],"['tracks', 'drift chamber, gas', 'argon, organic compounds', 'electrode, plastics', 'electronics, readout', 'electric field', 'efficiency', 'spatial resolution', 'magnetic detector, LHC-B', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007007'],"['The triple GEM detector is a micropattern gas detector which consists of a primary ionisation gap and three consecutive gas electron multiplier (GEM) foils. A printed circuit board with readout strips detects the current induced by the drifting electron cloud originating from the last GEM stage. Thus the gas amplification and the signal readout are completely separated. Triple GEM detectors are being developed as a possible technology for the inner tracking in the LHCb experiment. In an earlier note we have reported first experience with such a detector in a test beam at PSI. Here we describe the construction of an improved version (thinner transfer gaps, segmented GEM foils, two dimensional readout). Results from performance measurements are presented using intense hadronic beams as well as cosmic ray data.']",['2000-07-05']
754,['eng'],"['Mambriani, G', 'Trentadue, L G']",['Testing CP Conservation at KLOE'],['Particle Physics - Experimental Results'],"['K0(L), hadronic decay', 'CP, invariance', 'external field, scalar', 'gravitation, geophysics', 'K0 anti-K0', 'magnetic detector, KLOE', 'proposed experiment, Frascati Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007004'],"['A proposal for maintaining CP conservation in $K_{L}^{0}$ decays is resumed, by adding a heterodox hypothesis. One recovers a consistent picture with a $2\\pi$ $K_{L}^{0}$ decay branching ratio proportional to the vertical $K_{L}^{0}$ displacement. This can be clearly tested at the KLOE experiment, where important vertical $K_{L}^{0}$ displacements occur.']",['2000-07-04']
755,['eng'],"['Iashvili, I']",['MSSM SUSY Searches at LEP2'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'supersymmetry', 'R parity, invariance', 'sparticle, search for', 'sparticle, pair production', 'slepton', 'squark', 'chargino', 'neutralino', 'sparticle, mass', 'lower limit', 'experimental results', 'CERN LEP Stor', '192-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007001'],"['The status of SUSY searches at LEP2 up to centre-of-mass energy of 202 GeV is presented. Search strategies for sleptons, squarks, charginos and neutralinos are discussed in the framework of Minimal Supersymmetric Standard Model with R-parity conservation. With no indication for the production of these particles new limits are set on their masses.']",['2000-07-04']
756,['eng'],"['Lai, A', 'Marras, D', 'Bevan, A', 'Dosanjh, R S', 'Gershon, T J', 'Hay, B', 'Kalmus, George Ernest', 'Lazzeroni, C', 'Munday, D J', 'Needham, M D', 'Olaiya, E', 'Parker, M A', 'White, T O', 'Wotton, S A', 'Barr, Giles David', 'Bocquet, G', 'Ceccucci, Augusto', 'Çuhadar-Dönszelmann, T', 'Cundy, Donald C', ""D'Agostini, G"", 'Debu, P', 'Doble, Niels T', 'Falaleev, V P', 'Gatignon, L', 'Gonidec, A', 'Gorini, B', 'Govi, G', 'Grafström, P', 'Kubischta, W', 'Lacourt, A', 'Lenti, M', 'Norton, Alan Robert', 'Palestini, S', 'Panzer-Steindel, B', 'Tatishvili, G T', 'Taureg, Hans', 'Velasco, M', 'Wahl, H', 'Cheshkov, C', 'Gaponenko, A N', 'Khristov, P Z', 'Kekelidze, V D', 'Madigozhin, D T', 'Molokanova, N A', 'Potrebenikov, Yu K', 'Tkachev, A L', 'Zinchenko, A I', 'Knowles, I', 'Martin, V', 'Sacco, R', 'Walker, A', 'Contalbrigo, M', 'Dalpiaz, P F', 'Duclos, J', 'Frabetti, P L', 'Gianoli, A', 'Martini, M', 'Petrucci, F', 'Savrié, M', 'Bizzeti, A', 'Calvetti, M', 'Collazuol, G', 'Graziani, G', 'Iacopini, E']",['Measurement of the $K_{L} \\to e^{+} e^{-} e^{+} e^{-}$ Decay Rate'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'K0(L), secondary beam', 'K0(L), semileptonic decay', 'electron, multiple production', 'K0(L), branching ratio', 'magnetic spectrometer, experimental results', 'CERN SPS', 'K0(L) --> 2positron 2electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006040'],"['The decay rate of the neutral long-lived K meson into the e+ e- e+ e- final state has been measured with the NA48 detector at the CERN SPS. Using data collected in 1999, a total of 132 events has been observed with negligible background. The total number of kaons was determined to be 5.1 x 10^10. This observation corresponds to a preliminary branching ratio of Gamma(K_L -> e+ e- e+ e-)/Gamma(K_L -> all) = (3.67 +- 0.32(stat) +- 0.23(sys) +- 0.08(norm)) x 10^-8, where the first error is statistical, the second systematic, and the third error is due to the uncertainty in the normalization.']",['2000-07-03']
757,['eng'],"['Adinolfi, M', 'Aloisio, A', 'Ambrosino, F', 'Andryakov, A', 'Antonelli, A', 'Antonelli, M', 'Anulli, F', 'Bacci, Cesare', 'Bankamp, A', 'Barbiellini, Guido', 'Bellini, F', 'Bencivenni, G', 'Bertolucci, S', 'Bini, C', 'Bloise, C', 'Bocci, V', 'Bossi, F', 'Branchini, P', 'Bulychjov, S A', 'Cabibbo, G', 'Calcaterra, A', 'Caloi, R M', 'Campana, P', 'Capon, G', 'Carboni, G', 'Cardini, A', 'Casarsa, M', 'Cataldi, G', 'Ceradini, F', 'Cervelli, F', 'Cevenini, F', 'Chiefari, G', 'Ciambrone, P', 'Conetti, S', 'De Lucia, E', 'De Robertis, G', 'De Sangro, R', 'De Simone, P', 'De Zorzi, G', ""Dell'Agnello, S"", 'Denig, A', 'Di Domenico, A', 'Di Donato, C', 'Di Falco, S', 'Doria, A', 'Drago, E', 'Elia, V', 'Erriquez, O', 'Farilla, A', 'Felici, G', 'Ferrari, A', 'Ferrer, M L', 'Finocchiaro, G', 'Forti, C', 'Franceschi, A', 'Franzini, P', 'Gao, M L', 'Gatti, C', 'Gauzzi, P', 'Giovannella, S', 'Golovatyuk, V M', 'Gorini, E', 'Grancagnolo, F', 'Grandegger, W', 'Graziani, E', 'Guarnaccia, P', 'Von Hagel, U', 'Han, H G', 'Han, S W', 'Huang, X', 'Incagli, M', 'Ingrosso, L', 'Jiang, Y Y', 'Kim, W', 'Kluge, W', 'Kulikov, V', 'Lacava, F', 'Lanfranchi, G', 'Lee-Franzini, Juliet', 'Lomtadze, T A', 'Luisi, C', 'Mao Chen Sheng', 'Martemyanov, M', 'Martini, A', 'Matsyuk, M', 'Mei, W', 'Merola, L', 'Messi, R', 'Miscetti, S', 'Moalem, A', 'Moccia, S', 'Moulson, M', 'Müller, S', 'Murtas, F', 'Napolitano, M', 'Nedosekin, A A', 'Panareo, M', 'Pacciani, L', 'Pages, P', 'Palutan, M', 'Paoluzi, L', 'Pasqualucci, E', 'Passalacqua, L', 'Passaseo, M', 'Passeri, A', 'Patera, V', 'Petrolo, E', 'Petrucci, G', 'Picca, D', 'Pirozzi, G', 'Pistillo, C', 'Pollack, M E', 'Pontecorvo, L', 'Primavera, M', 'Ruggieri, F', 'Santangelo, P', 'Santovetti, E', 'Saracino, G', 'Schamberger, R D', 'Schwick, C', 'Sciascia, B', 'Sciubba, A', 'Scuri, F', 'Sfiligoi, I', 'Shan, J', 'Silano, P', 'Spadaro, T', 'Spagnolo, S', 'Spiriti, E', 'Stanescu, C', 'Tong, G L', 'Tortora, L', 'Valente, E', 'Valente, P', 'Valeriani, B', 'Venanzoni, G', 'Veneziano, Stefano', 'Wu, Y', 'Xie, Y G', 'Zhao, P P', 'Zhou, Y']",['Novel DAQ and Trigger Methods for the KLOE experiment'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'data acquisition', 'trigger', 'time resolution', 'electronics', 'calorimeter', 'drift chamber', 'programming', 'magnetic detector, KLOE', 'Frascati Stor']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006039', 'http://arXiv.org/abs/hep-ex/?0006039']","['KLOE, a new state of the art detector recently commissioned for physics operation at DAFNE, has many innovative interesting features, especially in the DAQ and Trigger areas. Custom electronics assert a trigger in a 2 microseconds decision time and distributes it to the FEE with a 50 ps time resolution. Data are read out using 10 front-end data acquisition chains and sent to a farm of online servers through a FDDI Gigaswitch. This design of the KLOE DAQ system allows us to manage an input data rate as high as 50 Mbyte/s, and is completely scalable by extending the number of computers connected to the switch.']",['2000-07-03']
758,['eng'],"['Giacomelli, Giorgio']",['Total Cross Sections'],['Particle Physics - Experimental Results'],"['talk', 'particle physics', 'hadron hadron, interaction', 'hadron nucleus, interaction', 'total cross section, measurement', 'energy dependence', 'experimental methods', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006038'],['The measurements of the hadron-hadron total cross sections are the first measurements performed when a new hadron accelerator opens up a new energy region; the measurements were made as function of the incoming beam momentum or c.m. energy and have often been repeated with improved accuracy and finer energy spacing.'],['2000-07-03']
759,['eng'],"['Kulyavtsev, A I', 'Procario, M', 'Russ, J', 'You, J', 'Cumalat, J P', 'Appel, J A', 'Brown, C N', 'Butler, J', 'Cheung, H', 'Christian, D', 'Chiodini, G', 'Cihangir, S', 'Gaines, I', 'Garbincius, P H', 'Garren, L A', 'Gottschalk, E E', 'Jackson, G', 'Kasper, P', 'Kasper, P H', 'Kutschke, R', 'Kwan, S W', 'Lebrun, Philippe.', 'McBride, P', 'Stutte, L', 'Yarba, J V', 'Avery, P', 'Lohner, M', 'Burnstein, R A', 'Kaplan, D M', 'Lederman, L M', 'Rubin, H A', 'White, C', 'Kim, D', 'Selen, M', 'Wiss, J', 'Rust, R W', 'Gardner, D R', 'Casimiro, E', 'Menasce, D', 'Moroni, L', 'Pedrini, D', 'Sala, S', 'Boca, G', 'Liguori, G', 'Torre, P', 'Derevshchikov, A A', 'Goncharenko, Yu M', 'Khodyrev, V Yu', 'Meshchanin, A P', 'Nogach, L V', 'Shestermanov, K E', 'Soloviev, L F', 'Vasilev, A N', 'Newsom, C R', 'Kubota, Y', 'Poling, R A', 'Speakman, A', 'Smith, B', 'Chen, T Y', 'Papavassiliou, V', 'Honscheid, K', 'Kagan, H', 'Selove, W', 'López, A', 'Coan, T E', 'Alam, M', 'Yu, X Q', 'He, M', 'Shapiro, S', 'Artuso, M', 'Majumder, G', 'Mountain, R', 'Skwarnicki, T', 'Stone, S', 'Wang, J C', 'Wolf, A', 'Cho, K', 'Mitchell, T', 'Handler, R', 'Napier, A', 'Koetke, D D', 'Johns, W', 'Sheldon, P', 'Stenson, K', 'Webster, M', 'Sheaff, M', 'Slaughter, J', 'Menary, S R']","['BTeV - an Experiment to Measure Mixing, CP Violation, and Rare Decays of Beauty and Charm at the Fermilab Collider']",['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'anti-p p, colliding beams', 'quark, pair production', 'quark, charm', 'quark, beauty', 'CP, violation', 'Kobayashi-Maskawa angle', 'beautiful meson, decay modes', 'magnetic detector, proposed', 'forward spectrometer', 'semiconductor detector, pixel', 'semiconductor detector, vertex', 'trigger', 'calorimeter, electromagnetic', 'data acquisition', 'particle identification', 'numerical calculations, Monte Carlo', 'Batavia TEVATRON Coll']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006037', 'http://arXiv.org/abs/hep-ex/?0006037']",['We discuss the physics goals and rationale for a detector to study Beauty and Charm decays in the forward direction at the Fermilab Tevatron Collider. We then describe the BTeV detector which has been designed to achieve these goals and present its physics reach based on extensive simulation. We conclude by comparing BTeV to other experiments designed to explore similar topics.'],['2000-07-03']
760,['eng'],"['Adinolfi, M', 'Aloisio, A', 'Ambrosino, F', 'Andryakov, A', 'Antonelli, A', 'Antonelli, M', 'Anulli, F', 'Bacci, Cesare', 'Bankamp, A', 'Barbiellini, Guido', 'Bellini, F', 'Bencivenni, G', 'Bertolucci, S', 'Bini, C', 'Bloise, C', 'Bocci, V', 'Bossi, F', 'Branchini, P', 'Bulychjov, S A', 'Cabibbo, G', 'Calcaterra, A', 'Caloi, R M', 'Campana, P', 'Capon, G', 'Carboni, G', 'Cardini, A', 'Casarsa, M', 'Cataldi, G', 'Ceradini, F', 'Cervelli, F', 'Cevenini, F', 'Chiefari, G', 'Ciambrone, P', 'Conetti, S', 'De Lucia, E', 'De Robertis, G', 'De Sangro, R', 'De Simone, P', 'De Zorzi, G', ""Dell'Agnello, S"", 'Denig, A', 'Di Domenico, A', 'Di Donato, C', 'Di Falco, S', 'Doria, A', 'Drago, E', 'Elia, V', 'Erriquez, O', 'Farilla, A', 'Felici, G', 'Ferrari, A', 'Ferrer, M L', 'Finocchiaro, G', 'Forti, C', 'Franceschi, A', 'Franzini, P', 'Gao, M L', 'Gatti, C', 'Gauzzi, P', 'Giovannella, S', 'Golovatyuk, V M', 'Gorini, E', 'Grancagnolo, F', 'Grandegger, W', 'Graziani, E', 'Guarnaccia, P', 'Hagel, U v', 'Han, H G', 'Han, S W', 'Huang, X', 'Incagli, M', 'Ingrosso, L', 'Jiang, Y Y', 'Kim, W', 'Kluge, W', 'Kulikov, V', 'Lacava, F', 'Lanfranchi, G', 'Lee-Franzini, Juliet', 'Lomtadze, T A', 'Luisi, C', 'Mao Chen Sheng', 'Martemyanov, M', 'Martini, A', 'Matsyuk, M', 'Mei, W', 'Merola, L', 'Messi, R', 'Miscetti, S', 'Moalem, A', 'Moccia, S', 'Moulson, M', 'Müller, S', 'Murtas, F', 'Napolitano, M', 'Nedosekin, A A', 'Panareo, M', 'Pacciani, L', 'Pages, P', 'Palutan, M', 'Paoluzi, L', 'Pasqualucci, E', 'Passalacqua, L', 'Passaseo, M', 'Passeri, A', 'Patera, V', 'Petrolo, E', 'Petrucci, G', 'Picca, D', 'Pirozzi, G', 'Pistillo, C', 'Pollack, M E', 'Pontecorvo, L', 'Primavera, M', 'Ruggieri, F', 'Santangelo, P', 'Santovetti, E', 'Saracino, G', 'Schamberger, R D', 'Schwick, C', 'Sciascia, B', 'Sciubba, A', 'Scuri, F', 'Sfiligoi, I', 'Shan, J', 'Silano, P', 'Spadaro, T', 'Spagnolo, S', 'Spiriti, E', 'Stanescu, C', 'Tong, G L', 'Tortora, L', 'Valente, E', 'Valente, P', 'Valeriani, B', 'Venanzoni, G', 'Veneziano, Stefano', 'Wu, Y', 'Xie, Y G', 'Zhao, P P', 'Zhou, Y']",['KLOE first results on hadronic physics'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), hadroproduction', 'Phi(1020), radiative decay', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'pi', 'eta', 'eta(958)', 'pseudoscalar meson, radiative decay', 'f0(975), hadronic decay', 'a0(980)', 'photon, energy spectrum', 'mixing angle, (eta(958) eta)', 'magnetic detector, KLOE', 'experimental results', 'Frascati Stor', 'Phi(1020) --> pseudoscalar meson photon', 'Phi(1020) --> 2pseudoscalar meson photon', 'Phi(1020) --> scalar meson photon', 'Phi(1020) --> pi+ pi- pi0']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006036', 'http://arXiv.org/abs/hep-ex/?0006036']","[""The KLOE detector at DAFNE, the Frascati Phi-factory, has collected about 8 millions phi decays in 1999. Measurements of Phi decays into pi0, eta, eta', f0(980), a0(980) and pi+pi-pi0 have been performed with statistical accuracy better than previously in a single detector, as well as new decay modes. Phi radiative decays can clarify the nature of f0 and a0 (are they 4 quark states?) and measure the eta-eta' mixing angle. Analysis of Phi->pi+pi-pi0 allows us to extract the possible existence of direct decay in addition to the dominant rho-pi mode and to obtain a precise measurement of the rho parameters such as the mass difference between the charged and neutral rho, previously never seen.""]",['2000-06-30']
761,['eng'],"['Adinolfi, M', 'Aloisio, A', 'Ambrosino, F', 'Andryakov, A', 'Antonelli, A', 'Antonelli, M', 'Anulli, F', 'Bacci, Cesare', 'Bankamp, A', 'Barbiellini, Guido', 'Bellini, F', 'Bencivenni, G', 'Bertolucci, S', 'Bini, C', 'Bloise, C', 'Bocci, V', 'Bossi, F', 'Branchini, P', 'Bulychjov, S A', 'Cabibbo, G', 'Calcaterra, A', 'Caloi, R M', 'Campana, P', 'Capon, G', 'Carboni, G', 'Cardini, A', 'Casarsa, M', 'Cataldi, G', 'Ceradini, F', 'Cervelli, F', 'Cevenini, F', 'Chiefari, G', 'Ciambrone, P', 'Conetti, S', 'De Lucia, E', 'De Robertis, G', 'De Sangro, R', 'De Simone, P', 'De Zorzi, G', ""Dell'Agnello, S"", 'Denig, A', 'Di Domenico, A', 'Di Donato, C', 'Di Falco, S', 'Doria, A', 'Drago, E', 'Elia, V', 'Erriquez, O', 'Farilla, A', 'Felici, G', 'Ferrari, A', 'Ferrer, M L', 'Finocchiaro, G', 'Forti, C', 'Franceschi, A', 'Franzini, P', 'Gao, M L', 'Gatti, C', 'Gauzzi, P', 'Giovannella, S', 'Golovatyuk, V M', 'Gorini, E', 'Grancagnolo, F', 'Grandegger, W', 'Graziani, E', 'Guarnaccia, P', 'Hagel, U v', 'Han, H G', 'Han, S W', 'Huang, X', 'Incagli, M', 'Ingrosso, L', 'Jiang, Y Y', 'Kim, W', 'Kluge, W', 'Kulikov, V', 'Lacava, F', 'Lanfranchi, G', 'Lee-Franzini, Juliet', 'Lomtadze, T A', 'Luisi, C', 'Mao Chen Sheng', 'Martemyanov, M', 'Martini, A', 'Matsyuk, M', 'Mei, W', 'Merola, L', 'Messi, R', 'Miscetti, S', 'Moalem, A', 'Moccia, S', 'Moulson, M', 'Müller, S', 'Murtas, F', 'Napolitano, M', 'Nedosekin, A A', 'Panareo, M', 'Pacciani, L', 'Pages, P', 'Palutan, M', 'Paoluzi, L', 'Pasqualucci, E', 'Passalacqua, L', 'Passaseo, M', 'Passeri, A', 'Patera, V', 'Petrolo, E', 'Petrucci, G', 'Picca, D', 'Pirozzi, G', 'Pistillo, C', 'Pollack, M E', 'Pontecorvo, L', 'Primavera, M', 'Ruggieri, F', 'Santangelo, P', 'Santovetti, E', 'Saracino, G', 'Schamberger, R D', 'Schwick, C', 'Sciascia, B', 'Sciubba, A', 'Scuri, F', 'Sfiligoi, I', 'Shan, J', 'Silano, P', 'Spadaro, T', 'Spagnolo, S', 'Spiriti, E', 'Stanescu, C', 'Tong, G L', 'Tortora, L', 'Valente, E', 'Valente, P', 'Valeriani, B', 'Venanzoni, G', 'Veneziano, Stefano', 'Wu, Y', 'Xie, Y G', 'Zhao, P P', 'Zhou, Y']",['First results from $\\phi \\to K_{L}K_{S}$ decays with the KLOE detector'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), hadronic decay', 'K0, pair production', 'K0, hadronic decay', 'K0(L)', 'K0(S), regeneration', 'dependence, mass number', 'K0(S), lifetime', 'decay, path length', 'angular distribution', 'magnetic detector, KLOE', 'experimental results', 'Frascati Stor', 'Phi(1020) --> K0(L) K0(S)', 'K0(L) --> pi+ pi-']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006035', 'http://arXiv.org/abs/hep-ex/?0006035']","['The KLOE experiment has collected 2.4 1/pb of integrated luminosity during the commissioning of the DAFNE phi-factory in 1999. The performance of the detector has been studied using phi -> KL KS decays collected during this period, yielding also first measurements of relevant K parameters such as masses and lifetimes. A clean Kshort -> pi+ pi- sample is used to select Klong -> 2pi CP-violating decays and Klong -> Kshort regeneration events in the detector material. Results on the regeneration probability in beryllium-alluminum alloy and carbon-fiber plus aluminum composite are presented.']",['2000-06-30']
762,['eng'],"['Altmann, M', 'Balata, M', 'Belli, P', 'Bellotti, E', 'Bernabei, R', 'Burkert, E', 'Cattadori, C', 'Cerichelli, G', 'Chiarini, M', 'Cribier, M', 'Re, G D', 'Ebert, K H', 'Von Feilitzsch, F', 'Ferrari, N', 'Hampel, W', 'Handt, J', 'Henrich, E', 'Heusser, G', 'Kiko, J', 'Kirsten, T', 'Lachenmaier, T', 'Lanfranchi, J', 'Laubenstein, M', 'Motta, D', 'Rau, W', 'Richter, H', 'Wänninger, S', 'Wójcik, M', 'Zanotti, L']",['GNO Solar Neutrino Observations'],['Particle Physics - Experimental Results'],"['neutrino, solar', 'neutrino nucleus, nuclear reaction', 'gallium', 'neutrino, flux', 'deep underground detector, GNO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006034'],"['We report the first GNO solar neutrino results for the measuring period GNOI, solar exposure time May 20, 1998 till January 12, 2000. In the present analysis, counting results for solar runs SR1 - SR19 were used till April 4, 2000. With counting completed for all but the last 3 runs (SR17 - SR19), the GNO I result is [65.8 +10.2 -9.6 (stat.) +3.4 -3.6 (syst.)]SNU (1sigma) or [65.8 + 10.7 -10.2 (incl. syst.)]SNU (1sigma) with errors combined. This may be compared to the result for Gallex(I-IV), which is [77.5 +7.6 -7.8 (incl. syst.)] SNU (1sigma). A combined result from both GNOI and Gallex(I-IV) together is [74.1 + 6.7 -6.8 (incl. syst.)] SNU (1sigma).']",['2000-06-30']
763,['eng'],"['Frlez, E', 'Wright, B K', 'Pocanic, D']",['Optics'],['Particle Physics - Experimental Results'],"['scintillation counter, crystal', 'cesium, iodine', 'scintillation counter, plastics', 'radiation, spectra', 'optics, absorption', 'programming, Monte Carlo', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006033'],"['We present the program optics that simulates the light response of an arbitrarily shaped scintillation particle detector. Predicted light responses of pure CsI polygonal detectors, plastic scintillator staves, cylindrical plastic target scintillators and a Plexiglas light-distribution plate are illustrated. We demonstrate how different bulk and surface optical properties of a scintillator lead to specific volume and temporal light collection probability distributions. High-statistics optics simulations are calibrated against the detector responses measured in a custom-made cosmic muon tomography apparatus. The presented code can also be used to track particles intersecting complex geometrical objects.']",['2000-06-28']
764,['eng'],"['Nisius, R', 'Haas, D', 'Grupen, Claus']",['Hadronic Structure Functions of the Photon Measured at LEP'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'exchange, two-photon', 'photon photon, interaction', 'hadron, multiple production', 'photon, structure function', 'x-dependence', 'momentum transfer, dependence', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006032'],['The measurements of hadronic structure functions of the photon based on the reaction ee --> ee gamma^(*)(P^2) gamma^*(Q^2)--> ee hadrons are discussed.'],['2000-06-28']
765,['eng'],"['Sarazin, X']",['Status Report on the double-$\\beta$ decay experiment NEMO-3'],['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'talk, Sudbury 2000/06/16', 'double-beta decay, (0neutrino)', 'drift chamber', 'calorimeter', 'magnet, solenoid', 'performance', 'efficiency', 'energy resolution', 'background', 'deep underground detector, Frejus']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006031', 'http://arXiv.org/abs/hep-ex/?0006031']","[""The NEMO collaboration is presently mounting the NEMO-3 detector in the Fr\\'ejus Underground Laboratory. This detector, which will be completed by the end of the year 2000, is devoted to the search of neutrinoless double beta decay with various isotopes. Much attention has been focused on ^{100}Mo and ^{82}Se with their large Q_{\\beta\\beta}-values. The detector is based on the direct detection of the two electrons by a tracking device and on the measurement of their energies by a calorimeter. The aim of the experiment is to have a sensitivity for the effective neutrino mass on the order of 0.1 eV. The status and the expected performance of the NEMO-3 detector for both internal and external background rejections and for signal detection are presented.""]",['2000-06-27']
766,['eng'],"['Çiftçi, A K', 'Sultansoy, S F', 'Yavas, O']","['Linac*LHC Based $ep, \\gamma p, eA, \\gamma A$ and $FEL\\gamma-A$ Colliders']",['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'photon p, colliding beams', 'electron nucleus, colliding beams', 'photon nucleus, colliding beams', 'colliding beams, proposed', 'electron, linear accelerator', 'luminosity', 'Compton scattering, backscatter', 'free electron laser', 'numerical calculations', 'CERN LHC Coll']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006030', 'http://arXiv.org/abs/hep-ex/?0006030']","['Main parameters and physics goals of different colliders, which can be realized if a special 1 TeV energy linear electron accelerator or corresponding linear collider is constructed tangential to LHC, are discussed. It is shown that L_(ep)=10^(32)cm^(-2)s^(-1) at sqrt(s_(ep))=5.29 TeV can be achieved within moderate upgrade of LHC parameters. Then, Gamma-p collider with he same luminosity and sqrt(s)=4.82 TeV can be realized using Compton backscattering of laser beam off the electron beam. Concerning the nucleus beam, L*A=10^(31)cm^(-2)s^(-1) can be achieved at least for light and medium nuclei for both eA and Gamma-A options. Finally, colliding of FEL beam from an electron linac and nucleus beam from LHC will give a new opportunity to investigate nuclear spektroscopy and photo-nuclei reactions.']",['2000-06-26']
767,['eng'],"['Filkov, L V', 'Kashevarov, V L', 'Konobeevski, E S', 'Mordovskoy, M V', 'Potashev, S Yu', 'Simonov, V A', 'Skorkin, V M', 'Zuev, S V']",['Evidence for supernarrow dibaryons observed in pd interactions'],['Particle Physics - Experimental Results'],"['p deuteron, interaction', 'baryon resonance, search for', 'narrow resonance, dibaryon', 'mass spectrum, missing-mass', 'angular dependence', 'baryon resonance, radiative decay', 'baryon resonance, mass', 'fermion, statistics', 'magnetic spectrometer, experimental results', 'p deuteron --> p anything', 'p deuteron --> 2p anything', '0.305 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006029'],"['An analysis of new experimental data, obtained at Linear Accelerator of INR, is carried out with the aim of searching for supernarrow dibaryons in the reactions pd->p+X and pd->p+pX_1. Dibaryons with masses 1904\\pm 2, 1926\\pm 2, and 1942\\pm 2 MeV have been observed in missing mass M_X spectra. In missing mass M_{X_1} spectra, the resonancelike states X_1=\\gamma+n at M_{X_1}=966\\pm 2, 986\\pm 2, and 1003\\pm 2 MeV have been found. The analysis of the data obtained leads to the conclusion that the observed dibaryons are supernarrow dibaryons, the decay of which into two nucleons is forbidden by the Pauli exclusion principle. A possible interpretation of exited nucleon states with small masses is suggested.']",['2000-06-26']
768,['eng'],"['Frlez, E', 'Brönnimann, C', 'Krause, B', 'Pocanic, D', 'Renker, D', 'Ritt, S', 'Slocum, P L', 'Supek, I', 'Wirtz, H P']",['Light response of pure CsI calorimeter crystals painted with wavelength-shifting lacquer'],['Particle Physics - Experimental Results'],"['pi+, semileptonic decay', 'pi+, branching ratio', 'calorimeter', 'scintillation counter, crystal', 'cesium, iodine', 'optics, transformation', 'radiation, yield', 'time resolution', 'PSI Cycl', 'pi+ --> pi0 positron neutrino/e']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006027'],"['We have measured scintillation properties of pure CsI crystals used in the shower calorimeter built for a precise determination of the pi+ -> pi0 e+ nu decay rate at the Paul Scherrer Institute (PSI). All 240 individual crystals painted with a special wavelength-shifting solution were examined in a custom-build detection apparatus (RASTA=radioactive source tomography apparatus) that uses a 137Cs radioactive gamma source, cosmic muons and a light emitting diode as complementary probes of the scintillator light response. We have extracted the total light output, axial light collection nonuniformities and timing responses of the individual CsI crystals. These results predict improved performance of the 3 pi sr PIBETA calorimeter due to the painted lateral surfaces of 240 CsI crystals. The wavelength-shifting paint treatment did not affect appreciably the total light output and timing resolution of our crystal sample. The predicted energy resolution for positrons and photons in the energy range of 10-100 MeV was nevertheless improved due to the more favorable axial light collection probability variation. We have compared simulated calorimeter ADC spectra due to 70 MeV positrons and photons with a Monte Carlo calculation of an ideal detector light response.']",['2000-06-22']
769,['eng'],"['Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Ferguson, T', 'Vogel, H', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J']","['Measurements of the Mass, Total Width and Two-Photon Partial Width of the $\\eta_{c}$ Meson']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, inelastic scattering', 'exchange, two-photon', 'photon photon, interaction', 'eta/c(2980), photoproduction', 'eta/c(2980), mass', 'eta/c(2980), width', 'eta/c(2980), hadronic decay', 'eta/c(2980), radiative decay', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> eta/c(2980) positron electron', 'eta/c(2980) --> K0(S) K pi', 'eta/c(2980) --> 2photon', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006026'],"['Using 13.4 $fb^{-1}$ of data collected with the CLEO detector at the Cornell Electron Storage Ring, we have observed 300 events for the two-photon production of ground-state pseudo-scalar charmonium in the decay $\\eta_c$ -> $K_S K^{\\mp} \\pi^{\\pm}$. We have measured the $\\eta_c$ mass to be (2980.4 +- 2.3 (stat) +- 0.6 (sys)) MeV and its full width as (27.0 +- 5.8 (stat) +- 1.4 (sys)) MeV. We have determined the two-photon partial width of the $\\eta_c$ meson to be (7.6 +- 0.8 (stat) +- 0.4 (sys) +- 2.3 (br)) keV, with the last uncertainty associated with the decay branching fraction.']",['2000-06-22']
770,['eng'],"['Affolder, T']",['Measurement of $d\\sigma/dy$ for High Mass Drell-Yan $e^{+}e^{-}$ Pairs from $p\\overline{p}$ Collisions at $\\sqrt{s}$= 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electron, pair production', 'Drell-Yan process', 'channel cross section', 'rapidity spectrum, (positron electron)', 'quantum chromodynamics, perturbation theory', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> positron electron anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006025'],['We report on the first measurement of the rapidity distribution dsigma/dy over nearly the entire kinematic region of rapidity for e^+e^- pairs in the Z-boson region of 66<M_{ee}<116 GeV/c^2 and at higher mass M_{ee}>116 GeV/c^2. The data sample consists of 108 pb^{-1} of ppbar collisions at \\sqrt{s}=1.8 TeV taken by the Collider Detector at Fermilab during 1992--1995. The total cross section in the $Z$-boson region is measured to be 252 +- 11 pb. The measured total cross section and d\\sigma/dy are compared with quantum chromodynamics calculations in leading and higher orders.'],['2000-06-22']
771,['eng'],"['Appel, J A', 'Brown, C N', 'Cooper, P S', 'White, H B']",['In Celebration of the Fixed Target Program with the Tevatron'],['Particle Physics - Experimental Results'],"['conference, Batavia 2000/06/02', 'review', 'data compilation', 'hadron hadron, interaction', 'photon hadron, interaction', 'quantum chromodynamics', 'structure function', 'quark, heavy', 'symmetry, validity test', 'hyperon', 'neutrino', 'Batavia TEVATRON PS', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008076'],"['This document is an abridgement of the commemorative book prepared on the occasion of the symposium ""In Celebration of the Fixed Target Program with the Tevatron"" held at Fermilab on June 2, 2000. The full text with graphics contains, in addition to the material here, a section for each experiment including a ""plain text"" description, lists of all physics publications, lists of all degree recipients and a photo from the archives. The full text is available on the web at: http://conferences.fnal.gov/tevft/book/']",['2000-08-31']
772,['eng'],"['Kappes, A']",['Study of Deep Inelastic ep-Scattering at High-$Q^{2}$ with ZEUS at HERA'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'electron p, colliding beams', 'positron p, deep inelastic scattering', 'electron p, deep inelastic scattering', 'neutral current', 'charged current', 'p, structure function', 'electroweak interaction, validity test', 'channel cross section, momentum transfer', 'x-dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300, 318 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006024'],"[""Measurements of differential cross sections for deep inelastic ep neutral-current (NC) and charged-current (CC) reactions are presented using data taken during the 1994-97 e^+p and the 1998-99 e^-p running periods. The structure function xF_3 has been extracted combining NC e^-p and e^+p data sets. Both the measured cross sections and xF_3 are well described by the standard model predictions using standard PDF's.""]",['2000-06-21']
773,['eng'],"['Kerger, R']",['Lepton Flavour Violation at HERA'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'positron p, colliding beams', 'violation, flavor', 'leptoquark, exchange', 'leptoquark, coupling', 'transition, positron muon', 'transition, positron tau', 'final state, (jet muon)', 'tau, semileptonic decay', 'leptoquark, mass', 'lower limit', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006023'],"[""The $e^+p$-data collected with the ZEUS (${\\cal L}=47.7$ pb$^{-1}$) and the H1 (${\\cal L}=37$ pb$^{-1}$) detectors at HERA in 1994--1997 are analysed for signals of lepton flavour violation mediated by leptoquark exchange, both in the muon and the tau channels. No evidence for lepton flavour violation is found and limits on the leptoquarks' Yukawa couplings are set.""]",['2000-06-20']
774,['eng'],"['Anciant, E', 'Auger, T', 'Audit, G', 'Battaglieri, M', 'Laget, J M', 'Marchand, C', 'Adams, G S', 'Amaryan, M J', 'Anghinolfi, M', 'Armstrong, D', 'Asavapibhop, B', 'Avakian, H', 'Barrow, S', 'Beard, K', 'Bektasoglu, M', 'Berman, B L', 'Bianchi, N', 'Biselli, A', 'Boiarinov, S', 'Briscoe, W J', 'Brooks, W', 'Burkert, V D', 'Calarco, J R', 'Capitani, G P', 'Carman, D S', 'Carnahan, B', 'Cetina, C', 'Cole, P L', 'Coleman, A', 'Connelly, J', 'Cords, D', 'Corvisiero, P', 'Crabb, D', 'Crannell, H', 'Cummings, J', 'Degtyarenko, P V', 'Dennis, L C', 'De Sanctis, E', 'De Vita, R', 'Dhuga, K S', 'Djalali, C', 'Dodge, G E', 'Doughty, D', 'Dragovitsch, P', 'Dugger, M R', 'Dytman, S A', 'Efremenko, Yu V', 'Egiyan, H', 'Egiyan, K S', 'Elouadrhiri, L', 'Farhi, L', 'Feuerbach, R J', 'Ficenec, J', 'Forest, T A', 'Freyberger, A P', 'Funsten, H O', 'Gai, M', 'Garçon, M', 'Gilfoyle, G P', 'Giovanetti, K L', 'Girard, P M', 'Griffioen, K A', 'Guidal, M', 'Gyurjyan, V', 'Heddle, D', 'Hersman, F W', 'Hicks, K', 'Hicks, R S', 'Holtrop, M', 'Hyde-Wright, C E', 'Ito, M M', 'Jenkins, D', 'Joo, K K', 'Khandaker, M', 'Kim, D H', 'Kim, W', 'Klein, A', 'Klein, F J', 'Klusman, M', 'Kossov, M', 'Kramer, L H', 'Kuhn, S E', 'Lawrence, D', 'Longhi, A', 'Loukachine, K', 'Magahiz, R', 'Major, R W', 'Manak, J J', 'Matthews, S K', 'McAleer, S', 'McCarthy, J', 'McCormick, K', 'McNabb, J W C', 'Mecking, B A', 'Mestayer, M D', 'Meyer, C A', 'Minehart, R C', 'Miskimen, R', 'Muccifora, V', 'Müller, J', 'Murphy, L', 'Mutchler, G S', 'Napolitano, J', 'Niczyporuk, B', 'Niyazov, R A', 'Opper, A K', ""O'Brien, J T"", 'Philips, S', 'Pivnyuk, N A', 'Pocanic, D', 'Pogorelko, O I', 'Polli, E', 'Preedom, B M', 'Price, J W', 'Qin, L M', 'Raue, B A', 'Reolon, A R', 'Riccardi, G', 'Ricco, G', 'Ripani, M', 'Ritchie, B G', 'Ronchetti, F', 'Rossi, P', 'Roudot, F', 'Rowntree, D', 'Rubin, P D', 'Salgado, C W', 'Sapunenko, V', 'Schumacher, R A', 'Shafi, A', 'Sharabyan, Yu G', 'Skabelin, A', 'Smith, C', 'Smith, E S', 'Sober, D I', 'Stepanyan, S', 'Stoler, P', 'Taiuti, M', 'Taylor, S', 'Tedeschi, D J', 'Thompson, R', 'Vineyard, M F', 'Vlasov, A', 'Weller, H', 'Weinstein, L B', 'Welsh, R', 'Weygand, D', 'Whisnant, S', 'Witkowski, M T', 'Wolin, E', 'Yegneswaran, A', 'Yun, J', 'Zhang, B', 'Zhao, J']",['Photoproduction of $\\phi$(1020) mesons on the proton at large momentum transfer'],['Particle Physics - Experimental Results'],"['photon p, inclusive reaction', 'photon p, tagged beam', 'momentum transfer, high', 'Phi(1020), photoproduction', 'Phi(1020), hadronic decay', 'mass spectrum, (K+ K-)', 'pomeron, exchange', 'exchange, two-gluon', 'pomeron, resolved', 'differential cross section, momentum transfer', 'angular distribution', 'magnetic spectrometer, experimental results', 'Newport News CEBAF Linac', 'photon p --> Phi(1020) anything', 'Phi(1020) --> K+ K-', '3.3-3.9 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006022'],"['The cross section for $\\phi$ meson photoproduction on the proton has been measured for the first time up to a four-momentum transfer -t = 4 GeV^2, using the CLAS detector at the Thomas Jefferson National Accelerator Facility. At low four-momentum transfer, the differential cross section is well described by Pomeron exchange. At large four-momentum transfer, above -t = 1.8 GeV^2, the data support a model where the Pomeron is resolved into its simplest component, two gluons, which may couple to any quark in the proton and in the $\\phi$.']",['2000-06-19']
775,['eng'],"['Solomey, N']",['Physics Prospects with an Intense Neutrino Experiment'],['Particle Physics - Experimental Results'],"['talk, Quebec City 2000/05/22', 'neutrino, beam', 'antineutrino nucleus, interaction', 'charged current', 'production, strangeness', 'hyperon, neutrinoproduction', 'K, neutrinoproduction', 'dependence, mass number', 'counters and detectors, proposed', 'proposed experiment, Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006021'],"['With new forthcoming intense neutrino beams, for the study of neutrino oscillations, it is possible to consider other physics experiments that can be done with these extreme neutrino fluxes available close to the source.']",['2000-06-19']
776,['eng'],"['Biebel, O']",['Event Shapes and Power Corrections in $e^{+}e^{-}$ Annihilation'],['Particle Physics - Experimental Results'],"['talk, Liverpool 2000/04/25', 'electron positron, annihilation', 'hadron, multiple production', 'event shape analysis', 'strong interaction, coupling constant', 'correction, hadronization', 'parametrization', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006020'],['The effects of the hadronisation of partons on the distribution of event shape observables are associated with corrections which are suppressed by reciprocal powers of the energy scale of the process. The correction is determined by one non-calculable parameter \\alpha_0 for which an universal value of 0.5 +/- 20% is found from the investigation of the distribution of event shape observables and their mean values measured in e^+e^- annihilation.'],['2000-06-16']
777,['eng'],"['Abe, K', 'Abe, K', 'Abe, T', 'Adam, I', 'Akimoto, H', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Berger, R', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Cassell, R', 'Chou, A', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Crawford, G', 'Damerell, C J S', 'Daoudi, M', 'Dasu, S', 'De Groot, N', 'De Sangro, R', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Erofeeva, I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fernández, J P', 'Flood, K', 'Frey, R', 'Hart, E L', 'Hasuko, K', 'Hertzbach, S S', 'Huffer, M E', 'Huynh, X', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Kajikawa, R', 'Kalelkar, M S', 'Kang, H J', 'Kofler, R R', 'Kroeger, R S', 'Langston, M', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'McKemey, A K', 'Messner, R', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Narita, S', 'Nauenberg, U', 'Neal, H', 'Nesom, G', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Ratcliff, B N', 'Reidy, J', 'Reinertsen, P L', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schumm, B A', 'Schwiening, J', 'Serbo, V V', 'Shapiro, G', 'Sinev, N B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, A', 'Swartz, M', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Usher, T', 'Vavra, J', 'Verdier, R', 'Wagner, D L', 'Waite, A P', 'Walston, S', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Wright, T R', 'Yamamoto, R K', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H']",['First Direct Measurement of the Parity-Violating Coupling of the $Z^{0}$ to the s-Quark'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, strangeness', 'quark, pair production', 'particle identification, strangeness', 'angular distribution', 'Z0, branching ratio', 'coupling, (Z0 strangeness)', 'parity, violation', 'analyzing power', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.2 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006019'],"['We have made the first direct measurement of the parity-violating coupling of the Z^0 boson to the strange quark, A_s, using ~550,000 e^+e^- ->Z^0->hadrons events produced with a polarized electron beam and recorded by the SLD experiment. Z^0 -> s-sbar events were tagged by the absence of B or D hadrons and the presence in each hemisphere of a high-momentum K^+- or K^0_s. From the polar angle distributions of the strangeness-signed thrust axis, we obtained A_s=0.895+-0.066(stat.)+-0.062(syst.). The analyzing power and u-ubar plus d-dbar background were constrained using the data.']",['2000-06-15']
778,['eng'],"['Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Chen, G P', 'Ferguson, T', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Urner, D', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T']","['$B \\to D^{*}\\pi^{+}\\pi^{-}\\pi^{-}\\pi^{o}$, $D^{(*)}\\omega\\pi^{-}$ and the Observation of a Wide $1^{-} \\omega\\pi^{-}$ Enhancement at 1418 MeV']",['Particle Physics - Experimental Results'],"['talk, Osaka 2000/07/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'mass spectrum, (4pi)', 'meson resonance, (1418)', 'rho(1450)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D*(2010) pi+ 2pi- pi0', 'B --> D*(2010) omega(783) pi-', '10.6 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006018', 'http://arXiv.org/abs/hep-ex/?0006018']","[""We report on the observation of B->D{*}pi+pi-pi-pio decays. The branching ratios for D*+ and D*o are (1.72+/-0.14+/-0.24)% and (1.80+/-0.24+/-0.25)%, respectively. Each final state has a D{*} omega pi- component, with branching ratios (0.29+/-0.03+/-0.04)% and (0.45+/-0.10+/-0.07)% for the D*+ and D*o modes, respectively. We also observe B->D omega pi- decays. The branching ratios for D+ and Do are (0.28+/-0.05+/-0.03)% and (0.41+/-0.07+/-0.04)%, respectively. The omega pi- appears to come from the decay of a wide 1- resonance. A fit to a Breit-Wigner shape gives a mass of 1418+/-26+/-19 MeV and width of 388+/-44+/-32 MeV. We identify this object as the rho(1450) or rho'.""]",['2000-06-15']
779,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bähr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bertrand-Coremans, G', 'Bizot, J C', 'Borras, K', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P D', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Donovan, K T', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Ebert, J', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferrarotto, F', 'Ferron, S', 'Fleischer, M', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Glazov, A', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haustein, V', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hilgers, M', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Kaufmann, O', 'Kausch, M', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolanoski, H', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krücker, D', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Kutuev, R K', 'Lachnit, W A', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebedev, A', 'Leiner, B', 'Lemaître, V', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'Lobo, G', 'Lobodzinska, E', 'Lobodzinski, B', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, A', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, D', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Negri, I', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Passaggio, S', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Smith, M', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Sutton, J P', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vazdik, Ya', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Inclusive Photoproduction of Neutral Pions in the Photon Hemisphere at HERA'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, inclusive reaction', 'pi0, photoproduction', 'pi0, radiative decay', 'differential cross section, transverse momentum', 'rapidity dependence', 'x-dependence', 'mass spectrum, two-photon', 'numerical calculations, Monte Carlo', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> pi0 positron anything', 'approx. 300 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006017', 'http://arXiv.org/abs/hep-ex/?0006017://www-h1.desy.de/h1/www/publications/htmlsplit/DESY-00-085.long.html']","['The inclusive cross section for the photoproduction of neutral pions has been measured as a function of the transverse momentum, rapidity, and Feynman x of the pizero mesons at an average photon--proton centre-of-mass energy of 208 GeV and for photon virtualities below Q^2=0.01 GeV^2. The pizero measurement extends the range covered by previous charged particle measurements at HERA by two units of rapidity in the photon direction down to a value of -5.5 in the gamma p centre-of-mass frame. The pizero transverse momentum distribution is well described over the whole measured range by a power law ansatz, while an exponential fit falls below the data at transverse momentum values above 1.5 GeV/c. Good agreement with the predictions of the Monte Carlo models PYTHIA and PHOJET is found. In the context of the PYTHIA model the data are inconsistent with large intrinsic transverse momentum values in the photon.']",['2000-06-15']
780,['eng'],"['Gianotti, F', 'Pepé-Altarelli, M']",['Precision Physics at the LHC'],"['Particle Physics - Experimental Results', 'Detectors and Experimental Techniques']","['talk, Koenigstein-Weissig 2000/04/09', 'p p, interaction', 'W, hadroproduction', 'W, mass', 'W, leptonic decay', 'mass spectrum, transverse', 'lepton, pair production', 'mass spectrum, dilepton', 'Drell-Yan process', 'gauge boson, pair production', 'coupling, (3gauge boson)', 'quark, truth', 'quark, pair production', 'Higgs particle, search for', 'Higgs particle, mass', 'Higgs particle, width', 'supersymmetry', 'supergravity', 'sparticle, mass spectrum', 'magnetic detector, CMS', 'magnetic detector, ATLAS', 'numerical calculations', 'proposed experiment, CERN LHC Coll', 'talk, Koenigstein-Weissig 2000/04/09', 'p p, interaction', 'W, hadroproduction', 'W, mass', 'W, leptonic decay', 'mass spectrum, transverse', 'lepton, pair production', 'mass spectrum, dilepton', 'Drell-Yan process', 'gauge boson, pair production', 'coupling, (3gauge boson)', 'quark, truth', 'quark, pair production', 'Higgs particle, search for', 'Higgs particle, mass', 'Higgs particle, width', 'supersymmetry', 'supergravity', 'sparticle, mass spectrum', 'magnetic detector, CMS', 'magnetic detector, ATLAS', 'numerical calculations', 'proposed experiment, CERN LHC Coll']","['http://documents.cern.ch/cgi-bin/setlink?base=atlnot&categ=Note&id=conf-2000-003', 'http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006016']","['A large number of precision measurements will be possible with the ATLAS and CMS experiments at the CERN Large Hadron Collider (LHC). Examples from W physics, Drell-Yan production of lepton pairs, Triple-Gauge Couplings,top physics, Higgs and Supersymmetry are discussed.']",['2000-06-15']
781,['eng'],"['Brandi, F', 'Bregant, M', 'Cantatore, G', 'Valle, F D', 'Carusotto, S', 'Domenico, G D', 'Gastaldi, Ugo', 'Milotti, E', 'Pengo, R', 'Polacco, E', 'Rizzo, C', 'Ruoso, G', 'Zavattini, Emilio', 'Zavattini, G']",['Optical production and detection of dark matter candidates'],['Particle Physics - Experimental Results'],"['talk, La Biodola 2000/05/21', 'astrophysics, missing-mass', 'photon, polarized beam', 'radiation, laser', 'magnetic field, transverse', 'polarization, measurement', 'scalar particle, production', 'pseudoscalar particle, production', 'coupling, (axion 2photon)', 'experimental methods, optical']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006015'],"['The PVLAS collaboration is at present running, at the Laboratori Nazionali di Legnaro of I.N.F.N., Padova, Italy, a very sensitive optical ellipsometer capable of measuring the small rotations or ellipticities which can be acquired by a linearly polarized laser beam propagating in vacuum through a transverse magnetic feld (vacuum magnetic birefringence). The apparatus will also be able to set new limits on mass and coupling constant of light scalar/pseudoscalar particles coupling to two photons by both producing and detecting the hypothetical particles. The axion, introduced to explain parity conservation in strong interactions, is an example of this class of particles, all of which are considered possible dark matter candidates. The PVLAS apparatus consists of a very high finesse (> 140000), 6.4 m long, Fabry-Perot cavity immersed in an intense dipolar magnetic field (~6.5 T). A linearly polarized laser beam is frequency locked to the cavity and analysed, using a heterodyne technique, for rotation and/or ellipticity acquired within the magnetic field.']",['2000-06-15']
782,['eng'],"['Böhm, F', 'Busenitz, J K', 'Cook, B', 'Gratta, Giorgio', 'Henrikson, H', 'Lawrence, J K D', 'Lee, K B', 'McKinny, K', 'Miller, L', 'Novikov, V', 'Piepke, A', 'Ritchie, B', 'Tracy, D', 'Vogel, P', 'Wang, Y F', 'Wolf, J']",['Neutron production by cosmic-ray muons at shallow depth'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'muon nucleus, nuclear reaction', 'n, yield', 'scintillation counter, liquid', 'gadolinium', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006014'],"['The yield of neutrons produced by cosmic ray muons at a shallow depth of 32 meters of water equivalent has been measured. The Palo Verde neutrino detector, containing 11.3 tons of Gd loaded liquid scintillator and 3.5 tons of acrylic served as a target. The rate of one and two neutron captures was determined. Modeling the neutron capture efficiency allowed us to deduce the total yield of neutrons $ Y_{tot} = (3.60 \\pm 0.09 \\pm 0.31) \\times 10^{-5}$ neutrons per muon and g/cm$^2$. This yield is consistent with previous measurements at similar depths.']",['2000-06-14']
783,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Abbiendi, G', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Coppola, N', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Brock, I', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Hartmann, H', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Rautenberg, J', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Foster, B', 'Heath, G P', 'Heath, H F', 'McFall, J D', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Borras, K', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Goers, S', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hasell, D', 'Hebbel, K', 'Kasemann, M', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Lindemann, L', 'Löhr, B', 'Mankel, R', 'Martínez, M', 'Milite, M', 'Moritz, M', 'Notz, D', 'Pelucchi, F', 'Petrucci, M C', 'Rohde, M', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'Votano, L', 'Bamberger, Andreas', 'Benen, A', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Bell, M', 'Doyle, A T', 'Lee, S W', 'Lupi, A', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Garfagnini, A', 'Gialas, I', 'Gladilin, L K', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Poelz, G', 'Zetsche, F', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Mallik, U', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Park, I H', 'Son, D', 'Barreiro, F', 'García, G', 'Glasman, C', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Barbi, M S', 'Corriveau, F', 'Hanna, D S', 'Ochs, A', 'Padhi, S', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Antonov, A', 'Bashkirov, V', 'Danilov, M V', 'Dolgoshein, B A', 'Gladkov, D', 'Sosnovtsev, V V', 'Suchkov, S', 'Dementev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Sheheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tassi, E', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dosselli, U', 'Dusini, S', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Turcato, M', 'Voci, C', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Saull, P R B', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sabetfakhri, A', 'Simmons, D', 'Butterworth, J M', 'Catterall, C D', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Pawlak, R', 'Smalska, B', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Gadaj, T', 'Deppe, O', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Badgett, W F', 'Chapin, D', 'Cross, R', 'Foudas, C', 'Mattingly, S E', 'Reeder, D D', 'Smith, W H', 'Vaiciulis, A W', 'Wildschek, T', 'Wodarczyk, M', 'Deshpande, A A', 'Dhawan, S K', 'Hughes, V W', 'Bhadra, S', 'Catterall, C D', 'Cole, J E', 'Frisken, W R', 'Hall-Wilton, R', 'Khakzad, M', 'Menary, S R']",['Measurement of exclusive $\\omega$ electroproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, exclusive reaction', 'vector meson, electroproduction', 'omega(783), hadronic decay', 'Phi(1020), hadronic decay', 'rho(770)0', 'channel cross section, ratio', 'energy dependence', 'momentum transfer, dependence', 'symmetry, SU(4)', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> p omega(783) positron', 'positron p --> Phi(1020) positron', 'omega(783) --> pi+ pi- pi0', 'Phi(1020) --> pi+ pi- pi0', 'approx. 300 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006013', 'http://www-zeus.desy.de/~schlenst/conf/osaka_paper.html']","['The exclusive electroproduction of omega mesons, ep -> e omega p, has been studied in the kinematic range 3<Q^2<20 GeV^2, 40<W<120 GeV and |t|<0.6 GeV^2 with the ZEUS detector at HERA using an integrated luminosity of 37.7 pb^{-1}. The omega mesons were identified via the decay omega -> pi^+pi^-pi^0. The exclusive (ep -> e omega p) cross section in the above kinematic region is 0.108 +- 0.014(stat.) +- 0.026(syst.) nb. The reaction ep -> e phi p, phi -> pi^+pi^-pi^0, has also been measured. The cross sections, as well as the cross-section ratios omega/rho and omega/phi, are presented as a function of W and Q^2. Thus, for the first time, the properties of omega electroproduction can be compared to those of rho^0, phi and J/psi electroproduction at high W.']",['2000-06-13']
784,['eng'],"['Dorfan, J']",['Status of PEP-II and BaBar'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, storage ring', 'B, particle source', 'performance', 'luminosity', 'electron positron, colliding beams', 'semiconductor detector, vertex', 'drift chamber', 'Cherenkov counter', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006012'],"['In this report, the status of the PEP-II machine and the BaBar detector are presented. Performance will be presented as of the Lepton Photon Conference (August 1999) with subsequent performance levels footnoted as appropriate.']",['2000-06-12']
785,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bean, A', 'Begel, M', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Besson, A', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, G A', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Demina, R', 'Demine, P', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Filthaut, F', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Kuznetsov, V', 'Landsberg, G L', 'Leflat, A', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramberg, E', 'Reay, N W', 'Reucroft, S', 'Rha, J', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Scully, J R', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thompson, J', 'Toback, D', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Wang, Z M', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Search for New Physics in $e\\muX$ Data at D0 Using Sherlock'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, new interaction', 'electroweak interaction, symmetry breaking', 'transverse momentum, high', 'data analysis method, proposed', 'particle identification', 'efficiency', 'lepton, pair production', 'final state, (muon electron)', 'quark, truth', 'quark, pair production', 'W, pair production', 'numerical calculations', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> muon electron anything', '1800 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006011', 'http://arXiv.org/abs/hep-ex/?0006011']","['We present a quasi-model-independent search for the physics responsible for electroweak symmetry breaking. We define final states to be studied, and construct a rule that identifies a set of relevant variables for any particular final state. A new algorithm (""Sherlock"") searches for regions of excess in those variables and quantifies the significance of any detected excess. After demonstrating the sensitivity of the method, we apply it to the semi-inclusive channel e mu X collected in 108 pb^-1 of ppbar collisions at sqrt(s) = 1.8 TeV at the D0 experiment during 1992-1996 at the Fermilab Tevatron. We find no evidence of new high p_T physics in this sample.']",['2000-06-12']
786,['eng'],"['Naroska, B']",['New Results on Vector Meson Production at HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'positron p, colliding beams', 'positron p, exclusive reaction', 'vector meson, photoproduction', 'J/psi(3100), leptonic decay', 'Phi(1020), hadronic decay', 'omega(783), hadronic decay', 'quantum chromodynamics, perturbation theory', 'exchange, two-gluon', 'Regge poles', 'differential cross section, transverse momentum', 'energy dependence', 'channel cross section, ratio', 'momentum transfer, dependence', 'cross section, longitudinal', 'cross section, transverse', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006010'],"['New results on elastic (exclusive) production of vector mesons are presented, mainly on J/\\psi and phi mesons with emphasis on an interpretation of the data within pQCD.']",['2000-06-12']
787,['eng'],"['Iacobucci, G']",['Structure Functions and Large $Q^{2}$ Cross Sections at HERA'],['Particle Physics - Experimental Results'],"['talk, La Thuile 2000/02/27', 'electron p, colliding beams', 'positron p, colliding beams', 'electron p, deep inelastic scattering', 'positron p, deep inelastic scattering', 'neutral current', 'charged current', 'p, structure function', 'differential cross section', 'dependence, momentum transfer', 'momentum transfer, high', 'small-x', 'momentum spectrum, parton', 'quantum chromodynamics, perturbation theory', 'structure function, longitudinal', 'structure function, charm', 'W, propagator', 'W, mass', 'magnetic detector, H1', 'talk, La Thuile 2000/02/27', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006009'],['The data collected with the H1 and ZEUS detectors during the running period 1994-99 are used to give an experimental review on the proton structure functions and the neutral current and charged current large Q^2 cross sections in e^\\pm p scattering at HERA.'],['2000-06-08']
788,['eng'],"['Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Nelson, H N', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H']",['Study of Charmless Hadronic B Meson Decays to Pseudoscalar-Vector Final States'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'meson, pair production', 'pseudoscalar meson', 'pi', 'K', 'vector meson', 'omega(783)', 'rho(770)', 'K*(892)', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> rho(770) pi', 'B- --> omega(783) pi-', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006008'],"['We report results of searches for charmless hadronic B meson decays to pseudoscalar ($\\pi^{\\pm}$, $K^{\\pm}$ or $\\pi^{0}$) -vector($\\rho$, $K^{*}$ or $\\omega$) final states. Using 9.7 million $B\\bar{B}$ pairs collected with the CLEO detector, we report first observation of $B^{-}\\to\\pi^{-}\\rho^{0}$, $B^{0}\\to\\pi^{\\pm}\\rho^{\\mp}$ and $B^{-}\\to\\pi^{-}\\omega$, which are expected to be dominated by hadronic b to u transitions. The measured branching fractions are (10.4 +3.3-3.4 +- 2.1) x 10$^{-6}$, (27.6 +8.4-7.4 +- 4.2) x 10$^{-6}$ and (11.3 +3.3-2.9 +- 1.4) x 10$^{-6}$, respectively. Branching fraction upper limits are set for all the other decay modes investigated.']",['2000-06-08']
789,['eng'],"['Alexander, Gideon', 'Cohen, I']",['Moller Scattering Polarimetry for High Energy $e^{+}e^{-}$ Linear Colliders'],['Particle Physics - Experimental Results'],"['electron positron, linear collider', 'linear collider, proposed', 'electron electron, elastic scattering', 'iron, atom', 'polarization, measurement', 'electron, polarized beam', 'beam monitoring', 'differential cross section, angular dependence', 'asymmetry', 'electron, momentum spectrum', 'numerical calculations', 'DESY TESLA Linac']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006007'],['The general features of the Moller scattering and its use as an electron polarimeter are described and studied in view of the planned future high energy e^+e^- linear colliders. In particular the study concentrates on the TESLA collider which may operate with longitudinal polarised beams at a centre of mass energy of the order of 0.5 TeV with a luminosity of about L = 10^33 cm^-2 sec^-1.'],['2000-06-08']
790,['eng'],"['Schneider, O']",['Heavy flavour physics results from LEP1'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, fragmentation function', 'quark, semileptonic decay', 'Kobayashi-Maskawa angle', 'B0, semileptonic decay', 'D*(2010)', 'final state, (0charm)', 'B/s0, decay', 'anti-B/s0, decay', 'width, difference', 'B/s0 anti-B/s0, interference', 'B0, hadronic decay', 'violation, CP', 'asymmetry, time dependence', 'experimental results', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, OPAL', 'CERN LEP Stor', 'B0 --> D*(2010) lepton neutrino', 'B0 --> J/psi(3100) K0(S)', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006006'],"['Recent heavy flavour results from the LEP experiments are presented. These include a search for new physics in rare B decays, a new model-independent measurement of the b-quark fragmentation function at the Z peak, updated measurements of |Vcb|, results on DeltaGamma_s, searches for B0s oscillations, as well as a new measurement of sin(2beta). Many combined results, obtained by dedicated working groups are also given...']",['2000-06-08']
791,['eng'],"['Schmelling, M']",['Averaging Measurements with Hidden Correlations and Asymmetric Errors'],['Particle Physics - Experimental Results'],"['statistical analysis', 'correlation', 'error, asymmetry']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006004'],['Properties of weighted averages are studied for the general case that the individual measurements are subject to hidden correlations and have asymmetric statistical as well as systematic errors. Explicit expressions are derived for an unbiased average with a well defined error estimate.'],['2000-06-05']
792,['eng'],"['Appel, R', 'Atoyan, G S', 'Bassalleck, B', 'Bergman, D', 'Cheung, N', 'Dhawan, S K', 'Do, H', 'Egger, J', 'Eilerts, S W', 'Fischer, H', 'Herold, W D', 'Issakov, V V', 'Kaspar, H', 'Kraus, D E', 'Lazarus, D M', 'Lichard, P', 'Lowe, J', 'Lozano-Bahilo, J', 'Ma, H', 'Majid, W A', 'Menzel, W', 'Pislak, S', 'Poblaguev, A A', 'Rehak, P', 'Sher, A E', 'Thompson, J A', 'Truöl, P', 'Zeller, M E']",['Search for Lepton Flavor Violation in $K^{+}$ Decays'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'pi0, leptonic decay', 'violation, flavor', 'K+, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi- 2muon+', 'K+ --> pi- 2positron', 'K+ --> pi+ muon- positron', 'K+ --> pi- muon+ electron', 'pi0 --> muon- positron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006003'],"['A search for lepton flavor violating decays, \\kmmp, \\keep, \\kpem, \\kmep and \\pizem, was performed using the data collected in E865 at the Brookhaven Alternating Gradient Synchrotron. No signal was found in any of the decay modes. At the 90% confidence level, the branching ratios are less than $3.0\\times10^{-9}$, $6.4\\times10^{-10}$, $5.2\\times10^{-10}$, $5.0\\times10^{-10}$ and $3.4\\times10^{-9}$ respectively.']",['2000-06-05']
793,['eng'],"['Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gwon, E Eckhart C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G']",['Measurement of the Relative Branching Fraction of $\\Upsilon(4S)$ to Charged and Neutral B-Meson Pairs'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'Upsilon(10570), hadronic decay', 'B, pair production', 'yield, (B+ B0)', 'Upsilon(10570), branching ratio', 'B, hadronic decay', 'J/psi(3100), leptonic decay', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> J/psi(3100) K0', 'B+ --> J/psi(3100) K+', 'B --> J/psi(3100) K*(892)', 'approx. 10.6 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006002'],"['We analyze 9.7 x 10^6 B\\bar{B}$ pairs recorded with the CLEO detector to determine the production ratio of charged to neutral B-meson pairs produced at the Y(4S) resonance. We measure the rates for B^0 -> J/psi K^{(*)0} and B^+ -> J/psi K^{(*)+} decays and use the world-average B-meson lifetime ratio to extract the relative widths f+-/f00 = Gamma(Y(4S) -> B+B-)/Gamma(Y(4S) -> B0\\bar{B0}) = = 1.04 +/- 0.07(stat) +/- 0.04(syst). With the assumption that f+- + f00 = 1, we obtain f00 = 0.49 +/- 0.02(stat) +/- 0.01(syst) and f+- = 0.51 +/- 0.02(stat) +/- 0.01(syst). This production ratio and its uncertainty apply to all exclusive B-mescon branching fractions measured at the Y(4S) resonance.']",['2000-06-05']
794,['eng'],"['Manayenkov, S I']",['New Method for Data Treating in Polarization Measurements'],['Detectors and Experimental Techniques'],"['polarization, measurement', 'data analysis method', 'spin, asymmetry', 'Lambda, hadronic decay', 'background', 'statistical analysis', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006001'],"['Precise formulas are derived for the expected values $<\\xi>$, $<\\eta>$ and variances $\\delta \\xi ^2$, $\\delta \\eta ^2$ of random variables $\\xi$, $\\eta$ describing the spin asymmetry of some reaction when a background process contribution is negligible and appreciable, respectively. The variances of $\\xi$ and $\\eta$ are proved to be finite. This property differs from that of the Caushy distribution which has an infinite variance. It is shown that $<\\xi>$ is equal to the physical asymmetry which allows to find the asymmetry from experimental data without studying the detector efficiency. This is the base of the proposed method of data treating. Asymptotic formulas for $<\\eta>$ and $\\delta \\eta ^2$ are also derived for a total number of events tending to infinity for a finite value of the background to signal ratio.']",['2000-06-02']
795,['eng'],"['Jung, C K']",['Feasibility of a Next Generation Underground Water Cherenkov Detector'],['Detectors and Experimental Techniques'],"['talk, Stony Brook 1999/09/23', 'deep underground detector, proposed', 'Cherenkov counter, water', 'p, decay modes', 'neutrino, solar', 'neutrino, cosmic radiation', 'costs']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005046'],"['The feasibility of a next generation underground water Cherenkov detector is examined and a conceptual design (UNO) is presented. The design has a linear detector configuration with a total volume of 650 kton which is 13 times the total volume of the Super-Kamiokande detector. It corresponds to a 20 times increase in fiducial volume for physics analyses. The physics goals of UNO are to increase the sensitivity of the searches for nucleon decays about a factor of ten and to make precision measurements of the solar and atmospheric neutrino properties. In addition, the detection sensitivity for Supernova neutrinos will reach as far as the Andromeda galaxy.']",['2000-06-01']
796,['eng'],"['Park, H']",['$D^{0}-\\overline{D}^0$ Mixing and Rare Decays'],['Particle Physics - Experimental Results'],"['review, Taipei 1999/12/03', 'D0 anti-D0, interference', 'D0, rare decay', 'D0, decay modes', 'D0, branching ratio', 'D0, lifetime', 'anti-D0, lifetime', 'lifetime, difference', 'violation, CP', 'electron positron, annihilation', 'photon nucleon, inclusive reaction', 'hadron nucleon, inclusive reaction', 'D*(2010), hadronic decay', 'neutral current, flavor changing', 'flavor, violation', 'lepton number, violation', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005044'],"['Current status of charm mixing search, lifetime difference measurement and rare decay search are reported. The best upper limit at 95% CL for mixing is reported from the CLEO collaboration. E791 has reported lifetime difference measurement and results of rare decay searches. Rare decay searches of the FOCUS collaboration are in progress and their sensitivities to branching ratios are at the level of a few x 10^{-6}.']",['2000-05-30']
797,['eng'],"['Sergey, A']",['Statistical properties of the estimator using covariance matrix'],['Detectors and Experimental Techniques'],"['statistical analysis', 'data analysis method']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005042'],"['The statistical properties of estimator using covariance matrix for the account of point-to-point correlations due to systematic errors are analyzed. It is shown that the covariance matrix estimator (CME) is consistent for the realistic cases (when systematic errors on the fitted parameters are not extremely large comparing with the statistical ones) and its dispersion is always smaller, than the dispersion of the simplified $\\chi^2$ estimator applied to the correlated data. The CME bias is negligible for the realistic cases if the covariance matrix is calculated during the fit iteratively using the parameter estimator itself. Analytical formula for the covariance matrix inversion allows to perform fast and precise calculations even for very large data sets. All this allows for efficient use of the CME in the global fits.']",['2000-05-30']
798,['eng'],"['Giacomelli, Giorgio', 'Giorgini, M', 'Lari, T', 'Ouchrif, M', 'Patrizii, L', 'Popa, V', 'Spada, P F', 'Togo, V']",['Magnetic monopole bibliography'],['Particle Physics - Experimental Results'],"['data compilation', 'magnetic monopole', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005041'],['We present a bibliography compilation on magnetic monopoles updated to include references till the end of year 1999. It is intended to contain nearly all the experimental papers on the subject and only the theoretical papers which have some specific experimental implications.'],['2000-06-23']
799,['eng'],"['Biebel, O']",['$\\alpha_{S}$ Evolution from 35 GeV to 202 GeV and Flavour Independence'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'jet, multiplicity', 'strong interaction, coupling constant', 'energy dependence', 'dependence, flavor', 'experimental results', 'DESY DORIS Stor', 'CERN LEP Stor', '35-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005040'],['Determinations of the strong coupling constant alpha_S at centre-of-mass energies of 192 through 202 GeV at LEP are presented. The energy evolution of alpha_S is in agreement with the prediction of QCD. The combined investigation of OPAL and JADE data in the energy range of 35 through 189 GeV yields alpha_S(m_Z)=0.1187^{+0.0034}_{-0.0019}. The strenght of the strong coupling is flavour independent if quark mass effects are taken into account.'],['2000-05-29']
800,['eng'],"['Avakian, R O', 'Ispirian, K A', 'Ispirian, R K', 'Khachatrian, V G', 'Sona, P', 'Uggerhøj, E']",['Charge Asymmetry in 1-1000 GeV Electromagnetic Showers and Possibility of Its Measurementnt'],['Detectors and Experimental Techniques'],"['photon nucleus, nuclear reaction', 'showers, electromagnetic', 'electron, energy spectrum', 'positron, energy spectrum', 'charge, asymmetry', 'energy dependence', 'dependence, path length', 'showers, spatial distribution', 'radiation, Cherenkov', 'magnetic spectrometer', 'numerical calculations, Monte Carlo', '1-1000 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005039'],"['For the high energy electromagnetic showers the thickness dependence of a) the development of electron and positron components, b) the difference between the secondary electron and positron numbers, c) the charge asymmetry of high energy electromagnetic showers, as well as d) the spectral distributions of the components at the shower maxima for various energies of primary particle energies,1 - 1000 GeV were investigated employing GEANT Monte Carlo simulation package. Using these simulation results it is discussed the possibility of observation and study of the charge asymmetry with the help of a magnetic spectrometer which is important for the current and future experiments on the detection of radiowaves produced by high energy neutrinos.']",['2000-05-29']
801,['eng'],"['Wengler, T']",['The Parton Content of the Photon'],['Particle Physics - Experimental Results'],"['review, Les Arcs 2000/03/18', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, inclusive reaction', 'photon electron, deep inelastic scattering', 'photon, structure function', 'x-dependence', 'D*(2010), photoproduction', 'quark, charm', 'quark, pair production', 'channel cross section, transverse momentum', 'quantum chromodynamics, perturbation theory', 'validity test', 'structure function, charm', 'quark, beauty', 'experimental results', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005038'],"['The structure of the photon is studied in photon-photon collisions at LEP. New measurements have become available exploring the structure function F2g of the photon to the lowest values of x yet, where the hadronic component of the photon is most important. Inclusive cross sections for charged D* have been measured as a function of their transverse momenta and are used to test the validity of perturbative QCD in NLO in this region. The total charm quark production cross section is extracted. For the first time the inclusive production of D* mesons in deep inelastic electron-photon scattering has been used to extract the charm structure function of the photon. A first sign of beauty production in photon-photon collisions is reported.']",['2000-05-26']
802,['eng'],"['Link, J M', 'Alimonti, G', 'Anjos, J C', 'Arena, V', 'Bediaga, I', 'Bianco, S', 'Boca, G', 'Bonomi, G', 'Boschini, M', 'Brambilla, D', 'Butler, J N', 'Caccianiga, B', 'Calandrino, A', 'Carrillo, S', 'Casimiro, E', 'Cawlfield, C', 'Cheung, H W K', 'Cho, K', 'Chung, Y S', 'Cinquini, L', 'Copty, N K', 'Cumalat, J P', ""D'Angelo, P"", 'Davenport, T F', 'De Miranda, J M', 'Di Corato, M', 'Dini, P', 'Dos Reis, A C', 'Engh, D', 'Fabbri, F L', 'Gaines, I', 'Garbincius, P H', 'Gardner, R', 'Garren, L A', 'Giammarchi, M G', 'Gianini, G', 'Gottschalk, E E', 'Gourlay, S A', 'Göbel, C', 'Handler, T', 'Hernández, H', 'Hosack, M', 'Inzani, P', 'Johns, W E', 'Kang, J S', 'Kasper, P H', 'Kim, D Y', 'Ko, B R', 'Kreymer, A E', 'Kutschke, R', 'Kwak, J W', 'Kwon, Y', 'Lee, K B', 'Leveraro, F', 'Liguori, G', 'López, A M', 'Magnin, J', 'Malvezzi, S', 'Menasce, D', 'Méndez, H', 'Méndez, L', 'Merlo, M', 'Mezzadri, M', 'Milazzo, L', 'Mirles, M A', 'Montiel, E', 'Moroni, L', 'Myung, S S', 'Nehring, M S', ""O'Reilly, B"", 'Olaya, D', 'Pantea, D', 'Paolone, V S', 'Park, H', 'Park, K S', 'Pedrini, D', 'Pepe, I M', 'Prelz, F', 'Purohit, M', 'Quinones, J', 'Rahimi, A', 'Ramírez, J E', 'Ratti, S P', 'Reyes, M', 'Riccardi, C', 'Rivera, C', 'Rovere, M', 'Sala, A', 'Sala, S', 'Sales, M', 'Sarwar, S', 'Sheaff, M', 'Sheldon, P D', 'Simão, F R A', 'Stenson, K', 'Sánchez-Hernández, A', 'Torre, P', 'Uribe, C', 'Vaandering, E W', 'Vázquez, F', 'Viola, L', 'Vitulo, P', 'Webster, M S', 'Wilson, J R', 'Wiss, J', 'Yager, P M', 'Zallo, A', 'Zhang, Y']",['Search for CP violation in $D^{0}$ and $D^{+}$ decays'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium, oxygen', 'D, photoproduction', 'D+, hadronic decay', 'D0, hadronic decay', 'violation, CP', 'mass spectrum, (K (n)pi)', 'mass spectrum, (K+ K-)', 'D0, momentum spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> K+ K- pi+', 'D0 --> K+ K-', 'D0 --> pi+ pi-', 'approx. 180 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005037'],"['A high statistics sample of photoproduced charm particles from the FOCUS (E831) experiment at Fermilab has been used to search for CP violation in the Cabibbo suppressed decay modes D+ to K-K+pi+, D0 to K-K+ and D0 to pi-pi+. We have measured the following CP asymmetry parameters: A_CP(K-K+pi+) = +0.006 +/- 0.011 +/- 0.005, A_CP(K-K+) = -0.001 +/- 0.022 +/- 0.015 and A_CP(pi-pi+) = +0.048 +/- 0.039 +/- 0.025 where the first error is statistical and the second error is systematic. These asymmetries are consistent with zero with smaller errors than previous measurements.']",['2000-05-26']
803,['eng'],"['Kuzmichev, L A']",['On the Velocity of Light Signals in the Deep Underwater Neutrino Experiments'],['Detectors and Experimental Techniques'],"['neutrino, counters and detectors', 'deep underground detector', 'Cherenkov counter, water', 'signal processing, velocity']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005036'],['During the last few years deep underwater neutrino telescopes of a new generation with dimensions close to 100 m or more were taken into operation. For the correct track reconstruction and for the interpretation of light pulses from calibration lasers one has to use the group velocity for light signals. The difference between group velocity leads to an additional delay of about 10 ns for a distance of 100 m between light source and photjmultiplier. From the time of the appearance of the first projects of deep underwater neutrino telescopes in the middle of 70th this fact was never mentioned in the literature.'],['2000-05-26']
804,['eng'],"['Yavas, O', 'Çiftçi, A K', 'Sultansoy, S F']",['TAC Proposal for Fundamental and Applied Research'],['Accelerators and Storage Rings'],"['talk, Vienna 2000/06/26', 'electron positron, linac-ring collider', 'linac-ring collider, proposed', 'Phi(1020), particle source', 'Phi(1020), decay modes', 'meson, pair production', 'synchrotron radiation, particle source', 'free electron laser']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005035'],"['Main parameters of linac-ring type $phi$-factory proposed as the part of the Turkic Accelerator Complex (TAC) in the framework of ATAM Science Sity Project are discussed. Two sets of parameters, corresponding to E=130(260) MeV for electron linac and E=2000(1000) MeV positron ring, are considered. It is swoun that, in principle, L=10^(34)cm^(-2)s^(-1) can be achieved, which is more than an order exceeds the design luminosity of the DA$Phi$NE. Parameters of the FEL based on electron linac and synchrotron radiation sources based on the positron ring are estimated.']",['2000-05-25']
805,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Akimov, V E', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bean, A', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Landsberg, G L', 'Leflat, A', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lu, J G', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Reay, N W', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Scully, J R', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Song, X F', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thomas, T L T', 'Thompson, J', 'Toback, D', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Search for R-parity Violation in Multilepton Final States in $p \\overline{p}$ Collisions at $\\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'gaugino, pair production', 'lepton, multiple production', 'final state, (3lepton)', 'R parity, violation', 'supergravity', 'parametrization', 'neutralino, LSP', 'sparticle, mass', 'sparticle, decay modes', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005034', 'http://arXiv.org/abs/hep-ex/?0005034']","['The result of a search for gaugino pair production with a trilepton signature is reinterpreted in the framework of minimal supergravity (mSUGRA) with R-parity violation via leptonic lambda Yukawa couplings. The search used 95 pb^{-1} of p-barp collisions at sqrt{s}=1.8 TeV recorded by the D0 detector at the Fermilab Tevatron. A large domain of the mSUGRA parameter space is excluded for lambda_{121}, lambda_{122} > 10^{-4}.']",['2000-05-25']
806,['eng'],"['Vacavant, L', 'Hinchliffe, Ian']",['Model Independent Extra-dimension signatures with ATLAS'],['Detectors and Experimental Techniques'],"['p p, interaction', 'jet, hadroproduction', 'graviton, direct production', 'space-time, higher-dimensional', 'transverse energy, missing-energy', 'cross section, energy dependence', 'transverse momentum, spectra', 'rapidity spectrum', 'topology', 'trigger', 'background', 'photon, energy spectrum', 'numerical calculations, Monte Carlo', 'magnetic detector, ATLAS', 'CERN LHC Coll', 'p p --> jet graviton', 'p p --> graviton photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005033'],['The generic missing transverse energy signals at LHC for theories having large extra dimensions are discussed. Final states of jets plus missing energy and photons plus missing energy are simulated in the ATLAS detector. The discovery limit of LHC and the methods to determine the parameters of the underlying model are discussed.'],['2000-05-24']
807,['eng'],"['Achasov, M N', 'Beloborodov, K I', 'Berdyugin, A V', 'Bogdanchikov, A G', 'Bozhenok, A V', 'Bukin, D A', 'Burdin, S V', 'Golubev, V B', 'Dimova, T V', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Ivanchenko, V N', 'Korol, A A', 'Koshuba, S V', 'Kukartsev, G A', 'Nesterenko, I N', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Popov, V M', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Skripkin, A G', 'Usov, Yu V', 'Valishev, A A', 'Velikzhanin, Yu S']",['The process $e^{+}e^{-}\\to\\omega\\pi^{0}\\to\\ pi^{0})\\pi^{0}\\gamma$ up to 1.4 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'omega(783), electroproduction', 'pi0, associated production', 'omega(783), radiative decay', 'channel cross section, energy dependence', 'radiative correction', 'amplitude analysis', 'rho(1450)', 'rho(1700)', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> omega(783) pi0', 'omega(783) --> pi0 photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005032'],"['The cross section of the $e^+e^-\\to\\omega\\pi^0\\to\\pi^0\\pi^0\\gamma$ reaction was measured by the SND detector at VEPP-2M $e^+e^-$ collider in the energy range from threshold up to 1.4 GeV. Results of the cross section fitting by the sum of $\\rho$, $\\rho^{\\prime}$ and $\\rho^{\\prime\\prime}$ contributions are presented.']",['2000-05-24']
808,['eng'],"['Kudryavtsev, V A', 'Spooner, N J C', 'Tovey, D R', 'Roberts, J W', 'Lehner, M J', 'McMillan, J E', 'Lightfoot, P K', 'Lawson, T B', 'Peak, C D', 'Lüscher, R', 'Barton, J C']",['CsI(Tl) for WIMP dark matter searches'],['Detectors and Experimental Techniques'],"['astrophysics, missing-mass', 'search for, WIMP', 'neutralino', 'scintillation counter, crystal', 'cesium, iodine']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005031'],"['We report a study of CsI(Tl) scintillator to assess its applicability in experiments to search for dark matter particles. Measurements of the mean scintillation pulse shapes due to nuclear and electron recoils have been performed. We find that, as with NaI(Tl), pulse shape analysis can be used to discriminate between electron and nuclear recoils down to 4 keV. However, the discrimination factor is typically (10-15)% better than in NaI(Tl) above 4 keV. The quenching factor for caesium and iodine recoils was measured and found to increase from 11% to ~17% with decreasing recoil energy from 60 to 12 keV. Based on these results, the potential sensitivity of CsI(Tl) to dark matter particles in the form of neutralinos was calculated. We find an improvement over NaI(Tl) for the spin independent WIMP-nucleon interactions up to a factor of 5 assuming comparable electron background levels in the two scintillators.']",['2000-05-23']
809,['eng'],"['Kulchitskii, Yu A']",['On the e/h Ratio of the Electromagnetic Calorimeter'],['Detectors and Experimental Techniques'],"['calorimeter, electromagnetic', 'calorimeter, liquid argon', 'energy resolution', 'particle identification, (hadron electron)', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005029'],"['The method of extraction of the e/h ratio for an electromagnetic compartment of a combined calorimeter is suggested and the non-compensation was determined. The results agree with the Monte Carlo prediction and results of the weighting method for electromagnetic compartment of combined calorimeter. The new easy method of a hadronic energy reconstruction for a combined calorimeter is also suggested. The proposed methods can be used for a combined calorimeter, which is being designed to perform energy measurement in a next-generation high energy collider experiment like ATLAS at LHC.']",['2000-05-23']
810,['eng'],"['Acciarri, M', 'Achard, P', 'Adriani, O', 'Aguilar-Benítez de Lugo, M', 'Alcaraz, J', 'Alemanni, G', 'Allaby, James V', 'Aloisio, A', 'Alviggi, M G', 'Ambrosi, G', 'Anderhub, H', 'Andreev, V P', 'Angelescu, T', 'Anselmo, F', 'Arefev, A', 'Azemoon, T', 'Aziz, T', 'Bagnaia, P', 'Bajo, A', 'Baksay, L', 'Balandras, A', 'Baldew, S V', 'Banerjee, S', 'Banerjee, Sw', 'Barczyk, A', 'Barillère, R', 'Barone, L', 'Bartalini, P', 'Basile, M', 'Battiston, R', 'Bay, A', 'Becattini, F', 'Becker, U', 'Behner, F', 'Bellucci, L', 'Berbeco, R', 'Berdugo, J', 'Berges, P', 'Bertucci, B', 'Betev, B L', 'Bhattacharya, S', 'Biasini, M', 'Biland, A', 'Blaising, J J', 'Blyth, S C', 'Bobbink, Gerjan J', 'Böhm, A', 'Boldizsar, L', 'Borgia, B', 'Bourilkov, D', 'Bourquin, Maurice', 'Braccini, S', 'Branson, J G', 'Brigljevic, V', 'Brochu, F', 'Buffini, A', 'Buijs, A', 'Burger, J D', 'Burger, W J', 'Cai, X D', 'Campanelli, M', 'Capell, M', 'Cara Romeo, G', 'Carlino, G', 'Cartacci, A M', 'Casaus, J', 'Castellini, G', 'Cavallari, F', 'Cavallo, N', 'Cecchi, C', 'Cerrada-Canales, M', 'Cesaroni, F', 'Chamizo-Llatas, M', 'Chang, Y H', 'Chaturvedi, U K', 'Chemarin, M', 'Chen, A', 'Chen, G', 'Chen, G M', 'Chen, H F', 'Chen, H S', 'Chiefari, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Civinini, C', 'Clare, I', 'Clare, R', 'Coignet, G', 'Colino, N', 'Costantini, S', 'Cotorobai, F', 'de la Cruz, B', 'Csilling, Akos', 'Cucciarelli, S', 'Dai, T S', 'van Dalen, J A', ""D'Alessandro, R"", 'De Asmundis, R', 'Déglon, P L', 'Degré, A', 'Deiters, K', 'Della Volpe, D', 'Delmeire, E', 'Denes, P', 'De Notaristefani, F', 'De Salvo, A', 'Diemoz, Marcella.', 'Dierckxsens, M', 'Van Dierendonck, D N', 'Di Lodovico, F', 'Dionisi, C', 'Dittmar, Michael', 'Dominguez, A', 'Doria, A', 'Dova, M T', 'Duchesneau, D', 'Dufournaud, D', 'Duinker, P', 'Durán, I', 'El-Mamouni, H', 'Engler, A', 'Eppling, F J', 'Erné, Frits C', 'Extermann, Pierre', 'Fabre, M', 'Faccini, R', 'Falagán, M A', 'Falciano, S', 'Favara, A', 'Fay, J', 'Fedin, O', 'Felcini, Marta', 'Ferguson, T', 'Ferroni, F', 'Fesefeldt, H S', 'Fiandrini, E', 'Field, J H', 'Filthaut, F', 'Fisher, P H', 'Fisk, I', 'Forconi, G', 'Freudenreich, Klaus', 'Furetta, C', 'Galaktionov, Yu', 'Ganguli, S N', 'García-Abia, P', 'Gataullin, M', 'Gau, S S', 'Gentile, S', 'Gheordanescu, N', 'Giagu, S', 'Gong, Z F', 'Grenier, G', 'Grimm, O', 'Grünewald, M W', 'Guida, M', 'van Gulik, R', 'Gupta, V K', 'Gurtu, A', 'Gutay, L J', 'Haas, D', 'Hasan, A', 'Hatzifotiadou, D', 'Hebbeker, T', 'Hervé, Alain', 'Hidas, P', 'Hirschfelder, J', 'Hofer, H', 'Holzner, G', 'Hoorani, H', 'Hou, S R', 'Hu, Y', 'Iashvili, I', 'Jin, B N', 'Jones, L W', 'de Jong, P', 'Josa-Mutuberria, I', 'Khan, R A', 'Kaur, M', 'Kienzle-Focacci, M N', 'Kim, D', 'Kim, J K', 'Kirkby, Jasper', 'Kiss, D', 'Kittel, E Wolfram', 'Klimentov, A', 'König, A C', 'Kopp, A', 'Koutsenko, V F', 'Kräber, M H', 'Krämer, R W', 'Krenz, W', 'Krüger, A', 'Kunin, A', 'Ladrón de Guevara, P', 'Laktineh, I', 'Landi, G', 'Lassila-Perini, K M', 'Lebeau, M', 'Lebedev, A', 'Lebrun, Philippe.', 'Lecomte, P', 'Lecoq, P', 'Le Coultre, P', 'Lee, H J', 'Le Goff, J M', 'Leiste, R', 'Leonardi, E', 'Levchenko, P M', 'Li Chuan', 'Likhoded, S A', 'Lin, C H', 'Lin, W T', 'Linde, F L', 'Lista, L', 'Liu, Z A', 'Lohmann, W', 'Longo, E', 'Lü, Y S', 'Lübelsmeyer, K', 'Luci, C', 'Luckey, D', 'Lugnier, L', 'Luminari, L', 'Lustermann, W', 'Ma, W G', 'Maity, M', 'Malgeri, L', 'Malinin, A', 'Maña, C', 'Mangeol, D J', 'Mans, J', 'Marchesini, P A', 'Marian, G', 'Martin, J P', 'Marzano, F', 'Mazumdar, K', 'McNeil, R R', 'Mele, S', 'Merola, L', 'Meschini, M', 'Metzger, W J', 'Von der Mey, M', 'Mihul, A', 'Milcent, H', 'Mirabelli, G', 'Mnich, J', 'Mohanty, G B', 'Molnár, P', 'Moulik, T', 'Muanza, G S', 'Muijs, A J M', 'Musicar, B', 'Musy, M', 'Napolitano, M', 'Nessi-Tedaldi, F', 'Newman, H', 'Niessen, T', 'Nisati, A', 'Nowak, H', 'Organtini, G', 'Oulianov, A', 'Palomares, C', 'Pandoulas, D', 'Paoletti, S', 'Paolucci, P', 'Paramatti, R', 'Park, H K', 'Park, I H', 'Passaleva, G', 'Patricelli, S', 'Paul, T', 'Pauluzzi, M', 'Paus, C', 'Pauss, Felicitas', 'Pedace, M', 'Pensotti, S', 'Perret-Gallix, D', 'Petersen, B', 'Piccolo, D', 'Pierella, F', 'Pieri, M', 'Piroué, P A', 'Pistolesi, E', 'Plyaskin, V', 'Pohl, M', 'Pozhidaev, V', 'Postema, H', 'Pothier, J', 'Prokofiev, D O', 'Prokofev, D', 'Quartieri, J', 'Rahal-Callot, G', 'Rahaman, M A', 'Raics, P', 'Raja, N', 'Ramelli, R', 'Rancoita, P G', 'Raspereza, A V', 'Raven, G', 'Razis, P A', 'Ren, D', 'Rescigno, M', 'Reucroft, S', 'Riemann, S', 'Riles, K', 'Robohm, A', 'Rodin, J', 'Roe, B P', 'Romero, L', 'Rosca, A', 'Rosier-Lees, S', 'Rubio, Juan Antonio', 'Ruggiero, G', 'Ruschmeier, D', 'Rykaczewski, H', 'Saremi, S', 'Sarkar, S', 'Salicio, J', 'Sánchez, E', 'Sanders, M P', 'Sarakinos, M E', 'Schäfer, C', 'Shchegelskii, V', 'Schmidt-Kärst, S', 'Schmitz, D', 'Schopper, Herwig Franz', 'Schotanus, D J', 'Schwering, G', 'Sciacca, C', 'Sciarrino, D', 'Seganti, A', 'Servoli, L', 'Shevchenko, S', 'Shivarov, N', 'Shoutko, V', 'Shumilov, E', 'Shvorob, A V', 'Siedenburg, T', 'Son, D', 'Smith, B', 'Spillantini, P', 'Steuer, M', 'Stickland, D P', 'Stone, A', 'Stoyanov, B', 'Strässner, A', 'Sudhakar, K', 'Sultanov, G G', 'Sun, L Z', 'Suter, H', 'Swain, J D', 'Szillasi, Z', 'Sztaricskai, T', 'Tang, X W', 'Tauscher, Ludwig', 'Taylor, L', 'Tellili, B', 'Timmermans, C', 'Ting, S C C', 'Ting, S M', 'Tonwar, S C', 'Tóth, J', 'Tully, C', 'Tung, K L', 'Uchida, Y', 'Ulbricht, J', 'Valente, E', 'Vesztergombi, György', 'Vetlitskii, I', 'Vicinanza, D', 'Viertel, Gert M', 'Villa, S', 'Vivargent, M', 'Vlachos, S', 'Vodopyanov, I', 'Vogel, H', 'Vogt, H', 'Vorobev, I', 'Vorobyov, A A', 'Vorvolakos, A', 'Wadhwa, M', 'Wallraff, W', 'Wang, M', 'Wang, X L', 'Wang, Z M', 'Weber, A', 'Weber, M', 'Wienemann, P', 'Wilkens, H', 'Wu, S X', 'Wynhoff, S', 'Xia, L', 'Xu, Z Z', 'Yamamoto, J', 'Yang, B Z', 'Yang, C G', 'Yang, H J', 'Yang, M', 'Ye, J B', 'Yeh, S C', 'Zalite, A', 'Zalite, Yu', 'Zhang, Z P', 'Zhu, G Y', 'Zhu, R Y', 'Zichichi, Antonino', 'Zilizi, G', 'Zöller, M']",['Search for Manifestations of New Physics in Fermion-Pair Production at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, pair production', 'lepton, pair production', 'channel cross section', 'angular distribution, asymmetry', 'search for, new interaction', 'four-fermion interaction', 'leptoquark, exchange', 'squark, exchange', 'sneutrino, exchange', 'coupling constant, upper limit', 'leptoquark, mass', 'lower limit', 'string, effect', 'quantum gravity, higher-dimensional', 'fermion, extended particle', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', '130-189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005028'],"['The measurements of hadron and lepton-pair production cross sections and leptonic forward-backward asymmetries performed with the L3 detector at centre-of-mass energies between 130 GeV and 189 GeV are used to search for new physics phenomena such as: contact interactions, exchange of virtual leptoquarks, scalar quarks and scalar neutrinos, effects of TeV strings in models of quantum gravity with large extra dimensions and non-zero sizes of the fermions. No evidence for these phenomena is found and new limits on their parameters are set.']",['2000-05-23']
811,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the $\\omega\\omega$ channel produced in central pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'omega(783), pair production', 'postulated particle, f2(1910)', 'spin, parity', 'f4(2300)', 'postulated particle, f0(2000)', 'angular distribution', 'mass spectrum, (2omega(783))', 'mass spectrum, (pi+ pi- pi0)', 'magnetic spectrometer, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p 2omega(783)', '450 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005027'],"['The reaction pp -> pf (omega omega) ps has been studied at 450 GeV/c and a spin analysis of the omega omega channel has been performed for the first time in central production. Evidence is found for the f2(1910) in the JPC = 2++ wave with spin projection JZ = 2. This is the only state observed in central production with spin projection JZ = 2. Its dPT and phi dependencies are similar to those observed for other glueball candidates. In addition, evidence is found for a state with JPC = 4++ consistent with the f4(2300). The f0(2000), previously observed in the rho rho final state, is confirmed.']",['2000-05-22']
812,['eng'],"['Brooijmans, G']",['Top Quark Mass Measurements at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, La Thuile 2000/02/27', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'mass, truth', 'quark, pair production', 'quark, decay', 'final state, ((n)jet)', 'final state, ((n)jet lepton)', 'final state, dilepton', 'jet, energy', 'radiative correction, initial-state interaction', 'radiative correction, final-state interaction', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'upgrade, proposed', '1800 GeV-cms', 'talk, La Thuile 2000/02/27']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005030'],"['The general strategy, as well as channel-specific details, applied to the measurement of the top quark mass at the Tevatron in Run I are reviewed, and the combination of the results obtained by the CDF and DO collaborations presented. The accelerator and detector upgrades for Run II are described, and expected improvements in the systematic uncertainties on the measurement evaluated.']",['2000-05-23']
813,['eng'],"['Babukhadia, L R']",['Central and Forward Inclusive Jets at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'differential cross section, rapidity dependence', 'transverse energy, dependence', 'energy dependence', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005026'],"['We report on a new measurement of the rapidity dependence of the inclusive jet production cross section in pbar p collisions at sqrt(s)=1.8 TeV using 92 pb^-1 of data collected by the DZero detector at the Tevatron collider. The differential cross sections, d^2sigma/(dEt deta), are presented as a function of jet transverse energy (Et) in five pseudorapidity (eta) intervals, up to |eta|=3, significantly extending previous CDF and DZero measurements beyond |eta|=0.7. The extended range of the measurement should provide greater discrimination among different parton distribution functions. We also discuss previous measurements of the inclusive jet cross sections made by the two collider experiments at central pseudorapidities up to |eta|=0.7. Finally, we present recent measurements from the CDF and DZero experiments of the ratio of central inclusive cross sections from two center-of-mass energies, 0.63 TeV and 1.8 TeV, as a function of jet Xt. Experimental results are compared to next-to-leading order QCD predictions.']",['2000-05-18']
814,['eng'],"['Jain, S', 'Gupta, A K', 'Mondal, N K']",['Search for Quark-Lepton Compositeness at Tevatron and LHC'],['Particle Physics - Experimental Results'],"['anti-p p, inclusive reaction', 'p p, inclusive reaction', 'quark, composite', 'lepton, composite', 'electron, pair production', 'Drell-Yan process', 'mass spectrum, (positron electron)', 'effective Lagrangian', 'model, new interaction', 'particle identification, efficiency', 'numerical calculations, Monte Carlo', 'Batavia TEVATRON Coll', 'CERN LHC Coll', '2000, 14000 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005025'],"['We make a Monte Carlo study on compositeness of first generation quarks and leptons using the Drell-Yan distribution in the high dielectron mass region at the Tevatron and LHC energies. The current experimental lower limits on the compositeness scale, \\Lambda, vary from 2.5 to 6.1 TeV. In the present analysis, we assume that there will be no deviation of the dielectron mass spectrum from Standard Model prediction at center of mass energy 2 TeV (Tevatron) and 14 TeV (LHC). We then find that in the LL, RR, RL and LR chirality channels of the quark-electron currents, it is possible to extend the lower limits on \\Lambda (at 95% {CL}) to a range of 6 to 10 TeV for 2 fb^{-1} and 9 to 19 TeV for 30 fb^{-1} of integrated luminosity at Tevatron. At LHC, the corresponding limits extend to a range of 16 to 25 TeV for 10 fb^{-1} and 20 to 36 TeV for 100 fb^{-1} of integrated luminosity.']",['2000-05-18']
815,['eng'],"['Kado, M']",['Cornering Higgs Bosons at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, pair production', 'Higgs particle, decay modes', 'Higgs particle, multiplet', 'Higgs particle, mass', 'Higgs particle, coupling', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'Higgs particle --> charm strangeness', 'Higgs particle --> 2W', 'Higgs particle --> 2photon', 'Higgs particle --> 2beauty', 'Higgs particle --> tau neutrino/tau', '192-202 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005022'],['The most recent results of the searches for Higgs bosons in the data taken at LEP in 1999 and their interpretation in a variety of theoretical framework are reviewed.'],['2000-05-16']
816,['eng'],"['Bodek, Arie', 'Yang, U K', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'Bazarko, A O', 'Bernstein, R H', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Fleming, B T']","['Measurements of $F2, x F3 \\nu-x F3 \\nu b$ from CCFR neutrino-Fe and antineutrino-Fe data in a model independent way']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/18', 'neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'neutrino/mu', 'iron', 'charged current', 'nucleon, structure function', 'x-dependence', 'momentum transfer, dependence', 'differential cross section', 'muon nucleon, deep inelastic scattering', 'experimental results', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005021'],"['We report on the extraction of the structure functions F2 and Delta xF3 = xF3nu-xF3nub from CCFR neutrino-Fe and antineutrino-Fe differential cross sections. The extraction is performed in a physics model independent (PMI) way. This first measurement for Delta xF3 which is useful in testing models of heavy charm production, is higher than current theoretical predictions. The F2 (PMI) values measured in neutrino and muon scattering are in good agreement with the predictions of Next to Leading Order PDFs (using massive charm production schemes), thus resolving the long-standing discrepancy between the two sets of data.']",['2000-05-16']
817,['eng'],"['Toback, D']","['New Phenomena; 2, Recent Results from the Fermilab Tevatron']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/11', 'anti-p p, colliding beams', 'new particle, search for', 'supersymmetry', 'R parity, violation', 'vector meson, technicolor', ""Z', hadronic decay"", 'quark, pair production', 'quark, truth', 'vector meson, leptonic decay', 'electron, pair production', 'supergravity', 'gaugino, pair production', 'gaugino, decay modes', 'final state, (3lepton)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005020'],"[""The CDF and D\\O collaborations continue to search for new physics using more than 100~pb$^{-1}$ of \\xxbar{p} collisions at $\\sqrt{s}=1.8$ TeV collected at the Fermilab Tevatron. We present recent results from both experiments on R-parity violating Supersymmetry and $Z'$/Technicolor production with $ee$ and \\xxbar{t} final states. In addition we introduce Sherlock, a new quasi-model-independent search strategy.""]",['2000-05-15']
818,['eng'],"['Narsky, I']",['Expected Coverage of Bayesian Confidence Intervals for the Mean of a Poisson Statistic in Measurements with Background'],['Detectors and Experimental Techniques'],"['statistical analysis', 'background']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005019'],"['Expected coverage and expected length of 90% upper and lower limit and 68.27% central intervals are plotted as functions of the true signal for various values of expected background. Results for several objective priors are shown, and formulas for calculation of confidence intervals are obtained. For comparison, expected coverage and length of frequentist intervals constructed with the unified approach of Feldman and Cousins and a simple classical method are also shown. It is assumed that the expected background is accurately known prior to performing an experiment. The plots of expected coverage and length are provided for values of signal and background typical for particle experiments with small numbers of events.']",['2000-05-14']
819,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Abbiendi, G', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Coppola, N', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Brock, I', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Hartmann, H', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Foster, B', 'Heath, G P', 'Heath, H F', 'McFall, J D', 'Piccioni, D', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Burgard, C', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hasell, D', 'Hebbel, K', 'Johnson, K F', 'Kasemann, M', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Lindemann, L', 'Löhr, B', 'Martínez, M', 'Milite, M', 'Monteiro, T', 'Moritz, M', 'Notz, D', 'Pelucchi, F', 'Petrucci, M C', 'Rohde, M', 'Saull, P R B', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Tassi, E', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'Votano, L', 'Bamberger, Andreas', 'Benen, A', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Bell, M', 'Doyle, A T', 'Lee, S W', 'Lupi, A', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Garfagnini, A', 'Gialas, I', 'Gladilin, L K', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Poelz, G', 'Zetsche, F', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Mallik, U', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Park, I H', 'Son, D', 'Barreiro, F', 'García, G', 'Glasman, C', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Barbi, M S', 'Corriveau, F', 'Hanna, D S', 'Ochs, A', 'Padhi, S', 'Riveline, M', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Antonov, A', 'Bashkirov, V', 'Danilov, M V', 'Dolgoshein, B A', 'Gladkov, D', 'Sosnovtsev, V V', 'Suchkov, S', 'Dementev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Shcheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Acosta, D', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Quadt, A', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dosselli, U', 'Dusini, S', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Turcato, M', 'Voci, C', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sabetfakhri, A', 'Simmons, D', 'Butterworth, J M', 'Catterall, C D', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Pawlak, R', 'Smalska, B', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Gadaj, T', 'Deppe, O', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Badgett, W F', 'Chapin, D', 'Cross, R', 'Foudas, C', 'Mattingly, S E', 'Reeder, D D', 'Smith, W H', 'Vaiciulis, A W', 'Wildschek, T', 'Wodarczyk, M', 'Deshpande, A A', 'Dhawan, S K', 'Hughes, V W', 'Bhadra, S', 'Catterall, C D', 'Cole, J E', 'Frisken, W R', 'Hall-Wilton, R', 'Khakzad, M', 'Menary, S R']",['Measurement of the Proton Structure Function $F_{2}$ at Very Low $Q^{2}$ at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'p, structure function', 'x-dependence', 'momentum transfer, dependence', 'semiconductor detector, microstrip', 'tables', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005018'],"['A measurement of the proton structure function F_2(x,Q^2) is presented in the kinematic range 0.045 GeV^2 < Q^2 < 0.65 GeV^2 and 6*10^{-7} < x < 1*10^{-3}. The results were obtained using a data sample corresponding to an integrated luminosity of 3.9pb^-1 in e^+p reactions recorded with the ZEUS detector at HERA. Information from a silicon-strip tracking detector, installed in front of the small electromagnetic calorimeter used to measure the energy of the final-state positron at small scattering angles, together with an enhanced simulation of the hadronic final state, has permitted the extension of the kinematic range beyond that of previous measurements. The uncertainties in F_2 are typically less than 4%. At the low Q^2 values of the present measurement, the rise of F_2 at low x is slower than observed in HERA data at higher Q^2 and can be described by Regge theory with a constant logarithmic slope. The dependence of F_2 on Q^2 is stronger than at higher Q^2 values, approaching, at the lowest Q^2 values of this measurement, a region where F_2 becomes nearly proportional to Q^2.']",['2000-05-14']
820,['eng'],"['Achasov, M N', 'Baru, S E', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Koop, I A', 'Koshuba, S V', 'Kukartsev, G A', 'Mamutkin, A A', 'Pakhtusova, E V', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Valishev, A A']",['The $\\phi(1020) \\to \\pi^{0}\\pi^{0}\\gamma$ decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), branching ratio', 'f0(975), intermediate state', 'f0(975), mass', 'f0(975), width', 'mass spectrum, (2pi0)', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> 2pi0 photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005017'],"['In the SND experiment at VEPP-2M $e^+e^-$ collider the $\\phi(1020)\\to\\pi^0\\pi^0\\gamma$ decay was studied and its branching ratio was measured: $B(\\phi\\to\\pi^0\\pi^0\\gamma)=(1.221\\pm 0.098\\pm0.061)\\cdot10^{-4}$. It was shown, that $f_0(980)\\gamma$ intermediate state dominates in this decay and the $f_0(980)$-meson parameters were obtained.']",['2000-05-14']
821,['eng'],"['Appel, R', 'Atoyan, G S', 'Bassalleck, B', 'Bergman, D R', 'Brown, D N', 'Cheung, N', 'Dhawan, S K', 'Do, H', 'Egger, J', 'Eilerts, S W', 'Felder, C', 'Fischer, H', 'Gach, M', 'Herold, W D', 'Issakov, V V', 'Kaspar, H', 'Kraus, D E', 'Lazarus, D M', 'Leipune, L']",['An Improved Limit on the Rate Of Decay $K^{+} \\to \\pi^{+}mu^{+}e^{-}$'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'violation, flavor', 'K+, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ muon+ electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005016'],['The experiment E865 at BNL places an upper limit on the branching ratio for the decay K+ -> pi+ mu+ e- of 3.9x10^-11 (90% C.L.). Along with with other results this yields a combined upper limit on this branching ratio of 2.8x10^-11. A new upper limit on the branching ratio for pi0 -> mu+ e- of 3.8x10^-10 (90% C.L.) is also established. The experiment and analysis are described.'],['2000-06-23']
822,['eng'],"['Cinabro, D']",['The $t\\overline{t}$ Threshold and Machine Parameters at the NLC'],['Detectors and Experimental Techniques'],"['talk, Sitges 1999/04/28', 'electron positron, linear collider', 'linear collider, proposed', 'luminosity', 'beam, radiation', 'quark, pair production', 'quark, truth', 'channel cross section']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005015'],"['One of the problems in the design of a high energy e+e- linear collider is the distribution of the luminosity as a function of real collision energy, dL/dE, due to initial state radiation, beamstrahlung, and the energy spread of the collider. These effects smear a sharp feature in the cross section of e+e- -> hadrons such as the ttbar threshold into a flatter structure. This study reviews the impact on dL/dE of these effects as a function of machine parameters, explores some methods of measuring dL/dE with Bhabha scattering, how the dL/dE flattens the ttbar cross section near threshold, and the effect the dL/dE measurement has on extracting parameters of the top quark, such as the mass and width, in a 2.5/fb scan of the ttbar threshold.']",['2000-05-10']
823,['eng'],"['Blaufuss, E', 'Guillian, G', 'Fukuda, Y', 'Fukuda, S', 'Ishitsuka, M', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kobayashi, K', 'Kobayashi, Y', 'Koshio, Y', 'Miura, M', 'Moriyama, S', 'Nakahata, M', 'Nakayama, S', 'Obayashi, Y', 'Okada, A', 'Okumura, K', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, H', 'Takeuchi, Y', 'Toshito, T', 'Totsuka, Y', 'Yamada, S', 'Earl, M A', 'Habig, A', 'Kearns, E T', 'Messier, M D', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Goldhaber, M', 'Barszczak, T', 'Casper, David William', 'Gajewski, W', 'Kropp, W R', 'Mine, S', 'Price, L R', 'Smy, M B', 'Sobel, H W', 'Vagins, M R', 'Ganezer, K S', 'Keig, W E', 'Ellsworth, R W', 'Tasaka, S', 'Kibayashi, A', 'Learned, J G', 'Matsuno, S', 'Takemori, D', 'Hayato, Y', 'Ishii, T', 'Kobayashi, T', 'Nakamura, K', 'Oyama, Y', 'Sakai, A', 'Sakuda, M', 'Sasaki, O', 'Echigo, S', 'Kohama, M', 'Suzuki, A T', 'Inagaki, T', 'Nishikawa, K', 'Haines, T J', 'Kim, B K', 'Sanford, R', 'Svoboda, R', 'Chen, M L', 'Goodman, J A', 'Sullivan, G W', 'Hill, J', 'Jung, C K', 'Martens, K', 'Malek, M', 'Mauger, C', 'McGrew, C', 'Sharkey, E', 'Viren, B M', 'Yanagisawa, C', 'Kirisawa, M', 'Inaba, S', 'Mitsuda, C', 'Miyano, K', 'Okazawa, H', 'Saji, C', 'Takahashi, M', 'Takahata, M', 'Nagashima, Y', 'Nitta, K', 'Takita, M', 'Yoshida, M', 'Kim, S B', 'Etoh, M', 'Gando, Y', 'Hasegawa, T', 'Inoue, K', 'Ishihara, K', 'Maruyama, T', 'Shirai, J', 'Suzuki, A', 'Koshiba, M', 'Hatakeyama, Y', 'Ichikawa, Y', 'Koike, M', 'Nishijima, K', 'Fujiyasu, H', 'Ishino, H', 'Morii, M', 'Watanabe, Y', 'Golebiewska, U', 'Kielczewska, D', 'Boyd, S C', 'Stachyra, A L', 'Wilkes, R J', 'Young, K K']",['$^{16}N$ as a calibration source for Super-Kamiokande'],['Detectors and Experimental Techniques'],"['neutrino, solar', 'Cherenkov counter, water', 'calibration', 'nitrogen, nuclide', 'nitrogen, particle source', 'n nucleus, nuclear reaction', 'oxygen', 'deep underground detector, KAMIOKANDE']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005014'],"['The decay of 16-N is used to cross check the absolute energy scale calibration for solar neutrinos established by the electron linear accelerator (LINAC). A deuterium-tritium neutron generator was employed to create 16-N via the (n,p) reaction on 16-O in the water of the detector. This technique is isotropic and has different systematic uncertainties than the LINAC. The results from this high statistics data sample agree with the absolute energy scale of the LINAC to better than 1%. A natural source of 16-N from the capture of mu^- on 16-O, which is collected as a background to the solar neutrino analysis, is also discussed.']",['2000-05-10']
824,['eng'],"['Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Morrison, R J', 'Nelson, H N', 'Briere, R A']",['Precise Measurement of $B^{0}-\\overline{B}^{0}$ Mixing Parameters at the $\\Upsilon(4S)$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0 anti-B0, interference', 'parametrization', 'anti-B0, hadronic decay', 'D*(2010)', 'rho(770)', 'B0, mass difference', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> B0 anti-B0', 'anti-B0 --> D*(2010) pi', 'anti-B0 --> D*(2010) rho(770)', '10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005013'],"['We describe a measurement of B^0-B^0bar mixing parameters exploiting a method of partial reconstruction of the decay chains B0 -> D^{*-}\\pi^+ and B0 -> D^{*-}\\rho^+. Using 9.6 x 10^6 BBbar pairs collected at the Cornell Electron Storage Ring, we find \\chi_d = 0.198 +- 0.013 +- 0.014, |y_d|<0.41 at 95% confidence level, and |Re(\\epsilon_B)|<0.034 at 95% confidence level.']",['2000-05-09']
825,['eng'],"['Blazey, G C', 'Dittmann, J R', 'Ellis, S D', 'Elvira, V D', 'Frame, K', 'Grinstein, S', 'Hirosky, R', 'Piegaia, R', 'Schellman, H', 'Snihur, R', 'Sorin, V', 'Zeppenfeld, Dieter']",['Run II Jet Physics'],['Particle Physics - Experimental Results'],"['talk, Batavia 1999/11/04', 'anti-p p, colliding beams', 'jet, hadroproduction', 'jet, particle identification', 'jet, multiple production', 'energy flow', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'data analysis method', 'momentum, calibration', 'event shape analysis', 'numerical calculations, Monte Carlo', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005012'],"['The Run II jet physics group includes the Jet Algorithms, Jet Shape/Energy Flow, and Jet Measurements/Correlations subgroups. The main goal of the jet algorithm subgroup was to explore and define standard Run II jet finding procedures for CDF and DO. The focus of the jet shape/energy flow group was the study of jets as objects and the energy flows around these objects. The jet measurements/correlations subgroup discussed measurements at different beam energies; strong coupling constant measurements; and LO, NLO, NNLO, and threshold jet calculations. As a practical matter the algorithm and shape/energy flow groups merged to concentrate on the development of Run II jet algorithms that are both free of theoretical and experimental difficulties and able to reproduce Run I measurements. Starting from a review of the experience gained during Run I, the group considered a variety of cone algorithms and KT algorithms. The current understanding of both types of algorithms, including calibration issues, are discussed in this report along with some preliminary experimental results. The jet algorithms group recommends that CDF and DO employ the same version of both a cone algorithm and a KT algorithm during Run II. Proposed versions of each type of algorithm are discussed. The group also recommends the use of full 4-vector kinematic variables whenever possible. The recommended algorithms attempt to minimize the impact of seeds in the case of the cone algorithm and preclustering in the case of the KT algorithm. Issues regarding precluster definitions and merge/split criteria require further study.']",['2000-05-09']
826,['eng'],"['Link, J M', 'Paolone, V S', 'Reyes, M', 'Yager, P M', 'Anjos, J C', 'Bediaga, I', 'Göbel, C', 'Magnin, J', 'De Miranda, J M', 'Pepe, I M', 'Dos Reis, A C', 'Simão, F R A', 'Carrillo, S', 'Casimiro, E', 'Méndez, H', 'Sánchez-Hernández, A', 'Uribe, C', 'Vázquez, F', 'Cinquini, L', 'Cumalat, J P', 'Ramírez, J E', ""O'Reilly, B"", 'Vaandering, E W', 'Butler, J N', 'Cheung, H W K', 'Gaines, I', 'Garbincius, P H', 'Garren, L A', 'Gottschalk, E E', 'Gourlay, S A', 'Kasper, P H', 'Kreymer, A E', 'Kutschke, R', 'Bianco, S', 'Fabbri, F L', 'Sarwar, S', 'Zallo, A', 'Cawlfield, C', 'Kim, D Y', 'Park, K S', 'Rahimi, A', 'Wiss, J', 'Gardner, R', 'Chung, Y S', 'Kang, J S', 'Ko, B R', 'Kwak, J W', 'Lee, K B', 'Myung, S S', 'Park, H', 'Alimonti, G', 'Boschini, M', 'Brambilla, D', 'Caccianiga, B', 'Calandrino, A', ""D'Angelo, P"", 'Di Corato, M', 'Dini, P', 'Giammarchi, M G', 'Inzani, P', 'Leveraro, F', 'Malvezzi, S', 'Menasce, D', 'Mezzadri, M', 'Milazzo, L', 'Moroni, L', 'Pedrini, D', 'Prelz, F', 'Rovere, M', 'Sala, A', 'Sala, S', 'Davenport, T F', 'Arena, V', 'Boca, G', 'Bonomi, G', 'Gianini, G', 'Liguori, G', 'Merlo, M', 'Pantea, D', 'Ratti, S P', 'Riccardi, C', 'Torre, P', 'Viola, L', 'Vitulo, P', 'Hernández, H', 'López, A M', 'Méndez, L', 'Mirles, M A', 'Montiel, E', 'Olaya, D', 'Quinones, J', 'Rivera, C', 'Zhang, Y', 'Copty, N K', 'Purohit, M', 'Wilson, J R', 'Cho, K', 'Handler, T', 'Engh, D', 'Johns, W E', 'Hosack, M', 'Nehring, M S', 'Sales, M', 'Sheldon, P D', 'Stenson, K', 'Webster, M S', 'Sheaff, M', 'Kwon, Y J']",['Measurements of the $\\Sigma_{c}^{0}$ and $\\Sigma_{c}^{++}$ Mass Splittings'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium', 'oxygen', 'charmed baryon, hadronic decay', 'Sigma/c0', 'Sigma/c++', 'Lambda/c+', 'charmed baryon, photoproduction', 'mass difference, (Sigma/c0 Lambda/c+)', 'mass difference, (Sigma/c++ Lambda/c+)', 'mass difference, (Sigma/c++ Sigma/c0)', 'forward spectrometer, experimental results', 'Batavia TEVATRON PS', '180 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005011'],"['Using a high statistics sample of photoproduced charmed particles from the FOCUS experiment at Fermilab (FNAL-E831), we measure the mass splittings of the charmed baryons Sigma_c^0 and Sigma_c^{++}. We find M(Sigma_c^0 - Lambda_c^+) = 167.38 +/- 0.21 +/- 0.13 MeV/c^2 and M(Sigma_c^++ - Lambda_c^+) = 167.35 +/- 0.19 +/- 0.12 MeV/c^2 with samples of 362 +/- 36 and 461 +/- 39 events, respectively. We measure the isospin mass splitting M(Sigma_c^++ - Sigma_c^0) to be -0.03 +/- 0.28 +/- 0.11 Mev/c^2. The first errors are statistical and the second are systematic.']",['2000-05-09']
827,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bähr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Borras, K', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P D', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hilgers, M', 'Hiller, K H', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Kaufmann, O', 'Kausch, M', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krücker, D', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Kutuev, R K', 'Lachnit, W A', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'Lobodzinska, E', 'Lobodzinski, B', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vazdik, Ya', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Measurement of elastic electroproduction of $\\phi$ mesons at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, exclusive reaction', 'Phi(1020), electroproduction', 'vector meson, electroproduction', 'channel cross section, momentum transfer', 'Phi(1020), polarization', 'polarization, longitudinal', 'polarization, transverse', 'Phi(1020), hadronic decay', 'channel cross section, ratio', 'angular distribution', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> Phi(1020) p positron', 'Phi(1020) --> K+ K-', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005010'],"['The elastic electroproduction of phi mesons is studied at HERA with the H1 detector for photon virtualities 1 < Q^2 < 15 GeV^2 and hadronic centre of mass energies 40 < W < 130 GeV. The Q^2 and t dependences of the cross section are extracted (t being the square of the four-momentum transfer to the target proton). When plotted as function of (Q^2 + M_V^2) and scaled by the appropriate SU(5) quark charge factor, the phi meson cross section agrees within errors with the cross sections of the vector mesons V = rho, omega and J/psi. A detailed analysis is performed of the phi meson polarisation state and the ratio of the production cross sections for longitudinally and transversely polarised phi mesons is determined. A small but significant violation of s-channel helicity conservation (SCHC) is observed.']",['2000-05-09']
828,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A measurement of the $\\tau$ mass and the first CPT test with $\\tau$ leptons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'tau, pair production', 'tau, semileptonic decay', 'tau, mass', 'invariance, CPT', 'validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005009'],['We measure the mass of the tau lepton to be 1775.1+-1.6(stat)+-1.0(sys t.) MeV using tau pairs from Z0 decays. To test CPT invariance we compare the masses of the positively and negatively charged tau leptons. The relative mass difference is found to be smaller than 3.0 10^-3 at the 90% confidence level.'],['2000-05-05']
829,['eng'],"['King, B J']",['Prospects for Colliders and Collider Physics to the 1 PeV Energy Scale'],['Particle Physics - Experimental Results'],"['talk, Montauk 1999/09/27', 'electron positron, linear collider', 'muon+ muon-, storage ring', 'muon+ muon-, linear collider', 'p p, storage ring', 'energy', 'luminosity', 'neutrino, particle source', 'synchrotron radiation', 'magnet', 'technology', 'costs']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005008'],"[""A review is given of the prospects for future colliders and collider physics at the energy frontier. A proof-of-plausibility scenario is presented for maximizing our progress in elementary particle physics by extending the energy reach of hadron and lepton colliders as quickly and economically as might be technically and financially feasible. The scenario comprises 5 colliders beyond the LHC -- one each of e+e- and hadron colliders and three muon colliders -- and is able to hold to the historical rate of progress in the log-energy reach of hadron and lepton colliders, reaching the 1 PeV constituent mass scale by the early 2040's. The technical and fiscal requirements for the feasibility of the scenario are assessed and relevant long-term R&D projects are identified. Considerations of both cost and logistics seem to strongly favor housing most or all of the colliders in the scenario in a new world high energy physics laboratory""]",['2000-05-05']
830,['eng'],"['King, B J']",['Mighty MURINEs'],['Particle Physics - Experimental Results'],"['talk, Montauk 1999/09/27', 'muon+ muon-, colliding beams', 'neutrino, particle source', 'neutrino, beam', 'luminosity', 'neutrino nucleon, interaction', 'charged current', 'neutral current, flavor changing', 'counters and detectors', 'B, particle source', 'Kobayashi-Maskawa angle', 'violation, CP', 'Feynman graph', 'quark, truth', 'leptoquark', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005007'],"['An overview is given of the potential for neutrino physics studies through parasitic use of the intense high energy neutrino beams that would be produced at future many-TeV muon colliders. Neutrino experiments clearly cannot compete with the collider physics. Except at the very highest energy muon colliders, the main thrust of the neutrino physics program would be to improve on the measurements from preceding neutrino experiments at lower energy muon colliders, particularly in the fields of B physics, quark mixing and CP violation. Muon colliders at the 10 TeV energy scale might already produce of order 10^8 B hadrons per year in a favorable and unique enough experimental environment to have some analytical capabilities beyond any of the currently operating or proposed B factories. The most important of the quark mixing measurements at these energies might well be the improved measurements of the important CKM matrix elements |V_ub| and |V_cb| and, possibly, the first measurements of |V_td| in the process of flavor changing neutral current interactions involving a top quark loop. Muon colliders at the highest center-of-mass energies that have been conjectured, 100--1000 TeV, would produce neutrino beams for neutrino-nucleon interaction experiments with maximum center-of-mass energies from 300--1000 GeV. Such energies are comparable to the 314 GeV center-of-mass energy for electron-proton scattering at the HERA collider, but the luminosity would would be several orders of magnitude larger. This would potentially open up the possibility for high statistics studies of any exotic particles, such as leptoquarks, that might have been previously discovered at these energy scales.']",['2000-05-05']
831,['eng'],"['King, B J']",['Neutrino Radiation Challenges and Proposed Solutions for Many-TeV Muon Colliders'],['Particle Physics - Experimental Results'],"['talk, Montauk 1999/09/27', 'muon+ muon-, storage ring', 'muon+ muon-, linear collider', 'neutrino, radiation', 'dosimetry', 'energy dependence', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005006'],"['Neutrino radiation is expected to impose major design and siting constraints on many-TeV muon colliders. Previous predictions for radiation doses at TeV energy scales are briefly reviewed and then modified for extension to the many-TeV energy regime. The energy-cubed dependence of lower energy colliders is found to soften to an increase of slightly less than quadratic when averaged over the plane of the collider ring and slightly less than linear for the radiation hot spots downstream from straight sections in the collider ring. Despite this, the numerical values are judged to be sufficiently high that any many-TeV muon colliders will likely be constructed on large isolated sites specifically chosen to minimize or eliminate human exposure to the neutrino radiation. It is pointed out that such sites would be of an appropriate size scale to also house future proton-proton and electron-positron colliders at the high energy frontier, which naturally leads to conjecture on the possibilities for a new world laboratory for high energy physics. Radiation dose predictions are also presented for the speculative possibility of linear muon colliders. These have greatly reduced radiation constraints relative to circular muon colliders because radiation is only emitted in two pencil beams directed along the axes of the opposing linacs.']",['2000-05-04']
832,['eng'],"['Kalbfleisch, G R', 'Milton, K A', 'Strauss, M G', 'Gamberg, L P', 'Smith, E H', 'Luo, W']",['Improved Experimental Limits on the Production of Magnetic Monopoles'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'magnetic monopole, search for', 'magnetic monopole, pair production', 'charge, magnetic', 'Drell-Yan process', 'channel cross section, mass', 'upper limit', 'superconducting, interference', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005005'],"['We present new limits on low mass accelerator-produced point-like Dirac magnetic monopoles trapped and bound in matter surrounding the D\\O collision region of the Tevatron at Fermilab (experiment E-882). In the context of a Drell-Yan mechanism, we obtain cross section limits for the production of monopoles with magnetic charge values of 1, 2, 3, and 6 times the minimum Dirac charge of the order of picobarns, some hundred times smaller than found in similar previous Fermilab searches. Mass limits inferred from these cross section limits are presented.']",['2000-05-04']
833,['eng'],"['Luk, K B']",['Examining CP Symmetry in Strange Baryon Decays'],['Particle Physics - Experimental Results'],"['talk, Taipei 1999/12/03', 'p nucleus, inclusive reaction', 'beryllium', 'hyperon, hadroproduction', 'hyperon, polarization', 'Xi-, hadronic decay', 'Antixi-, hadronic decay', 'angular distribution, asymmetry', 'invariance, CP', 'validity test', 'helicity', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'proposed experiment', 'Xi- --> Lambda pi-', 'Antixi- --> Antilambda pi+', '800 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005004'],"['Non-conservation of CP symmetry can manisfest itself in non-leptonic hyperon decays as a difference in the decay parameter between the strange-baryon decay and its charge conjugate. By comparing the decay distribution in the $\\Lambda$ helicity frame for the decay sequence $\\Xi^{-} \\to \\Lambda \\pi^{-}$, $\\Lambda \\to p \\pi^{-}$ with that of $\\bar{\\Xi}^{+}$ decay, E756 at Fermilab did not observe any CP-odd effect at the $10^{-2}$ level. The status of a follow-up experiment, HyperCP (FNAL E871), to search for CP violation in charged $\\Xi-\\Lambda$ decay with a sensitivity of $10^{-4}$ is also presented.']",['2000-05-04']
834,['eng'],"['Jochum, J', 'Bravin, M', 'Bruckmayer, M', 'Bucci, C', 'Cooper, S', 'Cozzini, C', 'Di Stefano, P', 'Von Feilitzsch, F', 'Frank, T', 'Jagemann, T', 'Keeling, R', 'Kraus, H', 'Lush, G J', 'Marchese, J', 'Meier, O', 'Meunier, P', 'Nagel, U', 'Pergolesi, D', 'Pröbst, F', 'Ramachers, Y', 'Schnagl, J', 'Seidel, W', 'Sergeyev, I', 'Stark, M', 'Stodolsky, L', 'Uchaikin, S V', 'Wulandari, H']",['The CRESST dark matter search'],['Particle Physics - Experimental Results'],"['talk, Dubna 1999/06/28', 'talk, Marina del Rey 2000/02/23', 'astrophysics, missing-mass', 'WIMP, search for', 'scattering, WIMP nucleon', 'channel cross section, mass', 'counters and detectors, superconducting', 'scintillation counter, crystal', 'performance', 'deep underground detector, Gran Sasso', 'numerical calculations', 'proposed experiment', 'talk, Heidelberg 2000/07/10']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005003'],"['We present the current status of CRESST(Cryogenic Rare Event Search using Superconducting Thermometers) project and new results concerning the development of new detectors based on the simultaneous measurement of phonons and scintillation light. A significant reduction in the background rate could recently be achieved. With our newly developed method for the simultaneous measurement of scintillation light, strong background discrimination is possible also in larger detectors, resulting in a substantial increase in WIMP detection sensitivity.']",['2000-05-03']
835,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Ainsley, C', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fleck, I', 'Ford, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Pooth, O', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Vossebeld, J H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Photonic events with missing energy in $e^{+}e^{-}$ collisions at $\\sqrt{s}=189 GeV$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'neutrino, pair production', 'photon, associated production', 'missing-energy, high', 'new particle, search for', 'neutrino, excited state', 'neutralino', 'gravitino', 'postulated particle, pair production', 'postulated particle, radiative decay', 'space-time, higher-dimensional', 'channel cross section, branching ratio', 'mass, dependence', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> photon missing-energy', 'electron positron --> neutrino antineutrino photon', '189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005002'],"['Photonic events with large missing energy have been observed in e+e- collisions at a centre-of-mass energy of 189GeV using the OPAL detector at LEP. Results are presented for event topologies consistent with a single photon or with an acoplanar photon pair. Cross-section measurements are performed within the kinematic acceptance of each selection, and the number of light neutrino species is measured. Cross-section results are compared with the expectations from the Standard Model process e+e- to nu nubar + photon(s). No evidence is observed for new physics contributions to these final states. Upper limits are derived on sigma(e+e- to XY).BR(X to Y gamma) and sigma(e+e- to XX).BR**2(X to Y gamma) for the case of stable and invisible Y. These limits apply to single and pair production of excited neutrinos (X=nu*, Y = nu), to neutralino production (X=neutralino_2, Y=neutralino_1) and to supersymmetric models in which X = neutralino_1 and Y = light gravitino. The case of macroscopic decay lengths of particle X is considered for e+e- to XX, X to Y gamma, when M_Y is of order zero. The single-photon results are also used to place upper limits on superlight gravitino pair production as well as graviton-photon production in the context of theories with additional space dimensions.']",['2000-05-03']
836,['eng'],"['Abe, K', 'Abe, K', 'Abe, T', 'Adam, I', 'Akagi, T', 'Allen, N J', 'Ash, William W', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barakat, M B', 'Bardon, O', 'Barklow, T L', 'Bashindzhagian, G L', 'Bauer, J M', 'Bellodi, G', 'Ben-David, R', 'Benvenuti, Alberto C', 'Bilei, G M', 'Bisello, D', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Calloway, D', 'Camanzi, B', 'Carpinelli, M', 'Cassell, R', 'Castaldi, R', 'Castro, A', 'Cavalli-Sforza, M', 'Chou, A', 'Church, E', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cotton, R', 'Cowan, R F', 'Coyne, D G', 'Crawford, G', 'Damerell, C J S', 'Danielson, M N', 'Daoudi, M', 'De Groot, N', ""Dell'Orso, R"", 'Dervan, P J', 'De Sangro, R', 'Dima, M', 'de Oliveira, A', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Eisenstein, B I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fan, C', 'Fernández, J P', 'Fero, M J', 'Flood, K', 'Frey, R', 'Gifford, J A', 'Gillman, T', 'Gladding, G E', 'González, S', 'Goodman, E R', 'Hart, E L', 'Harton, J L', 'Hasan, A', 'Hasuko, K', 'Hedges, S J', 'Hertzbach, S S', 'Hildreth, M D', 'Huber, J', 'Huffer, M E', 'Hughes, E W', 'Huynh, X', 'Hwang, H', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Johnson, R A', 'Junk, T R', 'Kajikawa, R', 'Kalelkar, M S', 'Kamyshkov, Yu A', 'Kang, H J', 'Karliner, I', 'Kawahara, H', 'Kim, Y D', 'King, M E', 'King, R', 'Kofler, R R', 'Krishna, N M', 'Kroeger, R S', 'Langston, M', 'Lath, A', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Liu, M X', 'Liu, X', 'Loreti, M', 'Lu, A', 'Lynch, H L', 'Ma, J', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'Masuda, H', 'Mazzucato, E', 'McKemey, A K', 'Meadows, B T', 'Menegatti, G', 'Messner, R', 'Mockett, P M', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Nagamine, T', 'Narita, S', 'Nauenberg, U', 'Neal, H', 'Nussbaum, M', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Pavel, T J', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Pitts, K T', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Punkar, G D', 'Quigley, J', 'Ratcliff, B N', 'Reeves, T W', 'Reidy, J', 'Reinertsen, P L', 'Rensing, P E', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schindler, R H', 'Schumm, B A', 'Schwiening, J', 'Sen, S', 'Serbo, V V', 'Shaevitz, M H', 'Shank, J T', 'Shapiro, G', 'Sherden, D J', 'Shmakov, K D', 'Simopoulos, C', 'Sinev, N B', 'Smith, S R', 'Smy, M B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Steiner, R', 'Strauss, M G', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Szumilo, A', 'Takahashi, T', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Toumbas, N K', 'Usher, T', 'Vannini, C', 'Vavra, J', 'Vella, E N', 'Venuti, J P', 'Verdier, R', 'Verdini, P G', 'Wagner, D L', 'Wagner, S R', 'Waite, A P', 'Walston, S', 'Wang, J', 'Watts, S J', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'White, S L', 'Wickens, F J', 'Williams, B', 'Williams, D C', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Word, G B', 'Wright, T R', 'Wyss, J', 'Yamamoto, R K', 'Yamartino, J M', 'Yang, X', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H', 'Zapalac, G H', 'Zdarko, R W', 'Zhou, J']",['Measurements of $Z^{0}$ Electroweak Couplings at SLD'],['Particle Physics - Experimental Results'],"['talk, La Thuile 2000/02/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'polarization, longitudinal', 'Z0, electroproduction', 'Z0, leptonic decay', 'Z0, hadronic decay', 'lepton, pair production', 'quark, pair production', 'quark, charm', 'quark, beauty', 'quark, semileptonic decay', 'charmed meson, decay', 'Z0, coupling', 'angular distribution, asymmetry', 'polarization, asymmetry', 'Weinberg angle', 'tau, polarization', 'talk, La Thuile 2000/02/27', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0005001'],"['We present a summary of the results of several electroweak measurements performed by the SLD experiment at the Stanford Linear Collider (SLC). Most of these results are preliminary and are based, unless otherwise indicated, on the full 1993-8 data set of approximately 550,000 hadronic decays of Z0 bosons produced with an average electron beam polarization of 73%.']",['2000-05-02']
837,['eng'],"['Green, J A']",['Searches for Compositeness at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Blois 1999/06/28', 'anti-p p, colliding beams', 'neutrino nucleon, interaction', 'search for, composite', 'quark, composite', 'quark, excited state', 'lepton, composite', 'new interaction', 'jet, pair production', 'mass spectrum, (2jet)', 'angular distribution, jet', 'postulated particle, coloron', 'lepton, pair production', 'Drell-Yan process', 'electroweak interaction, validity test', 'calorimeter', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004035'],"['Quark-quark and quark-lepton searches for compositenss at the Fermilab Tevatron are summarized. These are of the contact-interaction variety where sqrt(s-hat) < the hypothesized mass scales, Lambda. Tevatron experiments limit a variety of compositeness phenomena in the range from 1.9 to 8.3 TeV. These limits result from measurements of: the Ht spectrum (D0), dijet mass (D0), dijet angular distribution (CDF, D0), drell-yan production (CDF, D0), and the Neutral Current to Charged Current ratio (CCFR/NuTeV).']",['2000-05-01']
838,['eng'],"['Link, J M', 'Paolone, V S', 'Reyes, M', 'Yager, P M', 'Anjos, J C', 'Bediaga, I', 'Göbel, C', 'Magnin, J', 'De Miranda, J M', 'Pepe, I M', 'Dos Reis, A C', 'Simão, F R A', 'Do Vale, M A B', 'Carrillo, S', 'Casimiro, E', 'Méndez, H', 'Sánchez-Hernández, A', 'Uribe, C', 'Vázquez, F', 'Cinquini, L', 'Cumalat, J P', 'Ramírez, J E', ""O'Reilly, B"", 'Vaandering, E W', 'Butler, J N', 'Cheung, H W K', 'Gaines, I', 'Garbincius, P H', 'Garren, L A', 'Gottschalk, E E', 'Gourlay, S A', 'Kasper, P H', 'Kreymer, A E', 'Kutschke, R', 'Bianco, S', 'Fabbri, F L', 'Sarwar, S', 'Zallo, A', 'Cawlfield, C', 'Kim, D Y', 'Park, K S', 'Rahimi, A', 'Wiss, J', 'Gardner, R', 'Chung, Y S', 'Kang, J S', 'Ko, B R', 'Kwak, J W', 'Lee, K B', 'Myung, S S', 'Park, H', 'Alimonti, G', 'Boschini, M', 'Brambilla, D', 'Caccianiga, B', 'Calandrino, A', ""D'Angelo, P"", 'Di Corato, M', 'Dini, P', 'Giammarchi, M G', 'Inzani, P', 'Leveraro, F', 'Malvezzi, S', 'Menasce, D', 'Mezzadri, M', 'Milazzo, L', 'Moroni, L', 'Pedrini, D', 'Prelz, F', 'Rovere, M', 'Sala, A', 'Sala, S', 'Davenport, T F', 'Arena, V', 'Boca, G', 'Bonomi, G', 'Gianini, G', 'Liguori, G', 'Merlo, M', 'Pantea, D', 'Ratti, S P', 'Riccardi, C', 'Torre, P', 'Viola, L', 'Vitulo, P', 'Hernández, H', 'López, A M', 'Méndez, L', 'Mirles, M A', 'Montiel, E', 'Olaya, D', 'Quinones, J', 'Rivera, C', 'Zhang, Y', 'Copty, N K', 'Purohit, M', 'Wilson, J R', 'Cho, K', 'Handler, T', 'Engh, D', 'Johns, W E', 'Hosack, M', 'Nehring, M S', 'Sales, M', 'Sheldon, P D', 'Stenson, K', 'Webster, M S', 'Sheaff, M', 'Kwon, Y J']",['A measurement of lifetime differences in the neutral D-meson system'],['Particle Physics - Experimental Results'],"['photon nucleus, inclusive reaction', 'beryllium, oxygen', 'charmed meson, photoproduction', 'D0, hadronic decay', 'CP', 'lifetime, difference', 'D0 anti-D0, interference', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> K- pi+', 'D0 --> K+ pi-', '800 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004034'],"['Using a high statistics sample of photoproduced charm particles from the FOCUS experiment at Fermilab, we compare the lifetimes of neutral D mesons decaying via D0 to K- pi+ and K- K+ to measure the lifetime differences between CP even and CP odd final states. These measurements bear on the phenomenology of D0 - D0bar mixing. If the D0 to K-pi+ is an equal mixture of CP even and CP odd eigenstates, we measure yCP = 0.0342 \\pm 0.0139 \\pm 0.0074.']",['2000-05-01']
839,['eng'],"['Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Brabant, P', 'Bull, H', 'Davis, R', 'Holliday, J', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Robertson, I', 'Stutz, R P', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Dambasuren, E', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chan, S', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, T K', 'Richman, J D', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J']",['Measurement of the product branching fraction $B(c \\to \\Theta_{c}X) \\cdot B(\\Theta_{c} \\to \\LambdaX)$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, charm', 'quark, pair production', 'charmed baryon, decay', 'Lambda, final state', 'charmed baryon, branching ratio', 'Lambda/c+', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Lambda/c+ anything', 'Lambda/c+ --> Lambda anything', '10.52-10.58 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004033'],"['Based on an a high statistics e+e- -> ccbar data sample, we report on the inclusive rate for charmed baryons to decay into / particles using charm-event tagging. We select e+e- -> ccbar events which have a clear anti-charm tag and measure the / content in the hemisphere opposite the tag (charge conjugate modes are implicit). This allows us to determine the product branching fraction: B(/)=B(c->Theta_c)*B(Theta_c->/\\X), where Theta_c represents a sum over all charmed baryons produced in e+e- fragmentation at sqrt(s)=10.5 GeV, given our specific tags. We obtain B(/)=(1.87+/-0.03+/-0.33)%']",['2000-05-01']
840,['eng'],"['Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Stepaniak, C J', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Eckhart, E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Mahmood, A H', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Briere, R A', 'Ferguson, T', 'Vogel, H', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A']",['Study of exclusive two-body $B^{0}$ meson decays to charmonium'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'meson, pair production', 'J/psi(3100), leptonic decay', 'chi/c1(3510), radiative decay', 'K0(S), hadronic decay', 'B0, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> J/psi(3100) K0(S)', 'B0 --> chi/c1(3510) K0(S)', 'B0 --> J/psi(3100) pi0', 'K0(S) --> 2pi']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004032'],"['We present a study of three B0 decay modes useful for time-dependent CP asymmetry measurements. From a sample of 9.7 million B meson pairs collected with the CLEO detector, we have reconstructed B0 -> J/psi K0S, B0 -> chi_c1 K0S, and B0 -> J/psi pi0 decays. The latter two decay modes have been observed for the first time. We describe a K0S -> pi0 pi0 detection technique and its application to the reconstruction of the decay B0 -> J/psi K0S. Combining the results obtained using K0S -> pi+ pi- and K0S -> pi0 pi0 decays, we determine Br(B0 -> J/psi K0) = (9.5 +- 0.8 +- 0.6)*10^-4, where the first uncertainty is statistical and the second one is systematic. We also obtain Br(B0 -> chi_c1 K0)= (3.9 +1.9/-1.3 +- 0.4)*10^-4 and Br(B0 -> J/psi pi0) = (2.5 +1.1/-0.9 +- 0.2)*10^-5.']",['2000-04-28']
841,['eng'],"['Albrecht, H', 'Hamacher, T', 'Hofmann, R P', 'Kirchhoff, T', 'Mankel, R', 'Nau, A', 'Nowak, S', 'Ressing, D', 'Schröder, H', 'Schulz, H D', 'Walter, M', 'Wurth, R', 'Hast, C', 'Kapitza, H', 'Kolanoski, H', 'Kosche, A', 'Lange, A', 'Lindner, A', 'Schieber, M', 'Siegmund, T', 'Thurn, H', 'Töpfer, D', 'Wegener, D', 'Frankl, C', 'Graf, J', 'Schmidtler, M', 'Schramm, M', 'Schubert, K R', 'Schwierz, R', 'Spaan, B', 'Waldi, R', 'Reim, K', 'Wegener, H', 'Eckmann, R', 'Kuipers, H', 'Mai, O', 'Mundt, R', 'Oest, T', 'Reiner, R', 'Rohde, A', 'Schmidt-Parzefall, W', 'Stiewe, J', 'Werner, S', 'Ehret, K', 'Hofmann, W', 'Hüpper, A', 'Knöpfle, K T', 'Spengler, J', 'Krieger, P', 'MacFarlane, D B', 'Prentice, J D', 'Saull, P R B', 'Tzamariudaki, K', 'Van de Water, R G', 'Yoon, T S', 'Schneider, M', 'Weseler, S', 'Bracko, M', 'Kernel, G', 'Krizan, P', 'Kriznic, E', 'Medin, G', 'Podobnik, T', 'Zivko, T', 'Balagura, V', 'Barsuk, S', 'Belyaev, I', 'Chistov, R', 'Danilov, M V', 'Eiges, V', 'Gershtein, L I', 'Gershtein, Yu', 'Golutvin, A', 'Igonkina, O', 'Korolko, I', 'Kostina, G', 'Litvintsev, D O', 'Pakhlov, P', 'Semenov, S V', 'Snizhko, A', 'Tichomirov, I', 'Zaitsev, Yu']",['A Search for the Electric Dipole Moment of the $\\tau$-Lepton'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, electric moment', 'form factor, electric', 'invariance, CP', 'tau, semileptonic decay', 'rho(770)', 'tau, leptonic decay', 'magnetic detector, ARGUS', 'experimental results', 'DESY DORIS Stor', 'electron positron --> tau+ tau-', 'tau --> rho(770) neutrino/tau', 'tau --> lepton neutrino/tau neutrino', '10.38 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004031'],"['Using the ARGUS detector at the e+e- storage ring DORIS II, we have searched for the real and imaginary part of the electric dipole formfactor d_tau of the tau lepton in the production of tau pairs at q^2=100 GeV^2. This is the first direct measurement of this CP violating formfactor. We applied the method of optimised observables which takes into account all available information on the observed tau decay products. No evidence for CP violation was found, and we derive the following results: Re(d_tau)=(1.6+-.9)*10^(-16) ecm and Im(d_tau)=(-0.2+-0.8)*10^(-16) ecm, where statistical and systematic errors have been combined.']",['2000-04-28']
842,['eng'],"['Ouchrif, M']","['Energy losses of Q-balls in Matter, Earth and Detectors']",['Particle Physics - Experimental Results'],"['talk, Trieste 1999/09/27', 'Q-ball, interaction', 'matter', 'Q-ball, energy loss', 'deep underground detector, acceptance', 'scintillation counter', 'radiation, yield', 'streamer chamber, drift tube', 'ionization']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004030'],"['We present a sudy of the interactions of Q-balls with matter, and their energy losses in the earth, for a large range of velocities. These calculations are used to computethe fractional geometrical acceptance of underground detectors. Furthermore we computed the light yield in liquidscintillators, the ionization in streamer tubes and the Restricted Energy Loss in nuclear track detectors.']",['2000-04-28']
843,['eng'],"['Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Dambasuren, E', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'Jain, V', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chan, S', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, T K']",['Measurements of Charm Fragmentation into $D_{s}^{*+}$ and $D_{s}^{+}$ in $e^{+}e^{-}$ Annihilations at $\\sqrt{s}$=10.5 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, charm', 'quark, pair production', 'quark, fragmentation', 'D/s*(2110), radiative decay', 'D/s+, hadronic decay', 'yield, (D/s*(2110) D/s+)', 'channel cross section, branching ratio', 'momentum dependence', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.5 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004028'],"['A study of charm fragmentation into $D_s^{*+}$ and $D_s^+$ in $e^+e^-$ annihilations at $\\sqrt{s}$=10.5 GeV is presented. This study using $4.72 \\pm 0.05$ fb$^{-1}$ of CLEO II data reports measurements of the cross-sections $\\sigma(D_s^{*+})$ and $\\sigma(D_s^+)$ in momentum regions above $x=0.44$, where $x$ is the $D_s$ momentum divided by the maximum kinematically allowed $D_s$ momentum. The $D_s$ vector to vector plus pseudoscalar production ratio is measured to be $P_V(x(D_s^+)>0.44)=0.44\\pm0.04$']",['2000-04-26']
844,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Furic, I K', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kirby, M', 'Kirk, M', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mulhearn, M', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Safonov, A', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Measurement of $J/\\psi$ and $\\psi(2S)$ Polarization in $p\\overline{p}$ Collisions at $\\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'psi mesons, direct production', 'J/psi(3100)', 'psi(3685)', 'gluon, fragmentation', 'psi mesons, polarization', 'B, hadroproduction', 'B, hadronic decay', 'psi mesons, leptonic decay', 'angular distribution', 'transverse momentum, dependence', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> psi mesons anything', 'anti-p p --> B anything', 'B --> psi mesons anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004027'],"['We have measured the polarization of J/Psi and Psi(2S) mesons produced in p\\bar{p} collisions at \\sqrt{s} = 1.8 TeV, using data collected at CDF during 1992-95. The polarization of promptly produced J/Psi [Psi(2S)] mesons is isolated from those produced in B-hadron decay, and measured over the kinematic range 4[5.5] < P_T < 20 GeV/c and |y| < 0.6. For P_T \\gessim 12 GeV/c we do not observe significant polarization in the prompt component.']",['2000-04-26']
845,['eng'],"['Alekseev, I G', 'Budkovsky, P E', 'Kanavets, V P', 'Koroleva, L I', 'Morozov, B V', 'Nesterov, V M', 'Ryltzov, V V', 'Svirida, D N', 'Sulimov, A D', 'Zhurkin, V V', 'Beloglazov, Yu A', 'Kovalev, A I', 'Kruglov, S P', 'Novinsky, D V', 'Shchedrov, V A', 'Sumachev, Yu V', 'Trautman, V Yu', 'Bazhanov, N A', 'Bunyatova, E I']",['Measurements of spin rotation parameter A in pion-proton elastic scattering at 1.62 GeV/c'],['Particle Physics - Experimental Results'],"['pi+ p, elastic scattering', 'pi- p, elastic scattering', 'p, polarized target', 'polarization, longitudinal', 'spin, rotator', 'p, polarization', 'polarization, asymmetry', 'partial wave analysis', 'experimental results', 'Moscow ITEF PS', '1.62 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004025'],"['The ITEP-PNPI Collaboration presents the results of the measurements of the spin rotation parameter A in the elastic scattering of positive and negative pions on protons at P/sub beam/=1.62 GeV/c. The setup included a longitudinally-polarized proton target with superconductive magnet, multiwire spark chambers and a carbon polarimeter with thick filter. Results are compared with the predictions of partial wave analyses. The experiment was performed at the ITEP proton synchrotron, Moscow. (13 refs). The ITEP-PNPI collaboration presents the results of the measurements of the spin rotation parameter A in the elastic scattering of positive and negative pions on protons at P_beam = 1.62 GeV/c. The setup included a longitudinally-polarized proton target with superconductive magnet, multiwire spark chambers and a carbon polarimeter with thick filter. Results are compared to the predictions of partial wave analyses. The experiment was performed at the ITEP proton synchrotron, Moscow.']",['2000-04-26']
846,['eng'],"['Suzuki, A', 'Park, H', 'Aoki, S', 'Echigo, S', 'Fujii, K', 'Hara, T', 'Iwashita, T', 'Kitamura, M', 'Kohama, M', 'Kume, G', 'Onchi, M', 'Otaki, T', 'Sato, K', 'Takatsuki, M', 'Takenaka, K', 'Tanaka, Y', 'Tashiro, K', 'Inagaki, T', 'Kato, I', 'Mukai, S', 'Nakaya, T', 'Nishikawa, K', 'Sasao, N', 'Shima, A', 'Yokoyama, H', 'Chikamatsu, T', 'Hayato, Y', 'Ishida, T', 'Ishii, T', 'Ishino, H', 'Jeon, E J', 'Kobayashi, T', 'Lee, S B', 'Nakamura, K', 'Oyama, Y', 'Sakai, A', 'Sakuda, M', 'Tumakov, V', 'Fukuda, S', 'Fukuda, Y', 'Ishizuka, M', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kaneyuki, K', 'Kobayashi, K', 'Kobayashi, Y', 'Koshio, Y', 'Miura, M', 'Moriyama, S', 'Nakahata, M', 'Nakayama, S', 'Obayashi, Y', 'Okada, A', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, H', 'Takeuchi, Y', 'Totsuka, Y', 'Toshito, T', 'Yamada, S', 'Miyano, K', 'Nakamura, M', 'Tamura, N', 'Nakano, I', 'Yoshida, M', 'Kadowaki, T', 'Kishi, S', 'Yokoyama, H', 'Maruyama, T', 'Etoh, M', 'Nishijima, K', 'Bhang, H C', 'Khang, B H', 'Kim, B J', 'Kim, H I', 'Kim, J H', 'Kim, S B', 'So, H', 'Yoo, J H', 'Choi, J H', 'Jang, H I', 'Jang, J S', 'Kim, J Y', 'Lim, I T', 'Pac, M Y', 'Kearns, E T', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Casper, David William', 'Gajewski, W', 'Kropp, W R', 'Mine, S', 'Sobel, H', 'Vagins, M R', 'Matsuno, S', 'Hill, J', 'Jung, C K', 'Martens, K', 'Mauger, C', 'McGrew, C', 'Sharkey, E', 'Yanagisawa, C', 'Berns, H', 'Boyd, S', 'Wilkes, J', 'Kielczewska, D', 'Golebiewska, U']","['Design, construction, and operation of SciFi tracking detector for K2K experiment']",['Particle Physics - Experimental Results'],"['talk, Hamamatsu 1999/11/15', 'neutrino, oscillation', 'scintillation counter, fibre', 'radiation, yield', 'semiconductor, optical', 'efficiency', 'spatial resolution', 'particle identification', 'deep underground detector, KAMIOKANDE', 'KEK PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004024'],"['We describe the construction and performance of a scintillating fiber detector used in the near detector for the K2K (KEK to Kamioka, KEK E362) long baseline neutrino oscillation experiment. The detector uses 3.7 m long and 0.692 mm diameter scintillating fiber coupled to image-intensifier tubes (IIT), and a CCD camera readout system. Fiber sheet production and detector construction began in 1997, and the detector was commissioned in March, 1999. Results from the first K2K runs confirm good initial performance : position resolution is estimated to be about 0.8 mm, and track finding efficiency is $98 \\pm 2$ % for long tracks (i.e., those which intersect more than 5 fiber planes). The hit efficiency was estimated to be $92 \\pm 2$ % using cosmic-ray muons, after noise reduction at the offline stage. The possibility of using the detector for particle identification is also discussed.']",['2000-04-26']
847,['eng'],"['Towers, S']",['Charged Higgs Mass Limits from the $\\tau^{-} \\to \\nu_{\\tau}K^{-}$ and $K^{-} \\to \\overline {\\nu}_{l}l^{-}(\\gamma)$ Branching Fractions'],['Particle Physics - Experimental Results'],"['tau-, semileptonic decay', 'K-, leptonic decay', 'K-, radiative decay', 'tau-, branching ratio', 'K-, branching ratio', 'Higgs particle, charged particle', 'Higgs particle, mass', 'Higgs particle, multiplet', 'doublet, 2', 'supersymmetry', 'numerical calculations, interpretation of experiments', 'K- --> lepton- antineutrino', 'K- --> lepton- antineutrino photon', 'tau- --> K- neutrino/tau']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004022'],"['From an analysis of the current world averages of the charged kaon and tau to kaon branching fractions, we derive, within the framework of type II Higgs doublets models such as the Minimal Supersymmetric Extension of the Standard Model, $\\tan{\\beta}/m_H < 0.21$ GeV$^{-1}$ at a 90% confidence limit.']",['2000-04-25']
848,['eng'],"['Abe, K', 'Abe, K', 'Abe, T', 'Adam, I', 'Akimoto, H', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Berger, R', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Cassell, R', 'Chou, A', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Crawford, G', 'Damerell, C J S', 'Daoudi, M', 'Dasu, S', 'De Groot, N', 'De Sangro, R', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Erofeeva, I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fernández, J P', 'Flood, K', 'Frey, R', 'Hart, E L', 'Hasuko, K', 'Hertzbach, S S', 'Huffer, M E', 'Huynh, X', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Kajikawa, R', 'Kang, H J', 'Kalelkar, M S', 'Kofler, R R', 'Kroeger, R S', 'Langston, M', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'McKemey, A K', 'Messner, R', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Narita, S', 'Nauenberg, U', 'Nesom, G', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Ratcliff, B N', 'Reidy, J', 'Reinertsen, P L', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schumm, B A', 'Schwiening, J', 'Serbo, V V', 'Shapiro, G', 'Sinev, N B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Swartz, M', 'Taylor, F E', 'Thom, J', 'Usher, T', 'Vavra, J', 'Verdier, R', 'Wagner, D L', 'Waite, A P', 'Walston, S', 'Wang, J', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Wright, T R', 'Yamamoto, R K', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H']",['A High-Precision Measurement of the Left-Right Z Boson Cross-Section Asymmetry'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'polarization, longitudinal', 'Z0, electroproduction', 'Z0, decay', 'polarization, asymmetry', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.23 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004026'],"['We present a measurement of the left-right cross-section asymmetry (ALR) for Z boson production by e+e- collisions. The measurement includes the final data taken with the SLD detector at the SLAC Linear Collider (SLC) during the period 1996-1998. Using a sample of 383,487 Z decays collected during the 1996-1998 runs we measure the pole-value of the asymmetry, ALR0, to be 0.15056+-0.00239 which is equivalent to an effective weak mixing angle of sin2th(eff) = 0.23107+-0.00030. Our result for the complete 1992-1998 dataset comprising 537 thousand Z decays is sin2th(eff) = 0.23097+-0.00027.']",['2000-04-26']
849,['eng'],"['Bethke, Siegfried']",['Determination of the QCD Coupling $\\alpha_{s}$'],['Particle Physics - Experimental Results'],"['review, experimental results', 'strong interaction, coupling constant', 'energy dependence', 'quantum chromodynamics, perturbation theory', 'renormalization, dependence', 'color, 3', 'asymptotic freedom', 'confinement', 'Lambda parameter', 'quark, mass', 'lattice field theory', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004021'],"['Theoretical basics and experimental determinations of the coupling parameter of the Strong Interaction, $\\alpha_s$, are reviewed. The world average value of $\\alpha_s$, expressed at the energy scale of the rest mass of the $Z^0$ boson, is determined from analyses which are based on complete NNLO perturbative QCD. The result is $\\alpha_s (M_Z) = 0.1184 \\pm 0.0031$. No significant deviations or systematic biases of subsamples of experimental results are found. From the observed energy dependence of $\\alpha_s$, which is in excellent agreement with the expectations of QCD, the number of colour degrees of freedom can be constrained to $N_c = 3.03 \\pm 0.12$.']",['2000-04-21']
850,['eng'],"['Cline, David B', 'Fukui, Y', 'Garren, A A']",['A Neutrino-Factory Muon Storage Ring to Provide Beams for Multiple Detectors Around the World'],['Accelerators and Storage Rings'],"['talk, San Francisco 1999/12/15', 'neutrino, particle source', 'muon, storage ring', 'storage ring, lattice', 'neutrino, oscillation', 'deep underground detector, Gran Sasso']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004020'],"['We briefly discuss the physics motivation for a neutrino factory with varying baseline distances of about 1000 to 9000 km. We describe the amount of non planarity of the storage ring required to service three or four detectors at once. A novel bowtie storage ring is described that could in part provide these beams; a preliminary lattice design is given. We give the space angles between the various detector locations and possible sites for neutrino factories. Finally we describe detectors at the Gran Sasso Laboratory and at a new laboratory near Carlsbad, NM to observe the neutrino interactions with wrong sign leptons.']",['2000-04-19']
851,['eng'],"['Bakari, D']","['Magnetic monopoles, nuclearites, Q-balls']",['Particle Physics - Experimental Results'],"['magnetic monopole', 'matter, strangeness', 'quark, matter', 'Q-ball', 'matter, mass', 'astrophysics, missing-mass', 'cosmic radiation, flux', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004019'],"['We present qualitative pictures of the structures of magnetic monopoles (MMs), nuclearites (nuggets of strange quark matter, strangelets, surrounded by electrons) and Q-balls (supersymmetric states of squarks, sleptons and Higgs fields). In particular we discuss the relation between their mass and size. MMs, nuclearites and Q-balls could be part of the cold Dark Matter (DM); we consider astrophysical limits on the flux of these particles in the cosmic radiation.']",['2000-04-19']
852,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A search for charmonium states produced in central pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, exclusive reaction', 'exchange, (2pomeron)', 'quarkonium, charm', 'quarkonium, search for', 'quarkonium, hadronic decay', 'quarkonium, radiative decay', 'eta/c(2980)', 'chi/c1(3510)', 'chi/c2(3555)', 'J/psi(3100), leptonic decay', 'mass spectrum, (positron electron)', 'mass spectrum, two-photon', 'mass spectrum, (eta pi+ pi-)', 'mass spectrum, (K0(S) K pi)', 'calorimeter, GAMS', 'experimental results', 'CERN SPS', 'p p --> quarkonium 2p', 'chi mesons --> J/psi(3100) photon', 'eta/c(2980) --> eta pi+ pi-', 'eta/c(2980) --> K0(S) K pi', '450 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0006005'],['A search for centrally produced charmonium states has been presented. There is no significant evidence for any charmonium production. An upper limit of 2 nb is found for the cross section of chic production using the decay chic(1P)-> J/psi gamma.'],['2000-06-07']
853,['eng'],"['Cline, David B']",['The Scientific Need for a Scalar/Higgs Factory'],['Detectors and Experimental Techniques'],"['talk, San Francisco 1999/12/15', 'muon+ muon-, colliding beams', 'Higgs particle, particle source', 'electron positron, annihilation', 'Higgs particle, electroproduction', 'channel cross section, energy dependence', 'electroweak interaction, symmetry breaking', 'neutrino, particle source', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004018'],"['The scalar sector of the electroweak theory can be probed by a mu^+mu^- collider S channel resonance machine. We give arguments for when such a machine may be needed and when this information could be obtained by the LHC detector. A very interesting case is the possibility that several scalar particles are in the same mass range for the supersymmetric Higgs bosons h, H, and A, which would definitely require such a machine. The Higgs factory could follow the construction of a neutrino factory.']",['2000-04-18']
854,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Frisch, H', 'Fukui, Y', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kirby, M', 'Kirk, M', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Safonov, A', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Direct Measurement of the W Boson Width in $\\overline{p}p$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'W, width', 'mass spectrum, transverse', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'W --> electron neutrino/e', 'W --> muon neutrino/mu', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004017'],"['This Letter describes a direct measurement of the $W$ boson total decay width, $\\gw$, using the Collider Detector at Fermilab. The measurement uses an integrated luminosity of $90\\invpb$, collected during the 1994--1995 run of the Fermilab Tevatron $p\\pbar$ collider. The width is determined by normalizing predicted signal and background distributions to 49844 $\\wenu$ candidates and 21806 $\\wmunu$ candidates in the transverse-mass region $M_T<200\\gev$ and then fitting the predicted shape to the 438 electron events and 196 muon events in the high-$M_T$ region, $100<M_T<200\\gev$. The result is $\\Gamma_W=2.04\\pm0.11$(stat)$\\pm0.09$(syst)GeV.']",['2000-04-18']
855,['eng'],"['Yavas, O', 'Çiftçi, A K', 'Sultansoy, S F']","['Linac*LHC based ep, $\\gamma-p$, eA, $\\gamma-A$ and FEL $\\gamma-A$ Colliders']",['Detectors and Experimental Techniques'],"['talk, Vienna 2000/06/26', 'electron p, linac-ring collider', 'electron nucleus, linac-ring collider', 'photon p, colliding beams', 'photon nucleus, colliding beams', 'free electron laser', 'luminosity', 'CERN LHC Coll', 'CERN Lab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004016'],"['Main parameters of different colliders which can be realized if a special 1 TeV energy linear electron accelerator or corresponding linear collider is constructed tangential to LHC are estimated. It is shown that L_ep=10^32cm^-2s^-1 at sqrt(s_ep)=5.29 TeV can be achieved within moderate upgrade of LHC parameters. Then, gamma-p collider with the same luminosity and sqrt(s)=4.82 TeV can be realized using Compton backscattering of laser beam off the electron beam. Concerning the nucleus beam, L*A=10^31cm^-2s^-1 can be achieved at least for light and medium nuclei both for eA and gamma-A options. Finally, colliding of the FEL beam from an electron linac with nucleus beams from LHC will give a new opportunity to investigate nuclear spectroscopy and photo-nuclei reactions.']",['2000-04-14']
856,['eng'],"['Oyama, Y']",['Current status of K2K long-baseline neutrino-oscillation experiment'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 2000/03/11', 'neutrino, oscillation', 'neutrino/mu, beam', 'neutrino/mu, energy spectrum', 'ratio, (neutrino/mu neutrino/e)', 'deep underground detector, KAMIOKANDE', 'experimental results', 'KEK PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004015'],"['The K2K (KEK to Kamioka) long-baseline neutrino-oscillation experiment was successfully started in early 1999. A total intensity of 7.20 x 10^18 protons on target, which is about 7% of the goal of the experiment, was accumulated in 39.4 days of data-taking in 1999. We obtained 3 neutrino events in the fiducial volume of the Super-Kamiokande detector, whereas the expectation based on observations in the front detectors is 12.3 +1.7/-1.9. An analysis of oscillation searches from the view points of absolute event numbers, distortion of neutrino energy spectrum, and nu_e/nu_mu ratio is in progress.']",['2000-04-13']
857,['eng'],[],['Measurement of the flux of atmospheric muons with the CAPRICE94 apparatus'],['Particle Physics - Experimental Results'],"['muon+, cosmic radiation', 'muon-, cosmic radiation', 'cosmic radiation, flux', 'cosmic radiation, momentum spectrum', 'spatial distribution', 'magnetic spectrometer, satellite', 'drift chamber', 'Cherenkov counter, ring imaging', 'scintillation counter', 'calorimeter', 'efficiency', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004014'],"['A new measurement of the momentum spectra of both positive and negative muons as function of atmospheric depth was made by the balloon-borne experiment CAPRICE94. The data were collected during ground runs in Lynn Lake on the 19-20th of July 1994 and during the balloon flight on the 8-9th of August 1994. We present results that cover the momentum intervals 0.3-40 GeV/c for negative muons and 0.3-2 GeV/c for positive muons, for atmospheric depths from 3.3 to 1000 g/cm**2, respectively. Good agreement is found with previous measurements for high momenta, while at momenta below 1 GeV/c we find latitude dependent geomagnetic effects. These measurements are important cross-checks for the simulations carried out to calculate the atmospheric neutrino fluxes and to understand the observed atmospheric neutrino anomaly.']",['2000-04-12']
858,['eng'],"['Yavas, O', 'Çiftçi, A K', 'Sultansoy, S F']",['TESLA*HERA as Lepton (Photon)-Hadron Collider'],['Detectors and Experimental Techniques'],"['talk, Vienna 2000/06/26', 'electron p, linac-ring collider', 'electron nucleus, linac-ring collider', 'photon p, colliding beams', 'photon nucleus, colliding beams', 'luminosity', 'free electron laser', 'DESY HERA Stor', 'DESY TESLA Linac']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004013'],"['New facilities for particle and nuclear physics research, which will be available due to constructing the TESLA linear electron-positron collider tangentially to the HERA proton ring, are discussed.']",['2000-04-12']
859,['eng'],"['Apanasevich, L', 'Bacigalupi, J', 'Baker, W', 'Begel, M', 'Blusk, S R', 'Bromberg, C', 'Chang, P', 'Choudhary, B C', 'Chung, W H', 'De Barbaro, L', 'De Soi, W', 'Dlugosz, W', 'Dunlea, J', 'Engels, E', 'Fanourakis, G K', 'Ferbel, T', 'Ftácnik, J', 'Garelick, D', 'Ginther, G', 'Glaubman, M', 'Gutíerrez, P', 'Hartman, K', 'Huston, J', 'Johnstone, C', 'Kapoor, V S', 'Kuehler, J', 'Lirakis, C', 'Lobkowicz, F', 'Lukens, P', 'Mani, S', 'Mansour, J', 'Maul, A', 'Miller, R', 'Oh, B Y', 'Osborne, G', 'Pellett, D E', 'Prebys, E J', 'Roser, R M', 'Shepard, P', 'Shivpuri, R K', 'Skow, D', 'Slattery, P', 'Sorrell, L', 'Striley, D', 'Toothacker, W S', 'Varelas, N', 'Weerasundara, D', 'Whitmore, J J', 'Yasuda, T', 'Yosef, C', 'Zielinski, M', 'Zutshi, V']",['Inclusive production of $\\omega$ mesons at large transverse momenta in $\\pi-Be$ interactions at 515 GeV/c'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'beryllium', 'omega(783), hadroproduction', 'omega(783), radiative decay', 'transverse momentum, high', 'yield, (omega(783) pi0)', 'yield, (vector meson pseudoscalar meson)', 'mass spectrum, (pi0 photon)', 'differential cross section, transverse momentum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '515 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004012'],['We present results on the production of omega mesons at high transverse momenta in pi^-Be interactions at 515 GeV/c. The data span the kinematic range 3.5 < p_T < 8 GeV/c. We compare the measured cross section with expectations from Monte Carlo QCD generators. The relative yield of omega to pi^0 mesons is used to extract the ratio of vector to pseudoscalar meson production for the first generation of quarks.'],['2000-04-11']
860,['eng'],"['Zech, G']",['Confronting classical and Bayesian confidence limits to examples'],['Detectors and Experimental Techniques'],"['talk, Geneva 2000/01/17', 'statistical analysis', 'track data analysis', 'neutrino, flavor', 'lifetime, measurement']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004011'],"['Classical confidence limits are compared to Bayesian error bounds by studying relevant examples. The performance of the two methods is investigated relative to the properties coherence, precision, bias, universality, simplicity. A proposal to define error limits in various cases is derived from the comparison. It is based on the likelihood function only and follows in most cases the general practice in high energy physics. Classical methods are discarded because they violate the likelihood principle, they can produce physically inconsistent results, suffer from a lack of precision and generality. Also the extreme Bayesian approach with arbitrary choice of the prior probability density or priors deduced from scaling laws is rejected.']",['2000-04-11']
861,['eng'],"['Coutu, S', 'Beatty, J J', 'Duvernois, M A', 'Barwick, S W', 'Schneider, E', 'Bhattacharya, A', 'Bower, C', 'Musser, J A', 'Labrador, A W', 'Müller, D', 'Swordy, S P', 'Torbet, E', 'Chaput, C', 'McKee, S', 'Tarle, G', 'Tomasch, A D', 'Nutter, S L', 'De Nolfo, G A']","['Energy Spectra, Altitude Profiles and Charge Ratios of Atmospheric Muons']",['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'showers, air', 'cosmic radiation, flux', 'muon+ muon-, ratio', 'muon-, momentum spectrum', 'spatial distribution', 'neutrino, cosmic radiation', 'counters and detectors, satellite', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004010'],"['We present a new measurement of air shower muons made during atmospheric ascent of the High Energy Antimatter Telescope balloon experiment. The muon charge ratio mu+ / mu- is presented as a function of atmospheric depth in the momentum interval 0.3-0.9 GeV/c. The differential mu- momentum spectra are presented between 0.3 and about 50 GeV/c at atmospheric depths between 13 and 960 g/cm^2. We compare our measurements with other recent data and with Monte Carlo calculations of the same type as those used in predicting atmospheric neutrino fluxes. We find that our measured mu- fluxes are smaller than the predictions by as much as 70% at shallow atmospheric depths, by about 20% at the depth of shower maximum, and are in good agreement with the predictions at greater depths. We explore the consequences of this on the question of atmospheric neutrino production.']",['2000-04-10']
862,['eng'],"['Kulchitskii, Yu A']",['Hadron Energy Reconstruction for the ATLAS Barrel Prototype Combined Calorimeter in the Framework of the Non-parametrical Method'],['Detectors and Experimental Techniques'],"['calorimeter, liquid argon', 'lead', 'iron', 'scintillation counter', 'energy resolution', 'showers, hadronic', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004009'],"['Hadron energy reconstruction for the Atlas barrel prototype combined calorimeter, consisting of the lead-liquid argon electromagnetic part and the iron-scintillator hadronic part, in the framework of the non-parametrical method has been fulfilled. This method uses only the known e/h ratios and the electron calibration constants and does not require the determination of any parameters by a minimization technique and can be used for the fast energy reconstruction in the first level trigger. The obtained reconstruction of the mean values of energies is within $\\pm 1%$ and the fractional energy resolution is $[(58\\pm3)% \\sqrt{GeV}/\\sqrt{E}+(2.5\\pm0.3)%]\\oplus (1.7\\pm0.2) GeV/E$. The obtained value of the e/h ratio for electromagnetic compartment of the combined calorimeter is $1.74\\pm0.04$ and agrees with the prediction that $e/h > 1.7$ for this electromagnetic calorimeter. The results of the study of the longitudinal hadronic shower development are presented. The data have been taken in the H8 beam line of the CERN SPS using pions of 10 -- 300 GeV.']",['2000-04-07']
863,['eng'],"['Kowalewski, R V', 'Jackson, P D']",['Track Fit Hypothesis Testing and Kink Selection using Sequential Correlations'],['Detectors and Experimental Techniques'],"['track data analysis', 'statistical analysis', 'tracks, parametrization']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004008'],['Deviations between the form of trajectory assumed in a fit to a set of measurements and the actual form of the trajectory can give rise to sequential correlations in the residuals from the fit. These correlations can provide a more powerful goodness-of-fit test than that based on the minimum chi-square from a least squares fit. The use of this additional information is explored in the context of several common trajectory errors (e.g. decays in flight) encountered in charged particle tracking.'],['2000-04-07']
864,['eng'],"['Gorham, P W', 'Saltzberg, D', 'Schoessow, P', 'Gai, W', 'Power, J G', 'Konecny, R', 'Conde, M E']",['Radio-Frequency Measurements of Coherent Transition and Cerenkov Radiation'],['Particle Physics - Experimental Results'],"['accelerator, wake field', 'electron, beam', 'bunching', 'aluminum', 'silicon', 'microwaves, emission', 'transition radiation', 'radiation, Cherenkov', 'radiation, coherence', 'polarization, dependence', 'showers, electromagnetic', 'charge, asymmetry', 'neutrino, particle identification', 'experimental results', 'Argonne Lab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004007'],"['We report on measurements of 11-18 cm wavelength radio emission from interactions of 15.2 MeV pulsed electron bunches at the Argonne Wakefield Accelerator. The electrons were observed both in a configuration where they produced primarily transition radiation from an aluminum foil, and in a configuration designed for the electrons to produce Cherenkov radiation in a silica sand target. Our aim was to emulate the large electron excess expected to develop during an electromagnetic cascade initiated by an ultra high-energy particle. Such charge asymmetries are predicted to produce strong coherent radio pulses, which are the basis for several experiments to detect high-energy neutrinos from the showers they induce in Antarctic ice and in the lunar regolith. We detected coherent emission which we attribute both to transition and possibly Cherenkov radiation at different levels depending on the experimental conditions. We discuss implications for experiments relying on radio emission for detection of electromagnetic cascades produced by ultra high-energy neutrinos.']",['2000-04-06']
865,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Calafiura, P', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haas, R M', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kilminster, B', 'Kirby, M', 'Kirk, M', 'Kim, B J', 'Kim, D H', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Lee, K', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Orejudos, W', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Pukhov, O', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Yu, Z', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Search for Second and Third Generation Leptoquarks Including Production via Technicolor Interactions in $p\\overline{p}$ collisions at $\\sqrt{s}$=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'new particle, search for', 'meson, technicolor', 'leptoquark, pair production', 'leptoquark, scalar', 'leptoquark, vector', 'technipion', 'technirho', 'leptoquark, decay', 'final state, (quark neutrino)', 'final state, ((n)jet missing-energy)', 'channel cross section, mass', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004003'],"['We report the results of a search for second and third generation leptoquarks using 88 ${pb}^{-1}$ of data recorded by the Collider Detector at Fermilab. Color triplet technipions, which play the role of scalar leptoquarks, are investigated due to their potential production in decays of strongly coupled color octet technirhos. Events with a signature of two heavy flavor jets and missing energy may indicate the decay of a second (third) generation leptoquark to a charm (bottom) quark and a neutrino. As the data is found to be consistent with Standard Model expectations, mass limits are determined.']",['2000-04-04']
866,['eng'],"['Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Perera, L P', 'Zhou, G J', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V']",['Resonance structure of $\\tau^{-}\\to K^{-}\\pi^{+}\\pi^{-}\\nu_{\\tau}$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'mass spectrum, (K- pi+ pi-)', 'meson resonance, production', 'K1(1270)', 'K1(1400)', 'meson resonance, mass', 'meson resonance, width', 'tau-, branching ratio', 'form factor, parametrization', 'decay, amplitude analysis', 'mixing angle', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> K- pi+ pi- neutrino/tau', 'approx. 10.58 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004002'],"['Using a sample of 4.7/fb integrated luminosity accumulated with the CLEO II detector at the Cornell Electron Storage Ring (CESR), we investigate the mass spectrum and resonant structure in tau->Kpipi decays. We measure the relative fractions of K1(1270) and K1(1400) resonances in these decays, as well as the K1 masses and widths. Our fitted K1 resonances are somewhat broader than previous hadroproduction measurements, and in agreement with recent LEP results from tau decay. The larger central value of our measured width supports models which attribute the small tau->Kpipi branching fraction to larger K1 widths than are presently tabulated. We also determine the Ka-Kb mixing angle theta_K.']",['2000-04-04']
867,['eng'],"['Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Brabant, P', 'Cervantes, M', 'Kravchenko, I V', 'Stutz, R P', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Pedlar, T K', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Perera, L P', 'Zhou, G J', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F']",['Measurement of $\\beta(\\Lambda^{+}_{c} \\to pK^{-}\\pi^{+})$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, inclusive reaction', 'Lambda/c+, electroproduction', 'anti-p, associated production', 'anti-D, associated production', 'correlation', 'Lambda/c+, hadronic decay', 'mass spectrum, (p K- pi+)', 'Lambda/c+, branching ratio', 'background', 'particle identification', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Lambda/c+ anti-D anti-p anything', 'Lambda/c+ --> p K- pi+', '10.55 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004001'],"['The /\\c->pKpi yield has been measured in a sample of two-jet continuum events containing a both an anticharm tag (Dbar) as well as an antiproton (e+e- -> Dbar pbar X), with the antiproton in the hemisphere opposite the Dbar. Under the hypothesis that such selection criteria tag e+e- -> Dbar pbar (/\\c) X events, the /\\c->pkpi branching fraction can be determined by measuring the pkpi yield in the same hemisphere as the antiprotons in our Dbar pbar X sample. Combining our results from three independent types of anticharm tags, we obtain B(/\\c->pKpi)=(5.0+/-0.5+/-1.2)%']",['2000-04-04']
868,['eng'],"['Woods, M']",['Polarimetry at a Future Linear Collider'],['Detectors and Experimental Techniques'],"['talk, Santa Cruz 1999/12/10', 'linear collider, proposed', 'electron positron, colliding beams', 'electron electron, colliding beams', 'electron, polarized beam', 'polarization, measurement', 'Compton scattering', 'W, pair production', 'channel cross section, asymmetry', 'polarization, dependence', 'Feynman graph', 'effect, beam-beam', 'numerical calculations', '500 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0004004'],"['At a future linear collider, a polarized electron beam will play an important role in interpreting new physics signals. Backgrounds to a new physics reaction can be reduced by choice of the electron polarization state. The origin of a new physics reaction can be clarified by measuring its polarization-dependence. This paper examines some options for polarimetry with an emphasis on physics issues that motivate how precise the polarization determination needs to be. In addition to Compton polarimetry, the possibility of using Standard Model asymmetries, such as the asymmetry in forward W-pairs, is considered as a possible polarimeter. Both e+e- and e-e- collider modes are considered.']",['2000-04-04']
869,['eng'],"['De Jager, K']",['Nucleon Electromagnetic Form Factors'],['Particle Physics - Experimental Results'],"['talk, Cambridge 1999/11/03', 'n, form factor', 'p, form factor', 'form factor, magnetic', 'form factor, electric', 'dependence, momentum transfer', 'electron nucleon, elastic scattering', 'electron nucleus, inelastic scattering', 'deuterium', 'helium, nuclide', 'electron, polarized beam', 'nucleon, polarized target', 'experimental results', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003034'],['A review of data on the nucleon electromagnetic form factors in the space-like region is presented. Recent results from experiments using polarized beams and polarized targets or nucleon recoil polarimeters have yielded a significant improvement on the precision of the data obtained with the traditional Rosenbluth separation. Future plans for extended measurements are outlined.'],['2000-03-31']
870,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the $\\eta\\eta$ channel produced in central pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, exclusive reaction', 'eta, hadroproduction', 'mass spectrum, (2eta)', 'central region', 'mass spectrum, (2photon)', 'mass spectrum, (pi+ pi- pi0)', 'partial wave analysis', 'meson resonance, hadroproduction', 'f0(1500)', 'f0(1710)', 'f2(2150)', 'meson resonance, mass', 'meson resonance, width', 'meson resonance, hadronic decay', 'meson resonance, branching ratio', 'experimental results', 'magnetic detector, OMEGA', 'CERN SPS', 'p p --> 2p 2eta', 'eta --> 2photon', 'eta --> pi+ pi- pi0', '450 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003033'],"['The reaction pp -> pf (eta eta) ps has been studied at 450 GeV/c. For the first time a partial wave analysis of the centrally produced eta eta system has been performed. Signals for the f0(1500), f0(1710) and f2(2150) are observed and the decay branching fractions of these states are determined.']",['2000-03-31']
871,['eng'],"['Abramov, V V', 'Acharya, B S', 'Akchurin, N', 'Atanasov, I H', 'Baiatian, G', 'Ball, A', 'Banerjee, S', 'De Barbaro, P', 'Barnes, Virgil E', 'Bencze, G L', 'Bodek, Arie', 'Booke, M', 'Budd, H S', 'Cremaldi, L', 'Cushman, P B', 'Dugad, S R', 'Dimitrov, L', 'Dyshkant, A', 'Elias, J', 'Evdokimov, V N', 'Fong, D', 'Freeman, J', 'Genchev, V', 'Goncharov, P I', 'Green, D', 'Gurtu, A', 'Hagopian, V', 'Iaydjiev, P', 'Korneev, Yu P', 'Krinitsyn, A N', 'Krishnaswami, G S', 'Krishnaswamy, M R', 'Kryshkin, V I', 'Kunori, S']","['Studies of the Response of the Prototype CMS Hadron Calorimeter, Including Magnetic Field Effects, to Pion, Electron, and Muon Beams']",['Detectors and Experimental Techniques'],"['calorimeter, hadronic', 'copper', 'scintillation counter, plastics', 'optics, readout', 'optics, fibre', 'optics, transformation', 'energy resolution', 'magnetic field', 'magnetic detector, CMS', 'CERN LHC Coll', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007045'],"['We report on the response of a prototype CMS hadron calorimeter module to charged particle beams of pions, muons, and electrons with momenta up to 375 GeV/c. The data were taken at the H2 and H4 beamlines at CERN in 1995 and 1996. The prototype sampling calorimeter used copper absorber plates and scintillator tiles with wavelength shifting fibers for readout. The effects of a magnetic field of up to 3 Tesla on the response of the calorimeter to muons, electrons, and pions are presented, and the effects of an upstream lead tungstate crystal electromagnetic calorimeter on the linearity and energy resolution of the combined calorimetric system to hadrons are evaluated. The results are compared with Monte Carlo simulations and are used to optimize the choice of total absorber depth, sampling frequency, and longitudinal readout segmentation.']",['2000-07-24']
872,['eng'],"['Gorfine, G W', 'Hoeferkamp, M', 'Santistevan, G', 'Seidel, S']",['Capacitance of Silicon Pixels'],['Detectors and Experimental Techniques'],"['tracks', 'semiconductor detector, pixel', 'radiation, damage', 'magnetic detector, ATLAS', 'CERN LHC Coll', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003032'],"['Capacitance measurements have been made on silicon pixel sensors of types n+ on n, p+ on n, and n+ on p. The arrays test a variety of implant and gap widths, and the n+ on n devices test several p-stop designs. The measurements examine inter-pixel and backplane contributions and include studies of temperature dependence. Measurements were made before and after irradiation with fluences relevant to LHC experiments and Fermilab Tevatron Run 2.']",['2000-03-29']
873,['eng'],"['Achasov, M N', 'Baru, S E', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Mamutkin, A A', 'Pakhtusova, E V', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N']",['The $\\phi \\to \\eta\\pi^{0}\\gamma$ decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), rare decay', 'Phi(1020), branching ratio', 'eta, radiative decay', 'pi0, radiative decay', 'final state, (5photon)', 'a0(980), mass', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> eta pi0 photon', 'Phi(1020) --> a0(980) photon', 'approx. 1.02 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003031'],['Rare radiative decay $\\phi\\to\\eta\\pi^0\\gamma$ was studied with SND detector at {VEPP-2M} electron-positron collider and its branching ratio was measured: $B(\\phi\\to\\eta\\pi^0\\gamma)=(0.88\\pm0.14\\pm0.09)\\cdot 10^{-4}$. Significant contribution of the $a_0(980)\\gamma$ intermediate state was observed in the decay. The result is based on total integrated luminosity corresponding to $2\\cdot10^7$ produced $\\phi$ mesons.'],['2000-03-28']
874,['eng'],"['Saull, P R B']",['Prompt Photon Production and Observation of Deeply Virtual Compton Scattering'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon, direct production', 'photon, photoproduction', 'differential cross section, rapidity dependence', 'transverse energy, dependence', 'Compton scattering', 'angular distribution', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003030'],"['Two recent results in ep physics using the ZEUS detector at HERA are discussed: a measurement of the prompt photon production cross section in photoproduction, and the first observation of Deeply Virtual Compton Scattering in DIS.']",['2000-03-28']
875,['eng'],"['Buschbeck, Brigitte', 'Eggers, H C', 'Lipa, P']",['Multiplicity dependence of correlation functions in $\\overline{p}p$ reactions at sqrt(s) = 630 GeV'],['Particle Physics - Experimental Results'],"['anti-p p, inelastic scattering', 'charged particle, multiple production', 'boson, statistics', 'correlation function, two-particle', 'charge', 'multiplicity, dependence', 'cumulant expansion', 'resonance, decay', 'string model', 'statistical mechanics', 'numerical calculations', 'interpretation of experiments, UA1', '630 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003029'],['Discussions about Bose-Einstein correlations between decay products of coproduced W-bosons again raise the question about the behaviour of correlations if several strings are produced. This is studied by the multiplicity dependence of correlation functions of particle pairs with like-sign and opposite-sign charge in \\bar{p}p reactions at sqrt{s} = 630 GeV.'],['2000-03-28']
876,['eng'],"['Bakari, D', 'Cecchini, S', 'Dekhissi, H', 'Derkaoui, J E', 'Giacomelli, Giorgio', 'Giorgini, M', 'McDonald, J', 'Mandrioli, G', 'Manzoor, S', 'Margiotta, A', 'Marzari-Chiesa, A', 'Nogales, J A C', 'Ouchrif, M', 'Patrizii, L', 'Pinfold, James L', 'Popa, V', 'Saavedra, O', 'Serra, P', 'Spurio, M', 'Ticona, R', 'Togo, V', 'Velarde, A', 'Vilela, E', 'Zanini, A']","['Search for ""light"" magnetic monopoles']",['Particle Physics - Experimental Results'],"['cosmic radiation', 'new particle, search for', 'magnetic monopole', 'dyon', 'nuclear matter, strangeness', 'Q-ball', 'bound state, (magnetic monopole p)', 'plastics, track sensitive', 'proposed experiment']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003028'],"['We propose to implement one passive nuclear track detector array of 400 m^2 at the Chacaltaya High Altitude Laboratory (5230 m a.s.l.). The main purposes of the experiment concern the searches for magnetic monopoles of relatively low masses at the Parker bound level, searches for low mass nuclearites and searches for some supersymmetric dark matter candidates (Q-balls).']",['2000-03-27']
877,['eng'],"['Thorndike, E H']",['Bottom Quark Physics'],['Particle Physics - Experimental Results'],"['review, Rochester 1999/09/24', 'particle physics, history', 'quark, beauty', 'p nucleus, inclusive reaction', 'mass spectrum, dimuon', 'electron positron, annihilation', 'cross section, hadronic', 'energy dependence', 'upsilon mesons, electroproduction', 'Upsilon(10570), hadronic decay', 'B, pair production', 'B, decay modes', 'B, branching ratio', 'B, lifetime', 'B0 anti-B0, interference', 'family, 3', 'Kobayashi-Maskawa angle, unitarity', 'violation, CP', 'B, rare decay', 'quark, radiative decay', 'Feynman graph, penguin', 'electroweak interaction, model', 'supersymmetry', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003027'],"[""On the occasion of a symposium honoring my collegue Adrian Melissinos, I gave an informal, personal review of bottom quark physics. This paper is a writeup of that talk. I first summarize the early days, the decade from the discovery through the determination of the b quark's rough features. I note a change in objective which occurred around 1990, with the new emphasis being USING the b quark, to probe the Standard Model and to search for physics `beyond the Standard Model'. I review the flavor sector of the Standard Model, showing why the b quark is such a useful probe. I then discuss three topics of current interest: the determination of V_ub; studies of rare hadronic B decays; and the radiative penguin decay b -> s gamma.""]",['2000-03-24']
878,['eng'],"['Biryukov, V M']",['Computer simulation of the tevatron crystal extraction experiment'],['Particle Physics - Experimental Results'],"['talk, Dallas 1995/05/01', 'proton synchrotron', 'ejection, bent crystal', 'crystal, alignment', 'efficiency', 'numerical calculations, Monte Carlo', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0110060'],"['The Fermilab crystal-extraction experiment E853 at Tevatron was simulated by Monte Carlo code CATCH [1] tested earlier in the CERN-SPS experiment [2-4]. Predictions for the extraction efficiency, angular scans and extracted beam profiles are presented. Several ideas are proposed and tested by the simulation, how to get in E853 the key information of the extraction experiment: the ""septum width"" of a crystal and dependence of extraction efficiency on it, the impact parameters of protons at crystal, and the contribution of the first and multi passes to the extraction. The ways to optimize E853 are analyzed.']",['2001-10-26']
879,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bevensee, B', 'Bhatti, A A', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Field, R D', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kirk, M', 'Kim, B J', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Vaiciulis, T', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Limits on Gravitino Production and New Processes with Large Missing Transverse Energy in $p\\overline{p}$ Collisions at $\\sqrt{s}$=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'jet, hadroproduction', 'transverse energy, missing-energy', 'gravitino, search for', 'gravitino, pair production', 'supersymmetry, symmetry breaking', 'gravitino, mass', 'lower limit', 'electroweak interaction, validity test', 'acceptance, cross section', 'upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003026'],"['Events collected by the Collider Detector at Fermilab (CDF) with an energetic jet plus large missing transverse energy can be used to search for physics beyond the Standard Model. We see no deviations from the expected background and set upper limits on the production of new processes. We consider in addition the production of light gravitinos within the framework of the Gauge Mediated Supersymmetry Breaking models and set a limit at 95onfidence level on the breaking scale sqrt(F) >= 217 GeV, which excludes gravitino masses smaller than 1.1x10^-5 eV/c^2.']",['2000-03-22']
880,['eng'],"['Poling, R A']",['Heavy Quark Decays'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'quark, beauty', 'quark, decay', 'quark, electroproduction', 'Kobayashi-Maskawa angle, parametrization', 'B, semileptonic decay', 'lepton, momentum spectrum', 'B, rare decay', 'meson, pair production', 'final state, (0charm)', 'quark, radiative decay', 'photon, energy spectrum', 'B, branching ratio', 'HQET model', 'experimental results', 'magnetic detector, CLEO', 'Cornell CESR Stor', 'CERN LEP Stor', 'bibliography', 'B --> D*(2010) lepton- antineutrino', 'B --> K muon+ muon-', 'beauty --> strangeness photon', 'beauty --> strangeness lepton+ lepton-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003025'],"['The status of heavy-quark decays as of summer 1999 is reviewed. New measurements of semileptonic B decays from LEP and from CLEO are reported and the status of determining the CKM parameters |Vcb| and |Vub| is assessed. Rare charmless hadronic B decays are reviewed, including the first observation of B->pi pi from CLEO. First attempts to measure CP asymmetries in rare decays are described. The implications of all of the data for our understanding of the Standard Model are briefly assessed.']",['2000-03-24']
881,['eng'],"['Telnov, V I']",['Photon colliders'],['Particle Physics - Experimental Results'],"['talk, Santa Cruz 1999/12/10', 'electron positron, linear collider', 'photon photon, colliding beams', 'photon electron, colliding beams', 'laser, backscatter', 'optics, reflection', 'luminosity']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003024'],"['High energy photon colliders based on laser backscattering are a very natural extension of a e+e- linear colliders and open new possibilities to study of the matter. This option has been included in the pre-conceptual designs of linear colliders and work on Technical Design Reports is in progress. The physics motivation for photon colliders is quite clear though more studies are needed. The proof of its technical feasibility and the search for the best solutions is of first priority now. In this talk we discuss: physics motivation, laser problems and new possible solutions, and generation of low emittance beams needed for obtaining very high luminosities.']",['2000-03-24']
882,['eng'],[],['Measurement of the Lifetime of the $\\tau$ Lepton'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, leptonic decay', 'tau, pair production', 'tau, leptonic decay', 'tau, branching ratio', 'tau, lifetime', 'decay, path length', 'track data analysis, impact parameter', 'lepton, universality', 'strong interaction, coupling constant', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003023'],"['The tau lepton lifetime is measured with the L3 detector at LEP using the complete data taken at centre-of-mass energies around the Z pole resulting in tau_tau = 293.2 +/- 2.0 (stat) +/- 1.5 (syst) fs. The comparison of this result with the muon lifetime supports lepton universality of the weak charged current at the level of six per mille. Assuming lepton universality, the value of the strong coupling constant, alpha_s is found to be alpha_s(m_tau^2) = 0.319 +/- 0.015(exp.) +/- 0.014 (theory).']",['2000-03-17']
883,['eng'],"['Böhm, F', 'Busenitz, J K', 'Cook, B', 'Gratta, Giorgio', 'Henrikson, H', 'Kornis, J', 'Lawrence, D', 'Lee, K B', 'McKinny, K', 'Miller, L', 'Novikov, V', 'Piepke, A G', 'Ritchie, B', 'Tracy, D', 'Vogel, P', 'Wang, Y F', 'Wolf, J']",['Results from the Palo Verde Neutrino Oscillation Experiment'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'fission, particle source', 'antineutrino/e, flux', 'energy spectrum', 'antineutrino p, interaction', 'charged current', 'calibration', 'efficiency', 'data analysis method', 'neutrino, mass difference', 'neutrino, mixing angle', 'scintillation counter, liquid', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003022'],"['The $\\nuebar$ flux and spectrum have been measured at a distance of about 800 m from the reactors of the Palo Verde Nuclear Generating Station using a segmented Gd-loaded liquid scintillator detector. Correlated positron-neutron events from the reaction $\\nuebar$p$\\to$e^+n were recorded for a period of 200 d including 55 d with one of the three reactors off for refueling. Backgrounds were accounted for by making use of the reactor-on and reactor-off cycles, and also with a novel technique based on the difference between signal and background under reversal of the e^+ and n portions of the events. A detailed description of the detector calibration, background subtraction, and data analysis is presented here. Results from the experiment show no evidence for neutrino oscillations. $\\nuebar\\to\\bar\\nu_x$ oscillations were excluded at 90 CL for $\\dm>1.12\\times10^{-3}$ eV^2 for full mixing, and $\\sinq>0.21$ for large $\\dm$. These results support the conclusion that the observed atmospheric neutrino oscillations does not involve $\\nu_{\\rm e}$.']",['2000-03-17']
884,['eng'],"['Ziegler, T']",['Color Reconnection and Bose-Einstein Correlations at LEP2'],['Particle Physics - Experimental Results'],"['talk, Moscow 1999/09/20', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'W, mass', 'final-state interaction', 'color, recombination', 'hadron, multiple production', 'charged particle, multiplicity', 'charged particle, momentum spectrum', 'jet, energy flow', 'correlation, two-pion', 'boson, statistics', 'correlation function', 'momentum transfer, dependence', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', 'electron --> quark antiquark', '183 189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003021'],['Recent investigations of final state interactions of W+W- events in e+e- collisions up to center of mass energies sqrt{S}=189GeV at LEP2 are reviewed. The data were used to look for color reconnection and Bose-Einstein correlations between the two color singlets of fully hadronic W events.'],['2000-03-17']
885,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bähr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bizot, J C', 'Borras, K', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P D', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferron, S', 'Fleischer, M', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Hauschildt, T', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hilgers, M', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Kaufmann, O', 'Kausch, M', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolanoski, H', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krücker, D', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Kutuev, R K', 'Lachnit, W A', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'List, B', 'Lobodzinska, E', 'Lobodzinski, B', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, A', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, D', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Negri, I', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vazdik, Ya', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']",['Elastic Photoproduction of $J/\\psi$ and $\\Upsilon$ Mesons at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'J/psi(3100), photoproduction', 'Upsilon(9460), photoproduction', 'J/psi(3100), leptonic decay', 'Upsilon(9460), leptonic decay', 'cross section, energy dependence', 'parametrization', 'differential cross section, momentum transfer', 'Regge poles', 'quantum chromodynamics, perturbation theory', 'pomeron, exchange', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> J/psi(3100) p positron', 'positron p --> Upsilon(9460) p positron', 'J/psi(3100) --> positron electron', 'Upsilon(9460) --> muon+ muon-', 'approx. 300 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003020', 'http://arXiv.org/abs/hep-ex/?0003020://www-h1.desy.de/h1/www/publications/htmlsplit/DESY-00-037.long.html']","['Cross sections for elastic photoproduction of J/Psi and Upsilon mesons are presented. For J/Psi mesons the dependence on the photon-proton centre-of-mass energy W_gammap is analysed in an extended range with respect to previous measurements of 26<=W_gammap<= 285 GeV. The measured energy dependence is parameterized as sigma_gammap proportional W_gammap^delta with delta=0.83+-0.07. The differential cross section dsigma/dt for J/Psi mesons is derived, its dependence on W_gammap and on t is analysed and the effective trajectory (in terms of Regge theory) is determined to be alpha(t)=(1.27+-0.05)+(0.08+-0.17)*t/GeV^2. Models based on perturbative QCD and on pomeron exchange are compared to the data.']",['2000-03-17']
886,['eng'],"['Adler, Stephen Louis', 'Atiya, M S', 'Chiang, I H', 'Diwan, M V', 'Frank, J S', 'Haggerty, J S', 'Kettell, S H', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'Sambamurti, A K', 'Stevens, A', 'Strand, R C', 'Witzig, C', 'Komatsubara, T K', 'Kuriki, M', 'Muramatsu, N', 'Sugimoto, S', 'Inagaki, T', 'Kabe, S', 'Kobayashi, M', 'Kuno, Y', 'Sato, T', 'Shinkawa, T', 'Yoshimura, Y', 'Kishi, Y', 'Nakano, T', 'Ardebili, M', 'Convery, M R', 'Ito, M M', 'Marlow, D R', 'McPherson, R A', 'Meyers, P D', 'Shoemaker, F C', 'Smith, A J S', 'Stone, J R', 'Aoki, M', 'Blackmore, E W', 'Bergbusch, P C', 'Bryman, D A', 'Konaka, A', 'MacDonald, J A', 'Mildenberger, J L', 'Numao, T', 'Padley, P', 'Poutissou, J M', 'Poutissou, R', 'Redlinger, G', 'Kitching, P', 'Soluk, R']",['Measurement of Structure Dependent $K^{+} \\to \\mu^{+}\\nu_{\\mu}\\gamma$ Decay'],['Particle Physics - Experimental Results'],"['K+, radiative decay', 'K+, width', 'K+, form factor', 'form factor, vector', 'form factor, axial-vector', 'K+, branching ratio', 'experimental results', 'Brookhaven PS', 'K+ --> muon+ neutrino/mu photon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003019'],"['We report the first measurement of a structure dependent component in the decay K^+ -> mu^+ nu gamma. Using the kinematic region where the muon kinetic energy is greater than 137 MeV and the photon energy is greater than 90 MeV, we find that the absolute value of the sum of the vector and axial-vector form factors is |F_V+F_A| =0.165 \\pm 0.007 \\pm 0.011. This corresponds to a branching ratio of BR(SD^+) = (1.33 \\pm 0.12 \\pm 0.18) \\times 10^{-5}. We also set the limit -0.04 < F_V-F_A < 0.24 at 90.l.']",['2000-03-17']
887,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Abbiendi, G', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Coppola, N', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Brock, I', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Hartmann, H', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Foster, B', 'Heath, G P', 'Heath, H F', 'McFall, J D', 'Piccioni, D', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Burgard, C', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hasell, D', 'Hebbel, K', 'Johnson, K F', 'Kasemann, M', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Lindemann, L', 'Löhr, B', 'Martínez, M', 'Milite, M', 'Monteiro, T', 'Moritz, M', 'Notz, D', 'Pelucchi, F', 'Petrucci, M C', 'Rohde, M', 'Saull, P R B', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Tassi, E', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'Votano, L', 'Bamberger, Andreas', 'Benen, A', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Doyle, A T', 'Lee, S W', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Garfagnini, A', 'Gialas, I', 'Gladilin, L K', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Poelz, G', 'Zetsche, F', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Mallik, U', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Park, I H', 'Son, D', 'Barreiro, F', 'García, G', 'Glasman, C', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Barbi, M S', 'Corriveau, F', 'Hanna, D S', 'Ochs, A', 'Padhi, S', 'Riveline, M', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Bashkirov, V', 'Dolgoshein, B A', 'Dementev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Sheheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Acosta, D', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dosselli, U', 'Dusini, S', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sabetfakhri, A', 'Simmons, D', 'Butterworth, J M', 'Catterall, C D', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Pawlak, R', 'Smalska, B', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Adamus, M', 'Gadaj, T', 'Deppe, O', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Badgett, W F', 'Chapin, D', 'Cross, R', 'Foudas, C', 'Mattingly, S E', 'Reeder, D D', 'Smith, W H', 'Vaiciulis, A W', 'Wildschek, T', 'Wodarczyk, M', 'Deshpande, A A', 'Dhawan, S K', 'Hughes, V W', 'Bhadra, S', 'Catterall, C D', 'Cole, J E', 'Frisken, W R', 'Hall-Wilton, R', 'Khakzad, M', 'Menary, S R']",['Measurement of Inclusive $D_{s}^{pm}$ Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'photon p, inclusive reaction', 'D/s+, photoproduction', 'D/s-, photoproduction', 'differential cross section, transverse momentum', 'differential cross section, rapidity dependence', 'D*(2010), photoproduction', 'cross section, ratio', 'quantum chromodynamics, perturbation theory', 'quark, charm', 'quark, fragmentation', 'production, strangeness', 'structure function, parametrization', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', '130-280 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003018'],"['The first measurement of inclusive Ds+- photoproduction at HERA has been performed with the ZEUS detector for photon-proton centre-of-mass energies 130 < W < 280 GeV. The measured cross section for 3 < pt(Ds) < 12 GeV and |eta(Ds)|< 1.5 is sigma(ep -> Ds X) = 3.79 +- 0.59 (stat.) +0.26-0.46 (syst.) +- 0.94 (br.) nb, where the last error arises from the uncertainty in the Ds decay branching ratio. The measurements are compared with inclusive D*+- photoproduction cross sections in the same kinematic region and with QCD calculations. The Ds cross sections lie above a fixed-order next-to-leading order calculation and agree better with a tree-level O(alpha,alpha_s^3) calculation that was tuned to describe the ZEUS D* cross sections. The ratio of Ds+- to D*+- cross sections is 0.41 +- 0.07 (stat.) +0.03-0.05 (syst.) +- 0.10 (br.). From this ratio, the strangeness-suppression factor in charm photoproduction, within the LUND string fragmentation model, has been calculated to be gamma_s = 0.27 +- 0.05 +- 0.07 (br.). The cross-section ratio and gamma_s are in good agreement with those obtained in charm production in e+e- annihilation.']",['2000-03-15']
888,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Abbiendi, G', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Coppola, N', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Brock, I', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Hartmann, H', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Foster, B', 'Heath, G P', 'Heath, H F', 'McFall, J D', 'Piccioni, D', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sampson, S', 'Schmidke, W B', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Burgard, C', 'Dannheim, D', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hasell, D', 'Hebbel, K', 'Johnson, K F', 'Kasemann, M', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Lindemann, L', 'Löhr, B', 'Martínez, M', 'Milite, M', 'Monteiro, T', 'Moritz, M', 'Notz, D', 'Pelucchi, F', 'Petrucci, M C', 'Rohde, M', 'Saull, P R B', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Tassi, E', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'Votano, L', 'Bamberger, Andreas', 'Benen, A', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Doyle, A T', 'Lee, S W', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Garfagnini, A', 'Gialas, I', 'Gladilin, L K', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Poelz, G', 'Zetsche, F', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Mallik, U', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Park, I H', 'Son, D', 'Barreiro, F', 'García, G', 'Glasman, C', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Barbi, M S', 'Corriveau, F', 'Hanna, D S', 'Ochs, A', 'Padhi, S', 'Riveline, M', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Bashkirov, V', 'Dolgoshein, B A', 'Dementev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Shcheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Acosta, D', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dosselli, U', 'Dusini, S', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Adamczyk, L', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sabetfakhri, A', 'Simmons, D', 'Butterworth, J M', 'Catterall, C D', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Pawlak, R', 'Smalska, B', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Adamus, M', 'Gadaj, T', 'Deppe, O', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Badgett, W F', 'Chapin, D', 'Cross, R', 'Foudas, C', 'Mattingly, S E', 'Reeder, D D', 'Smith, W H', 'Vaiciulis, A W', 'Wildschek, T', 'Wodarczyk, M', 'Deshpande, A A', 'Dhawan, S K', 'Hughes, V W', 'Bhadra, S', 'Catterall, C D', 'Cole, J E', 'Frisken, W R', 'Hall-Wilton, R', 'Khakzad, M', 'Menary, S R']",['Measurement of Azimuthal Asymmetries in Deep Inelastic Scattering'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'neutral current', 'hadron, electroproduction', 'hadron, charged particle', 'angular distribution, asymmetry', 'angular distribution, moment', 'dependence, transverse momentum', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003017'],['The distribution of the azimuthal angle for the charged hadrons has been studied in the hadronic centre-of-mass system for neutral current deep inelastic positron-proton scattering with the ZEUS detector at HERA. Measurements of the dependence of the moments of this distribution on the transverse momenta of the charged hadrons are presented. Asymmetries that can be unambiguously attributed to perturbative QCD processes have been observed for the first time.'],['2000-03-15']
889,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Z boson pair production in $e^{+}e^{-}$ collisions at $\\sqrt{s}$ = 183 and 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, pair production', 'Z0, leptonic decay', 'Z0, hadronic decay', 'final state, (4lepton)', 'final state, (2lepton 2neutrino)', 'final state, (quark antiquark 2lepton)', 'final state, (quark antiquark 2neutrino)', 'final state, (2quark 2antiquark)', 'channel cross section', 'coupling, (3Z0)', 'coupling, (2Z0 photon)', 'statistical analysis', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '183, 189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003016'],"['A study of Z boson pair production in e+e- annihilation at center-of-mass energies near 183 GeV and 189 GeV is reported. Final states containing only leptons, (l+l-l+l- and l+l-nu nubar), quark and lepton pairs, (q qbar l+l-, q qbar nu nubar) and the all-hadronic final state (q qbar q qbar) are considered. In all states with at least one Z boson decaying hadronically, q qbar and b bbar final states are considered separately using lifetime and event-shape tags, thereby improving the cross-section measurement. At sqrt(s) = 189 GeV the Z-pair cross section was measured to be 0.80 (+0.14-0.13, stat.) (+0.06-0.05, syst.) pb, consistent with the Standard Model prediction. At sqrt(s) = 183 GeV the 95.L. upper limit is 0.55 pb. Limits on anomalous ZZgamma and ZZZ couplings are derived.']",['2000-03-14']
890,['eng'],"['Ter-Mikaelian, M L']",['Present Situation of Diffracted X-ray Radiation and Resonance (Coherent) Transition Radiation Induced by High Energy Charged Particles in Frequencies Region Exiding Atomic one'],['Detectors and Experimental Techniques'],"['review', 'charged particle, relativistic', 'radiation, emission', 'radiation, electromagnetic', 'diffraction', 'radiation, transition', 'resonance', 'crystal', 'matter', 'bremsstrahlung', 'effect, multiple scattering', 'effect, density', 'experimental methods', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003015'],"['The review is devoted to the modern investigations of electromagnetic radiation by relativistic charged particles propagating with constant velocity through the periodic media. Two examples of radiation are considered in this review, the first corresponds to the Bragg scattering of charged particles pseudophotons in crystals, the second one to the Fresnel scattering of pseudophotons in periodic medium. Both examples play essential role in construction new compact tunable sources in X-ray region.']",['2000-03-14']
891,['eng'],"['Ong, R A']",['High Energy Particles from the Universe'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'photon, cosmic radiation', 'cosmic radiation, particle source', 'cosmic radiation, flux', 'cosmic radiation, energy spectrum', 'neutrino, cosmic radiation', 'astrophysics', 'gamma ray burst', 'counters and detectors, satellite', 'Cherenkov counter', 'deep underground detector', 'experimental results', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003014'],"['The field of high energy particle astronomy is exciting and rapidly developing. In the last few years, we have detected extragalactic sources of intense TeV gamma radiation and individual cosmic ray particles with energies exceeding 25 Joules. Understanding the workings of astrophysics under extreme conditions is the primary goal of this field. Also important is the possibility of using high energy particles from space to probe beyond the standard models of particle physics and cosmology. This paper presents a review of high energy particle astronomy using photons, cosmic rays, and neutrinos.']",['2000-03-14']
892,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of |$V_{cb}$| using $\\overline{B}^{0} \\to D^{*+}l^{-}\\overline{\\nu}$ decays'],['Particle Physics - Experimental Results'],"['anti-B0, semileptonic decay', 'anti-B0, cascade decay', 'quark, charm', 'quark, beauty', 'Kobayashi-Maskawa angle', 'decay, form factor', 'anti-B0, branching ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'anti-B0 --> D*(2010) lepton- antineutrino', 'D*(2010) --> D0 pi+']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003013'],"['The magnitude of the Cabibbo-Kobayashi-Maskawa matrix element Vcb has been measured using B0 to D*l nu decays recorded on the Z0 peak using the OPAL detector at LEP. The D* to D0 pi+ decays were reconstructed both in the particular decay modes D0 to K- pi+ and D0 to K- pi+ pi- and via an inclusive technique. The product of |Vcb| and the decay form factor of the B0 to D* l nu transition at zero recoil F(1) was measured to be F(1)|Vcb| = (37.1+-1.0+-2.0)x10^-3, where the uncertainties are statistical and systematic respectively. By using Heavy Quark Effective Theory calculations for F(1), a value of |Vcb| = (40.7+-1.1+-2.2+-1.6)x 10^-3 was obtained, where the third error is due to theoretical uncertainties in the value of F(1). The branching ratio Br(B0 to D* l nu) was also measured to be (5.26+-0.20+-0.46)']",['2000-03-13']
893,['eng'],"['Moinester, M A', 'Chung, S U']",['Hybrid Meson Structure at COMPASS'],['Detectors and Experimental Techniques'],"['talk, Munich 1999/10/11', 'meson, hybrid', 'bound state, (quark antiquark gluon)', 'meson, production', 'pi nucleus, interaction', 'photon, exchange', 'Primakoff effect', 'pomeron, exchange', 'diffraction', 'Feynman graph', 'meson, decay', 'magnetic spectrometer, COMPASS', 'trigger', 'programming', 'proposed experiment, CERN SPS', '100-280 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003008'],"['We describe a pion physics program attainable with the CERN COMPASSspectrometer, involving tracking detectors and an electromagnetic calorimeter.COMPASS can realize state-of-the-art pion beam hybrid meson and meson radiativetransition studies. We review here the physics motivation for this program. Wedescribe the beam, detector, trigger requirements, and hardware/softwarerequirements for this program. The triggers for all this hybrid meson physicscan be implemented for simultaneous data taking. We will investigate hybrid meson production via pion-photon Primakoff andpion-Pomeron diffractive interactions. We will determine new properties ofquark-antiquark-gluon hybrid mesons, using unique production methods, toimprove our understanding of these exotic mesons. The CERN COMPASS experiment uses 100-280 GeV beams (muon, pion), and magneticspectrometers and calorimeters, to measure the complete kinematics ofpion-photon and pion-Pomeron reactions. The COMPASS experiment is currentlyunder construction, and scheduled to begin data runs in 2001. We carry outsimulation studies to optimize the beam, detector, trigger, andhardware/software for achieving high statistics data with low systematicuncertainties in the hybrid meson component of this program. We will improveprevious Primakoff Hybrid studies by three orders of magnitude. We implementspecial detectors and triggers for hybrid meson production reactions. Wepropose to prepare for these COMPASS pion beam hybrid studies by setting upwith muon beam tests.']",['2000-03-08']
894,['eng'],"['Ter-Antonian, S V', 'Haroyan, L S']",['About EAS size spectra and primary energy spectra in the knee region'],['Particle Physics - Experimental Results'],"['nucleus, cosmic radiation', 'showers, air', 'cosmic radiation, primary', 'cosmic radiation, energy spectrum', 'model, interaction', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003006'],"['Based on a unified analyses of KASCADE, AKENO, EAS-TOP and ANI EAS sizespectra, the approximations of energy spectra of different primary nuclei havebeen found. Calculations were carried out using SIBYLL and QGSJET interactionmodels in 0.1-100 PeV primary energy range. The results point to existence ofboth rigidity-dependent steepening energy spectra at R=200-400 TV and anadditional proton (neutron) component with differential energy spectrum(6.1+/-0.7)10^{-11}(E/Ek)^{-1.5} (m^2.s.sr.TeV)^{-1} before the kneeEk=2030+/-130 TeV and with power index g2=-3.1+/-0.05 after the knee.']",['2000-03-07']
895,['eng'],"['Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J', 'Lipeles, E', 'Pappas, S P', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Nelson, H N', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S']",['Search for CP violation in $B^{\\pm} \\to J/\\psi K^{\\pm}$ and $B^{\\pm} \\to \\psi(2S) K^{\\pm}$ decays'],['Particle Physics - Experimental Results'],"['B+, hadronic decay', 'B-, hadronic decay', 'J/psi(3100)', 'psi(3685)', 'violation, CP', 'Feynman graph', 'mass spectrum', 'charge, asymmetry', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B+ --> J/psi(3100) K+', 'B- --> J/psi(3100) K-', 'B+ --> psi(3685) K+', 'B- --> psi(3685) K-']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003004'],"['We present a search for direct CP violation in B+- -> J/psi K+- and B+- ->psi(2S) K+- decays. In a sample of 9.7 million B meson pairs collected with theCLEO detector, we have fully reconstructed 534 B+- -> J/psi K+- and 120 B+- ->psi(2S) K+- decays with very low background. We have measured the CP-violatingcharge asymmetry to be (+1.8+-4.3[stat]+-0.4[syst]) 0.000000or B+- -> J/psi K+- and(+2.0+-9.1[stat]+-1.0[syst]) 0.000000or B+- -> psi(2S) K+-.']",['2000-03-03']
896,['eng'],"['Bakari, D', 'Dekhissi, H', 'Derkaoui, J E', 'Giacomelli, Giorgio', 'Mandrioli, G', 'Ouchrif, M', 'Patrizii, L', 'Popa, V']",['Energy Losses of Q-balls'],['Detectors and Experimental Techniques'],"['astrophysics, missing-mass', 'matter, droplet', 'Q-ball, model', 'Q-ball, mass', 'Q-ball, quantum number', 'supersymmetry, symmetry breaking', 'Q-ball, interaction', 'matter, geophysics', 'energy loss', 'Q-ball, flux', 'deep underground detector, MACRO', 'acceptance', 'scintillation counter, liquid', 'photon, yield', 'streamer chamber, drift tube', 'ionization', 'plastics, track sensitive', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003003'],"['After a short review of Q-balls properties, in this paper we discuss theirinteraction with matter, and their energy losses in the earth, for a largerange of velocities. These calculations are used to compute the fractionalangular acceptance of a detector located at Gran Sasso Laboratory. Furthermorewe computed the light yield in liquid scintillators, the ionization in streamertubes and the Restricted Energy Loss in the CR39 nuclear track detector.']",['2000-03-03']
897,['eng'],"['Adloff, C', 'Andreev, V', 'Andrieu, B', 'Arkadov, V', 'Astvatsaturov, A R', 'Ayyaz, I', 'Babaev, A', 'Bähr, J', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Bassler, U', 'Bate, P', 'Beglarian, A', 'Behnke, O', 'Beier, C', 'Belousov, A', 'Benisch, T', 'Berger, C', 'Bernardi, G', 'Berndt, T', 'Bertrand-Coremans, G', 'Bizot, J C', 'Borras, K', 'Boudry, V', 'Braunschweig, W', 'Brisson, V', 'Broker, H B', 'Brown, D P D', 'Brückner, W', 'Bruel, P', 'Bruncko, D', 'Bürger, J', 'Büsser, F W', 'Bunyatyan, A', 'Burkhardt, H', 'Burrage, A', 'Buschhorn, G W', 'Campbell, A J', 'Cao, J', 'Carli, T', 'Caron, S', 'Chabert, E', 'Clarke, D', 'Clerbaux, B', 'Collard, C', 'Contreras, J G', 'Coughlan, J A', 'Cousinou, M C', 'Cox, B E', 'Cozzika, G', 'Cvach, J', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davidsson, M', 'Delcourt, B', 'Delerue, N', 'Demirchyan, R A', 'de Roeck, A', 'De Wolf, E A', 'Diaconu, C A', 'Dixon, P', 'Dodonov, V', 'Donovan, K T', 'Dowell, John D', 'Droutskoi, A', 'Duprel, C', 'Ebert, J', 'Eckerlin, G', 'Eckstein, D', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellerbrock, M', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Faulkner, P J W', 'Favart, L', 'Fedotov, A', 'Felst, R', 'Ferencei, J', 'Ferrarotto, F', 'Ferron, S', 'Fleischer, M', 'Flügge, G', 'Fomenko, A', 'Foresti, I', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gassner, J', 'Gayler, J', 'Gerhards, R', 'Kazarian, S', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goodwin, C', 'Grab, C', 'Grässler, H', 'Greenshaw, T', 'Grindhammer, G', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Haustein, V', 'Haynes, W J', 'Heinemann, B', 'Heinzelmann, G', 'Henderson, R C W', 'Hengstmann, S', 'Henschel, H', 'Heremans, R', 'Herrera, G', 'Herynek, I', 'Hilgers, M', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoting, P', 'Hoffmann, D', 'Hoprich, W', 'Horisberger, R P', 'Hurling, S', 'Ibbotson, M', 'Issever, C', 'Jacquet, M', 'Jaffré, M', 'Janauschek, L', 'Jansen, D M', 'Janssen, X', 'Jemanov, V', 'Jönsson, L B', 'Johnson, D P', 'Jones, M A S', 'Jung, H', 'Kastli, H K', 'Kant, D', 'Kapichine, M', 'Karlsson, M', 'Karschnick, O', 'Kaufmann, O', 'Kausch, M', 'Keil, F', 'Keller, N', 'Kennedy, J', 'Kenyon, Ian Richard', 'Kermiche, S', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Koblitz, B', 'Kolanoski, H', 'Kolya, S D', 'Korbel, V', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Kroseberg, J', 'Krücker, D', 'Krüger, K', 'Küpper, A', 'Kuhr, T', 'Kurca, T', 'Kutuev, R K', 'Lachnit, W A', 'Lahmann, R', 'Lamb, D', 'Landon, M P J', 'Lange, W', 'Lastoviicka, T', 'Lebedev, A', 'Leiner, B', 'Lemrani, R', 'Lendermann, V', 'Levonian, S', 'Lindstrøm, M', 'Lobo, G', 'Lobodzinska, E', 'Lobodzinski, B', 'Loktionova, N A', 'Lubimov, V', 'Lüders, S', 'Lüke, D', 'Lytkin, L K', 'Magnussen, N', 'Mahlke-Krüger, H', 'Malden, N', 'Malinovskii, E I', 'Malinovskii, E I', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martyn, H U', 'Martyniak, J', 'Maxfield, S J', 'Mehta, A', 'Meier, K', 'Merkel, P', 'Metlica, F', 'Meyer, A', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Mikocki, S', 'Milstead, D', 'Mkrtchyan, T', 'Mohr, R', 'Mohrdieck, S', 'Mondragón, M N', 'Moreau, F', 'Morozov, A', 'Morris, J V', 'Müller, D', 'Müller, K', 'Murn, P', 'Nagovizin, V', 'Naroska, B', 'Naumann, J', 'Naumann, T', 'Negri, I', 'Nellen, G', 'Newman, P R', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nix, O', 'Nowak, G', 'Nunnemann, T', 'Olsson, J E', 'Ozerov, D', 'Panassik, V', 'Pascaud, C', 'Patel, G D', 'Pérez, E', 'Phillips, J P', 'Pitzl, D', 'Pöschl, R', 'Potachnikova, I', 'Povh, B', 'Rabbertz, K', 'Rädel, G', 'Rauschenberger, J', 'Reimer, P', 'Reisert, B', 'Reyna, D', 'Riess, S', 'Rizvi, E', 'Robmann, P', 'Roosen, R', 'Rostovtsev, A A', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Sankey, D P C', 'Scheins, J', 'Schilling, F P', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, D', 'Schoeffel, L', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, V', 'Schultz-Coulon, H C', 'Sedlak, K', 'Sefkow, F', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Sievers, P', 'Sirois, Y', 'Sloan, Terence', 'Smirnov, P', 'Smith, M', 'Solochenko, V', 'Soloviev, Yu V', 'Spaskov, V', 'Specka, A', 'Spitzer, H', 'Stamen, R', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stiewe, J', 'Straumann, U', 'Struczinski, W', 'Swart, M', 'Tasevsky, M', 'Chernyshov, V', 'Chechelnitskii, S', 'Thompson, G', 'Thompson, P D', 'Tobien, N', 'Traynor, D', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Turney, J E', 'Tzamariudaki, E', 'Udluft, S', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Mechelen, P', 'Vazdik, Ya', 'Von Dombrowski, S', 'Wacker, K', 'Wallny, R', 'Walter, T', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'White, G', 'Wiesand, S', 'Wilksen, T', 'Winde, M', 'Winter, G G', 'Wissing, C', 'Wobisch, M', 'Wollatz, H', 'Wunsch, E', 'Wyatt, A C', 'Zaicek, J', 'Zaleisak, J', 'Zhang, Z', 'Zhokin, A S', 'Zomer, F', 'Zsembery, J', 'Zur Nedden, M']","['Search for Compositeness, Leptoquarks and Large Extra Dimensions in eq Contact Interactions at HERA']",['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'differential cross section, momentum transfer', 'new particle, search for', 'particle, composite', 'new interaction, contact interaction', 'quark, form factor', 'electroweak interaction, model', 'neutral current', 'leptoquark, exchange', 'graviton, exchange', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> positron anything', '300 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0003002', 'http://www-h1.desy.de/h1/www/publications/htmlsplit/H1prelim-00-062.long.html', 'http://arXiv.org/abs/hep-ex/?0003002']","['The reaction e+p --> e+X is studied with the H1 detector at Hera. The datacover momentum transfers Q^2 between 200 GeV^2 and 30,000 GeV^2 and correspondto an integrated luminosity of 35.6 pb^(-1). The differential cross sectiondsigma/dQ^2 is compared to the Standard Model expectation for neutral currentscattering and analysed to search for bar(e)e bar(q)q contact interactions. Noevidence for new phenomena is observed. The results are used to set limits onscales within models of electron--quark compositeness, quark form factors andthe exchange of virtual heavy leptoquarks. A search for gravitational effectsmediated through the exchange of virtual gravitons which propagate into largeextra dimensions is presented.']",['2000-03-03']
898,['eng'],"['Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Morrison, R J', 'Nelson, H N', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams1, J', 'Edwards, K W', 'Patel, R', 'Janicek, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Kopp, S E', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'McGee, S', 'Perera, L P', 'Zhou, G J']",['Study of the Decays $B^{0} \\to D^{(*)+}D^{(*)-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'B0, branching ratio', 'charmed meson, pair production', 'D*(2010), hadronic decay', 'D, hadronic decay', 'angular distribution', 'track data analysis, vertex', 'decay, path length', 'Kobayashi-Maskawa angle, unitarity', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> D*(2010) D', 'B0 --> 2D*(2010)', 'B0 --> D+ D-', '10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002065'],"['The decays B0 --> D*+D*-, B0 --> D*+D- and B0 --> D+D- are studied in 9.7million Y(4S) --> BBbar decays accumulated with the CLEO detector. We determineBr(B0 --> D*+D*-) = (9.9+4.2-3.3+-1.2)e-4 and limit Br(B0 --> D*+D-) < 6.3e-4and Br(B0 --> D+D-) < 9.4e-4 at 90onfidence level (CL). We also perform thefirst angular analysis of the B0 --> D*+D*- decay and determine that theCP-even fraction of the final state is greater than 0.11 at 90L. Futuremeasurements of the time dependence of these decays may be useful for theinvestigation of CP violation in neutral B meson decays.']",['2000-03-01']
899,['eng'],"['Teige, S']",['Dynamics of the decay $\\eta \\to 3\\pi0$'],['Particle Physics - Experimental Results'],"['pi p, inclusive reaction', 'eta, hadroproduction', 'eta, hadronic decay', 'pi0, multiple production', 'Dalitz plot, density', 'parametrization', 'experimental results', 'Brookhaven PS', 'pi- p --> eta anything', 'eta --> 3pi0', '18.3 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002064'],['The parameter $ \\alpha = -0.005 \\pm 0.007 (stat) \\pm 0.004 (syst)$ describingthe density of events within the $ \\eta \\to 3\\pi^0 $ Dalitz plot has beenmeasured using data from Brookhaven experiment E852. The result is compared toprevious values and theoretical predictions.'],['2000-02-28']
900,['eng'],"['Starostin, A S', 'Beda, A G']",['Germanium Detector with Internal Amplification for Investigation of Rare Processes'],['Detectors and Experimental Techniques'],"['talk, Dubna 1999/06/28', 'astrophysics, missing-mass', 'WIMP', 'neutrino, magnetic moment', 'neutrino nucleus, nuclear reaction', 'neutrino nucleus, coherent interaction', 'neutrino, solar', 'semiconductor detector', 'germanium']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002063'],"['Device of new type is suggested - germanium detector with internalamplification. Such detector having effective threshold about 10 eV opens upfresh opportunity for investigation of dark matter, measurement of neutrinomagnetic moment, of neutrino coherent scattering at nuclei and for study ofsolar neutrino problem. Construction of germanium detector with internalamplification and perspectives of its use are described.']",['2000-02-28']
901,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Transverse and Longitudinal Bose Einstein Correlations in hadronic $Z^0$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'correlation, two-pion', 'boson, statistics', 'momentum, difference', 'transverse momentum', 'longitudinal momentum', 'correlation function, parametrization', 'pi, particle source', 'string model, fragmentation', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002062'],"['Bose-Einstein correlations in pairs of identical charged pions produced in asample of 4.3 million Z0 hadronic decays are studied as a function of the threecomponents of the momentum difference, transverse (""out"" and ""side"") andlongitudinal with respect to the thrust direction of the event. A significantdifference between the transverse, r_t_side, and longitudinal, r_l, dimensionsis observed, indicating that the emitting source of identical pions, asobserved in the Longitudinally CoMoving System, has an elongated shape. This isobserved with a variety of selection techniques. Specifically, the values ofthe parameters obtained by fitting the extended Goldhaber parametrisation tothe correlation function C\'= C^{DATA}}/C^{MC} for two-jet events, selected withthe Durham algorithm and resolution parameter ycut=0.04, arer_t_out=(0.647+-0.011(stat})+0.022-0.124(syst)) fm,r_t_side=(0.809+-0.009(stat)+0.019-0.032}(syst)) fm, r_l=(0.989+-0.011(stat)+0.030-0.015(syst})) fm andr_l/r_t_side=1.222+- 0.027(stat})+0.075-0.012(syst). The results are discussedin the context of a recent model of Bose-Einstein correlations based on stringfragmentation.']",['2000-02-25']
902,['eng'],"['Bland, L C']",['Spin Physics with the STAR detector'],['Detectors and Experimental Techniques'],"['talk, Wako 1999/11/04', 'p p, colliding beams', 'p, polarized beam', 'jet, hadroproduction', 'photon, associated production', 'W, hadroproduction', 'W, leptonic decay', 'p, spin', 'p, structure function', 'parametrization', 'gluon, polarization', 'quark, polarization', 'quark, sea', 'magnetic detector, STAR', 'numerical calculations, Brookhaven RHIC Coll', 'p p --> jet photon anything', 'p p --> W anything', '200, 500 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002061'],"[""The STAR detector will bring unique capabilities to the study of$\\vec{p}+\\vec{p}$ collisions up to total center of mass energies of 500 GeV atRHIC. The large acceptance of the time projection chamber and theelectromagnetic calorimeter enable STAR to observe jets, and to detect photonsand electrons in important regions of phase space. The premier experiments ofthe STAR spin program are discussed in this contribution. Photon + jetcoincidence measurements will provide the world's best determination of thecontribution gluons make to the proton's spin. Detection of the daughterelectrons and positrons from $W^\\pm$ decay will enable the determination of thepolarization of the $q\\bar{q}$ sea within the proton.""]",['2000-02-25']
903,['eng'],"['Bartoli, B', 'Buonomo, R', 'Calloni, E', 'Catalanotti, S', 'Piazzoli, B D E', 'Sciascio, G D', 'Iacovacci, M']",['Study of RPC gas mixtures for the ARGO-YBJ experiment'],['Detectors and Experimental Techniques'],"['talk, Bari 1999/10/28', 'photon, cosmic radiation', 'showers, air', 'drift chamber, gas', 'electrode, impedance', 'argon, organic compounds', 'fluorine', 'efficiency', 'time resolution']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002060'],"['The ARGO-YBJ experiment consists of a RPC carpet to be operated at theYangbajing laboratory (Tibet, P.R. China), 4300 m a.s.l., and devoted to thedetection of showers initiated by photon primaries in the energy range 100 GeV- 20 TeV. The measurement technique, namely the timing on the shower front witha few tens of particles, requires RPC operation with 1 ns time resolution, lowstrip multiplicity, high efficiency and low single counting rate. We havetested RPCs with many gas mixtures, at sea level, in order to optimize theseparameters. The results of this study are reported.']",['2000-02-25']
904,['eng'],"['Willocq, S']",['A Review of $B_{s}$ Mixing'],['Particle Physics - Experimental Results'],"['talk, Taipei 1999/12/03', 'B/s0 anti-B/s0, interference', 'oscillation, time dependence', 'B/s0, mass difference', 'lower limit', 'B/s0, decay modes', 'particle identification, flavor', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'Batavia TEVATRON Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002059'],"['We review the experimental status of Bs mixing. After a brief historicaloverview, current studies of the time dependence of Bs oscillations aredescribed, with an emphasis on the different experimental techniques used bythe ALEPH, CDF, DELPHI, OPAL, and SLD Collaborations. To conclude, the outlookfor future experiments is presented.']",['2000-02-25']
905,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Akimov, V E', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bean, A', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Chen, W', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cobau, W G', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gobbi, B', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Jun, S Y', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Landsberg, G L', 'Leflat, A', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lu, J G', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Markeloff, R', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McKibben, T', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Reay, N W', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Scully, J R', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Song, X F', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Tarazi, J', 'Taylor, W', 'Tentindo-Repond, S', 'Thomas, T L T', 'Thompson, J', 'Toback, D', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Spin Correlation in $t\\overline{t}$ Production from $p\\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'W, leptonic decay', 'spin, correlation', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', '1800 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002058', 'http://fnalpubs.fnal.gov/archive/2000/pub/Pub-00-046-E.html']","['The D0 collaboration has performed a study of spin correlation in tt-barproduction for the process tt-bar to bb-bar W^+W^-, where the W bosons decay toe-nu or mu-nu. A sample of six events was collected during an exposure of theD0 detector to an integrated luminosity of approximately 125 pb^-1 ofsqrt{s}=1.8 TeV pp-bar collisions. The standard model (SM) predicts that theshort lifetime of the top quark ensures the transmission of any spininformation at production to the tt-bar decay products. The degree of spin correlation is characterized by a correlation coefficientk. We find that k>-0.25 at the 68onfidence level, in agreement with the SMprediction of k=0.88.']",['2000-02-24']
906,['eng'],"['Novikov, E', 'Pakhlov, P']",['Search for spatial anisotropy in $\\beta$-decays'],['Particle Physics - Experimental Results'],"['strontium, semileptonic decay', 'electron, energy spectrum', 'spatial distribution, anisotropy', 'upper limit', 'invariance, Lorentz', 'validity test', 'scintillation counter', 'semiconductor detector', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002057'],"['Theoretically a possibility of covariance violation in weak decays is notruled out from the first principles, while there are some models predictingnon-covariance revealed in weak interactions. The experimental evidence forisotropy violation in $\\beta$-decays was recently reported. We present a studyof the dependence of electron flow rate and $\\beta$-electron energy in thedecay of $Sr^{90}$ with respect to the direction of electron emission. An upperlimit of $1.4 \\cdot 10^{-5}$ on directional dependence of $\\beta$-electronenergy was obtained.']",['2000-02-24']
907,['eng'],"[""D'Agostini, G""]",['Confidence limits'],['Detectors and Experimental Techniques'],"['talk, Geneva 2000/01/17', 'statistical analysis', 'gravitational radiation, measurement', 'electron positron, annihilation', 'Higgs particle, search for', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002055'],"[""This contribution to the debate on confidence limits focuses mostly on thecase of measurements with `open likelihood', in the sense that it is defined inthe text. I will show that, though a prior-free assessment of {\\it confidence}is, in general, not possible, still a search result can be reported in a mostlyunbiased and efficient way, which satisfies some desiderata which I believe areshared by the people interested in the subject. The simpler case of `closedlikelihood' will also be treated, and I will discuss why a uniform prior on asensible quantity is a very reasonable choice for most applications. In bothcases, I think that much clarity will be achieved if we remove from scientificparlance the misleading expressions `confidence intervals' and `confidence levels'.""]",['2000-02-23']
908,['eng'],"['Morales, A', 'Aalseth, C E', 'Avignone, F T', 'Brodzinski, R L', 'Cebrian, S', 'García, E', 'González, D', 'Hensley, W K', 'Irastorza, I G', 'Kirpichnikov, I V', 'Klimenko, A A', 'Miley, H S', 'Morales, J', 'De Solorzano, A O', 'Osetrov, S B', 'Pogosov, V S', 'Puimedón, J', 'Reeves, J H', 'Sarsa, M L', 'Scopel, S', 'Smolnikov, A A', 'Tamanyan, A G', 'Vasenko, A A', 'Vasilev, S I', 'Villar, J A']",['New constraints on WIMPs from the Canfranc IGEX dark matter search'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'WIMP, search for', 'nucleus WIMP, elastic scattering', 'germanium, recoil', 'energy spectrum', 'semiconductor detector, experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002053'],"['The IGEX Collaboration enriched 76Ge double-beta decay detectors arecurrently operating in the Canfranc Underground Laboratory with an overburdenof 2450 m.w.e. A recent upgrade has made it possible to use them in a searchfor WIMPs. A new exclusion plot has been derived for WIMP-nucleonspin-independent interaction. To obtain this result, 30 days of data from oneIGEX detector, which has an energy threshold of ~4 keV, have been considered.These data improve the exclusion limits derived from other germanium diodeexperiments in the ~50 GeV DAMA region, and show that with a moderateimprovement of the background below 10 keV, the DAMA region may be tested withan additional 1 kg-year of exposure.']",['2000-02-22']
909,['eng'],"['Cecchini, S', 'Sioli, M']",['Cosmic Ray Muon Physics'],['Particle Physics - Experimental Results'],"['review, Trieste 1998/06/29', 'muon, cosmic radiation', 'cosmic radiation, flux', 'cosmic radiation, secondary radiation', 'spatial distribution', 'time variation', 'muon, momentum spectrum', 'muon+ muon-, ratio', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002052'],"['We present a review of atmospheric and underground muon flux measurements.The relevance of these data for the atmospheric neutrino flux computation isemphasized. Possible sources of systematic errors in the measurements arediscussed, focusing on the sea level muon data. Underground muon data are alsoreported.']",['2000-02-22']
910,['eng'],"['Sioli, M']",['Underground Muon Physics with the MACRO experiment'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1999/05/17', 'muon, cosmic radiation', 'multiplicity, spectra', 'muon, spatial distribution', 'cosmic radiation, primary', 'decoherence', 'track data analysis, cluster', 'numerical calculations, Monte Carlo', 'deep underground detector, MACRO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002051'],"['Underground muon events detected by the MACRO experiment at Gran Sasso havebeen studied for different purposes. The studies include the vertical muonintensity measurement, multiplicity distribution, lateral and angular muondistribution and searches for substructures inside muon bundles. These analyseshave contributed to bring new insights in cosmic ray physics, in particular inthe framework of primary cosmic ray composition studies. Moreover, thisactivity allows the testing and tuning of Monte Carlo simulations, inparticular for aspects associated with models of hadronic interactions and muonpropagation through the rock.']",['2000-02-22']
911,['eng'],"['Wang, Y F', 'Miller, L', 'Gratta, Giorgio']",['A New Approach to Background Subtraction in Low-Energy Neutrino Experiments'],['Detectors and Experimental Techniques'],"['neutrino, particle identification', 'n, background', 'neutrino, oscillation', 'fission, particle source', 'muon- nucleus, nuclear reaction', 'n, electroproduction']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002050'],['We discuss a new method to extract neutrino signals in low energyexperiments. In this scheme the symmetric nature of most backgrounds allows fordirect cancellation from data. The application of this technique to the PaloVerde reactor neutrino oscillation experiment allowed us to reduce themeasurement errors on the anti-neutrino flux from $\\sim 20$to $\\sim 10$Weexpect this method to substantially improve the data quality in future lowbackground experiments such as KamLAND and LENS.'],['2000-02-22']
912,['eng'],"['Alcaraz, J', 'Alvisi, D', 'Alpat, B', 'Ambrosi, G', 'Anderhub, H', 'Ao, L', 'Arefev, A', 'Azzarello, P', 'Babucci, E', 'Baldini, L', 'Basile, M', 'Barancourt, D', 'Barão, F', 'Barbier, G', 'Barreira, G', 'Battiston, R', 'Becker, R', 'Becker, U', 'Bellagamba, L', 'Béné, P', 'Berdugo, J', 'Berges, P', 'Bertucci, B', 'Biland, A', 'Bizzaglia, S', 'Blasko, S', 'Bölla, G', 'Boschini, M', 'Bourquin, Maurice', 'Bruni, G', 'Buénerd, M', 'Burger, J D', 'Burger, W J', 'Cai, X D', 'Cavalletti, R', 'Camps, C', 'Cannarsa, P', 'Capell, M', 'Casadei, D', 'Casaus, J', 'Castellini, G', 'Chang, Y H', 'Chen, H F', 'Chen, H S', 'Chen, Z G', 'Chernoplekov, N A', 'Chiarini, A', 'Tzi Hong Chiueh', 'Chuang, Y L', 'Cindolo, F', 'Commichau, V', 'Contin, A', 'Cotta-Ramusino, A', 'Crespo, P', 'Cristinziani, M', 'Da Cunha, J P', 'Dai, T S', 'Deus, J D', 'Dinu, N', 'Djambazov, L', ""D'Antone, I"", 'Dong, Z R', 'Emonet, P', 'Engelberg, J', 'Eppling, F J', 'Eronen, T', 'Esposito, G', 'Extermann, Pierre', 'Favier, J', 'Feng, C C', 'Fiandrini, E', 'Finelli, F', 'Fisher, P H', 'Flaminio, R', 'Flügge, G', 'Fouque, N', 'Galaktionov, Yu', 'Gervasi, M', 'Giusti, P', 'Grandi, D', 'Gu, W Q', 'Hangarter, K', 'Hasan, A', 'Hermel, V', 'Hofer, H', 'Huang, M A', 'Hungerford, W', 'Ionica, M', 'Ionica, R', 'Jongmanns, M', 'Karlamaa, K', 'Karpinski, W', 'Kenney, G', 'Kenny, J', 'Kim, W', 'Klimentov, A', 'Kossakowski, R', 'Koutsenko, V F', 'Laborie, G', 'Laitinen, T', 'Lamanna, G', 'Laurenti, G', 'Lebedev, A', 'Lee, S C', 'Levi, G', 'Levchenko, P M', 'Liu, C L', 'Liu Hong Tao', 'Lolli, M', 'Lopes, I', 'Lu, G', 'Lü, Y S', 'Lübelsmeyer, K', 'Luckey, D', 'Lustermann, W', 'Maña, C', 'Margotti, A', 'Massera, F', 'Mayet, F', 'McNeil, R R', 'Meillon, B', 'Menichelli, M', 'Mezzanotte, F', 'Mezzenga, R', 'Mihul, A', 'Molinari, G', 'Mourao, A', 'Mujunen, A', 'Palmonari, F', 'Pancaldi, G', 'Papi, A', 'Park, I H', 'Pauluzzi, M', 'Pauss, Felicitas', 'Perrin, E', 'Pesci, A', 'Pevsner, A', 'Pilastrini, R', 'Pimenta, M', 'Plyaskin, V', 'Pozhidaev, V', 'Postema, H', 'Postolache, V', 'Prati, E', 'Produit, N', 'Rancoita, P G', 'Rapin, D', 'Raupach, F', 'Recupero, S', 'Ren, D', 'Ren, Z', 'Ribordy, M', 'Richeux, J P', 'Riihonen, E', 'Ritakari, J', 'Röser, U', 'Roissin, C', 'Sagdeev, R', 'Santos, D', 'Sartorelli, G', 'Schultz von Dratzig, A', 'Schwering, G', 'Seo, E S', 'Shoutko, V', 'Shoumilov, E', 'Siedling, R', 'Son, D', 'Song, T', 'Steuer, M', 'Sun, G S', 'Suter, H', 'Tang, X W', 'Ting, S C C', 'Ting, S M', 'Tornikoski, M', 'Torromeo, G', 'Torsti, J', 'Trümper, J E', 'Ulbricht, J', 'Urpo, S', 'Usoskin, I', 'Valtonen, E', 'Van den Hirtz, J', 'Velcea, F', 'Velikhov, E P', 'Verlaat, B', 'Vetlitskii, I', 'Vezzu, F', 'Vialle, J P', 'Viertel, Gert M', 'Vite, D', 'Von Gunten, H P', 'Waldmeier-Wicki, S', 'Wallraff, W', 'Wang, B C', 'Wang, J Z', 'Wang, Y H', 'Wiik, K', 'Williams, C', 'Wu, S X', 'Xia, P C', 'Yan, J L', 'Yan Lu Guang', 'Yang, C G', 'Yang, M', 'Ye Shu Wei', 'Yeh, P', 'Xu, Z Z', 'Zhang, H Y', 'Zhang, Z P', 'Zhao, D X', 'Zhu, G Y', 'Zhu, W Z', 'Zhuang, H L', 'Zichichi, Antonino']",['Protons in near earth orbit'],['Particle Physics - Experimental Results'],"['p, cosmic radiation', 'cosmic radiation, energy spectrum', 'parametrization', 'cosmic radiation, flux', 'spatial distribution', 'magnetic spectrometer, satellite', 'experimental results', 'tables']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002049'],['The proton spectrum in the kinetic energy range 0.1 to 200 GeV was measuredby the Alpha Magnetic Spectrometer (AMS) during space shuttle flight STS-91 atan altitude of 380 km. Above the geomagnetic cutoff the observed spectrum isparameterized by a power law. Below the geomagnetic cutoff a substantial secondspectrum was observed concentrated at equatorial latitudes with a flux ~ 70m^-2 sec^-1 sr^-1. Most of these second spectrum protons follow a complicatedtrajectory and originate from a restricted geographic region.'],['2000-02-22']
913,['eng'],"['Uvarov, V']","[""Production Properties of the Orbitally Excited Mesons $f_{0}(980)$, $f_{2}(1270)$, $K^{*0}_{2}(1430)$ and $f'_{2}(1525)$ in $Z^{0}$ Hadronic Decays""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'meson resonance, production', 'meson resonance, neutral particle', 'rho(770)0', 'f0(975)', 'f2(1270)', 'K*2(1430)', 'f2(1525)', 'yield, ratio', 'channel cross section', 'differential cross section, x-dependence', 'model, thermodynamical', 'experimental results', 'magnetic detector, DELPHI', 'CERN LEP Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011092'],"[""DELPHI results are presented on the inclusive production of the neutral mesons rho^0, f_0(980), f_2(1270), K^*0_2(1430) and f'_2(1525) in hadronic Z^0 decays. They are based on about 2 million multihadronic events collected in 1994 and 1995, using the particle identification capabilities of the DELPHI Ring Imaging Cherenkov detectors and measured ionization losses in the Time Projection Chamber. The total production rates per hadronic Z^0 decay have been determined to be: 1.19 +/- 0.10 for rho^0; 0.164 +/- 0.021 for f_0(980); 0.214 +/- 0.038 for f_2(1270); 0.073 +/- 0.023 for K^*0_2(1430); and 0.012 +/- 0.006 for f'_2(1525). The total production rates for all mesons and differential cross-sections for the rho^0, f_0(980) and f_2(1270) are compared with the results of other LEP experiments and with models.""]",['2000-11-29']
914,['eng'],"['Pitzl, D']",['The H1 Silicon Vertex Detector'],['Detectors and Experimental Techniques'],"['semiconductor detector, vertex', 'semiconductor detector, readout', 'optics, fibre', 'integrated circuit', 'signal processing', 'alignment', 'efficiency', 'resolution, impact parameter', 'performance', 'magnetic detector, H1', 'DESY HERA Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002044'],"['The design, construction and performance of the H1 silicon vertex detector isdescribed. It consists of two cylindrical layers of double sided, double metalsilicon sensors read out by a custom designed analog pipeline chip. The analogsignals are transmitted by optical fibers to a custom designed ADC board andare reduced on PowerPC processors. Details of the design and construction aregiven and performance figures from the first data taking periods are presented.']",['2000-02-16']
915,['eng'],"['Giunti, C']",['Enhancing the physical significance of Frequentist confidence intervals'],['Detectors and Experimental Techniques'],"['talk, Geneva 2000/01/17', 'statistical analysis']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002042'],"['It is shown that all the Frequentist methods are equivalent from astatistical point of view, but the physical significance of the confidenceintervals depends on the method. The Bayesian Ordering method is presented andconfronted with the Unified Approach in the case of a Poisson process withbackground. Some criticisms to both methods are answered. It is also arguedthat a general Frequentist method is not needed.']",['2000-02-16']
916,['eng'],"['Akopov, N Z', 'Apyan, A B', 'Darbinian, S M']",['Use of Crystals for High Energy Photon Beam Linear Polarization Conversion into Circular'],['Accelerators and Storage Rings'],"['photon, particle source', 'photon, polarized beam', 'carbon, crystal', 'silicon, crystal', 'germanium, crystal', 'optics, dispersion', 'photon nucleus, nuclear reaction', 'nucleon, spin']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002041'],"['The possibility to convert the photon beam linear polarization into circularone at photon energies of hundreds GeV with the use of crystals is considered.The energy and orientation dependencies of refractive indexes are investigatedin case of diamond, silicon and germanium crystal targets. To maximize thevalues for figure of merit, the corresponding crystal optimal orientationangles and thickness are found. The degree of circular polarization andintensity of photon beam are estimated and possibility of experimentalrealization is discussed.']",['2000-02-16']
917,['eng'],"['Battaglia, M']",['Study of $b \\to u l \\nu$ Decays with an Inclusive Generator'],['Particle Physics - Experimental Results'],"['quark, beauty', 'quark, semileptonic decay', 'B, semileptonic decay', 'recoil, hadronic', 'mass spectrum, recoil', 'Kobayashi-Maskawa angle', 'kinematics', 'hadron, multiplicity', 'numerical calculations, Monte Carlo', 'proposed experiment', 'beauty --> up lepton antineutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002040'],['A generator for inclusive b -> u l nu decays has been developed. Differentprescriptions have been applied to describe the kinematics of the b-quarkinside the hadron and the generation of the hadronic final states. Results arepresented with particular attention to the invariant mass of the hadronicsystem recoiling against the lepton and its resonance decomposition. Thesestudies are of special relevance for the extraction of Vub from semileptonic Bdecays at LEP and at B factories.'],['2000-02-15']
918,['eng'],"['Nakada, Tatsuya']",['Physics of CP Violation and Rare Decays'],['Particle Physics - Experimental Results'],"['lectures, Cargese 1999/07/26', 'violation, CP', 'particle, antiparticle', 'K0 anti-K0, oscillation', 'B0 anti-B0, oscillation', 'B/s0 anti-B/s0, oscillation', 'K0, decay modes', 'K0(L)', 'K0(S)', 'B0, hadronic decay', 'electroweak interaction', 'Kobayashi-Maskawa angle', 'time dependence', 'Feynman graph, penguin', 'interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002039'],"['Lectures note for Cargese 99 Summer School Particle Physics: Ideas and RecentDevelopment NATO Advanced Institute, Corsica, July 26-August 7, 1999']",['2002-10-24']
919,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Abbiendi, G', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Coppola, N', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Brock, I', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Hartmann, H', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Foster, B', 'Heath, G P', 'Heath, H F', 'McFall, J D', 'Piccioni, D', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sacchi, R', 'Sampson, S', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Burgard, C', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hasell, D', 'Hebbel, K', 'Johnson, K F', 'Kasemann, M', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Lindemann, L', 'Löhr, B', 'Martínez, M', 'Milite, M', 'Monteiro, T', 'Moritz, M', 'Notz, D', 'Pelucchi, F', 'Petrucci, M C', 'Rohde, M', 'Saull, P R B', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Tassi, E', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'Grabosch, H J', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'Votano, L', 'Bamberger, Andreas', 'Benen, A', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Doyle, A T', 'Lee, S W', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Dannheim, D', 'Garfagnini, A', 'Gialas, I', 'Gladilin, L K', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Poelz, G', 'Zetsche, F', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Mallik, U', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Ahn, S H', 'Lee, S B', 'Park, S K', 'Lim, H', 'Park, I H', 'Son, D', 'Barreiro, F', 'García, G', 'Glasman, C', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Barbi, M S', 'Corriveau, F', 'Hanna, D S', 'Ochs, A', 'Padhi, S', 'Riveline, M', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Bashkirov, V', 'Dolgoshein, B A', 'Dementev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Shcheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Acosta, D', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dosselli, U', 'Dusini, S', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sabetfakhri, A', 'Simmons, D', 'Butterworth, J M', 'Catterall, C D', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Pawlak, R', 'Smalska, B', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Adamus, M', 'Gadaj, T', 'Deppe, O', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Badgett, W F', 'Chapin, D', 'Cross, R', 'Foudas, C', 'Mattingly, S E', 'Reeder, D D', 'Smith, W H', 'Vaiciulis, A W', 'Wildschek, T', 'Wodarczyk, M', 'Deshpande, A A', 'Dhawan, S K', 'Hughes, V W', 'Bhadra, S', 'Catterall, C D', 'Cole, J E', 'Frisken, W R', 'Hall-Wilton, R', 'Khakzad, M', 'Menary, S R', 'Schmidke, W B']",['Search for Resonances Decaying to $e^{+}$-jet in $e^{+}p$ Interactions at HERA'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, deep inelastic scattering', 'jet, electroproduction', 'mass spectrum, (jet positron)', 'resonance, search for', 'angular distribution', 'channel cross section, branching ratio', 'upper limit', 'leptoquark, coupling', 'squark, coupling', 'mass, dependence', 'R parity, violation', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> jet positron anything', 'approx. 300 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002038', 'http://www-zeus.desy.de/~schlenst/conf/osaka_paper.html']","['The e^+ jet invariant mass spectrum produced in the reaction e^+ p -> e^+ Xhas been studied at a center-of-mass energy of 300 GeV. The data were collectedusing the ZEUS detector operating at the HERA collider, and correspond to anintegrated luminosity of 47.7 pb^{-1}. The observed mass spectrum is in goodagreement with Standard Model expectations up to an e^+ jet mass of 210 GeV.Above this mass, some excess is seen. The angular distribution of these eventsis typical of high-Q^2 neutral current events and does not give convincingevidence for the presence of a narrow scalar or vector state. Limits arepresented on the product of cross section and branching ratio for such a stateand are interpreted as limits on leptoquark or R-parity-violating squarkproduction. Specific leptoquark types are ruled out at 95onfidence level forcoupling strength lambda=0.3 for masses between 150 and 280 GeV.']",['2000-02-15']
920,['eng'],"['Bosman, M', 'Kulchitskii, Yu A', 'Nessi, M']",['Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter'],['Detectors and Experimental Techniques'],"['calorimeter, energy resolution', 'scintillation counter', 'pi, beam', 'electronics, background', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002033'],"['The intrinsic performance of the ATLAS barrel and extended barrelcalorimeters for the measurement of charged pions is presented. Pion energyscans (E = 20, 50, 200, 400 and 1000 GeV) at two pseudo-rapidity points ($\\eta$= 0.3 and 1.3) and pseudorapidity scans ($-0.2 < \\eta < 1.8$) with pions ofconstant transverse energy ($E_T = 20$ and 50 GeV) are analysed. A simpleapproach, that accounts in first order for non-compensation and dead materialeffects, is used for the pion energy reconstruction. The intrinsic performancesof the calorimeter are studied: resolution, linearity, effect of dead material,tails in the energy distribution. The effect of electronic noise, cell energycuts and restricted cone size are investigated.']",['2000-02-15']
921,['eng'],"['Ukegawa, F']",['Spectroscopy and lifetime of bottom and charm hadrons'],['Particle Physics - Experimental Results'],"['review, Taipei 1999/12/03', 'hadron hadron, interaction', 'electron positron, annihilation', 'quark, charm', 'quark, beauty', 'quark, pair production', 'hadron spectroscopy', 'charmed particle, lifetime', 'beautiful particle, lifetime', 'charmed meson, mass spectrum', 'beautiful meson, mass spectrum', 'charmed baryon', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002031'],['We review recent experimental results on spectroscopy and lifetime of bottomand charm hadrons.'],['2000-02-15']
922,['eng'],"['Bertolucci, S']",['A Status Report of KLOE at DAFNE'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'K, pair production', 'K0, hadronic decay', 'K0(L)', 'K0(S)', 'CP, violation', 'pi, pair production', 'luminosity', 'magnetic field, effect', 'magnetic detector, KLOE', 'performance', 'Frascati Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002030'],"[""The major goal of the KLOE experiment is to measure Re(epsilon' /epsilon) inthe kkbar system, with a precision of 10^{-4},both via the traditional doubleratio method and quantum interferometry. The experiment has started taking dataat DAFNE, the phi-factory built at the Frascati National Laboratory (LNF) ofINFN in Italy, beginning in April 1999. In the early phase of the commissioning(before KLOE roll-in), DAFNE has achieved multi bunch luminosities of 10^{31}cm^{-2} s^{-1} with 13 bunches and 200 mA. Detailed studies are presentlyunderway to compensate for the large perturbation brought in by the KLOEsolenoid, which has caused a drastic decrease of the peak luminosity.Nevertheless the first collected data, corresponding to an integral luminosityof 220 nb^{-1}, show that KLOE is performing to the design specifications inall its hardware and software components.""]",['2000-02-11']
923,['eng'],"['Ambrosio, M', 'Antolini, R', 'Auriemma, G', 'Bakari, D', 'Baldini, A', 'Barbarino, G C', 'Barish, B C', 'Battistoni, G', 'Bellotti, R', 'Bemporad, C', 'Bernardini, P', 'Bilokon, H', 'Bisi, V', 'Bloise, C', 'Bower, C', 'Brigida, M', 'Bussino, S', 'Cafagna, F', 'Calicchio, M', 'Campana, D', 'Carboni, M', 'Cecchini, S', 'Cei, F', 'Chiarella, V', 'Choudhary, B C', 'Coutu, S', 'De Cataldo, G', 'Dekhissi, H', 'De Marzo, C', 'De Mitri, I', 'Derkaoui, J E', 'De Vincenzi, M', 'Di Credico, A', 'Erriquez, O', 'Favuzzi, C', 'Forti, C', 'Fusco, P', 'Giacomelli, Giorgio', 'Giannini, G', 'Giglietto, N', 'Giorgini, M', 'Grassi, M', 'Gray, L', 'Grillo, A', 'Guarino, F', 'Gustavino, C', 'Habig, A', 'Hanson, K', 'Heinz, R', 'Iarocci, Enzo', 'Katsavounidis, E', 'Katsavounidis, I', 'Kearns, E T', 'Kim, H', 'Kyriazopoulou, S', 'Lamanna, E', 'Lane, C', 'Levin, D S', 'Lipari, P', 'Longley, N P', 'Longo, M J', 'Loparco, F', 'Maaroufi, F', 'Mancarella, G', 'Mandrioli, G', 'Margiotta, A', 'Marini, A', 'Martello, D', 'Marzari-Chiesa, A', 'Mazziotta, M N', 'Michael, D G', 'Mikheyev, S P', 'Miller, L', 'Monacelli, P', 'Montaruli, T', 'Monteno, M', 'Mufson, S L', 'Musser, J', 'Nicolo, D', 'Nolty, R', 'Orth, C', 'Okada, C', 'Osteria, G', 'Ouchrif, M', 'Palamara, O', 'Patera, V', 'Patrizii, L', 'Pazzi, R', 'Peck, C W', 'Perrone, L', 'Petrera, S', 'Pistilli, P', 'Popa, V', 'Rainó, A', 'Reynoldson, J', 'Ronga, F', 'Satriano, C', 'Satta, L', 'Scapparone, E', 'Scholberg, K', 'Sciubba, A', 'Serra, P', 'Sioli, M', 'Sitta, M', 'Spinelli, P', 'Spinetti, M', 'Spurio, M', 'Steinberg, R', 'Stone, J L', 'Sulak, Lawrence R', 'Surdo, A', 'Tarle, G', 'Togo, V', 'Vakili, M', 'Vilela, E', 'Walter, C W', 'Webb, R']",['A Search for Lightly Ionizing Particles with the MACRO Detector'],['Particle Physics - Experimental Results'],"['new particle, search for', 'charge, fractional', 'flux, upper limit', 'track data analysis', 'deep underground detector, MACRO', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002029'],['A search for lightly ionizing particles has been performed with the MACROdetector. This search was sensitive to particles with charges between$\\fractional{5}'],['2000-02-11']
924,['eng'],"['Astone, P', 'Pizzella, G']",['Upper Limits in the Case That Zero Events are Observed'],['Particle Physics - Experimental Results'],"['talk, Geneva 2000/01/17', 'statistical analysis', 'upper limit']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002028'],"[""We compare the ``unified approach'' for the estimation of upper limits withan approach based on the Bayes theory, in the special case that no events areobserved. The ``unified approach'' predicts, in this case, an upper limit thatdecreases with the increase in the expected level of background. This seemsabsurd. On the other hand, the Bayesian approach leads to a result which isbackground independent. An explanation of the Bayesian result is presented,together with suggested reasons for the paradoxical result of the ``unifiedapproach''.""]",['2000-02-11']
925,['eng'],"['Zhao, Z G']",['R-values in Low Energy $e^{+}e^{-}$ Annihilation'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'cross section, hadronic', 'energy dependence', 'hadron, multiple production', 'pi, form factor', 'rho(770)', 'omega(783)', 'K', 'four-pi-detector, SND', 'magnetic detector, CMD', 'Novosibirsk Stor2', 'magnetic spectrometer, BES', 'Beijing Stor', 'bibliography', '0.3-5.0 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002025'],['This presentation briefly summarizes the recent measurements of R-values inlow energy e^+e^- annihilation. The new experiments aimed at reducing theuncertainties in R-values and performed with the upgraded Beijing Spectrometer(BESII) at Beijing Electron Positron Collider (BEPC) in Beijing and with CMD-2and SND at VEEP-2M in Novosibirsk are reviewed and discussed.'],['2000-02-09']
926,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']","['Measurements of $R_{b}$, $A_{FB}^{b}$ and $A_{FB}^{c}$ in $e^{+}e^{-}$ Collisions at 130-189 GeV']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, beauty', 'quark, charm', 'quark, pair production', 'channel cross section, ratio', 'angular distribution, asymmetry', 'particle identification, flavor', 'charge', 'quark, semileptonic decay', 'D*(2010), hadronic decay', 'particle identification, (pi lepton)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '130-189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002024'],"['The cross-section ratio Rb=sigma(e+e- to b-antib)/sigma(e+e- to q-antiq) andthe bottom and charm forward-backward asymmetries AFB^b and AFB^c are measuredusing event samples collected by the OPAL detector at centre-of-mass energiesbetween 130 and 189 GeV. Events with bottom quark production are selected witha secondary vertex tag, and a hemisphere charge algorithm is used to extractAFB^b. In addition, the bottom and charm asymmetries are measured using leptonsfrom semileptonic decays of heavy hadrons and pions from D*+ to D0pi+ decays.The results are in agreement with the Standard Model predictions.']",['2000-02-09']
927,['eng'],"['Cecchini, S', ""D'Antone, I"", 'Esposti, L D', 'Giacomelli, Giorgio', 'Guerra, M', 'Lax, I', 'Mandrioli, G', 'Parretta, A', 'Sarno, A', 'Schioppo, R', 'Sorel, M', 'Spurio, M']",['Solar panels as air Cherenkov detectors for extremely high energy cosmic rays'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1999/05/17', 'cosmic radiation', 'Cherenkov counter, readout', 'semiconductor, optical', 'efficiency']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002023'],['Increasing interest towards the observation of the highest energy cosmic rayshas motivated the development of new detection techniques. The properties ofthe Cherenkov photon pulse emitted in the atmosphere by these very rareparticles indicate low-cost semiconductor detectors as good candidates fortheir optical read-out. The aim of this paper is to evaluate the viability of solar panels for thispurpose. The experimental framework resulting from measurements performed withsuitably-designed solar cells and large conventional photovoltaic areas ispresented. A discussion on the obtained and achievable sensitivities follows.'],['2000-02-08']
928,['eng'],"['Appel, J A']",['Charm Results on CP Violation and Mixing'],['Particle Physics - Experimental Results'],"['review, Frascati 1999/11/16', 'charmed meson, electroproduction', 'charmed meson, hadroproduction', 'charmed meson, photoproduction', 'CP, violation', 'D0 anti-D0, interference', 'D0, hadronic decay', 'D0, semileptonic decay', 'D0, mass difference', 'lifetime, difference', 'D+, hadronic decay', 'decay, asymmetry', 'Dalitz plot', 'experimental results', 'CERN LEP Stor', 'Cornell CESR Stor', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002022'],"['The most recent results on CP violation and mixing in the charm system arereviewed as a guide to the future. While no surprising results are reported sofar, charm provides a unique window to physics beyond the Standard Model. Theresults reported here come from four sources: ALEPH at LEP, E791 and FOCUS/E831at Fermilab, and CLEO II.V at CESR. Results beyond these sources may beexpected as a byproduct of B-motivated experiments.']",['2000-02-08']
929,['eng'],"['Dima, M']",['Analytical and Numerical Flash-Algorithms for Track Fits'],['Detectors and Experimental Techniques'],"['semiconductor detector, pixel', 'track data analysis', 'statistical analysis', 'tracks, energy loss', 'multiple scattering', 'alignment', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002021'],"['Generalising the methods used in the analysis of ATLAS Pixel Detectors test-beam data, line and helix fit flash-algorithmsbased on semi/analytical methods are presented. Routines based on this approach are over 3000 times faster than the traditional iterative procedures, yielding a 60fold increase in alignment resolution for the same amount of CPU time.']",['2000-02-08']
930,['eng'],"['Giunti, C', 'Laveder, M']",['The statistical and physical significance of confidence intervals'],['Particle Physics - Experimental Results'],['statistical analysis'],['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002020'],"['It is shown that the necessity to choose a specific Frequentist method, amongseveral available, for the analysis of experimental data does not introduce anydegree of subjectivity from a statistical point of view. However, the physicalsignificance of confidence intervals obtained with different methods isdifferent. Considering the case of a Poisson process with known background, weshow that the expectation value (""exclusion potential"") and the standarddeviation of the upper limit in the absence of a signal can help to decidewhich is the most appropriate method from a physical point of view. In theframework of both Frequentist and Bayesian statistical theories, we also definethe ""Pull"" of a null result, expressing the reliability of an experimentalupper limit, the ""upper and lower detection functions"", that give informationon the possible outcome of an experiment if there is a signal, and the""sensitivity"", that quantifies the capability of an experiment to reveal thesignal that is searched for at the given confidence level.']",['2000-02-08']
931,['eng'],"['Asratyan, A E', 'Davidenko, G V', 'Dolgolenko, A G', 'Kaftanov, V S', 'Kubantsev, M A', 'Verebryusov, V S']",['Emulsion Chamber with Big Radiation Length for Detecting Neutrino Oscillations'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'tau, decay modes', 'magnetic spectrometer', 'nuclear emulsion, plastics', 'carbon, target', 'copper, target', 'deep underground detector, Gran Sasso', 'CERN SPS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002019'],"['A conceptual scheme of a hybrid-emulsion spectrometer for investigatingvarious channels of neutrino oscillations is proposed. The design emphasizesdetection of $\\tau$ leptons by detached vertices, reliable identification ofelectrons, and good spectrometry for all charged particles and photons. Adistributed target is formed by layers of low-Z material,emulsion-plastic-emulsion sheets, and air gaps in which $\\tau$ decays aredetected. The tracks of charged secondaries, including electrons, aremomentum-analyzed by curvature in magnetic field using hits in successive thinlayers of emulsion. The $\\tau$ leptons are efficiently detected in all majordecay channels, including \\xedec. Performance of a model spectrometer, thatcontains 3 tons of nuclear emulsion and 20 tons of passive material, isestimated for different experimental environments. When irradiated by the$\\nu_\\mu$ beam of a proton accelerator over a medium baseline of $<L/E_\\nu >\\sim 1$ km/GeV, the spectrometer will efficiently detect either the \\omutau and\\omue transitions in the mass-difference region of $\\Delta m^2 \\sim 1$ eV$^2$,as suggested by the results of LSND. When exposed to the neutrino beam of amuon storage ring over a long baseline of $<L/E_\\nu > \\sim$ 10-20 km/GeV, themodel detector will efficiently probe the entire pattern of neutrinooscillations in the region $\\Delta m^2 \\sim 10^{-2}-10^{-3}$ eV$^2$, assuggested by the data on atmospheric neutrinos.']",['2000-02-08']
932,['eng'],"['Bahcall, J N']",['Solar Neutrinos'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1999/09/23', 'neutrino, solar', 'neutrino, flux', 'model, solar', 'neutrino, energy spectrum', 'neutrino, oscillation', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002018'],['I summarize the current state of solar neutrino research and then give myanswer to the question: What should we do next?'],['2000-02-08']
933,['eng'],"['Ackerstaff, K', 'Airapetian, A', 'Akopov, N Z', 'Amarian, M', 'Aschenauer, E C', 'Avakian, H', 'Avakian, R', 'Avetisian, A', 'Bains, B', 'Beckmann, M', 'Belostotskii, S', 'Belz, J E', 'Benisch, T', 'Bernreuther, S', 'Bianchi, N', 'Blanchard, S', 'Blouw, J', 'Böttcher, H', 'Borisov, A', 'Brack, J', 'Braun, B', 'Bray, B', 'Brückner, W', 'Brüll, A', 'Bruins, E E W', 'Bulten, H J', 'Capitani, G P', 'Carter, P', 'Cisbani, E', 'Court, G R', 'Delheij, P P J', 'De Sanctis, E', 'De Schepper, D', 'Devitsin, E G', 'De Witt-Huberts, P K A', 'Düren, M', 'Dvoredsky, A P', 'Elbakian, G M', 'Emerson, J', 'Fantoni, A', 'Feshchenko, A', 'Ferstl, M', 'Fiedler, K', 'Filippone, B W', 'Fischer, H', 'Fox, B', 'Franz, J', 'Frullani, S', 'Funk, M A', 'Gärber, Y', 'Gagunashvili, N D', 'Galumian, P I', 'Gao, H', 'Garibaldi, F', 'Gavrilov, G', 'Geiger, P', 'Karibian, V', 'Golendukhin, A', 'Graw, G', 'Grebenyuk, O', 'Green, P W', 'Greeniaus, L G', 'Grosshauser, C', 'Gute, A', 'Gyurjyan, V', 'Haas, J P', 'Haeberli, W', 'Häusser, O', 'Hansen, J O', 'Hasch, D', 'Henderson, R', 'Henkes, T', 'Hertenberger, R', 'Holler, Y', 'Holt, R J', 'Ihssen, H', 'Iodice, M', 'Izotov, A A', 'Jackson, H E', 'Jgoun, A', 'Jones, C', 'Kaiser, R', 'Kinney, E R', 'Kirsch, M', 'Kiselev, A', 'Kitching, P', 'Königsmann, Kay C', 'Kolstein, M', 'Kolster, H', 'Korsch, W', 'Kozlov, V', 'Kramer, L H', 'Krause, B', 'Krivokhizhin, V G', 'Kückes, M', 'Kyle, G S', 'Lachnit, W A', 'Lorenzon, W', 'Lung, A', 'Makins, N C R', 'Manaenkov, S I', 'Martens, F K', 'Martin, J W', 'Mateos, A', 'McIlhany, K', 'McKeown, R D', 'Meissner, F', 'Menden, F', 'Mercer, D', 'Metz, A', 'Meyners, N', 'Miklukho, O', 'Miller, C A', 'Miller, M A', 'Milner, R', 'Mitsyn, V', 'Most, A', 'Mozzetti, R', 'Muccifora, V', 'Nagaitsev, A P', 'Naryshkin, Yu', 'Nathan, A M', 'Neunreither, F', 'Niczyporuk, J M', 'Nowak, W D', 'Nupieri, M', 'Oelwein, P', 'Ogami, H', ""O'Neill, T G"", 'Openshaw, R', 'Ouyang, J', 'Pate, S F', 'Pitt, M L', 'Poolman, H R', 'Potashov, S Yu', 'Potterveld, D H', 'Rakness, G', 'Redwine, R P', 'Reolon, A R', 'Ristinen, R', 'Rith, K', 'Roper, G', 'Roloff, H O', 'Rossi, P', 'Ruh, M', 'Ryckbosch, D', 'Sakemi, Y', 'Savin, I A', 'Schüler, K P', 'Schwind, A', 'Shibata, T A', 'Shin, T', 'Simon, A', 'Sinram, K', 'Smythe, W R', 'Sowinski, J', 'Spengos, M', 'Steffens, E', 'Stenger, J', 'Stewart, J', 'Stock, F', 'Stösslein, U', 'Sutter, M F', 'Tallini, H A', 'Taroian, S P', 'Terkulov, A R', 'Thiessen, D M', 'Tipton, B', 'Trudel, A', 'Tytgat, M', 'Urciuoli, G M', 'Van den Brand, J F J', 'van der Steenhoven, G', 'Van de Vyver, R', 'Vetterli, M C', 'Vincter, M G', 'Volk, E', 'Wander, W', 'Welch, T P', 'Williamson, S E', 'Wise, T', 'Zapfe, K', 'Zohrabyan, H G']",['Measurement of Angular Distributions and $R = \\sigma_{L}/\\sigma_{T}$ in Diffractive Electroproduction of $\\rho^{0}$ Mesons'],['Particle Physics - Experimental Results'],"['positron nucleus, inclusive reaction', 'positron, polarized beam', 'helium, nuclide', 'target, internal', 'rho(770)0, electroproduction', 'rho(770)0, hadronic decay', 'diffraction', 'coherent interaction', 'incoherent interaction', 'mass spectrum, (pi+ pi-)', 'spin, density matrix', 'helicity, conservation law', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'energy dependence', 'momentum transfer, dependence', 'angular distribution', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'positron helium-3 --> rho(770)0 anything', 'rho(770)0 --> pi+ pi-', '27.5 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002016'],"['Production and decay angular distributions were extracted from measurementsof exclusive electroproduction of the rho^0(770) meson over a range in thevirtual photon negative four-momentum squared 0.5< Q^2 <4 GeV^2 and thephoton-nucleon invariant mass range 3.8< W <6.5 GeV. The experiment wasperformed with the HERMES spectrometer, using a longitudinally polarizedpositron beam and a ^3He gas target internal to the HERA e^{+-} storage ring.The event sample combines rho^0 mesons produced incoherently off individualnucleons and coherently off the nucleus as a whole. The distributions in oneproduction angle and two angles describing the rho^0 -> pi+ pi- decay yieldedmeasurements of eight elements of the spin-density matrix, including one thathad not been measured before. The results are consistent with the dominance ofhelicity-conserving amplitudes and natural parity exchange. The improvedprecision achieved at 4< W <7 GeV, in combination with other data at W>7 GeV,reveals evidence for an energy dependence in the ratio R of the longitudinal totransverse cross sections at constant Q^2.']",['2000-02-08']
934,['eng'],"['Adler, Stephen Louis', 'Atiya, M S', 'Chiang, I H', 'Diwan, M V', 'Frank, J S', 'Haggerty, J S', 'Jain, V', 'Kettell, S H', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'Ng, C', 'Strand, R C', 'Witzig, C', 'Kazumori, M', 'Komatsubara, T K', 'Kuriki, M', 'Muramatsu, N', 'Otomo, A', 'Sugimoto, S', 'Inagaki, T', 'Kabe, S', 'Kobayashi, M', 'Kuno, Y', 'Sato, T', 'Shinkawa, T', 'Yoshimura, Y', 'Kishi, Y', 'Nakano, T', 'Sasaki, T', 'Ardebili, M', 'Bazarko, A O', 'Convery, M R', 'Ito, M M', 'Marlow, D R', 'McPherson, R A', 'Meyers, P D', 'Shoemaker, F C', 'Smith, A J S', 'Stone, J R', 'Aoki, M', 'Bergbusch, P C', 'Blackmore, E W', 'Bryman, D A', 'Konaka, A', 'MacDonald, J A', 'Mildenberger, J L', 'Numao, T', 'Padley, P', 'Poutissou, J M', 'Poutissou, R', 'Redlinger, G', 'Kitching, P', 'Soluk, R']",['Further Search for the Decay $K^{+} \\to \\pi^{+}\\nu\\overline{\\nu}$'],['Particle Physics - Experimental Results'],"['K+, rare decay', 'neutrino, pair production', 'pi+, leptonic decay', 'K+, branching ratio', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002015'],['A search for additional evidence for the rare kaon decay K^+ --> pi^+ nunubar has been made with a new data set comparable in sensitivity to theprevious exposure that produced a single event.'],['2000-02-08']
935,['eng'],"['Coan, T E']",['The Cleo III Upgrade'],['Particle Physics - Experimental Results'],"['talk, Hamamatsu 1999/11/15', 'luminosity, upgrade', 'RF system, superconducting', 'beam focusing, colliding beams', 'quadrupole lens, ferromagnet', 'quadrupole lens, superconducting', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'lithium, fluorine', 'photoelectron, readout', 'proportional chamber, wire', 'tracks', 'drift chamber, wire', 'helium, organic compounds', 'semiconductor detector, vertex', 'semiconductor detector, microstrip', 'trigger', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002014'],"[""The CLEO detector at the Cornell Electron Storage Ring (CESR) is completing amajor upgrade that significantly extends its physics reach in the study ofheavy quarks and leptons. The major elements of this detector upgrade are theinstallation of a ``fast'' ring imaging Cherenkov detector, a new central driftchamber and a new barrel-style silicon strip vertex detector. Trigger and dataacquisition systems are also upgraded. We summarize the status of thesedetector subsystems as well as the parallel CESR upgrade.""]",['2000-02-07']
936,['eng'],"['Ouchrif, M']",['Q-balls in Underground Experiments'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1999/05/17', 'astrophysics, missing-mass', 'Q-ball, energy loss', 'coupling, matter', 'deep underground detector, MACRO', 'photon, yield', 'scintillation counter, liquid', 'ionization', 'streamer chamber', 'solid-state counter, track sensitive', 'numerical calculations']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002013'],"['In this paper we present some features of Q-balls and we discuss theirinteractions with matter, and their energy losses in the Earth, for a largerange of velocities. These calculations are used to compute the fractionalgeometrical acceptance of the MACRO detector. Furthermore a systematic analysisof the energy losses of Q-balls in three types of detectors is investigated.More specifically we have computed the light yield in liquid scintillators, theionization in streamer tubes and the Restricted Energy Loss in the CR39 nucleartrack detectors.']",['2000-02-07']
937,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['QCD studies with $e^{+}e^{-}$ annihilation data at 172-189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, pair production', 'hadron, multiple production', 'event shape analysis', 'charged particle, multiplicity', 'momentum spectrum', 'rapidity spectrum', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tables', 'bibliography', '172, 183, 189 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002012'],"['We have studied hadronic events from e+e- annihilation data at centre-of-mass energies of sqrt{s}=172, 183 and 189 GeV. The total integrated luminosity of the three samples, measured with the OPAL detector, corresponds to 250 pb^-1. We present distributions of event shape variables, charged particle multiplicity and momentum, measured separately in the three data samples. From these we extract measurements of the strong coupling alpha_s, the mean charged particle multiplicity <nch> and the peak position xi_0 in the xi_p=ln(1/x_p) distribution. In general the data are described well by analytic QCD calculations and Monte Carlo models. Our measured values of alpha_s, <nch> and xi_0 are consistent with previous determinations at sqrt{s}=MZ.']",['2000-02-04']
938,['eng'],"['Kettell, S H']",['Rare Kaon Decays'],['Particle Physics - Experimental Results'],"['review, Taipei 1999/12/03', 'K, rare decay', 'flavor, violation', 'K0(L), leptonic decay', 'K0(L), radiative decay', 'K, semileptonic decay', 'K+, branching ratio', 'K0(L), branching ratio', 'Kobayashi-Maskawa angle', 'experimental results', 'K0(L) --> muon electron', 'K0(L) --> muon+ muon-', 'K --> pi muon electron', 'K --> pi neutrino antineutrino', 'K0(L) --> positron electron photon', 'K0(L) --> muon+ muon- positron electron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002011'],"['The current status of rare kaon decay experiments is reviewed. New limits inthe search for Lepton Flavor Violation are discussed, as are new measurementsof the CKM matrix.']",['2000-02-04']
939,['eng'],"['Breitweg, J', 'Chekanov, S', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Musgrave, B', 'Pellegrino, A R', 'Repond, J', 'Stanek, R', 'Yoshida, R', 'Mattingly, M C K', 'Abbiendi, G', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Coppola, N', 'Corradi, M', 'De Pasquale, S', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Brock, I', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Hartmann, H', 'Heinloth, K', 'Hilger, E', 'Irrgang, P', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Schnurbusch, H', 'Stifutkin, A', 'Tandler, J', 'Voss, K C', 'Weber, A', 'Wieber, H', 'Bailey, D S', 'Barret, O', 'Brook, N H', 'Foster, B', 'Heath, G P', 'Heath, H F', 'McFall, J D', 'Piccioni, D', 'Rodrigues, E', 'Scott, J', 'Tapper, R J', 'Capua, M', 'Mastroberardino, A', 'Schioppa, M', 'Susinno, G', 'Jeoung, H Y', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Ma, K J', 'Pac, M Y', 'Caldwell, A', 'Liu, W', 'Liu, X', 'Mellado, B', 'Paganis, S', 'Sacchi, R', 'Sampson, S', 'Sciulli, F', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Olkiewicz, K', 'Piotrzkowski, K', 'Przybycien, M B', 'Stopa, P', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowal, A M', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Szuba, D', 'Kotanski, Andrzej', 'Bauerdick, L A T', 'Behrens, U', 'Bienlein, J K', 'Burgard, C', 'Desler, K', 'Drews, G', 'Fox-Murphy, A', 'Fricke, U', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hartner, G F', 'Hasell, D', 'Hebbel, K', 'Johnson, K F', 'Kasemann, M', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Lindemann, L', 'Löhr, B', 'Martínez, M', 'Milite, M', 'Monteiro, T', 'Moritz, M', 'Notz, D', 'Pelucchi, F', 'Petrucci, M C', 'Rohde, M', 'Saull, P R B', 'Savin, A A', 'Schneekloth, U', 'Selonke, F', 'Sievers, M', 'Stonjek, S', 'Tassi, E', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Coldewey, C', 'Grabosch, H J', 'López-Duran-Viani, A', 'Meyer, A', 'Schlenstedt, S', 'Straub, P B', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'Votano, L', 'Bamberger, Andreas', 'Benen, A', 'Eisenhardt, S', 'Markun, P', 'Raach, H', 'Wölfle, S', 'Bussey, Peter J', 'Doyle, A T', 'Lee, S W', 'MacDonald, N', 'McCance, G J', 'Saxon, D H', 'Sinclair, L E', 'Skillicorn, Ian O', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Dannheim, D', 'Garfagnini, A', 'Gialas, I', 'Gladilin, L K', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Poelz, G', 'Zetsche, F', 'Goncalo, R', 'Long, K R', 'Miller, D B', 'Tapper, A D', 'Walker, R', 'Mallik, U', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Nagano, K', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Ahn, S H', 'An, S H', 'Hong, S J', 'Lee, S B', 'Nam, S W', 'Park, S K', 'Lim, H', 'Park, I H', 'Son, D', 'Barreiro, F', 'García, G', 'Glasman, C', 'González, O', 'Labarga, L', 'Del Peso, J', 'Redondo, I', 'Terron, J', 'Barbi, M S', 'Corriveau, F', 'Hanna, D S', 'Ochs, A', 'Padhi, S', 'Riveline, M', 'Stairs, D G', 'Wing, M', 'Tsurugai, T', 'Bashkirov, V', 'Dolgoshein, B A', 'Dementev, R K', 'Ermolov, P F', 'Golubkov, Yu A', 'Katkov, I I', 'Khein, L A', 'Korotkova, N A', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Shcheglova, L M', 'Solomin, A N', 'Vlasov, N N', 'Zotkin, S A', 'Bokel, C', 'Botje, M', 'Brümmer, N', 'Engelen, J', 'Grijpink, S', 'Koffeman, E', 'Kooijman, P M', 'Schagen, S', 'Van Sighem, A', 'Tiecke, H G', 'Tuning, N', 'Velthuis, J J', 'Vossebeld, J H', 'Wiggers, L', 'De Wolf, E', 'Bylsma, B', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Ling, T Y', 'Nylander, P', 'Boogert, S', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Grosse-Knetter, J', 'Matsushita, T', 'Ruske, O', 'Sutton, M R', 'Walczak, R', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'Dosselli, U', 'Dusini, S', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Iannotti, L', 'Oh, B Y', 'Okrasinski, J R', 'Toothacker, W S', 'Whitmore, J J', 'Iga, Y', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Cormack, C', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Epperson, D E', 'Heusch, C A', 'Sadrozinski, H F W', 'Seiden, A', 'Wichmann, R', 'Williams, D C', 'Pavel, N', 'Abramowicz, H', 'Dagan, S', 'Kananov, S', 'Kreisel, A', 'Levy, A', 'Abe, T', 'Fusayasu, T', 'Umemori, K', 'Yamashita, T', 'Hamatsu, R', 'Hirose, T', 'Inuzuka, M', 'Kitamura, S', 'Nishimura, T', 'Arneodo, M', 'Cartiglia, N', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Monaco, V', 'Peroni, C', 'Ruspa, M', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Fagerstroem, C P', 'Galea, R', 'Koop, T', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sabetfakhri, A', 'Simmons, D', 'Butterworth, J M', 'Catterall, C D', 'Hayes, M E', 'Heaphy, E A', 'Jones, T W', 'Lane, J B', 'West, B J', 'Ciborowski, J', 'Ciesielski, R', 'Grzelak, G', 'Nowak, R J', 'Pawlak, J M', 'Pawlak, R', 'Smalska, B', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Adamus, M', 'Gadaj, T', 'Deppe, O', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Badgett, W F', 'Chapin, D', 'Cross, R', 'Foudas, C', 'Mattingly, S E', 'Reeder, D D', 'Smith, W H', 'Vaiciulis, A W', 'Wildschek, T', 'Wodarczyk, M', 'Deshpande, A A', 'Dhawan, S K', 'Hughes, V W', 'Bhadra, S', 'Cole, J E', 'Frisken, W R', 'Hall-Wilton, R', 'Khakzad, M', 'Menary, S R', 'Schmidke, W B']",['The $Q^{2}$ Dependence of Dijet Cross Sections in $\\gamma p$ Interactions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'jet, photoproduction', 'final state, (2jet)', 'channel cross section, momentum dependence', 'momentum transfer, dependence', 'photon, structure function', 'momentum spectrum, parton', 'quantum chromodynamics, perturbation theory', 'photon, resolved', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002010'],"['The dependence of the photon structure on the photon virtuality, Q^2, isstudied by measuring the reaction e^+p\\to e^+ + {\\rm jet} + {\\rm jet} + {\\rm X}at photon-proton centre-of-mass energies 134 < W < 223 GeV. Events have beenselected in the Q^2 ranges \\approx 0 GeV^2, 0.1-0.55 GeV^2, and 1.5-4.5 GeV^2,having two jets with transverse energy E_T^{jet} > 5.5 GeV in the final state.The dijet cross section has been measured as a function of the fractionalmomentum of the photon participating in the hard process, x_gamma. The ratio ofthe dijet cross section with x_gamma < 0.75 to that with x_gamma > 0.75decreases as Q^2 increases. The data are compared with the predictions of NLOpQCD and leading-order Monte Carlo programs using various parton distributionfunctions of the photon. The measurements can be interpreted in terms of aresolved photon component that falls with Q^2 but remains present at values ofQ^2 up to 4.5 GeV^2. However, none of the models considered gives a gooddescription of the data.']",['2000-02-04']
940,['eng'],"['Kettell, S H']",['Experimental Results on Radiative Kaon Decays'],['Particle Physics - Experimental Results'],"['review, Frascati 1999/11/16', 'K, radiative decay', 'K0, branching ratio', 'K+, branching ratio', 'photon, on-shell', 'photon, off-shell', 'perturbation theory, chiral', 'experimental results', 'bibliography', 'K --> 2photon', 'K --> pi 2photon', 'K --> pi lepton+ lepton-', 'K --> pi lepton+ lepton- photon', 'K --> lepton neutrino photon', 'K --> 3lepton neutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002009'],"['This paper reviews the current status of experimental measurements ofradiative kaon decays. Several experiments at BNL, CERN and FNAL have recentlyor will soon complete data collection; as a result, several new results areavailable.']",['2000-02-04']
941,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Cammin, J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Gunther, P O', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauke, A', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Hensel, C', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klein, K', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lawson, I', 'Layter, J G', 'Leins, A', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tarem, S', 'Taylor, R J', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for new Physics in rare B Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B, rare decay', 'mass spectrum, (2K pi)', 'supersymmetry', 'R parity, violation', 'B, branching ratio', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'B --> 2K pi', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002008'],"['A search for the decay B+- to K+-K+-pi-+ was performed using data collected by the OPAL detector at LEP. These decays are strongly suppressed in the Standard Model but could occur with a higher branching ratio in supersymmetric models, especially in those with R-parity violating couplings. No evidence for a signal was observed and a 90% confidence level upper limit of 1.29x10^-4 was set for the branching ratio.']",['2000-02-04']
942,['eng'],"['Bai, J Z', 'Ban, Y', 'Bian, J G', 'Chen, A D', 'Chen, G P', 'Chen, H F', 'Chen, H S', 'Chen Jia Chao', 'Chen, X D', 'Chen, Y', 'Chen, Y B', 'Cheng, B S', 'Cui, X Z', 'Ding, H L', 'Dong, L Y', 'Du, Z Z', 'Gao, C S', 'Gao, M L', 'Gao, S Q', 'Gu, J H', 'Gu, S D', 'Gu, W X', 'Guo, Y N', 'Guo, Z J', 'Han, S W', 'Han, Y', 'He, J', 'He, J T', 'He, K L', 'He, M', 'Heng, Y K', 'Hu, G Y', 'Hu, H M', 'Hu, J L', 'Hu, Q H', 'Hu, T', 'Huang, G S', 'Huang, X P', 'Huang, Y Z', 'Jiang, C H', 'Jin, Y', 'Ju, X', 'Ke, Z J', 'Lai, Y F', 'Lang, P F', 'Li, C G', 'Li, D', 'Li, H B', 'Li, J', 'Li, J C', 'Li, P Q', 'Li, W', 'Li, W G', 'Li, X H', 'Li Xiao Nan', 'Li Xue Qian', 'Li Zhong Chao', 'Liu, B', 'Liu, F', 'Liu, F', 'Liu, H M', 'Liu, J', 'Liu, J P', 'Liu, R G', 'Liu, Y', 'Liu, Z X', 'Lu, G R', 'Lu, F', 'Lu, J G', 'Luo, X L', 'Ma, E C', 'Ma, J M', 'Mao, H S', 'Mao, Z P', 'Meng, X C', 'Mo, X H', 'Nie, J', 'Qi, N D', 'Qi, X R', 'Qian, C D', 'Qiu, J F', 'Qu, Y H', 'Que, Y K', 'Rong, G', 'Shao, Y Y', 'Shen, B W', 'Shen, D L', 'Shen, H', 'Shen, H Y', 'Shen, X Y', 'Shi, F', 'Shi, H Z', 'Song, X F', 'Sun, H S', 'Sun, L F', 'Sun, Y Z', 'Tang, S Q', 'Tong, G L', 'Wang, F', 'Wang, L', 'Wang, L S', 'Wang, L Z', 'Wang, P', 'Wang, P L', 'Wang, S M', 'Wang, Y Y', 'Wang, Z Y', 'Wei, C L', 'Wu, N', 'Wu, Y G', 'Xi, D M', 'Xia, X M', 'Xie, Y', 'Xie, Y H', 'Xu, G F', 'Xue, S T', 'Yan, J', 'Yan, W G', 'Yang, C M', 'Yang, C Y', 'Yang, H X', 'Yang, X F', 'Ye, M H', 'Ye Shu Wei', 'Ye, Y X', 'Yu, C S', 'Yu, C X', 'Yu, G W', 'Yu Yu Hei', 'Yu, Z Q', 'Yuan, C Z', 'Yuan, Y', 'Zhang Bing Yun', 'Zhang, C', 'Zhang, C C', 'Zhang, D H', 'Zhang, D', 'Zhang, H L', 'Zhang, J', 'Zhang, J W', 'Zhang, L', 'Zhang, L', 'Zhang, L S', 'Zhang, P', 'Zhang, Q J', 'Zhang, S Q', 'Zhang, X Y', 'Zhang, Y Y', 'Zhao, D X', 'Zhao, H W', 'Zhao, J', 'Zhao Jia Wei', 'Zhao, M', 'Zhao Wei Ren', 'Zhao, Z G', 'Zheng Jian Ping', 'Zheng Lin Sheng', 'Zheng Zhi Peng', 'Zhou, B Q', 'Zhou, L', 'Zhu, K J', 'Zhu, Q M', 'Zhu, Y C', 'Zhu, Y S', 'Zhu, Z A', 'Zhuang, B A', 'Bugg, D V', 'Zou Bing Song']",['Partial Wave Analysis of $J/\\psi \\to \\gamma (K^{\\pm}K_S^{0}\\pi^{\\mp})$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'J/psi(3100), electroproduction', 'J/psi(3100), radiative decay', 'mass spectrum, (K0(S) K pi)', 'partial wave analysis', 'eta(1440), hadronic decay', 'postulated particle, eta(1900)', 'postulated particle, eta(2040)', 'meson resonance, hybrid', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'J/psi(3100) --> K0(S) K pi photon', 'approx. 3.1 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002007'],"['BES data on $J/\\psi \\to \\gamma (K^{\\pm} K_S^0 \\pi^{\\mp})$ are presented.There is a strong peak due to $\\eta(1440)/\\iota$, which is fitted with aBreit-Wigner amplitude with $s$-dependent widths for decays to $K^*K$, $\\kappaK$, $\\eta \\pi\\pi$ and $\\rho\\rho$; $\\kappa$ refers to the $K\\pi$ S-wave. At a$K\\bar{K}\\pi$ mass of $\\sim 2040$ MeV, there is a second peak with width $\\sim400$ MeV; $J^P = 0^-$ is preferred over $1^+$ and $2^-$ respectively by 5.2 and6.8 standard deviations. It is a possible candidate for a $0^-$ $s\\bar sg$hybrid partner of $\\pi(1800)$.']",['2000-02-04']
943,['eng'],"['Bai, J Z', 'Ban, Y', 'Bian, J G', 'Blum, I K', 'Chen, A D', 'Chen, G P', 'Chen, H F', 'Chen, H S', 'Chen, J', 'Chen Jia Chao', 'Chen, X D', 'Chen, Y', 'Chen, Y B', 'Cheng, B S', 'Choi, J B', 'Cui, X Z', 'Ding, H L', 'Dong, L Y', 'Du, Z Z', 'Dunwoodie, W M', 'Gao, C S', 'Gao, M L', 'Gao, S Q', 'Gratton, P', 'Gu, J H', 'Gu, S D', 'Gu, W X', 'Guo, Y N', 'Guo, Z J', 'Han, S W', 'Han, Y', 'Harris, F A', 'He, J', 'He, J T', 'He, K L', 'He, M', 'Heng, Y K', 'Hitlin, D G', 'Hu, G Y', 'Hu, H M', 'Hu, J L', 'Hu, Q H', 'Hu, T', 'Huang, G S', 'Huang, X P', 'Huang, Y Z', 'Izen, J M', 'Jiang, C H', 'Jin, Y', 'Jones, B D', 'Ju, X', 'Kang, J S', 'Ke, Z J', 'Kelsey, M H', 'Kim, B K', 'Kim, H J', 'Kim, S K', 'Kim, T Y', 'Kong, D', 'Lai, Y F', 'Lang, P F', 'Lankford, A J', 'Li, C G', 'Li, D', 'Li, H B', 'Li, J', 'Li, J C', 'Li, P Q', 'Li, W', 'Li, W G', 'Li, X H', 'Li Xiao Nan', 'Li Xue Qian', 'Li Zhong Chao', 'Liu, B', 'Liu, F', 'Liu Feng', 'Liu, H M', 'Liu, J', 'Liu, J P', 'Liu, R G', 'Liu, Y', 'Liu, Z X', 'Lou, X C', 'Lowery, B', 'Lu, G R', 'Lu, F', 'Lu, J G', 'Luo, X L', 'Ma, E C', 'Ma, J M', 'Malchow, R', 'Mao, H S', 'Mao, Z P', 'Meng, X C', 'Mo, X H', 'Nie, J', 'Olsen, S L', 'Oyang, J Y T', 'Paluselli, D', 'Pan, L J', 'Panetta, J', 'Park, H', 'Porter, F', 'Qi, N D', 'Qi, X R', 'Qian, C D', 'Qiu, J F', 'Qu, Y H', 'Que, Y K', 'Rong, G', 'Schernau, M', 'Shao, Y Y', 'Shen, B W', 'Shen, D L', 'Shen, H', 'Shen, H Y', 'Shen, X Y', 'Shi, F', 'Shi, H Z', 'Song, X F', 'Standifird, J', 'Suh, J Y', 'Sun, H S', 'Sun, L F', 'Sun, Y Z', 'Tang, S Q', 'Toki, W', 'Tong, G L', 'Varner, G S', 'Wang, F', 'Wang, L', 'Wang, L S', 'Wang, L Z', 'Wang, P', 'Wang, P L', 'Wang, S M', 'Wang, Y Y', 'Wang, Z Y', 'Weaver, M', 'Wei, C L', 'Wu, N', 'Wu, Y G', 'Xi, D M', 'Xia, X M', 'Xie, Y', 'Xie, Y H', 'Xu, G F', 'Xue, S T', 'Yan, J', 'Yan, W G', 'Yang, C M', 'Yang, C Y', 'Yang, H X', 'Yang, W', 'Yang, X F', 'Ye, M H', 'Ye Shu Wei', 'Ye, Y X', 'Yu, C S', 'Yu, C X', 'Yu, G W', 'Yu Yu Hei', 'Yu, Z Q', 'Yuan, C Z', 'Yuan, Y', 'Zhang Bing Yun', 'Zhang, C', 'Zhang, C C', 'Zhang, D H', 'Zhang, D', 'Zhang, H L', 'Zhang, J', 'Zhang, J W', 'Zhang, L', 'Zhang Lei', 'Zhang, L S', 'Zhang, P', 'Zhang, Q J', 'Zhang, S Q', 'Zhang, X Y', 'Zhang, Y Y', 'Zhao, D X', 'Zhao, H W', 'Zhao, J', 'Zhao Jia Wei', 'Zhao, M', 'Zhao Wei Ren', 'Zhao, Z G', 'Zheng Jian Ping', 'Zheng Lin Sheng', 'Zheng, Y H', 'Zheng Zhi Peng', 'Zhou, B Q', 'Zhou, L', 'Zhu, K J', 'Zhu, Q M', 'Zhu, Y C', 'Zhu, Y S', 'Zhu, Z A', 'Zhuang, B A']",['A Measurement of the Mass and Full-Width of the $\\eta_{c}$ Meson'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'J/psi(3100), electroproduction', 'J/psi(3100), radiative decay', 'eta/c(2980), hadronic decay', 'eta/c(2980), mass', 'eta/c(2980), width', 'mass spectrum', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'J/psi(3100) --> eta/c(2980) photon', 'eta/c(2980) --> K+ K- pi+ pi-', 'eta/c(2980) --> 2pi+ 2pi-', 'eta/c(2980) --> K0(S) K pi', 'eta/c(2980) --> 2Phi(1020)', 'approx. 3.1 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002006'],"['In a sample of 7.8 million $J/\\psi$ decays collected in the BeijingSpectrometer, the process J/$\\psi\\to\\gamma\\eta_c$ is observed for fivedifferent $\\eta_c$ decay channels: $K^+K^-\\pi^+\\pi^-$, $\\pi^+\\pi^-\\pi^+\\pi^-$,$K^\\pm K^0_S \\pi^\\mp$ (with $K^0_S\\to\\pi^+\\pi^-$), $\\phi\\phi$ (with $\\phi\\toK^+K^-$) and $K^+K^-\\pi^0$. From these signals, we determine the mass of$\\eta_c$ to be $2976.6\\pm2.9\\pm1.3$ MeV. Combining this result with apreviously reported result from a similar study using $\\psi(2S)\\to\\gamma\\eta_c$detected in the same spectrometer gives $m_{\\eta_c} = 2976.3\\pm2.3\\pm1.2$ MeV.For the combined samples, we obtain $\\Gamma_{\\eta_c} = 11.0\\pm 8.1\\pm 4.1$ MeV.']",['2000-02-04']
944,['eng'],"['Roberts, B L']",['Status of the Muon (g-2) Experiment'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'muon, magnetic moment', 'muon, polarized beam', 'magnetic field', 'electric field', 'muon+, leptonic decay', 'experimental methods', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002005'],"['The status of the muon (g-2) experiment, E821 at the Brookhaven AGS, isgiven. A new result with a precision of 5 parts per million has been obtainedwith direct muon injection into the ring and is presented. The theoreticalmotivation for the experiment, and a discussion of the sensitivity tonon-standard model physics is also discussed.']",['2000-02-03']
945,['eng'],"['Hoeneisen, B', 'Marin, C P']",['Three generation neutrino mixing is compatible with all experiments'],['Particle Physics - Experimental Results'],"['neutrino, interference', 'electroweak interaction, model', 'flavor, 3', 'neutrino, Dirac', 'neutrino, Majorana', 'neutrino, mass', 'numerical calculations, interpretation of experiments']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002004'],['We consider the minimal extension of the Standard Model with threegenerations of massive neutrinos that mix. We then determine the parameters ofthe model that satisfy all experimental constraints.'],['2000-02-03']
946,['eng'],"['Danilov, M V', 'De Voe, R G', 'Dolgolenko, A', 'Giannini, G', 'Gratta, Giorgio', 'Picchi, P', 'Piepke, A G', 'Pietropaolo, Francesco', 'Vogel, P', 'Vuilleumier, J L', 'Wang, Y F', 'Zeldovich, O Ya']",['Detection of very small neutrino masses in double-beta decay using laser tagging'],['Particle Physics - Experimental Results'],"['xenon, double-beta decay', 'xenon, nuclide', 'final state, (0neutrino)', 'drift chamber, time projection', 'drift chamber, xenon', 'baryon, energy levels', 'radiation, laser', 'neutrino, mass', 'neutrino, Majorana']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002003'],"['We describe an approach to the study of neutrino masses that combines quantumoptics techniques with radiation detectors to obtain unprecedented sensitivity.With it the search for Majorana neutrino masses down to $\\sim$10 meV willbecome accessible. The experimental technique uses the possibility ofindividually detecting $\\rm Ba^+$-ions in the final state of $\\rm ^{136}Xe$double-beta decay via resonant excitation with a set of lasers aimed at aspecific location in a large Time Projection Chamber. The specificity of theatomic levels provides tagging and, together with more traditional eventrecognition parameters, greatly suppresses radioactive backgrounds.']",['2000-02-03']
947,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adam, I', 'Adams, D L', 'Adams, M', 'Ahn, S', 'Akimov, V E', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Belyaev, A', 'Beri, S B', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Bloom, P', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Boswell, C', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Bross, A', 'Buchholz, D', 'Burtovoi, V S', 'Butler, J M', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chekulaev, S V', 'Chen, W', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cobau, W G', 'Cochran, J', 'Coney, L', 'Cooper, W E', 'Coppage, D', 'Cretsinger, C E', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fatyga, M K', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Forden, G E', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Geld, T L', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gobbi, B', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, D R', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Guida, J A', 'Guida, J M', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Hernández-Montoya, R', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hsieh, F', 'Hu Tong', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Jun, S Y', 'Jung, C K', 'Kahn, S', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Koltick, D S', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Landry, F J', 'Landsberg, G L', 'Leflat, A', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Maciel, A K A', 'Madaras, R J', 'Madden, R', 'Magana-Mendoza, L', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Markeloff, R', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McKibben, T', 'McKinley, J', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mostafa, M A', 'Da Motta, H', 'Murphy, C', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Narayanan, A', 'Neal, H A', 'Negret, J P', 'Némethy, P', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Oshima, N', 'Owen, D', 'Padley, P', 'Para, A', 'Parashar, N', 'Park, Y M', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pishchalnikov, Yu', 'Pope, B G', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramírez, O', 'Reay, N W', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Sánchez-Hernández, A', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Scully, J R', 'Shabalina, E', 'Shaffer, C', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sosebee, M', 'Sotnikova, N', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Sznajder, A', 'Tamburello, P D', 'Tarazi, J', 'Tartaglia, M', 'Thomas, T L T', 'Thompson, J', 'Toback, D', 'Trippe, T G', 'Tuts, P M', 'Vaniev, V', 'Varelas, N', 'Varnes, E W', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yepes, P', 'Yip, K', 'Yoshikawa, C', 'Youssef, S', 'Yu, J', 'Yu, Y', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Inclusive Jet Cross Sections in $\\overline{p}p$ Collisions at $\\sqrt{s}$= 630 and 1800 GeV'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Zeuthen 1999/04/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'differential cross section, transverse energy', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'differential cross section, ratio', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001063'],"['We have made a precise measurement of the inclusive jet cross section at pb^{-1} collected at the Fermilab Tevatron $\\bar{p}p$ Collider with the DØ detector. The measurement is reported as a function of jet transverse energy (60 GeV <= E_{T} < 550 GeV), and in the pseudorapidity intervals |\\eta| <= 0.5 and 0.1 <= |\\eta| <= 0.7. A preliminary measurement of the pseudorapidity dependence of inclusive jet production (|\\eta| <= 1.5) is also discussed. The results are in good agreement with predictions from next-to-leading order (NLO) quantum chromodynamics (QCD). DØ has also determined the ratio of jet cross sections at $\\sqrt{s}$=630 GeV and $\\sqrt{s}$=1800 GeV (|\\eta| <= 0.5). This preliminary measurement differs from NLO QCD predictions.']",['2000-01-31']
948,['eng'],"['Babukhadia, L R']","['Forward Jets, Dijets, and Subjets at the Tevatron']",['Particle Physics - Experimental Results'],"['talk, Providence 1999/08/09', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'jet, pair production', 'charged particle, multiplicity', 'jet, multiplicity', 'differential cross section, transverse energy', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001062'],"['Recent new results on the determination of the rapidity dependence of the differential inclusive jet cross section, \\mycsav, as a function of jet \\et in the Tevatron, are presented along with the comparisons to theoretical next-to-leading order (NLO) perturbative QCD predictions. Triple differential dijet cross sections, \\tdcsav, at $\\sqrt{s}=1800$ GeV, as well as the new results on jet structure at $\\sqrt{s}=1800$ and 630 GeV, as measured by the CDF and \\dzero detectors, are also discussed.']",['2000-01-31']
949,['eng'],"['Ruhlmann-Kleider, V']",['New particle searches'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'new particle, search for', 'anti-p p, colliding beams', 'lepton p, colliding beams', 'electron positron, colliding beams', 'leptoquark', 'sparticle, spectra', 'R parity', 'supersymmetry, symmetry breaking', 'quantum gravity, higher-dimensional', 'Higgs particle, multiplet', 'experimental results', 'Batavia TEVATRON Coll', 'DESY HERA Stor', 'CERN LEP Stor', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001061'],"['This review presents recent results on new particle searches achieved at Tevatron, Hera and LEP. After a brief outline of the searches on exotic particles, results on supersymmetric particles and Higgs bosons are detailed. Near future prospects are also given.']",['2000-01-31']
950,['eng'],"['Godang, R']",['Search for $D^{0}-\\overline{D}^{0}$ Mixing'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, electroproduction', 'charmed meson, hadronic decay', 'D*(2010)', 'D0', 'decay, time dependence', 'D0 anti-D0, interference', 'CP, violation', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D*(2010) --> D0 pi+', 'D0 --> K+ pi-', 'approx. 10 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001060'],"[""We report on a search for D0-D0B mixing made by studying the `wrong-sign' process D0->K^+pi^-. The data come from an integrated luminosity of 9.0 1/fb of e^+e^- collisions at s^(1/2) of approximately 10 GeV recorded with the CLEO II.V detector. We measure the time integrated rate of the `wrong-sign' process D0->K^+pi^- relative to that of the Cabibbo-favored process D0B->K^+pi^- to be R=(0.332^{+0.063}_{-0.065}+-0.040)%. We study D0->K^+pi^- as a function of decay time to distinguish direct doubly Cabibbo-suppressed decay from D0-D0B mixing. The amplitudes that describe D0-D0B mixing, x' and y', are consistent with zero. At the 95% C.L. and without assumptions concerning charge-parity (CP) violating parameters, we find (1/2)x'^2<0.041% and -5.8%<y'<1.0%.""]",['2000-01-28']
951,['eng'],"['Klein, M']",['Structure Functions in Deep Inelastic Lepton-Nucleon Scattering'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'lepton nucleon, deep inelastic scattering', 'lepton nucleus, deep inelastic scattering', 'neutral current', 'charged current', 'hadron, electroproduction', 'hadron, photoproduction', 'small-x', 'nucleon, structure function', 'structure function, longitudinal', 'quark, momentum spectrum', 'quark, sea', 'quark, charm', 'gluon, momentum spectrum', 'strong interaction, coupling constant', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001059'],"['Latest results on structure functions, as available at the Lepton-Photon Symposium 1999, are presented. This report focusses on three experimental areas: new structure function measurements, in particular from HERA at low x and high Q2; results on light and heavy flavour densities; determinations of the gluon distribution and of alpha_s. As the talk was delivered at a historic moment and place, a few remarks were added recalling the exciting past and looking into the promising future of deep inelastic scattering.']",['2000-01-28']
952,['eng'],"['Ronga, F']",['Atmospheric Neutrinos'],['Particle Physics - Experimental Results'],"['talk, Paris 1999/09/06', 'neutrino, cosmic radiation', 'muon, cosmic radiation', 'cosmic radiation, flux', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'ratio, (neutrino/mu neutrino/e)', 'angular distribution', 'neutrino, sterile', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001058'],"['The results of experiments on atmospheric neutrinos are summarized, with the important exception of Superkamiokande. The main emphasis is given to the Soudan-2 and MACRO experiments. Both experiments observe atmospheric neutrino anomalies in agreement with nu_mu-->> nu_tau oscillations with maximum mixing. The nu_mu-->> nu_sterile oscillation is disfavored by the MACRO experiment.']",['2000-01-28']
953,['eng'],"['Ohshima, T']",['Test Result of Time-Of-Propagation Cherenkov Counter'],['Detectors and Experimental Techniques'],"['particle identification', 'Cherenkov counter, experimental methods', 'Cherenkov counter, ring imaging', 'silicon, glass', 'fast logic, time-of-flight', 'time resolution', 'photoelectron, amplifier', 'magnetic detector, BELLE', 'KEK TRISTAN Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001057'],['A new concept concerning Cherenkov detector for particle identification by means of measuring both the Time-of-Propagation (TOP) and horizontal emission angle ($\\Phi$) of Cherenkov photons is described here. Some R&D works are also reported.'],['2000-01-28']
954,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Leading Particle Production in Light Flavour Jets'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, jet', 'quark, hadronization', 'hadron, leading particle', 'pi', 'K', 'p', 'Lambda', 'hadron, energy spectrum', 'dependence, flavor', 'strange particle, yield', 'numerical calculations, Monte Carlo', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tables', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001054'],['The energy distribution and type of the particle with the highest momentum in quark jets are determined for each of the five quark flavours making only minimal model assumptions. The analysis is based on a large statistics sample of hadronic Z0 decays collected with the OPAL detector at the LEP e+e- collider. These results provide a basis for future studies of light flavour production at other centre-of-mass energies. We use our results to study the hadronisation mechanism in light flavour jets and compare the data to the QCD models JETSET and HERWIG. Within the JETSET model we also directly determine the suppression of strange quarks to be gamma_s=0.422+-0.049 (stat.)+-0.059 (syst.) by comparing the production of charged and neutral kaons in strange and non-strange light quark events. Finally we study the features of baryon production.'],['2000-01-25']
955,['eng'],"['Albrecht, E', 'Barber, G J', 'Bibby, J H', 'Brook, N H', 'Doucas, G', 'Duane, A', 'Easo, S', 'Eklund, L', 'French, M', 'Gibson, V', 'Gys, T', 'Halley, A W', 'Harnew, N', 'John, M', 'Piedigrossi, D', 'Rademacker, J', 'Simmons, B', 'Smale, N J', 'Teixeira-Dias, P', 'Toudup, L W', 'Websdale, David M', 'Wilkinson, G R', 'Wotton, S A']",['A Prototype RICH Detector Using Multi-Anode Photo Multiplier Tubes and Hybrid Photo-Diodes'],['Detectors and Experimental Techniques'],"['particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'Cherenkov counter, air', 'carbon, fluorine', 'angular resolution', 'photoelectron, amplifier', 'semiconductor, optical', 'photoelectron, yield', 'magnetic detector, LHC-B', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001053'],"['The performance of a prototype Ring Imaging Cherenkov Detector is studied using a charged particle beam. The detector performance, using CF4 and air as radiators, is described. Cherenkov angle precision and photoelectron yield using hybrid photo-diodes and multi-anode PMTs agree with simulations and are assessed in terms of the requirements of the LHCb experiment.']",['2000-01-25']
956,['eng'],"['Rubbia, André']",['ICANOE'],['Detectors and Experimental Techniques'],"['talk, Stony Brook 1999/09/23', 'neutrino, oscillation', 'calorimeter, liquid argon', 'showers, air', 'background', 'proposed experiment', 'deep underground detector, Gran Sasso', 'CERN Lab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001052'],"['The main scientific goal of the ICANOE detector is the one of elucidating in a comprehensive way the pattern of neutrino masses and mixings, following the SuperKamiokande results and the observed solar neutrinos deficit. To achieve these goals, the experimental method is based upon the complementary and simultaneous detection of CERN beam (CNGS) and cosmic ray (CR) events. For the currently allowed values of the SuperKamiokande results, both CNGS and cosmic ray data will give independent measurements and provide a precise determination of the oscillation parameters.']",['2000-01-24']
957,['eng'],"['Milshtein, A I']",['$a_{1}\\pi$ Contribution to $e^{+}e^{-} \\to 4\\pi$ Annihilation and $\\tau \\to 4\\pi\\nu_{\\tau}$ Decay'],['Particle Physics - Experimental Results'],"['talk, Frascati 1999/11/16', 'electron positron, colliding beams', 'electron positron, annihilation', 'pi, multiple production', 'final state, (4pi)', 'tau, semileptonic decay', 'intermediate state, (a1(1260) pi)', 'intermediate state, (omega(783) pi)', 'channel cross section, energy dependence', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> 2pi+ 2pi-', 'electron positron --> pi+ pi- 2pi0', 'tau --> 4pi neutrino/tau', '1.05-1.38 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001050'],"['The results of the study of the process e^+e^- \\to 4\\pi by the CMD-2 collaboration at VEPP-2M are presented. Analysis of the differential distributions demonstrates the dominance of the a_1\\pi and ømega\\pi intermediate states. Simple model, based on the assumption of a_1(1260)\\pi and data of CLEOII and ALEPH obtained recently for the decay \\tau\\to']",['2000-01-24']
958,['eng'],"['Milshtein, A I']",['Status of Experiments and Recent Results from CMD-2 Detector at Vepp-2M'],['Particle Physics - Experimental Results'],"['talk, Frascati 1999/11/16', 'electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'hadron, multiple production', 'pi, form factor', 'rho(770)', 'omega(783)', 'Phi(1020), decay modes', 'K0(S), semileptonic decay', 'channel cross section, energy dependence', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> eta photon', 'Phi(1020) --> eta(958) photon', 'Phi(1020) --> K0(L) K0(S)', 'K0(S) --> pi electron neutrino', 'Phi(1020) --> pseudoscalar meson positron electron', 'electron positron --> 4pi', 'electron positron --> 4pi pi0', '0.37-1.39 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001049'],['The Cryogenic Magnetic Detector (CMD-2) is shortly described. Preliminary results for the cross sections of $e^+$ $e^-$ annihilation into hadrons and leptons are presented in the c.m. energy range from 0.37 to 1.39 GeV. The total integrated luminosity of about 26 ${pb}^{-1}$ has been collected. The new results for the $\\rho$ and $\\omega$ meson parameters are reported. The major decay modes of the $\\phi$ meson as well as its rare decays have been observed.'],['2000-01-24']
959,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, D', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Bose-Einstein correlations in $K^{\\pm}K^{\\pm}$ pairs from $Z^{0}$ decays into two hadronic jets'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, pair production', 'correlation, (2K+)', 'correlation, (2K-)', 'boson, statistics', 'correlation function', 'momentum transfer, dependence', 'parametrization', 'final-state interaction, correction', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001045'],"['Bose-Einstein correlations in pairs of charged kaons produced in a sample of 3.9 million hadronic Z0 decays have been measured with the OPAL experiment at LEP. Charged kaons were identified in the central tracking detector using their specific energy loss in the drift chamber gas. The correlation function was studied in two-jet events using a double ratio, formed by the number of like-sign pairs normalised by a reference sample in the data, divided by the same ratio in a Monte Carlo simulation. The enhancement at small values of the four-momentum difference of the pair was parametrised using a Gaussian function. The parameters of the Bose-Einstein correlations were measured to be lambda = 0.82+-0.22(+0.17,-0.12) for the strength and R0 = 0.56+-0.08(+0.08, -0.06) fm for the kaon source radius, where the first errors are statistical and the second systematic. Corrections for final-state interactions are discussed.']",['2000-01-20']
960,['eng'],"['King, B J']",['High Rate Neutrino Detectors for Neutrino Factories'],['Detectors and Experimental Techniques'],"['talk, Lyon 1999/07/05', 'neutrino, counters and detectors', 'neutrino nucleus, nuclear reaction', 'neutrino electron, elastic scattering', 'semiconductor detector, pixel', 'hydrogen, polarized target', 'deuterium, polarized target', 'muon+ muon-, storage ring', 'neutrino, particle source']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001043'],"[""Three types of high rate neutrino detectors for neutrino interaction physics at neutrino factories are discussed. High performance general-purpose detectors might collect event samples on the order of a billion events or more. This could greatly improve on existing analyses of neutrino interactions and also lead to new and important analysis topics including, for example, precise determinations of the CKM matrix elements |Vub| and |Vcb|. The potential of such general purpose detectors is illustrated with reference to a detector, presented previously in reference hep-ex/9907033, that is structured around a novel and compact vertexing and tracking neutrino target comprising a stack of CCD pixel devices. Design ideas and prospects are also discussed for two types of specialized detectors: (i) polarized targets filled with polarized solid protium-deuterium (HD), for unique and powerful studies of the nucleon's spin structure, and (ii) Fully active liquid tracking targets with masses of several tonnes for precise determinations of the weak mixing angle, from the total cross-section for neutrino-electron scattering. All three detector types pose severe technical challenges but their utilization could add significantly to the physics motivation for neutrino factories.""]",['2000-01-20']
961,['eng'],"['Blücher, E']","[""$\\epsilon$' / $\\epsilon$ Results from KTeV""]",['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'K0, hadronic decay', 'K0(L), secondary beam', 'K0(S), secondary beam', 'mass spectrum, two-pion', 'violation, CP', 'calorimeter', 'magnetic spectrometer', 'experimental results', 'Batavia TEVATRON PS', 'K0 --> pi+ pi-', 'K0 --> 2pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001042'],['The first measurement of epsilon-prime / epsilon from the KTeV experiment at Fermilab is described.'],['2000-01-19']
962,['eng'],"['Gorham, P W']",['On the possibility of radar echo detection of ultra-high energy cosmic ray- and neutrino-induced extensive air showers'],['Detectors and Experimental Techniques'],"['cosmic radiation, primary', 'neutrino, cosmic radiation', 'showers, air', 'ionization', 'experimental methods, proposed', 'radiation, electromagnetic', 'reflection', 'shower detector']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001041'],"[""We show that cosmic-ray air showers resulting from primary particles with energies above 10^{18} eV should be straightforward to detect with radar ranging techniques, where the radar echoes are produced by scattering from the column of ionized air produced by the shower. If our analysis is correct, such systems could provide highly complementary measurements of air showers detected in existing and planned ground arrays such as the Fly's Eye or the Auger Project, and crucial additional information for proposed space missions such as OWL/AirWatch. The technique is particularly sensitive to showers that are transverse to and relatively distant from the detector, and is thus effective in characterization of penetrating horizontal showers such as those that might be induced by ultra-high energy neutrino primaries.""]",['2000-01-18']
963,['eng'],"['Artamonov, S A', 'Baru, S E', 'Blinov, A E', 'Blinov, V E', 'Bondar, A E', 'Bukin, A D', 'Chilingarov, A G', 'Denisov, N F', 'Eidelman, S I', 'Eidelman, Yu I', 'Groshev, V R', 'Inozemtsev, N I', 'Kezerashvili, G Ya', 'Kiselev, V A', 'Klimenko, S G', 'Kolachev, G M', 'Kuper, E A', 'Kurdadze, L M', 'Lelchuk, M Yu', 'Mishnev, S I', 'Nikitin, S A', 'Onuchin, A P', 'Pakhtusova, E V', 'Panin, V S', 'Petrov, V V', 'Protopopov, I Ya', 'Saldin, E L', 'Shamov, A G', 'Shatunov, Yu M', 'Shwartz, B A', 'Sidorov, V A', 'Skovpen, Yu I', 'Skrinsky, A N', 'Tayursky, V A', 'Telnov, V I', 'Temnykh, A B', 'Tikhonov, Yu A', 'Tumaikin, G M', 'Undrus, A E', 'Vorobiev, A I', 'Yurkov, M V', 'Zhilich, V N', 'Zholents, A A']",['High Precision Mass Measurements in $\\psi$ and $\\Upsilon$ Families Revisited'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'cross section, energy dependence', 'beam, energy', 'resonance, depolarization', 'psi mesons, mass', 'J/psi(3100)', 'psi(3685)', 'upsilon mesons, mass', 'Upsilon(9460)', 'Upsilon(10020)', 'Upsilon(10355)', 'electron, mass', 'radiative correction', 'experimental results', 'Novosibirsk Stor4']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001040'],['High precision mass measurements in $\\Psi$ and $\\Upsilon$ families performed in 1980-1984 at the VEPP-4 collider with OLYA and MD-1 detectors are revisited. The corrections for the new value of the electron mass are presented. The effect of the updated radiative corrections has been calculated for the $J/\\Psi(1S)$ and $\\Psi(2S)$ mass measurements.'],['2000-01-18']
964,['eng'],"['Kneringer, E']",['Higgs Searches at LEP2 with the ALEPH Detector'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 1999/02/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, decay modes', 'supersymmetry', 'Higgs particle, mass', 'lower limit', 'Z0, associated production', 'Z0, decay modes', 'Higgs particle, pair production', 'Higgs particle, neutral particle', 'Higgs particle, charged particle', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'electron positron --> Z0 Higgs particle', 'electron positron --> 2Higgs particle', 'Higgs particle --> 2beauty', 'Higgs particle --> tau+ tau-', '161, 172, 183, 189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001037'],['Data collected with the ALEPH detector at centre-of-mass energies between 130 and 189 GeV are used to search for Higgs bosons of the standard model and its supersymmetric extensions. No evidence for a Higgs particle has been found in 256 pb^-1 of LEP2 data. Mass exclusion limits were set.'],['2000-01-17']
965,['eng'],"['Bouchez, J']",['Confidence belts on bounded parameters'],['Particle Physics - Experimental Results'],['statistical analysis'],['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001036'],['We show that the unified method recently proposed by Feldman and Cousins to put confidence intervals on bounded parameters cannot avoid the possibility of getting null results. A modified bayesian approach is also proposed (although not advocated) which ensures no null results and proper coverage.'],['2000-01-14']
966,['eng'],"['Harris, D A', 'Para, A']",['Neutrino Oscillation Appearance Experiment using Nuclear Emulsion and Magnetized Iron'],['Particle Physics - Experimental Results'],"['talk, Lyon 1999/07/05', 'neutrino, oscillation', 'neutrino, beam', 'neutrino nucleus, interaction', 'charged current', 'lepton, particle identification', 'lepton, charge', 'neutrino, mixing angle', 'violation, CP', 'matter, effect', 'nuclear emulsion, sandwich', 'iron', 'magnetic field, effect', 'experimental methods, proposed']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001035'],"['This report describes an apparatus that could be used to measure both the identity and charge of an outgoing lepton in a charged current neutrino interaction. This capability in a massive detector would allow the most comprehensive set of neutrino oscillation physics measurements. By measuring the six observable transitions between initial and final state neutrinos, one would be able to measure all elements of the neutrino mixing matrix, as well as search for CP violation, and matter effects. If the measured matrix is not unitary, then one would also have an unambiguous determination of sterile neutrinos. Emulsion is considered as the tracking medium, and different techniques are discussed for the application of a magnetic field.']",['2000-01-14']
967,['eng'],"['Robertson, R G H']",['Neutrino Mass and Oscillations'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'neutrino, mass', 'neutrino, oscillation', 'neutrino, beam', 'fission, particle source', 'neutrino, cosmic radiation', 'neutrino, solar', 'neutrino, energy spectrum', 'MSW effect', 'flavor, 3', 'neutrino, sterile', 'tritium, semileptonic decay', 'double-beta decay', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001034'],"['Current evidence for neutrino oscillation is reviewed, some areas for closer investigation are suggested, and a plausible future experimental program is summarized.']",['2000-01-13']
968,['eng'],"['Telnov, V I']",['Some problems in plasma suppression of beam-beam interactions at muon colliders'],['Accelerators and Storage Rings'],"['talk, Montauk 1999/09/27', 'muon+ muon-, storage ring', 'scattering, beam-beam', 'correction, plasma', 'lithium, plasma', 'background, hadronic', 'photon nucleus, nuclear reaction', 'luminosity']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001033'],"[""The idea of plasma suppression of beam-beam effects at muon colliders is discussed. It is shown that one should take into account collisions in the plasma that were ignored before. Rough estimates show that this effect leads to a fast ``recovery'' of the beam magnetic field. For beam parameters characteristic for muon colliders the suppression of the magnetic component of the beam field (1/2 of the total force) is almost absent. It is also shown that the presence of the dense plasma (Li jet) at the interaction point leads to enormous hadronic background (due to photo-nuclear reactions) in the detector, about 10^{7} particles per crossing at large angles which creates serious problems for experimentation.""]",['2000-01-13']
969,['eng'],"['Telnov, V I']",['Coherent $e^{+}e^{-}$ pair creation at high energy muon colliders'],['Accelerators and Storage Rings'],"['talk, Montauk 1999/09/27', 'muon+ muon-, colliding beams', 'electron, pair production', 'beam, radiation', 'coherent interaction', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001031'],['It is shown that at muon colliders with the energy in the region of 100 TeV the process of coherent pair creation by the muon in the field of the opposing beam becomes important and imposes some limitations on collider parameters.'],['2000-01-13']
970,['eng'],"['Telnov, V I']","['Problems and stoppers for $\\gamma\\gamma$, $\\gamma\\mu$, $\\mu p$ colliders using very high energy muons']",['Accelerators and Storage Rings'],"['talk, Montauk 1999/09/27', 'electron positron, linear collider', 'linear collider, proposed', 'radiation, laser', 'photon electron, Compton scattering', 'muon+ muon-, colliding beams', 'photon muon, Compton scattering', 'photon muon, colliding beams', 'muon p, colliding beams', 'photon photon, colliding beams', 'luminosity', 'cross section']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001030'],"[""It is well known that at linear e^+e^-(e^-e^-) colliders using laser backscattering one can obtain colliding gamma-gamma, gamma-electron beams with energy and luminosity comparable to those in e^+e^- collisions. In this paper, it is explained why this can not be done at high energy muon colliders. Due to several physics reasons the gamma-gamma luminosity is suppressed here by a factor of 10^{14} ! Another option -- gamma's from a linear collider and muons from a muon collider -- is also discussed (and has no sense either). Of course, one can study gamma^*-muon and gamma^*-gamma^* interactions at muon colliders in collisions with virtual photons as it is done now at e^+e^- storage rings. Muon-proton colliders are attractive only if the proton beam is cooled and has the same parameters as the muon beam, in which case L_{\\mu p} \\sim L_{\\mu\\mu}.""]",['2000-01-13']
971,['eng'],"['Telnov, V I']",['High energy photon colliders'],['Accelerators and Storage Rings'],"['talk, Tokyo 1999/10/11', 'electron positron, linear collider', 'linear collider, proposed', 'photon photon, colliding beams', 'photon electron, colliding beams', 'Compton scattering, backscatter', 'radiation, laser', 'optics, laser', 'luminosity', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001029'],"['Using the laser backscattering method at future linear colliders one can obtain gamma-gamma and gamma-electron colliding beams (photon colliders) with energy and luminosity comparable to that in e^+e^- collisions. This option has been included in the pre-conceptual designs of linear colliders and in work on a Technical Design Report which is in progress. The physics motivation for photon colliders is quite clear. The proof of its technical feasibility and the search for the best solutions is of first priority now. A key element of a photon collider is a laser with high peak power and repetition rate. One very promising way to overcome this problem is the optical cavity approach which is discussed in this paper. A very high gamma-gamma luminosity could be achieved by further decreasing the beam emittances. This will be very challenging. One possible way is laser cooling of electron beams. This method is discussed in my second talk at this symposium. The solution to the first problem is vital for photon colliders and provides an interesting physics program. Solution of the second problem makes photon colliders a very powerful instrument for study of matter, the best for study of many phenomena. How to achieve these goals is the subject of this talk.']",['2000-01-13']
972,['eng'],"['Telnov, V I']",['Laser cooling of electron beams at linear colliders'],['Accelerators and Storage Rings'],"['talk, Tokyo 1999/10/11', 'electron positron, linear collider', 'linear collider, proposed', 'beam cooling, laser', 'optics, laser', 'beam emittance', 'electron, polarization', 'Compton scattering', 'photon photon, colliding beams']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001028'],"['A method of electron beam cooling is considered which can be used for linear colliders. The electron beam is cooled during collision with focused powerful laser pulse. The ultimate transverse emittances are much below those achievable by other methods. This method is especially useful for high energy gamma-gamma colliders. In this paper we review and analyse limitations in this method, also discuss a new method of obtaining very high laser powers required for the laser cooling, radiation conditions and finaly present a possible scheme for the laser cooling of electron beams.']",['2000-01-13']
973,['eng'],"['Kulchitskii, Yu A', 'Vinogradov, V B']",['On the Parameterization of the Longitudinal Hadronic Shower Profiles in Combined Calorimetry'],['Detectors and Experimental Techniques'],"['calorimeter, showers', 'showers, hadronic', 'parametrization', 'showers, spatial distribution', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001027'],['The extension of the longitudinal hadronic shower profile parameterization which takes into account non-compensations of calorimeters and the algorithm of the longitudinal hadronic shower profile curve making for a combined calorimeter are suggested. The proposed algorithms can be used for data analysis from modern combined calorimeters like in the ATLAS detector at the LHC.'],['2000-01-13']
974,['eng'],"['Molzon, W R']",['Quark Mixing Matrix Studies and Lepton Flavor Violation Searches Using Rare Decays of Kaons'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'K, rare decay', 'quark, mixing angle', 'flavor, violation', 'Kobayashi-Maskawa angle', 'K, semileptonic decay', 'mass spectrum, (muon electron)', 'mass spectrum, (pi muon electron)', 'K, leptonic decay', 'Feynman graph', 'K0(L), leptonic decay', 'transverse momentum, spectra', 'mass spectrum, dilepton', 'experimental results', 'Brookhaven PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001024'],"['I review recent results from experiments on rare decays of kaons, concentrating on searches for lepton flavor violation (LFV) and on measurements of quark mixing (CKM) matrix elements. The LFV results are the culmination of 15 years of experimentation at Brookhaven National Laboratory and are unlikely to be improved upon soon. The CKM studies derive from measurements of decay rates of charged and neutral kaons into lepton anti-lepton pairs, both with and without a charged or neutral pion. I discuss recent results and prospects for improved measurements that could provide an unambiguous test of the Standard Model explanation for CP violation. This paper is the written version of a talk presented at the Lepton-Photon Conference in August 1999.']",['2000-01-12']
975,['eng'],"['Bethke, Siegfried']",['Standard Model Physics at LEP'],['Particle Physics - Experimental Results'],"['review, Nijmegen 1999/08/08', 'electron positron, colliding beams', 'electron positron, annihilation', 'electroweak interaction, validity test', 'Z0, mass', 'Z0, width', 'strong interaction, coupling constant', 'Weinberg angle', 'neutrino, flavor', 'Higgs particle, mass', 'W, pair production', 'W, mass', 'coupling, (3gauge boson)', 'jet, electroproduction', 'quantum chromodynamics, validity test', 'hadronization', 'event shape analysis', 'experimental results', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001023'],"['Selected topics on precision tests of the Standard Model of the Electroweak and the Strong Interaction at the LEP $e^+e^-$ collider are presented, including an update of the world summary of measurements of $\\alpha_s$, representing the state of knowledge of summer 1999. This write-up of lecture notes consists of a reproduction of slides, pictures and tables, supplemented by a short descriptive text and a list of relevant references.']",['2000-01-12']
976,['eng'],"['Newman, P']",['Recent Low x and Diffractive Collider Data'],['Particle Physics - Experimental Results'],"['review, Durham 1999/09/19', 'positron p, colliding beams', 'anti-p p, colliding beams', 'electron positron, colliding beams', 'exchange, two-photon', 'factorization', 'diffraction', 'jet, electroproduction', 'jet, hadroproduction', 'production, small-angle', 'Regge poles', 'photon photon, interaction', 'quantum chromodynamics', 'small-x', 'Altarelli-Parisi equation', 'Lipatov equation', 'cross section, energy dependence', 'experimental results', 'DESY HERA Stor', 'Batavia TEVATRON Coll', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001022'],['Selected recent data from collider experiments pertaining to the understanding of QCD at low Bjorken-x are reviewed. The status of QCD and Regge factorisation in hard diffractive interactions is discussed in terms of data from HERA and the Tevatron. The possibility of anomalous behaviour in the measurements from LEP. Data from all three colliders that are sensitive to possible BFKL effects are presented and different interpretations are discussed.'],['2000-01-12']
977,['eng'],"['Bottai, S', 'Perrone, L']",['Simulation of UHE muons propagation for GEANT3'],['Detectors and Experimental Techniques'],"['muon, transport theory', 'matter', 'cross section, formula', 'energy loss', 'lepton, pair production', 'bremsstrahlung', 'photon nucleus, nuclear reaction', 'differential cross section', 'total cross section', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001018'],['A simulation package for the transport of high energy muons has been developed. It has been conceived to replace the muon propagation software modules implemented in the detector simulation program GEANT3. Here we discuss the results achieved with our package and we check the agreement with numerical calculations up to 10**8 GeV.'],['2000-01-10']
978,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']","['A study of the f0(1370), f0(1500), f0(2000) and f2(1950) observed in the centrally produced $4\\pi$ final states']",['Particle Physics - Experimental Results'],"['p p, exclusive reaction', 'central region', 'scalar meson, hadroproduction', 'tensor meson, hadroproduction', 'meson resonance, hadronic decay', 'mass spectrum, (2pi+ 2pi-)', 'mass spectrum, (2Phi(1020))', 'mass spectrum, (2K*(892))', 'f0(1370)', 'f0(1500)', 'postulated particle, f0(2000)', 'postulated particle, f2(1950)', 'transverse momentum, dependence', 'angular dependence', 'momentum transfer, dependence', 'slope', 'magnetic spectrometer, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p 2pi+ 2pi-', 'p p --> 2p pi+ pi- 2pi0', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001017'],"[""The production and decay properties of the f0(1370), f0(1500), f0(2000) and f2(1950) have been studied in central pp interactions at 450 GeV/c. The dPT, phi and |t| distributions of these resonances are presented. For the J = 0 states, the f0(1370) and f0(2000) have similar dPT and phi dependences. These are different to the dPT and phi dependences of the f0(980), f0(1500) and f0(1710). For the J = 2 states the f2(1950) has different dependences to the f2(1270) and f2'(1520). This shows that the dPT and phi dependences are not just J phenomena.""]",['2000-01-10']
979,['eng'],"['Wall, D']","['Search for Nucleon Decay with Final States $l+\\eta, \\overline\\nu \\eta,$ and $\\overline\\nu \\pi+,0$ using Soudan 2']",['Particle Physics - Experimental Results'],"['nucleon, semileptonic decay', 'decay, search for', 'p, lifetime', 'n, lifetime', 'lower limit', 'eta, radiative decay', 'eta, hadronic decay', 'calorimeter, experimental results', 'deep underground detector, Soudan', 'p --> eta muon+', 'p --> eta positron', 'n --> eta antineutrino', 'nucleon --> pi antineutrino', 'eta --> 2photon', 'eta --> 3pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001015'],"['We have searched for nucleon decay into five two-body final states using a 4.4 kiloton-year fiducial exposure of the Soudan 2 iron tracking calorimeter. For proton decay into the fully visible final states mu+ eta and e+ eta, we observe zero and one event, respectively, that satisfy our search criteria for nucleon decay. The lifetime lower limits (tau/B) thus implied are 89 x 10^30 years and 81 x 10^30 years at 90% confidence level. For neutron decay into nubar eta, we obtain the lifetime lower limit 71 x 10^30 years. Limits are also reported for neutron decay into nubar pi0, and for proton decay into nubar pi+.']",['2000-01-06']
980,['eng'],"['Mele, S']",['Recent Results from the L3 Experiment'],['Particle Physics - Experimental Results'],"['talk, Moscow 1999/05/27', 'electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'quark, pair production', 'gauge boson, pair production', 'Z0', 'W', 'photon, multiple production', 'gauge boson, electroproduction', 'channel cross section, energy dependence', 'angular distribution', 'coupling, (3gauge boson)', 'new interaction, search for', 'gravitation, higher-dimensional', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', '181.7-188.7 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001014'],"['A data sample corresponding to an integrated luminosity of 232pb^-1 was collected in 1997 and 1998 by the L3 experiment at LEP in e+e- collisions at centre-of-mass energies between 181.7GeV and 188.7GeV. Pair production of fermions and bosons is studied and compared with the Standard Model expectations. Events with a single detected photon or W boson are also considered. The measurement of several Standard Model cross sections is discussed. The presence and the magnitude of triple couplings of charged and neutral electroweak gauge bosons is investigated. These processes are used to probe New Physics beyond the Standard Model, including the existence of extra spatial dimensions.']",['2000-01-06']
981,['eng'],"['Csorna, S E']","[""Measurement of the $B^{0}$ and $B^{+}$ meson masses from $B^{0} \\to \\psi(') K_{S}$ and $B^{+} \\to \\psi(') K^{+}$ decays""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'J/psi(3100)', 'psi(3685)', 'mass spectrum, (psi mesons K)', 'B+, mass', 'B0, mass', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> psi mesons K0(S)', 'B+ --> psi mesons K+', 'approx. 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001013'],"[""Using 9.6 million B meson pairs collected with the CLEO detector, we have fully reconstructed 135 B0 -> psi(') K_S and 526 B+ -> psi(') K+ candidates with very low background. We fitted the psi(')K invariant mass distributions of these B meson candidates and measured the masses of the neutral and charged B mesons to be M(B0)=5279.1+-0.7[stat]+-0.3[syst] MeV/c^2 and M(B+)=5279.1+-0.4[stat]+-0.4[syst] MeV/c^2. The precision is a significant improvement over previous measurements.""]",['2000-01-06']
982,['eng'],"['Marler, J', 'McCauley, T', 'Reucroft, S', 'Swain, J D', 'Budil, D', 'Kolaczkowski, Z']",['Studies of Avalanche Photodiode Performance in a High Magnetic Field'],['Detectors and Experimental Techniques'],"['scintillation counter, readout', 'semiconductor, optical', 'magnetic field, high', 'performance', 'calorimeter, electromagnetic', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001011'],['We report the results of exposing a Hamamatsu avalanche photodiode (APD) to a 7.9 Tesla magnetic field. The effect of the magnetic field on the gain of the APD is shown and discussed. We find APD gain to be unaffected in the presence of such a magnetic field.'],['2000-01-05']
983,['eng'],"['Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Perera, L P', 'Zhou, G J', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, H N', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Pedlar, T K', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V']",['Study of Two-Body B Decays to Kaons and Pions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> pi+ pi-', 'B --> K pi', 'B+ --> pi+ pi0', 'B --> K anti-K', 'approx. 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001010'],"['We have studied charmless hadronic decays of B mesons into two-body final states with kaons and pions and observe three new processes with the following branching fractions: BR(B-> pi+ pi-) = (4.3^{+1.6}_{-1.4} \\pm 0.5) \\times 10^{-6}, BR(B-> K0 pi0) = (14.6^{+5.9+2.4}_{-5.1-3.3}) \\times 10^{-6}, and BR(B-> K+- pi0) = (11.6^{+3.0+1.4}_{-2.7-1.3}) \\times 10^{-6}. We also update our previous measurements for the decays B->K+- pi-+ and B-> K0 pi+-.']",['2000-01-05']
984,['eng'],"['Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Perera, L P', 'Zhou, G J', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, H N', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Pedlar, T K', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A']",['Measurement of Charge Asymmetries in Charmless Hadronic B Meson Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'charge, asymmetry', 'violation, CP', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> K pi', 'B --> eta(958) K', 'B --> omega(783) pi', 'approx. 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001009'],"[""We search for CP-violating asymmetries (Acp) in the B meson decays to K+- pi-+, K+- pi0, Ks pi+-, K+- eta', and omega pi+-. Using 9.66 million Upsilon(4S) decays collected with the CLEO detector, the statistical precision on Acp is in the range of \\pm 0.12 to \\pm 0.25 depending on decay mode. While CP-violating asymmetries of up to \\pm 0.5 are possible within the Standard Model, the measured asymmetries are consistent with zero in all five decay modes studied.""]",['2000-01-05']
985,['eng'],"['Giacomelli, Giorgio']",['Highlights in Neutrino and Astroparticle Physics'],['Particle Physics - Experimental Results'],"['conference, review', 'San Miniato 1999/05/17', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino, solar', 'neutrino, astrophysics', 'muon, cosmic radiation', 'photon, cosmic radiation', 'p, decay', 'WIMP, search for', 'gravitational radiation', 'magnetic monopole', 'astrophysics, missing-mass', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001008'],['The main highlights from the papers presented at this workshop are briefly reviewed and discussed in a general context.'],['2000-01-05']
986,['eng'],"['Alavi-Harati, A', 'Albuquerque, I F M', 'Alexopoulos, T', 'Arenton, M', 'Arisaka, K', 'Averitte, S', 'Barker, A R', 'Bellantoni, L', 'Bellavance, A', 'Belz, J E', 'Ben-David, R', 'Bergman, D R', 'Blücher, E', 'Bock, G J', 'Bown, C', 'Bright, S T', 'Cheu, E', 'Childress, S', 'Coleman, R', 'Corcoran, M D', 'Corti, G', 'Cox, B', 'Crisler, M B', 'Erwin, A R', 'Ford, R', 'Glazov, A', 'Golossanov, A', 'Graham, G', 'Graham, J', 'Hagan, K', 'Halkiadakis, E', 'Hanagaki, K', 'Hazumi, M', 'Hidaka, S', 'Hsiung, Y B', 'Jejer, V', 'Jennings, J', 'Jensen, D A', 'Kessler, R S', 'Kobrak, H G E', 'La Due, J', 'Lath, A', 'Ledovskoy, A A', 'McBride, P', 'McManus, A P', 'Mikelsons, P', 'Monnier, E', 'Nakaya, T', 'Nelson, K S', 'Nguyen, H', ""O'Dell, Vivian R"", 'Pang, M', 'Pordes, R', 'Prasad, V', 'Qiao, C', 'Quinn, B', 'Ramberg, E J', 'Ray, R E', 'Roodman, A', 'Sadamoto, M', 'Schnetzer, S R', 'Senyo, K', 'Shanahan, P', 'Shawhan, P S', 'Slater, W', 'Solomey, N', 'Somalwar, S V', 'Stone, R L', 'Suzuki, I', 'Swallow, E C', 'Swanson, R A', 'Taegar, S A', 'Tesarek, R J', 'Thomson, G B', 'Toale, P A', 'Tripathi, A K', 'Tschirhart, R S', 'Wah, Y W', 'Wang, J', 'White, H B', 'Whitmore, J', 'Winstein, Bruce D', 'Winston, R', 'Yamanaka, T', 'Zimmerman, E D']",['Search for the Decay $K_{L} \\to \\pi^{0}\\mu^{+}\\mu^{-}$'],['Particle Physics - Experimental Results'],"['K0(L), semileptonic decay', 'K0(L), secondary beam', 'violation, CP', 'K0(L), branching ratio', 'transverse momentum, spectra', 'mass, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi0 muon+ muon-']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001006', 'http://fnalpubs.fnal.gov/archive/2000/pub/Pub-00-022-E.html']","['We report on a search for the decay \\klpimumu carried out as a part of the KTeV experiment at Fermilab. This decay is expected to have a significant $CP$ violating contribution and a direct measurement will either support the CKM mechanism for CP violation or point to new physics. Two events were observed in the 1997 data with an expected background of $0.87 \\pm 0.15$ events, and we set an upper limit \\BR{\\klpimumu} $ <3.8 \\times 10^{-10}$ at the 90% confidence level.']",['2000-01-28']
987,['eng'],"['Alavi-Harati, A']",['Observation of the Decay $K_{L} \\to \\mu^{+}\\mu^{-}\\gamma\\gamma$'],['Particle Physics - Experimental Results'],"['K0(L), radiative decay', 'K0(L), secondary beam', 'K0(L), branching ratio', 'angular distribution, two-photon', 'transverse momentum, spectra', 'mass, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> muon+ muon- 2photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001005'],"['We have observed the decay $K_L\\to \\mu^+\\mu^- \\gamma \\gamma$ at the KTeV experiment at Fermilab. This decay presents a formidable background to the search for new physics in $K_L\\to\\pi^0\\mu^+\\mu^-$. The 1997 data yielded a sample of 4 signal events, with an expected background of 0.155 $\\pm$ 0.081 events. The branching ratio is ${\\mathcal B}(K_L\\to \\mu^+\\mu^- \\gamma \\gamma$) $ = (10.4^{+7.5}_{-5.9} {\\rm (stat)} \\pm 0.7 {\\rm (sys)})\\times 10^{-9}$ with $m_{\\gamma\\gamma} \\geq 1 {\\rm MeV/c}^2$, consistent with a QED calculation which predicts $(9.1\\pm 0.8)\\times 10^{-9}$.']",['2000-01-05']
988,['eng'],"['Bianco, S', 'Fabbri, F L', 'Giardoni, M', 'Passamonti, L', 'Russo, V', 'Sarwar, S', 'Zallo, A', 'Carrillo, S', 'Méndez, H', 'Gianini, G', 'Anjos, J C', 'Bediaga, I', 'Göbel, C', 'Laudo, A', 'Magnin, J', 'Miranda, J A', 'Pepe, I M', 'Simão, F R A', 'Sánchez, A', 'Reis, A']",['The upgraded Outer em calorimeter of FOCUS at Fermilab'],['Detectors and Experimental Techniques'],"['talk, Lisbon 1999/06/13', 'calorimeter, electromagnetic', 'lead', 'scintillation counter, organic compounds', 'efficiency', 'energy resolution', 'performance', 'charmed particle, photoproduction', 'Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912066'],"['Operational performance, algorithms, stability and physics results of the Outer em calorimeter of FOCUS are overviewed.']",['2000-02-14']
989,['eng'],"['Artuso, M', 'Ayad, R', 'Boulahouache, C', 'Bukin, K', 'Dambasuren, E', 'Karamov, S', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'Danko, I', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Perera, L P', 'Zhou, G J', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lohner, M', 'Magerkurth, A', 'Meyer, T O', 'Mistry, N B', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Bean, A', 'Besson, D', 'Davis, R', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Urheim, J', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Hufnagel, D', 'Kagan, H', 'Kass, R', 'Pedlar, T K', 'Schwarthoff, H', 'Thayer, J B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Pavlunin, V', 'Cronin-Hennessy, D', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T']",['Search for the Decay $\\overline{B}^{0} \\to D^{*0}\\gamma$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'anti-B0, radiative decay', 'D*(2010)', 'anti-B0, pair production', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'anti-B0 --> D*(2010) photon', 'beauty --> strangeness photon', '10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001002'],"['We report results of a search for the rare radiative decay B0 -> D*0 gamma. Using 9.7 million BB meson pairs collected with the CLEO detector at the Cornell Electron Storage Ring, we limit Br(B0->D*0 gamma) < 5.0 * 10^-5 at 90% CL. This provides evidence that anomalous enhancement is absent in W-exchange processes and that weak radiative B decays are dominated by the short-distance b -> s gamma mechanism in the Standard Model.']",['2000-01-04']
990,['eng'],"['Li, H B', 'Liu, Y', 'Chang, C C', 'Chang, C Y', 'Chao, J H', 'Chen, C P', 'Chen, T Y', 'He, M', 'Hou, L', 'Kiang, G C', 'Lai, W P', 'Lee, S C', 'Li, J', 'Lu, J G', 'Mao, Z P', 'Sheng, H Y', 'Su, R F', 'Teng, P K', 'Wang, C W', 'Wang Shui Cai', 'Wong, H T', 'Yeh, T R', 'Zhang, Z Y', 'Zhao, D X', 'Zhao, S Q', 'Zhou, Z Y', 'Zhuang, B A']",['A CsI(Tl) Scintillating Crystal Detector for the Studies of Low Energy Neutrino Interactions'],['Detectors and Experimental Techniques'],"['scintillation counter, crystal', 'cesium, iodine', 'antineutrino electron, interaction', 'antineutrino nucleus, nuclear reaction', 'antineutrino/e', 'optics, absorption', 'radiation, yield', 'analog-to-digital converter', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001001'],"['Scintillating crystal detector may offer some potential advantages in the low-energy, low-background experiments. A 500~kg CsI(Tl) detector to be placed near the core of Nuclear Power Station II in Taiwan is being constructed for the studies of electron-neutrino scatterings and other keV$-$MeV range neutrino interactions. The motivations of this detector approach, the physics to be addressed, the basic experimental design, and the characteristic performance of prototype modules are described. The expected background channels and their experimental handles are discussed.']",['2000-01-04']
991,['eng'],"['Sanders, D', 'Riley, C P', 'Cremaldi, L M', 'Summers, D', 'Petravick, D']",['Working with Arrays of Inexpensive EIDE Disk Drives'],['Detectors and Experimental Techniques'],"['talk, Chicago 1998/08/31', 'data management', 'computer, hardware', 'technology', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912067'],"[""In today's marketplace, the cost per Terabyte of disks with EIDE interfaces is about a third that of disks with SCSI. Hence, three times as many particle physics events could be put online with EIDE. The modern EIDE interface includes many of the performance features that appeared earlier in SCSI. EIDE bus speeds approach 33 Megabytes/s and need only be shared between two disks rather than seven disks. The internal I/O rate of very fast (and expensive) SCSI disks is only 50 per cent greater than EIDE disks. Hence, two EIDE disks whose combined cost is much less than one very fast SCSI disk can actually give more data throughput due to the advantage of multiple spindles and head actuators. We explore the use of 12 and 16 Gigabyte EIDE disks with motherboard and PCI bus card interfaces on a number of operating systems and CPUs. These include Red Hat Linux and Windows 95/98 on a Pentium, MacOS and Apple's Rhapsody/NeXT/UNIX on a PowerPC, and Sun Solaris on a UltraSparc 10 workstation.""]",['2000-01-03']
992,['eng'],"['Gladilin, L K']",['Charm Hadron Production Fractions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, charm', 'quark, pair production', 'quark, fragmentation', 'charmed particle, electroproduction', 'D*(2010)', 'D/s+', 'D0', 'D+', 'Lambda/c+', 'charmed particle, hadronic decay', 'yield, ratio', 'channel cross section', 'experimental results', 'CERN LEP Stor', 'Cornell CESR Stor', 'DESY DORIS Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912064'],"['The world average values for the probabilities that a charm quark fragments into D^*+ and Ds^+ have been calculated to be f(c->D^*+)=0.235+/-0.007(+/-0.007) and f(c->Ds^+)=0.101+/-0.009(+/-0.025), respectively. The average values for D^0, D^+ and Lambda_c^+ have been also calculated.']",['1999-12-28']
993,['eng'],"['Glamazdin, A V', 'Gorbenko, V G', 'Levchuk, L G', 'Pomatsalyuk, R I', 'Rubashkin, A L', 'Sorokin, P V', 'Dale, D S', 'Doyle, B', 'Gorringe, T P', 'Korsch, W', 'Zeps, V', 'Chen, J P', 'Chudakov, E A', 'Nanda, S', 'Saha, A', 'Gasparian, A']",['Electron Beam Møller Polarimeter at Jlab Hall a'],['Detectors and Experimental Techniques'],"['talk, Dubrovnik 1998/11/03', 'electron, linear accelerator', 'electron, polarized beam', 'beam monitoring, polarization', 'electron electron, elastic scattering', 'iron, target', 'target, ferromagnet', 'bending magnet', 'quadrupole lens', 'Newport News CEBAF Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912063'],"['As part of the spin physics program at Jefferson Laboratory (JLab), a Mø ller polarimeter was developed to measure the polarization of electron beam of energies 0.8 to 5.0 GeV. A unique signature for Mø ller scattering is obtained using a series of three quadrupole magnets which provide an angular selection, and a dipole magnet for energy analysis. The design, commissioning, and the first results of the polarization measurements of this polarimeter will be presented as well as future plans to use its small scattering angle capabilities to investigate physics in the very low $Q^2$ regime.']",['1999-12-28']
994,['eng'],"['Formaggio, J A', 'Zimmerman, E D', 'Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bugel, L', 'Case, S', 'Conrad, J M', 'Drucker, R B', 'Fleming, B T', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McFarland, K S', 'McNulty, C', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H M', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Vakili, M', 'Vaitaitis, A G', 'Wu, V', 'Yang, U K', 'Yu, J', 'Zeller, G P']",['Search for a $33.9 MeV/c^{2}$ Neutral Particle in Pion Decay'],['Particle Physics - Experimental Results'],"['pi, rare decay', 'new particle, search for', 'neutral particle, weak interaction', 'pi, branching ratio', 'upper limit', 'experimental results', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912062'],"[""The E815 (NuTeV) neutrino experiment has performed a search for a 33.9 MeV/c^2 weakly-interacting neutral particle produced in pion decay. Such a particle may be responsible for an anomaly in the timing distribution of neutrino interactions in the KARMEN experiment. E815 has searched for this particle's decays in an instrumented decay region; no evidence for this particle was found. The search is sensitive to pion branching ratios as low as 10^-13.""]",['1999-12-27']
995,['eng'],"['Abbott, B']",['Hard Single Diffraction in $\\overline{p}p$ Collisions at $\\sqrt{s}$ = 630 and 1800 GeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'diffraction', 'rapidity, gap', 'multiplicity, spectra', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912061', 'http://arXiv.org/abs/hep-ex/?9912061']","[""Using the D0 detector, we have studied events produced in proton-antiproton collisions that contain large forward regions with very little energy deposition (``rapidity gaps'') and concurrent jet production at center-of-mass energies of root-s = 630 and 1800 Gev. The fractions of forward and central jet events associated with such rapidity gaps are measured and compared to predictions from Monte Carlo models. For hard diffractive candidate events, we use the calorimeter to extract the fractional momentum loss of the scattered protons.""]",['1999-12-24']
996,['eng'],"['Kafka, T']",['Recent atmospheric neutrino results from Soudan 2'],['Particle Physics - Experimental Results'],"['talk, Paris 1999/09/06', 'neutrino/mu, cosmic radiation', 'neutrino/e, cosmic radiation', 'flux, ratio', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, Soudan', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912060'],"['An updated measurement of the atmospheric nu_mu/nu_e ratio-of-ratios, 0.68+-0.11+-0.06, has been obtained using a 4.6-kty exposure of the Soudan-2 iron tracking calorimeter. The L/E distributions have been analyzed for effects of nu_mu -> nu_x oscillations, and an allowed region in the Delta m^2 vs. sin^2 2 theta plane has been determined.']",['1999-12-24']
997,['eng'],[],"[""Two-body B Meson Decays to $\\eta$ and $\\eta$'""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, decay modes', 'K*(892)', 'eta', 'eta(958)', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> K*(892) eta', 'B --> eta(958) K', '10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912059'],"[""In a sample of 19 million produced B mesons, we have observed the decays B -> eta K* and improved our previous measurements of B -> eta'K. The branching fractions we measure for these decay modes are BR(B+ -> eta K*+) = (26.4 +9.6-8.2 +- 3.3) x $10^{-6}$, BR(B0 -> eta K*0) = (13.8 +5.5-4.6 +- 1.6) x $10^{-6}$, BR(B+ -> eta' K+) = (80 +10-9 +- 7) x $10^{-6}$ and BR(B0 -> eta' K0) = (89 +18-16 +- 9) x $10^{-6}$. We have searched with comparable sensitivity for related decays and report upper limits for these branching fractions.""]",['1999-12-24']
998,['eng'],"['Kenji, A']",['Precise measurement of the b-quark fragmentation function in $Z^{0}$ boson decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, fragmentation function', 'model, fragmentation', 'B, decay', 'B, energy', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912058'],"['We have developed a new technique for inclusive reconstruction of the energy of B hadrons. The excellent efficiency and resolution of this technique allow us to make the most precise determination of the b-quark fragmentation function, using e+e- -> Z0 decays recorded in the SLD experiment at SLAC. We compared our measurement with the predictions of a number of fragmentation models. We excluded several of these models and measured the average scaled energy of weakly-decaying B hadrons to be <x_B>=0.714+-0.005(stat)+-0.007(syst) +-0.002(model dependence).']",['1999-12-24']
999,['eng'],[],['Study of Exclusive Radiative B Meson Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, radiative decay', 'vector meson, production', 'rho(770)', 'omega(783)', 'Phi(1020)', 'K*(892)', 'K*2(1430)', 'B, branching ratio', 'upper limit', 'violation, CP', 'decay, form factor', 'Kobayashi-Maskawa angle', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> K*(892) photon', 'B --> K*2(1430) photon', 'approx. 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912057'],"['We have investigated exclusive, radiative B meson decays to charmless mesons accumulated with the CLEO detector. The B -> K^*(892)\\gamma branching fractions are determined to be Br(B^0 -> K^{*0}(892)\\gamma) = (4.55 +0.72-0.68 +-0.34)\\times 10^-5 and Br(B^+ -> K^{*+}(892)\\gamma) = (3.76 +0.89-0.83 +-0.28)\\times 10^-5. We have searched for CP asymmetry in B -> K^*(892)\\gamma decays and measure Acp = +0.08 +-0.13 +-0.03. We also report the first observation of the decay B -> K^*_2(1430)\\gamma with a branching fraction of (1.66 +0.59-0.53 +-0.13)\\times 10^-5 and determine $Br(B -> K^*_2(1430)\\gamma)/Br(B -> K^*(892)\\gamma) = 0.39 +0.15-0.13 consistent with only one of two available theoretical models. No significant evidence for the decays B -> \\rho\\gamma and B^0 -> ømega\\gamma is found and we limit Br(B -> no evidence for the exotic decay B^0 -> \\phi\\gamma.']",['1999-12-24']
1000,['eng'],"['Saint-Denis, R D']",['Heavy Flavours in Collider Experiments'],['Particle Physics - Experimental Results'],"['review, experimental results', 'positron p, colliding beams', 'anti-p p, colliding beams', 'electron positron, colliding beams', 'quark, charm', 'quark, beauty', 'quark, truth', 'quark, pair production', 'p, structure function', 'gluon, momentum spectrum', 'B, decay', 'model, spectator', 'B+, lifetime', 'B0, lifetime', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'violation, CP', 'cross section', 'DESY HERA Stor', 'Batavia TEVATRON Coll', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912056'],['Current issues in the studies of Heavy Flavours in colliders are described with particular emphasis on experiments in which the UK is involved. Results on charm production at HERA are examined and compared to those at the Tevatron. B production rates at the Tevatron as well as the status of B lifetimes and mixing in the LEP collaborations and at the Tevatron are highlighted. The measurement of sin2beta from CDF is described as well as the most recent results on top physics at the Tevatron.'],['1999-12-23']
1001,['eng'],"['Adloff, C']",['Investigation of Power Corrections to Event Shape Variables measured in Deep-Inelastic Scattering'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'hadron, multiple production', 'event shape analysis', 'kinematics, Breit frame', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'correction, hadronization', 'parametrization', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912052', 'http://arXiv.org/abs/hep-ex/?9912052://www-h1.desy.de/h1/www/publications/htmlsplit/DESY-99-193.long.html']","['Deep-inelastic ep scattering data, taken with the H1 detector at HERA, are used to study the event shape variables thrust, jet broadening, jet mass, C parameter and two kinds of differential two-jet rate. The data cover a large range of the four-momentum transfer Q, which is considered to be the relevant energy scale, between 7 GeV and 100 GeV. The Q dependences of the mean values are compared with second order calculations of perturbative QCD applying power law corrections proportional to 1/Q^p to account for hadronization effects. The concept of power corrections is investigated by fitting simultaneously a non-perturbative parameter alpha_p and the strong coupling constant alpha_s.']",['1999-12-23']
1002,['eng'],"['Biebel, O']",['Determination of $\\alpha_{S}$ at 500 GeV from Event Shapes and Jet Rates'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'jet, electroproduction', 'event shape analysis', 'jet, multiplicity', 'hadron, multiple production', 'strong interaction, coupling constant', 'error', 'background', 'intermediate boson', 'quark, truth', 'beam, radiation', 'hadronization, effect', 'renormalization, dependence', 'perturbation theory, higher-order', 'numerical calculations, Monte Carlo', '500 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912051'],"['The potential of the TESLA linear e+e- collider to determine the strong coupling constant, alpha_S, at 500 GeV is investigated. Experimental complications due to background from W- and Z-pairs, top-production, initial state photon radiation and from beamstrahlung are considered. The hadronic event selection procedures used by the experiments at LEP II are reviewed for the applicability at TESLA. An estimate of the various error contributions to the total uncertainty of an $\\alpha_S$ determination is presented. It confirms that hadronisation effects are diminished while the uncertainty from the choice of the renormalisation scale will dominate. Fits of the ln(R)-matched second order (O(alpha_S^2)) and resummed calculation (NLLA) to six observables are used to estimate the error contributions. This yields the expectation of the precision for alpha_S(500 GeV) of +-0.0025.']",['1999-12-23']
1003,['eng'],"['Böhm, F', 'Busenitz, J K', 'Cook, B', 'Gratta, Giorgio', 'Henrikson, H', 'Kornis, J', 'Lawrence, D', 'Lee, K B', 'McKinny, K', 'Miller, L', 'Novikov, V', 'Piepke, A G', 'Ritchie, B', 'Tracy, D', 'Vogel, P', 'Wang, Y F', 'Wolf, J']",['Search for Neutrino Oscillations at the Palo Verde Nuclear Reactors'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'fission, particle source', 'antineutrino/e, flux', 'antineutrino nucleon, interaction', 'charged current', 'energy spectrum', 'neutrino, mass difference', 'neutrino, mixing angle', 'scintillation counter, liquid', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912050'],"['We report on the initial results from a measurement of the anti-neutrino flux and spectrum at a distance of about 800 m from the three reactors of the Palo Verde Nuclear Generating Station using a segmented gadolinium-loaded scintillation detector. We find that the anti-neutrino flux agrees with that predicted in the absence of oscillations to better than 5%, excluding at 90% CL eV^2 for maximal mixing and $\\sin^2{2\\theta} > 0.21$ for large $\\Delta m^2$.']",['1999-12-23']
1004,['eng'],"['Nisius, R']",['The Photon Structure from Deep Inelastic Electron-Photon Scattering'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron p, colliding beams', 'photon electron, deep inelastic scattering', 'photon, structure function', 'exchange, two-photon', 'photon photon, interaction', 'photon p, interaction', 'structure function, leptonic', 'structure function, hadronic', 'parametrization', 'momentum spectrum, parton', 'equivalent photon approximation', 'hadron, photoproduction', 'hadron, multiple production', 'vector dominance', 'jet, photoproduction', 'quark, charm', 'differential cross section, transverse energy', 'transverse momentum, dependence', 'energy dependence', 'momentum transfer, dependence', 'proposed experiment', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912049'],"['The present knowledge of the structure of the photon is presented withemphasis on measurements of the photon structure obtained from deep inelasticelectron-photon scattering at e+e- colliders. This review covers the leptonicand hadronic structure of quasi-real and also of highly virtual photons, basedon measurements of structure functions and differential cross-sections. Futureprospects of the investigation of the photon structure in view of the ongoingLEP2 programme and of a possible linear collider are addressed. The mostrelevant results in the context of measurements of the photon structure fromphoton-photon scattering at LEP and from photon-proton and electron-protonscattering at HERA are summarised.']",['2000-02-14']
1005,['eng'],"['Punzi, G']",['A stronger classical definition of Confidence Limits'],['Detectors and Experimental Techniques'],['statistical analysis'],['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912048'],"[""A novel way of defining limits in classical statistics is proposed. This is anatural extension of the original Neyman's method, and has the desirableproperty that only information relevant to the problem is used in makingstatistical inferences. The result is a strong restriction on the allowedconfidence bands, excluding in full generality pathologies as empty confidenceregions or unstable solutions. The method is completely general and directlyapplicable to all problems of limits.""]",['2000-02-14']
1006,['eng'],"['Kozlov, Y V', 'Khalturtsev, S V', 'Machulin, I N', 'Martemyanov, A N', 'Martemyanov, B V', 'Sukhotin, S V', 'Tarasenkov, V G', 'Turbin, E V', 'Vyrodov, V N']",['Antineutrino-Deuteron Experiment at Krasnoyrsk'],['Particle Physics - Experimental Results'],"['antineutrino deuteron, interaction', 'antineutrino/e', 'fission, particle source', 'neutral current', 'charged current', 'channel cross section', 'experimental results', 'antineutrino/e deuteron --> n p antineutrino/e', 'antineutrino/e deuteron --> 2n positron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912047'],"['This report is represented the results of some experiments, which carried outat the neutrino underground laboratory of Kranoyarsk nuclear plant.']",['2000-02-14']
1007,['eng'],"['Kozlov, Y V', 'Khalturtsev, S V', 'Machulin, I N', 'Martemyanov, A N', 'Martemyanov, B V', 'Sabelnikov, A A', 'Tarasenkov, V G', 'Turbin, E V', 'Vyrodov, V N', 'Popeko, L A', 'Cherny, A Yu', 'Shishkina, G A']",['Today and Future Neutrino Experiments at Krasnoyarsk Nuclear Reactor'],['Particle Physics - Experimental Results'],"['antineutrino deuteron, nuclear reaction', 'deuteron, fission', 'antineutrino/e', 'fission, particle source', 'neutrino, magnetic moment', 'antineutrino electron, elastic scattering', 'experimental results', 'proposed experiment', 'antineutrino/e deuteron --> n p antineutrino', 'antineutrino/e deuteron --> 2n positron']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912046'],['The results of undergoing experiments and new experiment propositions atKrasnoyarsk underground nuclear reactor are presented'],['2000-02-14']
1008,['eng'],"['Bamberger, Andreas', 'Böttcher, S', 'Bohnet, I', 'Fernández, J P', 'Goebel, F', 'Göttlicher, P', 'Gabareen, A', 'García, G', 'Gendner, N', 'Graciani, R', 'Hauser, M G', 'Horstmann, D', 'Inuzuka, M', 'Kasemann, M', 'Löhr, B', 'Lewis, R', 'Lim, H', 'Lindemann, L', 'Markun, P', 'Martínez, M', 'Neumann, T', 'Park, I H', 'Del Peso, J', 'Raach, H', 'Savin, A', 'Son, D', 'Tokushuku, K', 'Wölfle, S', 'Whitmore, J', 'Wick, K', 'Wolf, G', 'Yamada, S', 'Yamashita, T', 'Yamazaki, Y']",['The ZEUS Forward Plug Calorimeter with Lead-Scintillator Plates and WLS Fiber Readout'],['Detectors and Experimental Techniques'],"['calorimeter, small-angle', 'lead', 'scintillation counter, fibre', 'optics, transformation', 'photoelectron, amplifier', 'energy resolution', 'magnetic detector, ZEUS', 'numerical calculations, Monte Carlo', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912045'],"['A Forward Plug Calorimeter (FPC) for the ZEUS detector at HERA has been built as a shashlik lead-scintillator calorimeter with wave length shifter fiber readout. Before installation it was tested and calibrated using the X5 test beam facility of the SPS accelerator at CERN. Electron, muon and pion beams in the momentum range of 10 to 100 GeV/c were used. Results of these measurements are presented as well as a calibration monitoring system based on a Co source.']",['1999-12-21']
1009,['eng'],"['Montgomery, H E']",['Recent Results and Perspectives at CDF and D0'],['Particle Physics - Experimental Results'],"['review, Cargese 1999/07/26', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'luminosity', 'jet, hadroproduction', 'W, hadroproduction', 'W, mass', 'mass, truth', 'differential cross section, transverse energy', 'transverse momentum, spectra', 'quark, charm', 'quark, beauty', 'Kobayashi-Maskawa angle, unitarity', 'B, lifetime', 'B, hadronic decay', 'violation, CP', 'new particle, search for', 'gauge boson, postulated particle', 'technicolor', 'Higgs particle', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'proposed experiment', 'Batavia TEVATRON Coll', 'bibliography', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912043'],"['Over the course of the past years the experimental measurements performed by the two large collaborations, CDF and D{Ø}, at the Fermilab Tevatron Collider have fueled advances in our understanding of physics at the energy frontier. At the present time the accelerator complex and the two detectors are undergoing substantial improvements. In this paper, we provide a discussion of some recent results which in turn provides a framework within which we can look to future prospects.']",['1999-12-21']
1010,['eng'],"['Barr, Giles David']",['Results on direct CP violation from NA48'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'K0, hadronic decay', 'K0(L), secondary beam', 'K0(S), secondary beam', 'violation, CP', 'calorimeter, electromagnetic', 'magnetic spectrometer', 'experimental results', 'CERN SPS', 'K0 --> pi+ pi-', 'K0 --> 2pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912042'],"['A report on the recent measurement of epsilon-prime, which characterises direct CP violation in the neutral kaon system, by the NA48 collaboration.']",['1999-12-21']
1011,['eng'],"['Juste, A']",['Higgs mass determination from direct reconstruction at a Linear $e^{+}e^{-}$ Collider'],['Detectors and Experimental Techniques'],"['talk, Sitges 1999/04/28', 'electron positron, annihilation', 'Higgs particle, electroproduction', 'Z0, associated production', 'Z0, hadronic decay', 'Higgs particle, mass', 'coupling, (Z0 Higgs particle)', 'coupling, Yukawa', 'channel cross section, mass', 'numerical calculations', '500 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912041'],"[""We study the feasibility of a precise measurement of the mass of a 120 GeV MSM Higgs boson through direct reconstruction of ZH->qqH events that would be achieved in a future e+e- linear collider operating at a center-of-mass energy of 500 GeV. Much effort has been put in a ``realistic simulation'' by including irreducible and reducible backgrounds, realistic detector effects and reconstruction procedures and sophisticated analysis tools involving Neural Networks and kinematical fitting. As a result, the Higgs mass is determined with a statistical accuracy of 50 MeV and the Z-Higgs Yukawa coupling measured to 0.7%, assuming 500 fb^-1 of integrated luminosity.""]",['1999-12-21']
1012,['eng'],"['Richter, Burton']",['Assessment and Outlook'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'electroweak interaction', 'violation, CP', 'K0, hadronic decay', 'neutrino, solar', 'neutrino, oscillation', 'neutrino, beam', 'accelerator, proposed', 'astrophysics', 'counters and detectors', 'supersymmetry', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001012'],"['My assignment at this conference is to assess where we are in high-energy physics and speculate on where we might be going. This frees me from any obligation to summarize all that went on here and allows me to talk just about those topics that interest me the most at this time. I will let my prejudices show and talk a bit about physics in general, CP violation, neutrinos, accelerators, non-accelerator experiments, and even theory.']",['2000-01-05']
1013,['eng'],"['Anjos, J C']",['Particle-antiparticle asymmetries in the production of baryons in 500 GeV/c$\\pi^{-}$-nucleon interactions'],['Particle Physics - Experimental Results'],"['talk, Batavia 1999/09/27', 'pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'baryon, hadroproduction', 'baryon antibaryon, asymmetry', 'Lambda', 'Xi', 'Omega-', 'Lambda/c+', 'x-dependence', 'transverse momentum, dependence', 'effect, leading particle', 'baryon, hadronic decay', 'experimental results', 'Batavia TEVATRON PS', '500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912039'],"['We present the Fermilab E791 measurement of baryon - antibaryon asymmetries in the production of Lambda^0, Cascade, Omega and Lambda_c in 500 GeV/c pi^- Nucleon interactions. Asymmetries have been measured as a function of x_F and p_T**2 over the range -0.12 < x_F < 0.12 and p_T**2 < 4$ (GeV/c)**2 for hyperons and -0.1 < x_F < 0.3 and p_T**2 < 8 (GeV/c)**2 for the Lambda_c baryons. We observe clear evidence of leading particle effects and a basic asymmetry even at x_F=0. These are the first high statistics measurements of the asymmetry in both the target and beam fragmentation regions in a fixed target experiment.']",['1999-12-20']
1014,['eng'],"['Blaylock, G']","['Heavy Quark Lifetimes, Mixing and CP Violation']",['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'anti-p p, interaction', 'quark, charm', 'quark, beauty', 'quark, pair production', 'charmed particle, lifetime', 'D0 anti-D0, interference', 'B/s0 anti-B/s0, interference', 'B/s0, mass difference', 'Kobayashi-Maskawa angle, unitarity', 'violation, CP', 'B0, hadronic decay', 'experimental results', 'Cornell CESR Stor', 'CERN LEP Stor', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912038'],"[""This paper emphasizes four topics that represent some of the year's highlights in heavy quark physics. First of all, a review is given of charm lifetime measurements and how they lead to better understanding of the mechanisms of charm decay. Secondly, the CLEO collaboration's new search for charm mixing is reported, which significantly extends the search for new physics in that sector. Thirdly, important updates in Bs mixing are summarized, which result in a new limit on the mass difference, and which further constrain the unitarity triangle. Finally, the first efforts to measure CP violation in the B system are discussed. Results are shown for the CDF and ALEPH measurements of sin(2beta), as well as the CLEO branching fraction measurements of B-->Kpi,pipi, which have implications for future measurements of alpha.""]",['1999-12-20']
1015,['eng'],"['Medinnis, M']",['HERA-B Status'],['Detectors and Experimental Techniques'],"['talk, Stanford 1999/08/09', 'p nucleus, inclusive reaction', 'B, hadroproduction', 'trigger', 'data acquisition', 'performance', 'magnetic detector, HERA-B', 'DESY HERA Stor', '920 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912037'],"[""The HERA-B experiment is designed for studying aspects of B-physics at DESY's HERA proton-electron storage ring, with emphasis on CP violation, particularly in the B->J/psi Kzero decay channel. The apparatus is nearing completion and the triggering system is being commissioned. A brief description of HERA-B is given and its present status is summarized.""]",['1999-12-20']
1016,['eng'],"['Delcourt, B']",['The excess of positive charges and the leading particles in DIS at HERA'],"['Particle Physics - Experimental Results', 'Accelerators and Storage Rings']","['talk, Hamburg 1998/1999', 'talk, Hamburg 1998/1999']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007013', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=scan&id=SCAN-0005115']","['The charge of the leading particle in DIS interactions is studied with the QCD models LEPTO, ARIADNE, RAPGAP and HERWIG. It is predicted to be preferentially positive, as is expected from the modified quark parton model and is studied over a wide range of x and Q^2.']",['2000-06-05']
1017,['eng'],"['Brook, N H', 'Carli, T', 'Rodrigues, E', 'Sutton, M R', 'Tobien, N', 'Weber, M']",['A Comparison of Deep Inelastic Scattering Monte Carlo Event Generators to HERA Data'],['Detectors and Experimental Techniques'],"['talk, Hamburg 1998/1999']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912053'],"['The Monte Carlo models ARIADNE, HERWIG and LEPTO are compared to deep-inelastic scattering data measured at the ep-collider HERA.']",['1999-12-23']
1018,['eng'],"['Engelfried, J']",['Experimental Techniques'],['Detectors and Experimental Techniques'],"['talk, Merida 1999/11/10', 'experimental methods', 'semiconductor detector, microstrip', 'proportional chamber', 'drift chamber', 'photon, counters and detectors', 'Cherenkov counter, ring imaging', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912036'],"['In this course we will give examples for experimental techniques used in particle physics experiments. After a short introduction, we will discuss applications in silicon microstrip detectors, wire chambers, and single photon detection in Ring Imaging Cherenkov (RICH) counters. A short discussion of the relevant physics processes, mainly different forms of energy loss in matter, is enclosed.']",['1999-12-17']
1019,['eng'],"['Chkhaidze, L V', 'Djobava, T', 'Kharkhelauri, L L']",['Study of collective matter flow in central C-Ne and C-Cu collisions at energy of 3.7 GeV per nucleon'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'nuclear reaction, particle flow', 'central region', 'carbon', 'neon', 'copper', 'pi, hadroproduction', 'p, hadroproduction', 'transverse momentum, spectra', 'angular distribution', 'dependence, mass number', 'anisotropy', 'experimental results', 'Dubna PS', '3.7 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912035'],"['The transverse momentum technique is used to analyse charged-particle exclusive data in the central C-Ne and C-Cu interactions at energy of 3.7 Gev per nucleon. The clear evidence of in-plane and out-of-plane (squeeze-out) flow effects for protons and $\\pi^{-}$ mesons have been obtained. In C-Ne interactions the $\\pi^{-}$ mesons in-plane flow is in the same direction to the protons, while in C-Cu collisions pions show antiflow behaviour. From the transverse momentum and azimuthal distributions of protons and pi^{-} mesons with respect to the reaction plane the flow F (the measure of the amount of collective transverse momentum transfer in the reaction plane) and the parameter a_{2} (the measure of the strength of the anisotropic emission) have been extracted. The flow effects increase with the mass of the particle and atomic number of target A_{T}. The comparison of our in-plane flow results with flow data of various projectile/target configurations had been done by a scaled flow F_{S}=F/(A_{P}^{1/3}+A_{T}^{1/3}). F_{S} demonstrates a common scaling behaviour among flow values from different systems.']",['1999-12-17']
1020,['eng'],"['Ecklund, K M']",['Semileptonic B Decays from CLEO'],['Particle Physics - Experimental Results'],"['talk, Southampton 1999/07/25', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'D*(2010)', 'rho(770)', 'Kobayashi-Maskawa angle', 'decay, form factor', 'Isgur-Wise function', 'momentum transfer, dependence', 'lepton, momentum spectrum', 'mass, hadronic', 'moment', 'HQET model', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D*(2010) lepton neutrino', 'B --> D lepton neutrino', 'B --> rho(770) lepton neutrino', 'B --> pi lepton neutrino', '10.57 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912034'],"['I report results in semileptonic decays of B mesons from the CLEOcollaboration, with a focus on recent results. Results for exclusivereconstruction of B -> D* l nu, B -> D l nu and B -> rho l nu are givenincluding the q^2 dependence of the form factors. These results are used tomeasure |V_cb| and |V_ub|. Two preliminary analyses using inclusive techniquesmeasure the lepton momentum spectrum and hadronic recoil mass spectrum in B ->X_c l nu decays, showing promise for future precision measurements of |V_cb|.']",['2000-02-14']
1021,['eng'],"['Abbott, B']",['Probing BFKL Dynamics in the Dijet Cross Section at Large Rapidity Intervals in $p\\overline{p}$ Collisions at $\\Sqrt{s}$ = 1800 and 630 GeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'jet, pair production', 'channel cross section', 'rapidity, gap', 'Lipatov equation', 'leading logarithm approximation', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912032'],['Inclusive dijet production at large pseudorapidity intervals (delta_eta) between the two jets has been suggested as a regime for observing BFKL dynamics. We have measured the dijet cross section for large delta_eta in ppbar collisions at sqrt{s}=1800 and 630 GeV using the DO detector. The partonic cross section increases strongly with the size of delta_eta. The observed growth is even stronger than expected on the basis of BFKL resummation in the leading logarithmic approximation. The growth of the partonic cross section can be accommodated with an effective BFKL intercept of a_{BFKL}(20GeV)=1.65+/-0.07.'],['1999-12-15']
1022,['eng'],"['Lancaster, M']",['Electroweak Measurements from Hadron Machines'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'neutrino nucleon, interaction', 'electron p, colliding beams', 'anti-p p, colliding beams', 'electroweak interaction, validity test', 'W, hadroproduction', 'quark, truth', 'quark, pair production', 'W, mass', 'mass, truth', 'Higgs particle, mass', 'Z0, leptonic decay', 'Z0, mass', 'W, width', 'W, leptonic decay', 'W, branching ratio', 'Weinberg angle', 'mass spectrum, transverse', 'experimental results', 'Batavia TEVATRON PS', 'Batavia TEVATRON Coll', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912031'],['A review of recent electroweak results from hadron machines including the measurements of the top quark and W boson mass.'],['1999-12-15']
1023,['eng'],"['Butterworth, J M']",['Structure of the Photon'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'photon photon, interaction', 'positron p, colliding beams', 'exchange, one-photon', 'photon, structure function', 'momentum transfer, dependence', 'quantum chromodynamics', 'quantum electrodynamics', 'Altarelli-Parisi equation', 'jet, photoproduction', 'jet, pair production', 'quark, charm', 'D*(2010), photoproduction', 'experimental results', 'proposed experiment', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912030'],['An overview of the current data and phenomenology on the structure of the photon and an outline of some opportunities available in the medium term future.'],['1999-12-15']
1024,['eng'],"['Lanaro, A']",['Detection of Pionium with DIRAC'],['Detectors and Experimental Techniques'],"['talk, Zuoz 1999/08/16', 'p nucleus, inclusive reaction', 'nickel', 'pi, pair production', 'pi, hadronium', 'pi+ pi-, atom', 'atom, lifetime', 'pi pi, scattering length', 'perturbation theory, chiral', 'symmetry breaking, chiral', 'magnetic spectrometer, experimental results', 'CERN SPS', 'p nickel --> pi+ pi- anything', '24 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912029'],"['The aim of the DIRAC experiment at CERN is to provide an accurate determination of S-wave pion-pion scattering lengths from the measurement of the lifetime of the pi+ pi- atom. The measurement will be done with precision comparable to the level of accuracy of theoretical predictions, formulated in the context of Chiral Perturbation Theory. Therefore, the understanding of chiral symmetry breaking of QCD will be submitted to a stringent test.']",['1999-12-15']
1025,['eng'],"['Kulchitskii, Yu A', 'Kuzmin, M V', 'Vinogradov, V B']",['Longitudinal Hadronic Shower Development in a Combined Calorimeter'],['Detectors and Experimental Techniques'],"['calorimeter, liquid argon', 'lead', 'iron', 'scintillation counter', 'showers, hadronic', 'showers, longitudinal', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912028'],"['This work is devoted to the experimental study of the longitudinal hadronic shower development in the ATLAS barrel combined prototype calorimeter consisting of the lead-liquid argon electromagnetic part and the iron-scintillator hadronic part. The results have been obtained on the basis of the 1996 combined test beam data which have been taken on the H8 beam of the CERN SPS, with the pion beams of 10, 20, 40, 50, 80, 100, 150 and 300 GeV/c. The degree of description of generally accepted Bock parameterization of the longitudinal shower development has been investigated. It is shown that this parameterization does not give satisfactory description for this combined calorimeter. Some modification of this parameterization, in which the e/h ratios of the compartments of the combined calorimeter are used, is suggested and compared with the experimental data. The agreement between such parameterization and the experimental data is demonstrated.']",['1999-12-15']
1026,['eng'],"['Sinclair, L']",['Hard Photoproduction and the Structure of the Photon'],['Particle Physics - Experimental Results'],"['talk, Tegernsee 1999/05/30', 'positron p, colliding beams', 'jet, photoproduction', 'hadron, multiple production', 'photon, resolved', 'quantum chromodynamics, perturbation theory', 'jet, multiplicity', 'jet, transverse energy', 'photon, structure function', 'gluon, momentum spectrum', 'differential cross section', 'momentum transfer, dependence', 'rapidity dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912027'],['A pedagogical introduction to the experimental results on hard photoproduction at HERA is provided. Then the latest results in this field from ZEUS and H1 are reviewed.'],['1999-12-14']
1027,['eng'],"['Swartz, M L']",['Precision Electroweak Physics at the Z'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'Z0, leptonic decay', 'electroweak interaction, validity test', 'polarization, asymmetry', 'angular distribution, asymmetry', 'Z0, width', 'tau, polarization', 'quark, pair production', 'quark, heavy', 'Z0, branching ratio', 'Z0, mass', 'neutrino, flavor', 'lepton, universality', 'Weinberg angle', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912026'],"[""A review of the decade of Z-pole electroweak physics is presented. Although all experimental work has been completed, it represents a ``Golden Age'' in our understanding of the Minimal Electroweak Standard Model (MSM). The latest (and nearly final) results from the LEP and SLC experiments are presented. The remaining inconsistencies are discussed and and their effects upon the MSM interpretation are explored.""]",['1999-12-14']
1028,['eng'],"['Ward, J J']",['Precision Measurements of Particle Masses using Jets at LEP2'],['Detectors and Experimental Techniques'],"['talk, Lisbon 1999/06/13', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, mass', 'Higgs particle, search for', 'Z0, associated production', 'intermediate boson, hadronic decay', 'Higgs particle, hadronic decay', 'Higgs particle, mass', 'final state, (4jet)', 'experimental results', 'CERN LEP Stor', '161, 172, 183, 189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912025'],"['How massive elementary particles get their mass is one of the greatest open questions in physics. Two of the major goals of the current LEP2 physics program that help to address this question are (a) to measure as precisely as possible the W Boson mass mW and (b) to exclude or discover the Higgs Boson within the available kinematic region. The reconstruction of invariant masses with jets from 4-jet channels (e.g. WW -> q qbar q qbar and HZ -> b bbar q qbar) and missing energy channels (e.g WW -> e nu q qbar and e+e- -> H nu nubar) is discussed. The emphasis is on the determination of mW, from which the role of calorimetry in such a precision measurement is emphasised.']",['1999-12-14']
1029,['eng'],"['Yamamoto, H']",['dEdx Particle Identification for Collider Detectors'],['Particle Physics - Experimental Results'],"['talk, Seoul 1999/02/19', 'colliding beam detector', 'drift chamber, gas', 'semiconductor detector, silicon', 'particle identification, energy loss', 'resolution']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912024'],['We review some basic features of dE/dx particle identification that are relevant to high energy physics tracking devices. Gas-based drift chambers as well as silicon trackers are discussed.'],['2000-10-05']
1030,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adams, D L', 'Adams, M', 'Akimov, V E', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Bassler, U', 'Bean, A', 'Belyaev, A', 'Beri, S B', 'Bernardi, G', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Brooijmans, G', 'Bross, A', 'Buchholz, D', 'Bühler, M', 'Büscher, V', 'Burtovoi, V S', 'Butler, J M', 'Canelli, F', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cochran, J', 'Coney, L', 'Connolly, B', 'Cooper, W E', 'Coppage, D', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Doulas, S', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fehér, S', 'Fein, D', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Fleuret, F', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gilmartin, R', 'Ginther, G', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Juste, A', 'Kahn, S', 'Kajfasz, E', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Landsberg, G L', 'Leflat, A', 'Lehner, F', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lu, J G', 'Lucotte, A', 'Lueking, L H', 'Lundstedt, C', 'Maciel, A K A', 'Madaras, R J', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McMahon, T', 'Melanson, H L', 'Meng, X C', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mihalcea, D', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mostafa, M A', 'Da Motta, H', 'Nagy, E', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Neal, H A', 'Negret, J P', 'Negroni, S', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Olivier, B', 'Oshima, N', 'Padley, P', 'Pan, L J', 'Para, A', 'Parashar, N', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Patwa, A', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pope, B G', 'Popkov, E', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Reay, N W', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Schwartzman, A', 'Scully, J R', 'Sen, N', 'Shabalina, E', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Simák, V', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Song, X F', 'Sorin, V', 'Sosebee, M', 'Sotnikova, N', 'Soustruznik, K', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Stutte, L', 'Sznajder, A', 'Taylor, W', 'Tentindo-Repond, S', 'Thomas, T L T', 'Thompson, J', 'Toback, D', 'Trippe, T G', 'Turcot, A S', 'Tuts, P M', 'Van Gemmeren, P', 'Vaniev, V', 'Van Kooten, R', 'Varelas, N', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, H', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Whiteson, D', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yip, K', 'Youssef, S', 'Yu, J', 'Yu, Z', 'Zanabria, M E', 'Zheng, H', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Limits on Quark Compositeness from High Energy Jets in $P\\overline{P}$ Collisions at 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'jet, hadroproduction', 'jet, multiple production', 'transverse energy, energy spectrum', 'quark, composite', 'lower limit', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912023', 'http://arXiv.org/abs/hep-ex/?9912023']","['Events in PbarP collisions at sqrt(s)=1.8 TeV with total transverse energy exceeding 500 GeV are used to set limits on quark substructure. The data are consistent with next-to-leading order QCD calculations. We set a lower limit of 2.0 TeV at 95% confidence on the energy scale Lambda_LL for compositeness in quarks, assuming a model with a left-left isoscalar contact interaction term. The limits on Lambda_LL are found to be insensitive to the sign of the interference term in the Lagrangian.']",['2000-10-05']
1031,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Anikeev, K', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bevensee, B', 'Bhatti, A A', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Brozovic, M', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Ciobanu, C I', 'Clark, A G', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Costanzo, D', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Grassmann, H', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Herndon, M', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kirk, M', 'Kim, B J', 'Kim, H S', 'Kim, M J', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korn, A', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mayer, J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Mesropian, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Mitselmakher, G V', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Paus, C', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Popovic, M', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Rakitine, A', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tamburello, P D', 'Tanaka, M', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Wolinski, S', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['A Measurement of the Differential Dijet Mass Cross Section in $p\\overline{p}$ Collisions at $\\sqrt{s}=1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'mass spectrum, (2jet)', 'differential cross section, mass', 'quantum chromodynamics, perturbation theory', 'momentum spectrum, parton', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912022'],"['We present a measurement of the cross section for production of two or more jets as a function of dijet mass, based on an integrated luminosity of 86 pb^-1 collected with the Collider Detector at Fermilab. Our dijet mass spectrum is described within errors by next-to-leading order QCD predictions using CTEQ4HJ parton distributions, and is in good agreement with a similar measurement from the D0 experiment.']",['2000-10-05']
1032,['eng'],"['Cheung, H W K']",['Review of Charm Lifetimes'],['Particle Physics - Experimental Results'],"['review, Southampton 1999/07/25', 'charmed particle, lifetime', 'charmed particle, hadronic decay', 'D/s+', 'D0', 'D+', 'Lambda/c+', 'W, exchange', 'W, annihilation', 'lifetime, ratio', 'quantum chromodynamics', 'operator product expansion', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912021'],"['A review of the latest experimental results on charm particle lifetimes is presented. The most significant update is that the D_s^+ lifetime is conclusively larger than the D^0 lifetime and signifies that W-exchange/W-annihilation contributions are large. Using new high statistics data on $D^+\\to K^+\\pi^+\\pi^-$ together with the D_s^+ lifetime and some assumptions, one can phenomenologically extract the strength of the W-exchange contribution in D^0 decays and of W-annihilation in D_s^+ decays. These are larger than or at the limit of theoretical expectations using QCD-based operator production expansion techniques.']",['2000-10-05']
1033,['eng'],"['Akhmetshin, R R', 'Anashkin, E V', 'Arpagaus, M', 'Aulchenko, V M', 'Banzarov, V S', 'Barkov, L M', 'Bashtovoy, N S', 'Bondar, A E', 'Bondarev, D V', 'Bragin, A V', 'Chernyak, D V', 'Eidelman, S I', 'Fedotovich, G V', 'Gabyshev, N I', 'Grebeniuk, A A', 'Grigoriev, D N', 'Hughes, V W', 'Karpov, S V', 'Kazanin, V F', 'Khazin, B I', 'Koop, I A', 'Korostelev, M S', 'Krokovnyi, P P', 'Kurdadze, L M', 'Kuzmin, A S', 'Logashenko, I B', 'Lukin, P A', 'Mikhailov, K Yu', 'Milshtein, A I', 'Nesterenko, I N', 'Okhapkin, V S', 'Otboev, A V', 'Polunin, A A', 'Popov, A S', 'Purlatz, T A', 'Root, N I', 'Ruban, A A', 'Ryskulov, N M', 'Shamov, A G', 'Shatunov, Yu M', 'Shwartz, B A', 'Sibidanov, A L', 'Sidorov, V A', 'Skrinsky, A N', 'Smakhtin, V P', 'Snopkov, I G', 'Solodov, E P', 'Stepanov, P Yu', 'Sukhanov, A Yu', 'Thompson, J A', 'Titov, V M', 'Valishev, A A', 'Yudin, Yu V', 'Zverev, S G']",['Cross section of the reaction $e^{+}e^{-} \\to \\pi^{+}\\pi^{-}\\pi^{+}\\pi ^{-}$ below 1 GeV at CMD-2'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'pi, multiple production', 'intermediate state, (a1(1260) pi)', 'rho(770)0, hadronic decay', 'rho(770)0, branching ratio', 'rho(770)0, width', 'channel cross section, energy dependence', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> 2pi+ 2pi-', 'rho(770)0 --> 2pi+ 2pi-', '0.60-0.97 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912020'],"['Using 3.07 ${pb}^{-1}$ of data collected in the energy range 0.60-0.97 GeV by CMD-2, about 150 events of the process $\\epm \\to \\pch$ have been selected. The energy dependence of the cross section agrees with the assumption of the $a_1(1260) \\pi$ intermediate state which is dominant above 1 GeV. For the first time \\fourpi events are observed at the $\\rho$ meson energy. Under the assumption that all these events come from the $\\rho$ meson decay, the value of the cross section at the $\\rho$ meson peak corresponds to the following decay width: \\Gamma(\\rho^0 \\to \\fourpi) = (2.8 \\pm 1.4 \\pm 0.5) {keV} or to the branching ratio B(\\rho^0 \\to \\fourpi) = (1.8 \\pm 0.9 \\pm 0.3) \\cdot 10 ^{-5}.']",['2000-10-05']
1034,['eng'],"['Charlton, D G']",['Precise Electroweak Results from LEP2'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'quark, pair production', 'channel cross section, energy dependence', 'angular distribution', 'quantum electrodynamics, validity test', 'Z0, pair production', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'W, mass', 'W, width', 'coupling, (3gauge boson)', 'coupling, (4gauge boson)', 'experimental results', 'CERN LEP Stor', '161-202 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912019'],['Precise electroweak results from LEP2 are reviewed.'],['1999-12-10']
1035,['eng'],"['Sheldon, P D']",['Charm Mixing and Rare Decays'],['Particle Physics - Experimental Results'],"['review, Southampton 1999/07/25', 'D0 anti-D0, interference', 'Kobayashi-Maskawa angle', 'neutral current, flavor changing', 'D, hadroproduction', 'D, electroproduction', 'D, hadronic decay', 'D, semileptonic decay', 'D0, rare decay', 'lifetime, difference', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912016'],"['There has been significant recent experimental activity on the related topics of charm mixing and rare (flavor changing neutral current) decay. For mixing, several new results from direct (wrong sign) searches and first results from lifetime difference (Delta Gamma) searches have been reported. Limits for r_mix of approximately 5 x 10^{-4} (or better) are possible from work in progress. For rare decays, sensitivities to branching ratios are now at the level of a few x 10^{-6}.']",['1999-12-08']
1036,['eng'],"['Hutchcroft, D E']","['The lower mass limit on the lightest supersymmetric particle, using ALEPH data up to 188.6 GeV']",['Particle Physics - Experimental Results'],"['talk, Paris 1999/09/06', 'electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'gaugino', 'slepton', 'LSP, mass', 'lower limit', 'R parity, invariance', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912015'],"['The lightest srpersymmetric particle (LSP) is expected to be stable, massive and neutral. Direct searches for supersymmetric particles in the context of the minimal supersymmetric extension to the standard model have been performed with the ALEPH detector. Using about 175pb-1 of data with centre-of-mass energies near 189GeV a limit on the mass of the LSP of M_LSP>32.3GeV/c2 at 95% confidence can be derived, assuming R-parity is conserved.']",['1999-12-08']
1037,['eng'],"['Kulchitskii, Yu A', 'Kuzmin, M V', 'Vinogradov, V B']",['The e/h Method of Energy Reconstruction for Combined Calorimeter'],['Detectors and Experimental Techniques'],"['calorimeter, electromagnetic', 'calorimeter, hadronic', 'energy, measurement', 'pi, beam', 'electron, beam', 'energy spectrum', 'energy resolution', 'magnetic detector, ATLAS', 'CERN LHC Coll', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912014'],"['The new simple method of the energy reconstruction for a combined calorimeter, which we called the e/h method, is suggested. It uses only the known e/h ratios and the electron calibration constants and does not require the determination of any parameters by a minimization technique. The method has been tested on the basis of the 1996 test beam data of the combined calorimeter and demonstrated the correctness of the reconstruction of the mean values of energies. The obtained fractional energy resolution is $[(58\\pm3)%/\\sqrt{E}+(2.5\\pm0.3)%]\\oplus (1.7\\pm0.2)/E$. This algorithm can be used for the fast energy reconstruction in the first level trigger.']",['1999-12-08']
1038,['eng'],[],['Search for Scalar Top Quark Production in $p\\overline{p}$ Collisions at $\\Sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'squark, pair production', 'squark, truth', 'squark, decay modes', 'final state, (2beauty lepton)', 'transverse energy, missing-energy', 'sparticle, mass', 'channel cross section, upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2squark anything', 'squark --> beauty chargino', 'squark --> beauty lepton sneutrino', 'chargino --> neutralino lepton neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912018'],"['We have searched for direct production of scalar top quarks at the Collider Detector at Fermilab in 88 pb-1 of p anti-p collisions at s**(1/2) = 1.8 TeV. We assume the scalar top quark decays into either a bottom quark and a chargino or a bottom quark, a lepton, and a scalar neutrino. The event signature for both decay scenarios is a lepton, missing transverse energy, and at least two b-quark jets. For a chargino mass of 90 GeV/c2 and scalar neutrino masses of at least 40 GeV/c2, we find no evidence for scalar top production and present upper limits on the production cross section in both decay scenarios.']",['1999-12-09']
1039,['eng'],"['Schwartz, A J']",['HERA-B'],['Particle Physics - Experimental Results'],"['talk, Bled 1999/06/21', 'p nucleus, inclusive reaction', 'B, hadroproduction', 'B/s0, hadroproduction', 'beautiful meson, decay modes', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'B/s0, mass difference', 'width, difference', 'magnetic detector, HERA-B', 'numerical calculations', 'proposed experiment, DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912012'],"[""HERA-B is a hadroproduction experiment located at DESY in Hamburg, Germany. The experiment produces B mesons and baryons by inserting thin wire targets into the halo of the proton beam circulating in the HERA storage ring. The B decays are studied to search for evidence of CP violation and constrain the angle $\\beta$ and possibly $\\gamma$ and $\\alpha$ of the CKM unitarity triangle. The experiment also produces B_s mesons; these decays are studied to measure or constrain the mass difference $\\Delta m_s$ and width difference the large number of B's produced allows HERA-B to search for rare and forbidden decays such as $B\\to K^{(*)}\\ell^+_1\\ell^-_2$. The experiment is scheduled to begin running in early 2000.""]",['1999-12-07']
1040,['eng'],"['Gallinaro, M']",['Recent Results from CDF'],['Particle Physics - Experimental Results'],"['talk, Moscow 1999/05/27', 'anti-p p, colliding beams', 'quark, beauty', 'quark, pair production', 'quark, truth', 'B0, hadronic decay', 'J/psi(3100), leptonic decay', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'quark, decay', 'channel cross section', 'new particle, search for', 'Higgs particle, charged particle', 'Higgs particle, neutral particle', 'squark, beauty', 'squark, truth', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912011'],"['We present the latest results from the CDF experiment at the Tevatron Collider in \\ppbar collisions at $\\sqrt{s} = 1.8$ TeV. The large data sample collected during Run 1, from 1992 until 1995, allows measurements in many domains of high-energy physics. Here, we report on the first measurement of top quark cross section. We also report on searches for the so-far elusive Higgs boson, and for SUSY, through searches for direct production of top and bottom scalar quarks. Finally, we outline the prospects for the physics during the upcoming Run 2, ready to start in the upcoming year 2000.']",['1999-12-07']
1041,['eng'],"['Di Lella, Luigi']",['Accelerator and Reactor Neutrino Experiments'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'neutrino, oscillation', 'neutrino/e', 'fission, particle source', 'neutrino/mu, beam', 'neutrino/tau', 'neutrino nucleon, interaction', 'charged current', 'positron, energy spectrum', 'neutrino, mass difference', 'neutrino, mixing angle', 'tau, search for', 'new particle, search for', 'experimental methods', 'proposed experiment', 'experimental results', 'deep underground detector']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912010'],['Present results from neutrino experiments at accelerators and nuclear reactors are reviewed with emphasis on neutrino oscillation searches. Future prospects in this field are also discussed.'],['1999-12-07']
1042,['eng'],"['Deines-Jones, P', 'Cherry, M L', 'Dabrowska, A', 'Holynski, R', 'Kudzia, D', 'Nilsson, B S', 'Olszewski, A', 'Szarska, M', 'Trzupek, A', 'Waddington, C Jake', 'Wefel, J P', 'Wilczynska, B', 'Wilczynski, H', 'Wolter, W', 'Wosiek, B', 'Wozniak, K']",['Charged particle production in the Pb + Pb system at 158 GeV/c per nucleon'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'lead', 'multiple production', 'charged particle, multiplicity', 'dependence, impact parameter', 'rapidity spectrum', 'numerical calculations, Monte Carlo', 'nuclear emulsion, experimental results', 'CERN SPS', 'bibliography', '158 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912008'],['Charged particle multiplicities from high multiplicity central interactions of 158 GeV/nucleon Pb ions with Pb target nuclei have been measured in the central and far forward projectile spectator regions using emulsion chambers. Multiplicities are significantly lower than predicted by Monte Carlo simulations. We examine the shape of the pseudorapidity distribution and its dependence on centrality in detail.'],['1999-12-07']
1043,['eng'],"['Mann, W A']",['Atmospheric Neutrinos and the Oscillations Bonanza'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino/e', 'neutrino/mu', 'neutrino/tau', 'neutrino, sterile', 'matter, effect', 'flux, ratio', 'neutrino, mass difference', 'neutrino, mixing angle', 'muon, angular distribution', 'deep underground detector, experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912007'],"['New observations with atmospheric neutrinos from the underground experiments SuperKamiokande, Soudan 2, and MACRO, together with earlier results from Kamiokande and IMB, are reviewed. The most recent observations reconfirm aspects of atmospheric flavor content and of zenith angle distributions which appear anomalous in the context of null oscillations. The anomalous trends, exhibited with high statistics in both sub-GeV and multi-GeV data of the SuperKamiokande water Cherenkov experiment, occur also in event samples recorded by the tracking calorimeters. The data are well-described by disappearence of nu_mu flavor neutrinos arising in oscillations with dominant two-state mixing, for which there exists a parameter region allowed by all experiments. In a new analysis by SuperKamiokande, nu_mu -> nu_tau is favored over nu_mu -> nu_s as the dominant oscillation based upon absence of oscillation suppression from matter effects at high energies. The possibility for sub-dominant nu_mu -> nu_e oscillations in atmospheric neutrinos which arises with three-flavor mixing, is reviewed, and intriguing possibilities for amplification of this oscillation by terrestrial matter-induced resonances are discussed. Developments and future measurements which will enhance our knowledge of the atmospheric neutrino fluxes are briefly noted.']",['1999-12-06']
1044,['eng'],"['Liu, F']",['Recent $\\psi(2S)$ results at BES'],['Particle Physics - Experimental Results'],"['talk, Beijing 1999/08/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), hadronic decay', 'quarkonium, hadron spectroscopy', 'chi mesons, charm', 'chi mesons, hadronic decay', 'eta/c(2980)', 'quantum chromodynamics, nonrelativistic', 'quarkonium, branching ratio', 'magnetic detector, BES', 'experimental results', 'Beijing Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912006'],"['Based on $(3.79\\pm0.31)\\times10^6 ~\\psip$ data sets collected with the BES detector at BEPC, the recent $\\psip$, $\\chi_{cJ}$ and $\\eta_c$ results from BES are presented. Some results are compared with NRQCD.']",['1999-12-03']
1045,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A spin analysis of the $4\\pi$ channels produced in central pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'central region', 'pi, multiple production', 'mass spectrum, (4pi)', 'meson resonance, hadroproduction', 'meson resonance, decay modes', 'postulated particle, eta2(1645)', 'eta2(1870)', 'f0(1370)', 'f0(1500)', 'postulated particle, f2(1950)', 'isobar model', 'spin, parity', 'magnetic spectrometer, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p 4pi0', 'p p --> 2p 2pi+ 2pi-', 'p p --> 2p pi+ pi- 2pi0', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912005'],"['The reactions pp -> pf (X0) ps, where X0 is observed decaying to pi0pi0pi0pi0, pi+pi-pi0pi0 and pi+pi-pi+pi-, have been studied at 450 GeV/c. There is evidence for an a2(1320)pi decay mode of the eta2(1645) and eta2(1870) in the pi+pi-pi0pi0 and pi+pi-pi+pi- final states. The f2(1950) is consistent with being a single resonance with a dominant f2(1270)pipi decay mode. The f0(1370) is found to decay dominantly to rho-rho while the f0(1500) is found to decay to rho-rho and sigma-sigma.']",['1999-12-03']
1046,['eng'],"['Takasaki, F']","['Status of KEKB accelerator and detector, BELLE']",['Detectors and Experimental Techniques'],"['talk, Stanford 1999/08/09', 'electron positron, storage ring', 'B, particle source', 'energy, asymmetry', 'luminosity', 'electron positron, colliding beams', 'semiconductor detector, vertex', 'semiconductor detector, microstrip', 'particle identification, (K pi)', 'calorimeter, electromagnetic', 'scintillation counter, crystal', 'cesium, iodine', 'background', 'magnetic detector, BELLE', 'KEK TRISTAN Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912004'],"['Status of the KEKB accelerator and the detector, BELLE, is reported. The construction of the 3.5 Gev x 8 GeV electron-positron collider, and the solenoid detector, BELLE, was completed in December, 1998. The commissioning of them has been made since then. The BELLE detector has observed the first hadronic event from the beam collision on Jun 1, 1999. The achieved maximum luminosity by August 4th, 1999, was 3 x 10^32 cm^-2 sec^-1. The KEKB operation will be continued after two months of summer break.']",['1999-12-03']
1047,['eng'],"['Aitala, E M']",['Multidimensional Resonance Analysis of $\\Lambda_{c}^{+} \\to p K^{-}\\pi^{+}$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'Lambda/c+, hadroproduction', 'Lambda/c+, hadronic decay', 'decay, amplitude analysis', 'K*(892)', 'Delta(1232)', 'Lambda(1520)', 'Lambda/c+, polarization', 'transverse momentum, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'Lambda/c+ --> p K- pi+', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912003'],"['We present the results of a five-dimensional resonant amplitude analysis of the $\\Lambda_c^+{\\to}pK^{-}\\pi^{+}$ system based on $946\\pm 38$ reconstructed decays. These data were produced in 500 GeV/$c$ $\\pi^-$-N interactions by Fermilab experiment E791. We report measurements of the amplitudes for possible resonant enhancements. This is the first complete amplitude analysis of the $\\Lambda_c^{+}{\\to}pK^{-}\\pi^{+}$ system. We find that $(54.8\\pm5.5\\pm3.5)$% of the decays are nonresonant, $(19.5\\pm2.6\\pm1.8)$% of the decays are via the $\\bar{K}^{*0}$ resonance, $(18.0\\pm2.9\\pm2.9)$% of the decays are via the $\\Delta^{++}$ resonance, and $(7.7\\pm1.8\\pm1.1)$% of the decays are via the $\\Lambda(1520)$ resonance. We find evidence for an increasingly negative polarization of the $\\Lambda_c^+$ baryons as a function of $p_T^2$, in agreement with a recent model\\cite{dha} and with a related measurement\\cite{jez}.']",['1999-12-02']
1048,['eng'],"['Bortoletto, D']",['The measurement of $\\sin(2\\beta)$'],['Particle Physics - Experimental Results'],"['talk, Southampton 1999/07/25', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0, hadronic decay', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'electroweak interaction, validity test', 'particle identification, flavor', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B0 --> J/psi(3100) K0(S)', 'J/psi(3100) --> muon+ muon-', 'K0(S) --> 2pi', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912002'],"[""Since the first observation in 1964, CP violation remains one of the most elusive aspects of the standard model. The CDF collaboration has reported the first evidence of CP violation in the B system using the world's largest sample of $B \\to J/\\psi K^0_S $ decays. The direct measurement of sin$(2\\beta)$=0.79$^{+0.41}_{-0.44}$ (combined statistical and systematic error) agrees with the standard model predictions. New data collected from the B-factories and from the upgraded experiments at the Tevatron should allow a more precise measurement of $\\sin 2\\beta$ in the near future.""]",['1999-12-02']
1049,['eng'],"['Melnitchouk, W', 'Afnan, I R', 'Bissey, F', 'Thomas, A W']","['Comment on ""Parton distributions, d/u and higher twist effects at high x""']",['Particle Physics - Experimental Results'],"['nucleon, structure function', 'nuclear physics, correction', 'dependence, mass number', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9912001'],"['In a recent paper Yang and Bodek extracted the free neutron structure function at large x by extrapolating the density dependence of the nuclear EMC ratios to the deuteron. We point out why this approach is likely to be misleading for light nuclei, and correctly applied predicts that the nuclear corrections in the deuteron should be zero.']",['1999-12-02']
1050,['eng'],"['Anikina, M K', 'Chkhaidze, L V', 'Djobava, T', 'Garsevanishvili, V R', 'Kharkhelauri, L L']",['The analysis of $\\pi^{-}$ mesons produced in nucleus-nucleus collisions at a momentum of 4.5 GeV/c/nucleon in light front variables'],['Particle Physics - Experimental Results'],"['nucleus nucleus, nuclear reaction', 'pi-, hadroproduction', 'helium', 'lithium', 'carbon', 'oxygen', 'neon', 'copper', 'lead', 'kinematics, light front', 'quark gluon, string model', 'thermodynamics', 'spectra, x-dependence', 'transverse momentum, spectra', 'angular distribution', 'momentum spectrum', 'streamer chamber, experimental results', 'Dubna PS', '4.5 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911052'],"['The light front analysis of pi^{-} mesons in He(Li,C), C-Ne, C-Cu and O-Pb collisions is carried out. The phase space of secondary pions is divided into two parts in one of which the thermal equilibrium assumption seems to be in a good agreement with the data. Corresponding temperatures T are extracted and their dependence on (A_{P}*A_{T})^{1/2} is studied. The results are compared with the predictions of the Quark-Gluon String Model (QGSM). The QGSM satisfactorily reproduces the experimental data for light and intermediate-mass nuclei.']",['1999-12-01']
1051,['eng'],"['MacDonald, N']",['Comparison of Dijet Cross Sections vs $Q^{2}$ with Various Monte Carlo Models'],['Particle Physics - Experimental Results'],"['talk, Hamburg 1998/03/27', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'final state, (2jet)', 'photon, resolved', 'momentum spectrum, parton', 'cross section, x-dependence', 'momentum transfer, dependence', 'numerical calculations, Monte Carlo', 'interpretation of experiments, ZEUS', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911050'],"[""The dijet cross section as a function of both the fraction of the photon momentum participating in the hard process, x_\\gamma^{OBS}, and the photon's virtuality, Q^2, is compared with the predictions of Herwig 5.9 for various photon parton distribution functions. The ratio of dijet cross sections with x_\\gamma^{OBS} < 0.75 and x_\\gamma^{OBS} > 0.75 is measured as a function of Q^2. This ratio is found to decrease as Q^2 increases consistent with the hypothesis that the photon parton distribution functions decrease with increasing photon virtuality.""]",['1999-12-01']
1052,['eng'],"['MacDonald, N']",['Structure of Real and Virtual Photons from ZEUS'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'jet, photoproduction', 'final state, (2jet)', 'photon, structure function', 'photon, resolved', 'differential cross section, transverse energy', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'momentum transfer, dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911049'],"['Measurements sensitive to the structure of both real and virtual photons are presented and compared to theoretical models with various photon parton distribution functions (PDFs). Measurements for real photons show a tendency for the available photon PDFs to be too small to describe the data. For virtual photons, the photon PDF is seen to decrease with increasing photon virtuality. In order to describe the data, resolved photon processes are required up to a photon virtuality of at least 4.5 GeV^2.']",['1999-12-01']
1053,['eng'],"['Doyle, A T']",['Event Shapes and Forward Jet Production at HERA'],['Particle Physics - Experimental Results'],"['talk, Beijing 1999/08/24', 'positron p, colliding beams', 'jet, electroproduction', 'production, small-angle', 'event shape analysis', 'small-x', 'Lipatov equation', 'Altarelli-Parisi equation', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911047'],['Analyses of event shapes and forward jet production in deep inelastic scattering at the HERA collider are described. The results are compared to QCD predictions.'],['1999-12-01']
1054,['eng'],"['Brook, N H']",['MLLA Parton Spectra Compared to ARIADNE'],['Particle Physics - Experimental Results'],"['talk, Hamburg 1998/04/27', 'electron positron, annihilation', 'electron p, deep inelastic scattering', 'momentum spectrum, parton', 'quantum chromodynamics', 'leading logarithm approximation', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911046'],"['The parton spectra as predicted by the ARIADNE Monte Carlo generator, for both e+e- annihilation and deep inelastic scattering, are compared to the QCD MLLA calculations.']",['1999-12-01']
1055,['eng'],"[""D'Almeida, F"", 'Barbi, M S', 'Do Vale, M A B']",['A Proposal for a Different Chi-square Function for Poisson Distributions'],['Detectors and Experimental Techniques'],"['statistical analysis', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911042'],"['We obtain an approximate Gaussian distribution from a Poisson distribution after doing a change of variable. A new chi-square function is obtained which can be used for parameter estimations and goodness-of-fit testing when adjusting curves to histograms. Since the new distribution is approximately Gaussian we can use it even when the bin contents are small. The corresponding chi-square function can be used for curve fitting. This chi-square function is simple to implement and presents a fast convergence of the parameters to the correct value, especially for the parameters associated with the width of the fitted curve. We present a Monte Carlo comparative study of the fitting method introduced here and two other methods for three types of curves: Gaussian, Breit-Wigner and Moyal, when each bin content obeys a Poisson distribution. It is also shown that the new method and the other two converge to the same result when the number of events increases']",['1999-11-30']
1056,['eng'],"['Barberis, D']","[""A study of the $\\eta \\eta{'}$ and $\\eta{'}\\eta{'}$ channels produced in central p p interactions at 450 GeV/c""]",['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'central region', 'pseudoscalar meson, pair production', 'eta', 'eta(958)', 'mass spectrum, (2eta(958))', 'mass spectrum, (eta(958) eta)', 'f0(1500)', 'mass enhancement, (1950)', 'spin, parity', 'magnetic spectrometer, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p eta(958) eta', 'p p --> 2p 2eta(958)', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911041'],"['The reactions pp -> pf (X0) ps, where X0 is observed decaying to eta etaprime and etaprime etaprime, have been studied at 450 GeV/c. This is the first time that these channels have been observed in central production and only the second time that the etaprime etaprime channel has been observed in any production mechanism. In the eta etaprime channel there is evidence for the f0(1500) and a peak at 1.95 GeV. The etaprime etaprime channel shows a peak at threshold which is compatible with having JPC = 2++ and spin projection JZ = 0.']",['1999-11-30']
1057,['eng'],"['Brau, J E']",['Electroweak Precision Measurements with Leptons'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'electroweak interaction, validity test', 'Z0, electroproduction', 'lepton, pair production', 'Weinberg angle', 'angular distribution, asymmetry', 'polarization, asymmetry', 'tau, polarization', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911040'],['The precision measurements of lepton electroweak parameters at SLD and LEP are reviewed and discussed. The updated SLD weak mixing angle measurement from $A_{LR}$ and the lepton left-right forward-backward asymmetries is lepton-based value is $0.23119 \\pm 0.00020$. This value differs by over $3\\sigma$ from the comparable quark-based value.'],['1999-11-29']
1058,['eng'],"['Battaglia, M', 'Caccia, M']",['The Vertex Tracker at the $e^{+}e^{-}$ Linear Collider'],['Detectors and Experimental Techniques'],"['talk, Lund 1999/09/23', 'electron positron, colliding beam detector', 'colliding beam detector, proposed', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'semiconductor, optical', 'resolution, impact parameter', 'background', 'electron positron, linear collider', 'linear collider, proposed']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911039'],"['The e+e- linear collider physics programme sets highly demanding requirements on the accurate determination of charged particle trajectories close to their production point. A new generation of Vertex Trackers, based on different technologies of high resolution silicon sensors, is being developed to provide the needed performances. These developments are based on the experience with the LEP/SLC vertex detectors and on the results of the R&D programs for the LHC trackers and also define a further program of R&D specific to the linear collider applications. In this paper the present status of the conceptual tracker design, silicon detector R&D and physics studies is discussed.']",['1999-11-29']
1059,['eng'],"['Barberis, D']",['A study of the $\\eta\\pi\\pi$ channel produced in central p p interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, interaction', 'central region', 'pseudoscalar meson, multiple production', 'mass spectrum, (eta pi+ pi-)', 'postulated particle, eta2(1645)', 'eta2(1870), decay modes', 'a2(1320)', 'a0(980)', 'f2(1270)', 'decay, amplitude analysis', 'spin, parity', 'magnetic spectrometer, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2eta pi+ pi-', 'eta2(1870) --> a2(1320) pi', 'eta2(1870) --> a0(980) pi', 'eta2(1870) --> f2(1270) eta', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911038'],"['The reaction pp -> pf (eta pi pi) ps has been studied at 450 GeV/c. There is clear evidence for an a2(1320)pi decay mode of the eta2(1645) and eta2(1870). In addition, there is evidence for an a0(980)pi$ decay mode of both resonances and an f2(1270)eta decay mode of the eta2(1870). No evidence is found for a JPC = 2++ a2(1320)pi wave.']",['1999-11-29']
1060,['eng'],"['Pérez, E']",['Searches for Exotics at HERA'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'positron p, colliding beams', 'electron p, colliding beams', 'new interaction, search for', 'new particle, search for', 'leptoquark, decay', 'leptoquark, coupling', 'violation, flavor', 'fermion, excited state', 'excited state, decay modes', 'electroweak interaction, validity test', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300, 320 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911037'],"['Searches for contact interactions, leptoquark bosons and excited fermions carried out at the HERA ep collider are presented here. The searches are based on ~ 40 pb^-1 of e+ p data per experiment collected at a centre of mass energy ~ 300 GeV. First results on e- p data collected in 1998-1999 are also presented.']",['1999-11-25']
1061,['eng'],[],"[""New measurement of the rare decay $\\phi \\to \\eta' \\gamma$ with CMD-2""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), rare decay', 'eta(958), hadronic decay', 'Phi(1020), branching ratio', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> eta(958) photon', 'eta(958) --> eta pi+ pi-', 'eta --> 2photon', 'approx. 1.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911036'],"[""A new measurement of the rare decay \\phi \\to \\eta' \\gamma performed with the CMD-2 detector at Novosibirsk is described. Of the data sample corresponding to the integrated luminosity of 14.5 pb^{-1}, twenty one events have been selected in the mode \\eta'\\to\\pi^+\\pi^-\\eta, \\eta\\to\\gamma\\gamma. The following branching ratio was obtained: B(\\phi \\to \\eta' \\gamma) = (8.2^{+2.1}_{-1.9} \\pm 1.1) 10^{-5}.""]",['1999-11-25']
1062,['eng'],"['Bianco, S']",['Charm Overview'],['Particle Physics - Experimental Results'],"['review, Ann Arbor 1999/06/24', 'quark, charm', 'quark, pair production', 'quark, hadronization', 'charmed particle, hadroproduction', 'charmed particle, photoproduction', 'charmed particle, neutrinoproduction', 'particle antiparticle, asymmetry', 'quarkonium, charm', 'charmed particle, lifetime', 'D', 'D/s', 'Lambda/c+', 'Xi/c+', 'Xi/c0', 'Omega/c0', 'charmed particle, decay modes', 'charmed meson, decay constant', 'violation, CP', 'D0 anti-D0, interference', 'HQET model', 'hadron spectroscopy', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911034'],['This paper is aimed at giving a complete review of the latest (post-1998 Physics in Collision conference) experimental results on charm physics.'],['1999-11-24']
1063,['eng'],"['Kulchitskii, Yu A', 'Kuzmin, M V', 'Vinogradov, V B']",['Non-compensation of an Electromagnetic Compartment of a Combined Calorimeter'],['Detectors and Experimental Techniques'],"['calorimeter, liquid argon', 'calorimeter, electromagnetic', 'showers, hadronic', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911033'],"['The method of extraction of the $e/h$ ratio, the degree of non-compensation, of the electromagnetic compartment of the combined calorimeter is suggested. The $e/h$ ratio of $1.74\\pm0.04$ has been determined on the basis of the 1996 combined calorimeter test beam data. This value agrees with the prediction that $e/h > 1.7$ for this electromagnetic calorimeter.']",['1999-11-24']
1064,['eng'],"['De Vivie de Régie, J B']",['Interpretation of Higgs and SUSY searches in MSUGRA and GMSB models'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'Higgs particle', 'sparticle, mass', 'lower limit', 'R parity, invariance', 'supersymmetry, symmetry breaking', 'supergravity', 'grand unified theory', 'neutralino', 'dependence, lifetime', 'slepton', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911032'],['Higgs and SUSY searches performed by the ALEPH Experiment at LEP are interpreted in the framework of two constrained R-parity conserving models: Minimal Supergravity and minimal Gauge Mediated Supersymmetry Breaking.'],['1999-11-23']
1065,['eng'],"['Winstein, Bruce D']",['CP and T Violation in $K_{L} \\to \\pi^{+}\\pi^{-}e^{+}e^{-}$'],['Particle Physics - Experimental Results'],"['talk, Blois 1999/06/28', 'K0(L), electromagnetic decay', 'violation, CP', 'time reversal, violation', 'mass spectrum, (pi+ pi- positron electron)', 'final-state interaction', 'angular distribution, asymmetry', 'numerical calculations', 'interpretation of experiments, CERN LEAR', 'K0(L) --> pi+ pi- positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911031'],['I will here make some brief comments on the T- and CP- odd asymmetry observed by KTeV in the KL -> pi^+pi^-e^+e^- decay.'],['1999-11-23']
1066,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barillari, T', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']","['Inclusive production of $D^{*\\pm}$ mesons in photon-photon collisions at $\\sqrt{s}_{ee}$= 183 and 189 GeV and a first measurement of $F^{\\gamma}_{2,c}$']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'quark, charm', 'quark, pair production', 'D*(2010), photoproduction', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'differential cross section, transverse momentum', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'photon, structure function', 'structure function, charm', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', 'electron positron --> D*(2010) positron electron anything', 'electron positron --> 2charm positron electron', 'D*(2010) --> D0 pi', 'D0 --> K- pi+', 'D0 --> K- 2pi+ pi-', '183, 189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911030'],"['The inclusive production of D*+- mesons in photon-photon collisions has been measured using the OPAL detector at LEP at e+e- centre-of-mass energies of 183 and 189GeV. The D* mesons are reconstructed in their decay to D0pi+ with the D0 observed in the two decay modes Kpi+ and Kpi+pi-pi+. After background subtraction, 100.4+-12.6(stat) D*+- mesons have been selected in events without observed scattered beam electron (""anti-tagged"") and 29.8+-5.9 (stat) D*+- mesons in events where one beam electron is scattered into the detector (""single-tagged""). Direct and single-resolved events are studied separately. Differential cross-sections as functions of the D* transverse momentum p_t and pseudorapidity \\eta are presented in the kinematic region 2<p_t<12GeV and calculations. The total cross-section for the process (e+e- to e+e-ccbar), where the charm quarks are produced in the collision of two quasi-real photons, is measured to be 842+-97(stat)+-75(syst)+-196(extrapolation)pb. A first measurement of the charm structure function F2 of the photon is performed in the kinematic range 0.0014<x<0.87 and 5<Q^2<100 GeV^2, and the result is compared to a NLO perturbative QCD calculation.']",['1999-11-23']
1067,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['$\\tau$ decays with neutral kaons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, leptonic decay', 'tau, pair production', 'tau-, semileptonic decay', 'K0', 'tau-, branching ratio', 'decay constant, ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau- --> anti-K0 pi- neutrino/tau', 'tau- --> anti-K0 pi- (n)pi0 neutrino/tau', 'tau- --> K0 K- (n)pi0 neutrino/tau', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911029'],"['The branching ratio of the tau lepton to a neutral K meson is measured from a sample of approximately 200,000 tau decays recorded by the OPAL detector at centre-of-mass energies near the Z0 resonance. The measurement is based on two samples which identify one-prong tau decays with KL and KS mesons. The combined branching ratios are measured to be B(tau- -->pi- K0bar nutau) = (9.33+-0.68+-0.49)x10^-3 B(tau- -->pi- K0bar [>=1pi0] nutau) = (3.24+-0.74+-0.66)x10^-3 B(tau- -->K- K0bar [>=0pi0] nutau) = (3.30+-0.55+-0.39)x10^-3 where the first error is statistical and the second systematic.']",['1999-11-23']
1068,['eng'],"['Pretzl, Klaus P']",['Cryogenic calorimeters in astro and particle physics'],['Detectors and Experimental Techniques'],"['talk, Lisbon 1999/06/13', 'calorimeter, energy resolution', 'temperature, low', 'temperature, measurement', 'cryogenics', 'tunneling', 'superconducting, droplet', 'astrophysics, missing-mass', 'double-beta decay', 'photon, cosmic radiation', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911028'],"['The development of cryogenic calorimeters was originally motivated by the fact that very low energy thresholds and excellent energy resolutions can be achieved by these devices. Cryogenic devices are widely used in double beta decay experiments, in cosmological dark matter searches, in x-ray detection of galactic and extragalactic objects as well as in cosmic background radiation experiments. An overview of the latest developments is given.']",['1999-11-23']
1069,['eng'],"['Daoudi, M']",['Review of $B\\overline{B}$ Mixing Results'],['Particle Physics - Experimental Results'],"['review, Southampton 1999/07/25', 'electron positron, colliding beams', 'electron positron, annihilation', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'B0, mass difference', 'B/s0, mass difference', 'time dependence', 'B0, hadronic decay', 'B/s0, hadronic decay', 'B/s0, semileptonic decay', 'experimental results', 'Cornell CESR Stor', 'CERN LEP Stor', 'SLAC SLC Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911027'],"['A review of B B-bar mixing results at the end of July 1999 is presented. Emphasis is put on recent measurements of Delta-Md and Delta-Ms. For Delta-Md, the new world average is Delta-Md = 0.473 +- 0.016 ps-1. For Delta-Ms, the new world average 95% CL limit is 12.4 ps-1, with a sensitivity of 14.2 ps-1. Other related results are covered very briefly.']",['1999-11-23']
1070,['eng'],"['Winstein, Bruce D']",['CP Violation in $K^{0}$ Decays'],['Particle Physics - Experimental Results'],"['talk, Blois 1999/06/28', 'K0(L), hadronic decay', 'K0(L), semileptonic decay', 'K0(L), rare decay', 'violation, CP', 'experimental results', 'Batavia TEVATRON PS', 'CERN SPS', 'K0(L) --> pi+ pi-', 'K0(L) --> 2pi0', 'K0(L) --> pi electron neutrino', 'K0(L) --> pi0 neutrino antineutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911026'],"['In this lecture, I will review results on the study of direct CP violation- where the violation occurs in a particle decay rather than in particle-anti particle mixing. Brief comments on rare decays, particularly those with a CP reach, will be made. Finally, I will indicate how the community would like to see the field evolve.']",['1999-11-22']
1071,['eng'],"['Vannucci, François']",['Search for Stimulated Neutrino Conversion with an RF Cavity'],['Particle Physics - Experimental Results'],"['talk, Blois 1999/06/28', 'neutrino, radiative decay', 'neutrino, lifetime', 'neutrino, beam', 'RF system, superconducting', 'transition, flavor', 'matter, effect', 'neutrino nucleon, interaction', 'charged current', 'numerical calculations', 'proposed experiment', 'neutrino/mu --> neutrino/e photon', 'neutrino/tau --> neutrino/e photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911025'],"['Little is known on radiative decays of numu and nutau. Lifetimes can be constrained, or the process discovered, by a search for flavour conversion in a superconducting RF cavity installed in a neutrino beam. The lifetimes tested with such a method can be of interest for astrophysics and cosmology. In particular the conjecture which explains both the LSND and the SuperKamiokande signals by radiative decays of numu can be straightforwardly put to the test.']",['1999-11-19']
1072,['eng'],"['Aguilar-Saavedra, J A']",['Computation of confidence intervals for Poisson processes'],['Detectors and Experimental Techniques'],"['statistical analysis', 'programming']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911024'],"['We present an algorithm which allows a fast numerical computation of Feldman-Cousins confidence intervals for Poisson processes, even when the number of background events is relatively large. This algorithm incorporates an appropriate treatment of the singularities that arise as a consequence of the discreteness of the variable.']",['1999-11-19']
1073,['eng'],"['Apyan, A B', 'Avakian, R O', 'Darbinian, S M', 'Ispirian, K A']",['Improved Crystal Method for Photon Beam Linear Polarization Measurement at High Energies'],['Detectors and Experimental Techniques'],"['photon, polarized beam', 'polarization, measurement', 'silicon, crystal', 'electron, pair production', 'experimental methods, proposed']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911021'],['A method for photon linear polarization determination based on the measurement of the asymmetry of the of pairs produced by polarized photon in single crystals in optimal intervals of pair particle energy is proposed. In contrast of known method the asymmetry in this case is essentially large. The optimal orientation of crystal is found which provide maximal values for analyzing power and merit factor as well as for minimal measurement time.'],['1999-11-18']
1074,['eng'],"['Burrows, P N']",['Searches for anomalous effects in the $b \\overline{b} g$ coupling$'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, beauty', 'jet, electroproduction', 'final state, (3jet)', 'vertex function, (quark antiquark gluon)', 'particle identification', 'angular distribution', 'parity, violation', 'time reversal, violation', 'violation, CP', 'final-state interaction', 'angular distribution, asymmetry', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911020'],"['The unique SLD CCD vertex detector combined with the highly-polarised electron beam allow us to search for an anomalous chromomagnetic coupling of the b-quark, as well as P-odd, T_N-odd and CP-odd processes at the b bbar g vertex.']",['1999-11-17']
1075,['eng'],"['Burrows, P N']",['A detector for precision study of high energy $e^{+}e^{-}$ annihilations'],['Detectors and Experimental Techniques'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beam detector', 'colliding beam detector, proposed', 'electron positron, annihilation', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'semiconductor, optical', 'drift chamber, time projection', 'calorimeter', 'electron positron, linear collider', 'linear collider, proposed']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911019'],['The status of the design of a detector for the TESLA collider is presented.'],['1999-11-16']
1076,['eng'],"['Siebel, M']",['Quark and gluon jet properties at LEP'],['Particle Physics - Experimental Results'],"['talk, Providence 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'final state, (3jet)', 'quark, jet', 'gluon, jet', 'gluon, fragmentation function', 'color', 'hadron, multiple production', 'scaling, violation', 'Altarelli-Parisi equation', 'eta', 'Phi(1020)', 'K*(892)', 'hadron, multiplicity', 'magnetic detector, OPAL', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', '((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911018'],"['The study of the differences of the fragmentation of quarks and gluons to jets of hadrons gives insight into the fundamental structure of QCD. Results from different approaches to properties of quarks and gluons are shown. The colour factor ratio $C_A/C_F$ is measured in agreement with the QCD prediction. Identified particles in quark and gluon jets are investigated, revealing no overproduction of isoscalar $\\eta^0$ and $\\phi(1020)$ in gluon jets, but an excess of protons.']",['1999-11-16']
1077,['eng'],"['Airapetian, A']",['Measurement of Longitudinal Spin Transfer to $\\Lambda$ Hyperons in Deep-Inelastic Lepton Scattering'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron, polarized beam', 'Lambda, electroproduction', 'Lambda, polarization', 'quark, polarization', 'quark, up', 'quark, fragmentation', 'helicity, conservation law', 'model, quark parton', 'mass spectrum, (p pi-)', 'angular distribution', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'positron p --> Lambda', 'Lambda --> p pi-', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911017'],"['Spin transfer in deep-inelastic Lambda electroproduction has been studied with the HERMES detector using the 27.5 GeV polarized positron beam in the HERA storage ring. For an average fractional energy transfer z=0.45, the measured longitudinal spin transfer from the virtual photon to the Lambda is 0.11 +/- 0.17 (stat) +/- 0.03 (sys). This quantity is expected to be sensitive to the up quark polarization in the Lambda hyperon and to the assumption of helicity conservation in the fragmentation process. The experimental result is interpreted in relation to various models of the Lambda spin content and found to favor the naive QPM. However, the present statistical precision is not yet sufficient to exclude a significant up quark polarization in the Lambda.']",['1999-11-16']
1078,['eng'],"['Bagliesi, G']",['Object oriented data analysis in ALEPH'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'data management', 'programming', 'magnetic detector, ALEPH', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911015'],"['This article describes the status of the ALPHA^{++} project of the ALEPH collaboration. The ALEPH data have been converted from Fortran data structures (BOS banks) into C^{++} objects and stored in a object oriented database (Objectivity/DB), using tools provided by the RD45 collaboration and the LHC^{++} software project at CERN. A description of the database setup and of a preliminary version of an object oriented analysis program is given.']",['1999-11-15']
1079,['eng'],"['Thomson, E J']",['New results on interference effects and correlations'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Lambda, pair production', 'hadron, multiple production', 'correlation, two-particle', 'correlation, (2Lambda)', 'correlation, (2Antilambda)', 'boson, statistics', 'fermion, statistics', 'correlation function', 'experimental results', 'CERN LEP Stor', '((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911014'],"['New results on interface effects and correlations are reviewed, including Fermi-Dirac and Bose-Einstein correlations in hadronic Z0 decays at LEP1.']",['1999-11-15']
1080,['eng'],"['Battaglia, M', 'Orava, Risto', 'Tammi, K', 'Österberg, K', 'Kucewicz, W', 'Zalewska, Agnieszka', 'Caccia, M', 'Campagnolo, R', 'Meroni, C', 'Grabiec, P', 'Jaroszewicz, B', 'Marczewski, J']",['High Resolution Hybrid Pixel Sensors for the $e^{+}e^{-}$ TESLA Linear Collider Vertex Tracker'],['Detectors and Experimental Techniques'],"['talk, Texel 1999/06/20', 'electron positron, colliding beam detector', 'colliding beam detector, background', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'resolution, impact parameter', 'background', 'electron positron, linear collider', 'linear collider, proposed']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911013'],"['In order to fully exploit the physics potential of a future high energy e+e- linear collider, a Vertex Tracker, providing high resolution track reconstruction, is required. Hybrid Silicon pixel sensors are an attractive option, for the sensor technology, due to their read-out speed and radiation hardness, favoured in the high rate environment of the TESLA e+e- linear collider design but have been so far limited by the achievable single point space resolution. In this paper, a conceptual design of the TESLA Vertex Tracker, based on a novel layout of hybrid pixel sensors with interleaved cells to improve their spatial resolution, is presented.']",['1999-11-12']
1081,['eng'],"['Loomba, D', 'Halyo, V', 'Lee, E R', 'Lee, I T', 'Kim, P C', 'Perl, Martin Lewis']",['A New Method for Searching for Free Fractional Charge Particles in Bulk Matter'],['Detectors and Experimental Techniques'],"['charged particle, search for', 'charge, fractional', 'experimental methods, droplet', 'experimental methods, optical', 'electric field', 'gravitation', 'mineral', 'astrophysics, matter']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001026'],"['We present a new experimental method for searching for free fractional charge in bulk matter; this new method derives from the traditional Millikan liquid drop method, but allows the use of much larger drops, 20 to 100 mm in diameter, compared to the traditional method that uses drops less than 15 mm in diameter. These larger drops provide the substantial advantage that it is then much easier to consistently generate drops containing liquid suspensions of powdered meteorites and other special minerals. These materials are of great importance in bulk searches for fractional charge particles that may have been produced in the early universe.']",['2000-01-13']
1082,['eng'],"['Gary, J W']",['Determination of the QCD color factor ratio CA/CF from the scale dependence of multiplicity in three jet events'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'jet, electroproduction', 'final state, (3jet)', 'hadron, multiplicity', 'quark, jet', 'gluon, jet', 'color', 'parametrization', 'numerical calculations, Monte Carlo', 'magnetic detector, DELPHI', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911011'],"['I examine the determination of the QCD color factor ratio CA/CF from the scale evolution of particle multiplicity in e+e- three jet events. I fit an analytic expression for the multiplicity in three jet events to event samples generated with QCD multihadronic event generators. I demonstrate that a one parameter fit of CA/CF yields the expected result CA/CF=2.25 in the limit of asymptotically large energies if energy conservation is included in the calculation. In contrast, a two parameter fit of CA/CF and a constant offset to the gluon jet multiplicity, proposed in a recent study, does not yield CA/CF=2.25 in this limit. I apply the one parameter fit method to recently published data of the DELPHI experiment at LEP and determine the effective value of CA/CF from this technique, at the finite energy of the Z0 boson, to be 1.74+-0.03+-0.10, where the first uncertainty is statistical and the second is systematic.']",['1999-11-10']
1083,['eng'],"['De Angelis, A']",['Jet and hadron production in $e^{+}e^{-}$ annihilations'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'hadron, multiple production', 'quark, pair production', 'quark, beauty', 'charged particle, multiplicity', 'quark, jet', 'gluon, jet', 'jet, multiplicity', 'particle identification, efficiency', 'leading logarithm approximation', 'duality, hadron parton', 'magnetic detector, DELPHI', 'CERN LEP Stor', '((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911010'],['The DELPHI detector at LEP is particularly suited for hadron identification and for the identification of b-initiated jets. This note presents recent results based on such characteristics.'],['1999-11-10']
1084,['eng'],"['Braun, G', 'Fischer, H', 'Franz, J', 'Grünemaier, A', 'Heinsius, F H', 'Hennig, L', 'Königsmann, Kay C', 'Niebuhr, M', 'Schierloh, M', 'Schmidt, T', 'Schmitt, H', 'Urban, H J']",['F1'],['Detectors and Experimental Techniques'],"['talk, Snowmass 1999/09/20', 'signal processing', 'integrated circuit', 'trigger', 'electronics', 'CERN SPS']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911009', 'http://documents.cern.ch/cgi-bin/setlink?base=yellowarticle&categ=99-09&id=p383']",['A new TDC chip has been developed for the COMPASS experiment at CERN. The resulting ASIC offers an unprecedented degree of flexibility and functionality. Its capability to handle highest hit and trigger input rates as well as its low power consumption makes it an ideal tool for future collider and fixed target experiments. First front-end boards equipped with the F1 chip have been used recently at testbeam experiments at CERN. A functional description and specification for this new TDC chip is presented.'],['1999-11-09']
1085,['eng'],"['King, B J']",['High Rate Physics at Neutrino Factories'],['Detectors and Experimental Techniques'],"['talk, Baltimore 1999/06/10', 'muon, storage ring', 'neutrino, particle source', 'neutrino, secondary beam', 'neutrino nucleon, deep inelastic scattering', 'charged current', 'neutral current', 'neutrino, counters and detectors', 'cross section', 'nucleon, structure function', 'quark, momentum spectrum', 'polarized target', 'structure function, polarization', 'Weinberg angle', 'neutrino electron, elastic scattering', 'Kobayashi-Maskawa angle', 'neutral current, flavor changing', 'production, charm', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911008'],"[""Both muon colliders and non-colliding muon storage rings using muon collider technology have the potential to become the first true ``neutrino factories'', with uniquely intense and precisely characterized neutrino beams that could usher in a new era of high rate and long baseline neutrino physics studies at accelerators. This paper gives an overview of the predicted capabilities of neutrino factories for high rate neutrino physics analyses that will use huge event samples collected with novel, high performance neutrino detectors.""]",['1999-11-09']
1086,['eng'],"['Abe, M', 'Emura, T', 'Odaka, S']",['Measurement of the trailing edge of cosmic-ray track signals from a round-tube drift chamber'],['Detectors and Experimental Techniques'],"['drift chamber, drift tube', 'argon, organic compounds', 'time resolution', 'numerical calculations, Monte Carlo', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911006'],"['The trailing edge of tube drift-chamber signals for charged particles is expected to provide information concerning the particle passage time. This information may be useful for separating meaningful signals from overlapping garbage at high-rate experiments, such as the future LHC experiments. We carried out a cosmic-ray test using a small tube chamber in order to investigate the feasibility of this idea. We achieved a trailing-edge time resolution of 12 ns in rms by applying simple pulse shaping to eliminate a signal tail. A comparison with a Monte Carlo simulation indicates the importance of well-optimized signal shaping to achieve good resolution. The resolution may be further improved with better shaping.']",['1999-11-08']
1087,['eng'],"['Amelung, C']",['Status of Measurements and Interpretation of Total Real and Virtual Photon-Proton Cross Sections'],['Particle Physics - Experimental Results'],"['talk, Protvino 1999/06/28', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'differential cross section', 'p, structure function', 'structure function, longitudinal', 'gluon, momentum spectrum', 'Altarelli-Parisi equation', 'scaling, violation', 'structure function, charm', 'momentum transfer, dependence', 'photon p, interaction', 'total cross section', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911005'],"['The status of measurements and interpretation of the proton structure function F2 is summarized. The measurements are subjected to DGLAP fits, from which the gluon density is extracted and a comparison to measurements of F2c is performed. The longitudinal structure function, FL, is extracted via an extrapolation of F2. At low Q2, the transition from virtual to real photon exchange is studied.']",['1999-11-05']
1088,['eng'],"['Adams, M R']",['$\\Lambda$ and $\\overline{\\Lambda}$ polarization from deep inelastic muon scattering'],['Particle Physics - Experimental Results'],"['muon+ nucleus, deep inelastic scattering', 'muon+, polarized beam', 'Lambda, electroproduction', 'Lambda, polarization', 'Antilambda, polarization', 'x-dependence', 'Lambda, hadronic decay', 'angular distribution', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '470 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911004'],['We report results of the first measurements of Lambda and Antilambda polarization produced in deep inelastic polarized muon scattering on the nucleon. The results are consistent with an expected trend towards positive polarization with increasing x_F. The polarizations of Lambda and Antilambda appear to have opposite signs. A large negative polarization for Lambda at low positive x_F is observed and is not explained by existing models.A possible interpretation is presented.'],['1999-11-05']
1089,['eng'],"['Weinstein, A J']",['$\\tau$ Electroweak Couplings'],['Particle Physics - Experimental Results'],"['review, Southampton 1999/07/25', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, decay modes', 'tau, branching ratio', 'Z0, leptonic decay', 'W-, leptonic decay', 'Z0, coupling', 'tau, polarization', 'weak interaction, moment', 'violation, CP', 'polarization, asymmetry', 'moment, electromagnetic', 'Michel parameter', 'neutral current, flavor changing', 'violation, flavor', 'neutrino, oscillation', 'neutrino/tau, mass', 'upper limit', 'lepton, universality', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'Cornell CESR Stor', 'bibliography', 'Z0 --> tau+ tau-', 'W- --> tau- neutrino/tau', 'Z0 --> tau+ tau- photon', 'tau- --> lepton- neutrino/tau antineutrino', 'tau- --> lepton- neutrino/tau antineutrino photon', '((3)) ((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911002'],"['We review world-average measurements of the tau lepton electroweak couplings, in both decay (including Michel parameters) and in production ($Z^0\\to anomalous weak and EM dipole couplings. Finally, we present the status of several other tau lepton studies: searches for lepton flavor violating decays, neutrino oscillations, and tau neutrino mass limits.']",['1999-11-03']
1090,['eng'],"['Majorovits, B', 'Klapdor-Kleingrothaus, H V']",['Digital Pulseshape Analysis by Neural Networks for the Heidelberg-Moscow- Double-$\\beta$-Decay-Experiment'],['Detectors and Experimental Techniques'],"['neutrino, mass', 'double-beta decay, (0neutrino)', 'germanium, crystal', 'background', 'signal processing', 'neural network', 'deep underground detector, Gran Sasso']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911001'],"['The Heidelberg-Moscow Experiment is presently the most sensitive experiment looking for neutrinoless double-beta decay. Recently the already very low background has been lowered by means of a Digital Pulseshape Analysis using a one parameter cut to distinguish between pointlike events and multiple scattered events. To use all the information contained in a recorded digital pulse, we developed a new technique for event recognition based on neural networks.']",['1999-11-03']
1091,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Albrecht, Z', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amapane, N', 'Amato, S', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Behrmann, A', 'Beillière, P', 'Belokopytov, Yu A', 'Benekos, N C', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Bertini, D', 'Bertrand, D', 'Besançon, M', 'Bigi, M', 'Bilenky, S M', 'Bizouard, M A', 'Bloch, D', 'Blom, H M', 'Bonesini, M', 'Bonivento, W', 'Boonekamp, M', 'Booth, P S L', 'Borgland, A W', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bourdarios, C', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Branchini, P', 'Brenke, T', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buran, T', 'Burgsmüller, T', 'Buschbeck, Brigitte', 'Buschmann, P', 'Cabrera, S', 'Caccia, M', 'Calvi, M', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chabaud, V', 'Charpentier, P', 'Chaussard, L', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Cieslik, K', 'Collins, P', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Cowell, J H', 'Crawley, H B', 'Crennell, D J', 'Crépé, S', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', 'Davenport, M', 'Da Silva, W', 'Deghorain, A', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Dolbeau, J', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Duperrin, A', 'Durand, J D', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ekspong, Gösta', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Erzen, B', 'Espirito-Santo, M C', 'Fanourakis, G K', 'Fassouliotis, D', 'Fayot, J', 'Feindt, Michael', 'Ferrari, P', 'Ferrer, A', 'Ferrer-Ribas, E', 'Ferro, F', 'Fichet, S', 'Firestone, A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J A', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Green, C', 'Grimm, H J', 'Gris, P', 'Grosdidier, G', 'Grzelak, K', 'Günther, M', 'Guy, J', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Hansen, J', 'Harris, F J', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hessing, T L', 'Heuser, J M', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Huet, K', 'Hughes, G J', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Janik, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kersevan, B P', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kinvig, A', 'Kjaer, N J', 'Klapp, O', 'Klein, H', 'Kluit, P M', 'Kokkinias, P', 'Koratzinos, M', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kriznic, E', 'Krumshtein, Z', 'Kubinec, P', 'Kurowska, J', 'Kurvinen, K L', 'Lamsa, J W', 'Lane, D W', 'Langefeld, P', 'Laugier, J P', 'Lauhakangas, R', 'Leder, Gerhard', 'Ledroit, F', 'Lefébure, V', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lemonne, J', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Lörstad, B', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Malmgren, T G M', 'Maltezos, S', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Martínez-Vidal, F', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Meroni, C', 'Meyer, W T', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Moch, M', 'Møller, R', 'Mönig, K', 'Monge, M R', 'Moreau, X', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mulet-Marquis, C', 'Muresan, R', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Naraghi, F', 'Nassiakou, M', 'Navarria, Francesco Luigi', 'Navas, S', 'Nawrocki, K', 'Negri, P', 'Némécek, S', 'Neufeld, N', 'Nicolaidou, R', 'Nielsen, B S', 'Niezurawski, P', 'Nikolenko, M', 'Nomokonov, V P', 'Normand, Ainsley', 'Nygren, A', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Orazi, G', 'Österberg, K', 'Ouraou, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Papageorgiou, K', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Pegoraro, M', 'Peralta, L', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Rodrigo, Germán', 'Røhne, O M', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Royon, C', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Schneider, H', 'Schwemling, P', 'Schwering, B', 'Schwickerath, U', 'Schyns, M A E', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Sekulin, R L', 'Shellard, R C', 'Sheridan, A', 'Siebel, M', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Smadja, G', 'Smirnova, O G', 'Smith, G R', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Sponholz, P', 'Squarcia, S', 'Stanescu, C', 'Stanic, S', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Tegenfeldt, F', 'Terranova, F', 'Thomas, J', 'Timmermans, J', 'Tinti, N', 'Tkatchev, L G', 'Todorova-Nová, S', 'Tomaradze, A G', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tranströmer, G', 'Treille, D', 'Tristram, G', 'Trochimczuk, M', 'Troncon, C', 'Tsirou, A L', 'Turluer, M L', 'Tyapkin, I A', 'Tzamarias, S', 'Ullaland, O', 'Valenti, G', 'Vallazza, E', 'Van der Velde, C', 'van Apeldoorn, G W', 'van Dam, P', 'Van Doninck, W K', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Remortel, N', 'Van Vulpen, I B', 'Vassilopoulos, N', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vodopyanov, A S', 'Vollmer, C F', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Walck, C', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zucchelli, G C', 'Zumerle, G']",['Consistent Measurements of $\\alpha_{s}$ from Precise Oriented Event Shape Distributions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'hadron, multiple production', 'event shape analysis', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002026'],"['An updated analysis using about 1.5 million events recorded at $\\sqrt{s} =M_Z$ with the DELPHI detector in 1994 is presented. Eighteen infrared and collinear safe event shape observables are measured as a function of the polar angle of the thrust axis. The data are compared to theoretical calculations in${\\cal O} (\\alpha_s^2)$ including the event orientation. A combined fit of $\\alpha_s$ and of the renormalization scale $x_{\\mu}$ in $\\cal O(\\alpha_s^2$)yields an excellent description of the high statistics data. The weighted average from 18 observables including quark mass effects and correlations is $\\alpha_s(M_Z^2) = 0.1174 \\pm 0.0026$. The final result, derived from the jet cone energy fraction, the observable with the smallest theoretical and experimental uncertainty, is $\\alpha_s(M_Z^2) = =0:1180 0:0006(exp:) 0:0013(hadr:) 0:0008(scale) 0:0007(mass). Further studies include an s determination using theoretical predictions in the next-to-leading log approximation (NLLA), matched NLLA and O(\\alpha^{2}_{s}) predictions as well as theoretically motivated optimized scale setting methods. The in uence of higher order contributions was also investigated by using the method of Pad e approximants. Average s values derived from the different approaches are in good agreement.']",['2000-02-09']
1092,['eng'],"['Ackerstaff, K']",['Nuclear Effects on $R = \\sigma_{L} / \\sigma_{T}$ in Deep-Inelastic Scattering'],['Particle Physics - Experimental Results'],"['positron nucleus, deep inelastic scattering', 'positron, polarized beam', 'deuteron', 'helium, nuclide', 'nitrogen', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'x-dependence', 'momentum transfer, dependence', 'dependence, mass number', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'bibliography', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910071'],"['Cross section ratios for deep-inelastic scattering from 14N and 3He with respect to 2H have been measured by the HERMES experiment at DESY using a 27.5 GeV positron beam. The data cover a range in the Bjorken scaling variable x between 0.013 and 0.65, while the negative squared four-momentum transfer Q^2 varies from 0.5 to 15 GeV^2. The data are compared to measurements performed by NMC, E665, and SLAC on 4He and 12C, and are found to be different for x < 0.06 and Q^2 < 1.5 GeV^2. The observed difference is attributed to an A-dependence of the ratio R = sigma_L / sigma_T of longitudinal to transverse deep-inelastic scattering cross sections at low x and low Q^2.']",['1999-11-02']
1093,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Korol, A A', 'Koshuba, S V', 'Kukartsev, G A', 'Nesterenko, I N', 'Otboev, A V', 'Pakhtusova, E V', 'Popov, V M', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Usov, Yu V', 'Zakharov, A S']",['New experimental data for the decays $\\phi \\to \\mu^{+}\\mu^{-}$ and $\\phi \\to \\pi^{+}\\pi^{-}$ from SND detector'],['Particle Physics - Experimental Results'],"['talk, Beijing 1999/08/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'muon, pair production', 'pi, pair production', 'Phi(1020), electroproduction', 'Phi(1020), leptonic decay', 'Phi(1020), electromagnetic decay', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'channel cross section, energy dependence', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> muon+ muon-', 'electron positron --> pi+ pi-', 'Phi(1020) --> muon+ muon-', 'Phi(1020) --> pi+ pi-', '0.98-1.06 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910070'],['The processes $e^+e^-\\to\\mu^+\\mu^-$ and $e^+e^-\\to\\pi^+\\pi^-$ have been studied with SND detector at VEPP-2M $e^+e^-$ collider in the vicinity of 0.45\\pm 0.32)\\times 10^{-4}$ and $B(\\phi\\to\\pi^+\\pi^-)=(0.71\\pm 0.11\\pm 0.09)\\times 10^{-4}$ were obtained.'],['1999-11-02']
1094,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Åkesson, P F', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Bailey, I', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karapetian, G V', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kupper, M', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wengler, T', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the $W^{+}W^{-} \\gamma$ Cross-section and First direct Limits on Anomalous Electroweak Quartic Gauge Couplings'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'photon, associated production', 'photon, energy spectrum', 'channel cross section', 'coupling, (4gauge boson)', 'coupling, (W+ W- 2photon)', 'coupling, (W+ W- Z0 photon)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W- photon', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910069'],"['A study of W+W- events accompanied by hard photon radiation produced in e+e- collisions at LEP is presented. Events consistent with two on-shell W-bosons and an isolated photon are selected from 183pb^-1 of data recorded at root{s}=189GeV. From these data, 17 W+W-gamma candidates are selected with photon energy greater than 10GeV, consistent with the Standard Model expectation. These events are used to measure the e+e- to W+W-gamma cross-section within a set of geometric and kinematic cuts; sigma{W+W-gamma} = 136+-37+-8 fb, where the first error is statistical and the second systematic. The photon energy spectrum is used to set the first direct, albeit weak, limits on possible anomalous contributions to the {W+ W- gamma gamma} and {W+ W- gamma Z0} vertices: -0.070GeV^{-2} < a_0/Lambda^2 < 0.070GeV^{-2}, -0.13GeV^{-2} < a_c/Lambda^2 < 0.19GeV^{-2}, -0.61GeV^{-2} < a_n/Lambda^2 < 0.57GeV^{-2}, where Lambda represents the energy scale for new physics.']",['1999-11-02']
1095,['eng'],"['Crittenden, J A']",['Topical Results on Vector-Meson Production from the HERA Collider Experiments'],['Particle Physics - Experimental Results'],"['talk, Newport News 1999/05/19', 'positron p, colliding beams', 'positron p, inclusive reaction', 'vector meson, photoproduction', 'diffraction, production', 'rho(770)0', 'Phi(1020)', 'J/psi(3100)', 'Upsilon(9460)', 'channel cross section, energy dependence', 'helicity, amplitude analysis', 'spin, density matrix', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910068'],"['The HERA collider experiments H1 and ZEUS have established extensive measurement programs for diffractive vector-meson production processes during the first six years of their operation. The results provide stringent phenomenological tests of quantum chromodynamical descriptions of hard diffraction. We discuss recent topical results on Upsilon photoproduction, on decay-angle analyses of rho^0, phi and J/psi electroproduction and on rho^0 and phi photoproduction at high momentum transfer.']",['1999-11-02']
1096,['eng'],"['Eerola, Paula Anna-Mari']","[""Beauty '99 Conference Summary""]",['Particle Physics - Experimental Results'],"['conference, review', 'Bled 1999/06/21', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'beautiful meson, hadronic decay', 'B/s0', 'B0', 'B+', 'time dependence', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'hadron hadron, interaction', 'electron positron, annihilation', 'quark, beauty', 'quark, pair production', 'K0(S), electroproduction', 'counters and detectors', 'experimental results', 'proposed experiment', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910067'],"[""Investigations of B hadrons are expected to break new ground in measuring CP-violation effects. This series of BEAUTY conferences, originating from the 1993 conference in Liblice, has contributed significantly in developing ideas of CP-violation measurements using B hadrons and formulating and comparing critically the B-physics experiments. In the '99 conference in Bled we saw the ripening of the field and the first fruit emerging - Tevatron have produced beautiful B-physics results and more are expected to come with the next run, while the B-physics experiments at DESY, SLAC and KEK are starting their operation. The longer-term projects at LHC and Tevatron have taken their shape and detailed prototyping work is going on. Meanwhile, on the phenomenological side, there has been impressive theoretical progress in understanding deeper the `standard' measurements and proposing new signatures. In this summary, I will highlight the status of the field as presented in the conference, concentrating on signatures, experiments, and R&D programmes.""]",['1999-11-02']
1097,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Darling, C L', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Evans, H', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Foucher, M', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hart, P', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Kirk, J', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lai, W P', 'Lafferty, G D', 'Lahmann, R', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Müller, U', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Palmonari, F', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Raith, B A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Springer, W', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Tecchio, M', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Wagner, D', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Precision Luminosity for $Z^{0}$ Lineshape Measurements with a Silicon-Tungsten Calorimeter'],['Particle Physics - Experimental Results'],"['electron positron, storage ring', 'beam monitoring, luminosity', 'electron positron, elastic scattering', 'calorimeter', 'tungsten', 'semiconductor detector', 'background', 'statistical analysis', 'Z0, width', 'magnetic detector, OPAL', 'CERN LEP Stor', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910066'],"['The measurement of small-angle Bhabha scattering is used to determine the luminosity at the OPAL interaction point for the LEP I data recorded between 1993 and 1995. The measurement is based on the OPAL Silicon-Tungsten Luminometer which is composed of two calorimeters encircling the LEP beam pipe, on opposite sides of the interaction point. The luminometer detects electrons from small-angle Bhabha scattering at angles between 25 and 58mrad. At LEP center-of-mass energies around the Z0, about half of all Bhabha electrons entering the detector fall within a 79nb fiducial acceptance region. The electromagnetic showers generated in the stack of 1 radiation length tungsten absorber plates are sampled by 608 silicon detectors with 38,912 radial pads of 2.5mm width.The fine segmentation of the detector, combined with the precise knowledge of its physical dimensions, allows the trajectories of incoming 45GeV electrons or photons to be determined with a total systematic error of less than 7microns. We have quantified all significant sources of systematic experimental error in the luminosity determination by direct physical measurement. All measured properites of the luminosity event sample are found to be in agreement with current theoretical expectations. The total systematic measurement uncertainty is 3.4x10^-4, significantly below the theoretical error of 5.4x10^-4 currently assigned to the QED calculation of the Bhabha acceptance, and contributes negligibly to the total uncertainty in the OPAL measurement of Gamma{invisible}/Gamma{l+l-}, a quantity of basic physical interest which depends crucially on the luminosity measurement.']",['1999-11-02']
1098,['eng'],"['Iwasaki, M']",['Study of top-quark reconstruction with LCD Fast Simulation'],['Particle Physics - Experimental Results'],"['talk, Sitges 1999/04/28', 'electron positron, annihilation', 'quark, pair production', 'quark, truth', 'quark, decay', 'jet, multiple production', 'final state, (4jet)', 'lepton, associated production', 'final state, (6jet)', 'particle identification, truth', 'charged particle, cluster', 'neutral particle, cluster', 'tracks', 'mass spectrum, (3jet)', 'numerical calculations, Monte Carlo', '500 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910065'],"['We report the study of top-quark reconstruction in $e^+e^- \\to t\\bar{t}$ events at a 500 GeV linear collider using the LCD Fast Simulator. The final states of 6 jets as well as 4 jets and lepton are used. In order to reconstruct the jets, the performance of charged and neutral cluster separation are studied. We compare top-quark reconstruction for the LCD Small and LCD Large detectors, including the effect of varying the calorimeter granularity.']",['1999-11-01']
1099,['eng'],"['Halyo, V', 'Kim, P', 'Lee, E R', 'Lee, I T', 'Loomba, D', 'Perl, Martin Lewis']",['Search for Free Fractional Electric Charge Elementary Particles'],['Particle Physics - Experimental Results'],"['charge, fractional', 'search for', 'experimental methods, droplet', 'electric field', 'gravitation', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910064'],['We have carried out a direct search in bulk matter for free fractional electric charge elementary particles using the largest mass single sample ever studied - about 17.4 mg of silicone oil. The search used an improved and highly automated Millikan oil drop technique. No evidence for fractional charge particles was found. The concentration of particles with fractional charge more than 0.16e (e being the magnitude of the electron charge) from the nearest integer charge is less than $4.71\\times10^{-22}$ particles per nucleon with 95% confidence.'],['1999-11-01']
1100,['eng'],"['Achasov, M N', 'Baru, S E', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Koop, I A', 'Korol, A A', 'Koshuba, S V', 'Kukartsev, G A', 'Pakhtusova, E V', 'Polunin, A A', 'Popov, V M', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Velikzhanin, Yu S', 'Zakharov, A S']",['Radiative decays of light vector mesons'],['Particle Physics - Experimental Results'],"['talk, Beijing 1999/08/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'vector meson, electroproduction', 'vector meson, radiative decay', 'rho(770)', 'omega(783)', 'Phi(1020)', 'pseudoscalar meson, production', 'pi0', 'eta', 'eta(958)', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> vector meson', 'vector meson --> pseudoscalar meson photon', '((1))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910063'],"['The new data on $\\rho,\\omega,\\phi$ radiative decays into collider are presented.']",['1999-11-01']
1101,['eng'],"['Airapetian, A']",['Observation of a Single-Spin Azimuthal Asymmetry in Semi-Inclusive Pion Electro-Production'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron p, inclusive reaction', 'positron, polarized beam', 'hydrogen, polarized target', 'polarization, longitudinal', 'pi+, electroproduction', 'spin, asymmetry', 'analyzing power', 'magnetic detector, HERMES', 'experimental results', 'DESY HERA Stor', '27.6 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910062'],['Single-spin asymmetries for semi-inclusive pion production in deep-inelastic scattering have been measured for the first time. A significant target-spin asymmetry of the distribution in the azimuthal angle phi of the pion relative to the lepton scattering plane was observed for pi+ electro-production on a longitudinally polarized hydrogen target. The corresponding analyzing power in the sin(phi) moment of the cross section is 0.022 +/- 0.005 +/- 0.003. This result can be interpreted as the effect of terms in the cross section involving chiral-odd spin distribution functions in combination with a time-reversal-odd fragmentation function that is sensitive to the transverse polarization of the fragmenting quark.'],['1999-10-29']
1102,['eng'],"['Aleev, A N', 'Amaglobeli, N S', 'Balandin, V P', 'Bugorski, A P', 'Cheshkov, C V', 'Gaponenko, A N', 'Geshkov, I M', 'Grigalashvili, T S', 'Khristov, P Z', 'Ivanchenko, I M', 'Ivanchenko, Z M', 'Kapishin, M N', 'Karpenko, N N', 'Kekelidze, V D', 'Khristova, T V', 'Kojenkova, Z I', 'Kopadze, M V', 'Kosarev, I G', 'Kretov, Yu A', 'Kurilin, A S', 'Kuzmin, N A', 'Kvatadze, R A', 'Lavrentyev, A A', 'Loktionov, A A', 'Lomidze, N L', 'Lyubimov, A L', 'Madigozhin, D T', 'Mestvirishvili, A S', 'Molokanova, N A', 'Morozov, A N', 'Panacik, A A', 'Ponta, T', 'Potrebenikov, Yu K', 'Preda, T', 'Skripnichuk, A G', 'Slepets, L A', 'Spaskov, V N', 'Tatishvili, G T', 'Tkachev, A L', 'Zinchenko, A I']",['Spin alignment of $K^{*}(892)^{\\pm}$ mesons produced in neutron-carbon interactions'],['Particle Physics - Experimental Results'],"['n nucleus, inclusive reaction', 'carbon', 'K*(892), hadroproduction', 'K*(892), hadronic decay', 'spin, density matrix', 'spin, alignment', 'transverse momentum, dependence', 'mass spectrum, (K0(S) pi)', 'pi, angular distribution', 'magnetic spectrometer, experimental results', 'Serpukhov PS', 'n carbon --> K*(892) anything', 'K*(892) --> K0(S) pi', 'approx. 60 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002054'],['A new precise measurements of spin density matrix element $\\rho_{00}$ of$K^*(892)^{\\pm}$ mesons produced inclusively in neutron-carbon interactions at\\~60 GeV have been carried out in the EXCHARM experiment at the Serpukhovaccelerator. The values of $\\rho_{00}$ obtained in the transversity frame are$0.424\\pm0.011(stat)\\pm0.018(sys)$ for $K^*(892)^+$ and$0.393\\pm0.025(stat)\\pm0.018(sys)$ for $K^*(892)^-$. Significant $P_T$dependence of $\\rho_{00}$ has been observed in $K^*(892)^+$ production.'],['2000-02-22']
1103,['eng'],"['Ahmed, S']",['Update of the Search for the Neutrinoless Decay $\\tau \\to \\mu\\gamma$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, radiative decay', 'violation, flavor', 'tau, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910060'],"['We present an update of the search for the lepton family number violating decay tau -> mu gamma using 12.6 million tau+tau- pairs collected with the CLEO detector. No evidence of a signal has been found and the corresponding upper limit is BR(tau -> mu gamma) < 1.1x10^{-6} at 90% CL, significantly smaller than previous experimental limits.']",['1999-10-28']
1104,['eng'],"['Nomokonov, V P']","['New results on multiplicity, identified particles and spin measurements in $e^{+}e^{-}$ collisions']",['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'quark, jet', 'gluon, jet', 'hadron, multiplicity', 'quantum chromodynamics, perturbation theory', 'validity test', 'leading logarithm approximation', 'color, coherence', 'duality, hadron parton', 'model, hadronization', 'Lambda(1520)', 'rho(770)', 'omega(783)', 'spin, density matrix', 'pseudoscalar meson', 'Lambda', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910059'],['The analyses of recent LEP data provide us with a rich ground for pQCD and LPHD tests. A number of non-trivial effects predicted in the framework of MLLA are experimentally verified. Recent measurements also enrich our knowledge about the hadronization process.'],['1999-10-28']
1105,['eng'],"['Serednyakov, S I']",['Rare Phi Decays and Exotic Hadrons'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'vector meson, electroproduction', 'vector meson, rare decay', 'vector meson, radiative decay', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'rho(770), branching ratio', 'omega(783), branching ratio', 'mass spectrum, (2pi0)', 'mass spectrum, (eta pi0)', 'mass spectrum, (pi+ pi- pi0)', 'a0(980)', 'f0(975)', 'hadron, exotic', 'baryon resonance, exotic', 'quark, multiquark', 'channel cross section, energy dependence', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> 2pi0 photon', 'electron positron --> eta pi0 photon', 'electron positron --> omega(783) pi0', 'electron positron --> pi+ pi-', 'electron positron --> vector meson', 'vector meson --> 2pi0 photon', 'Phi(1020) --> pi+ pi-', 'Phi(1020) --> omega(783) pi0', 'Phi(1020) --> eta(958) photon', 'electron positron --> pi+ pi- pi0', '0.4-1.4 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910058'],"['The results of the experimental study of the reactions e+e-->\\pi\\pi\\gamma, SND detectors are presented. The branching ratios of \\phi, \\rho, ømega rare decays were measured. The problem of the possible exotic nature of f0(980), a(980) scalar mesons is discussed.']",['1999-10-28']
1106,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Koop, I A', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Kukartsev, G A', 'Pakhtusova, E V', 'Popov, V M', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V', 'Velikzhanin, Yu S', 'Zakharov, A S']",['New Data from SND Detector in Novosibirsk'],['Particle Physics - Experimental Results'],"['talk, Beijing 1999/08/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'vector meson, electroproduction', 'vector meson, radiative decay', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'omega(783), branching ratio', 'rho(770), branching ratio', 'omega(783), excited state', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> vector meson', 'vector meson --> eta photon', 'vector meson --> pi0 photon', 'vector meson --> 2pi0 photon', 'vector meson --> eta pi0 photon', 'Phi(1020) --> omega(783) pi0', 'Phi(1020) --> pi+ pi-', 'Phi(1020) --> K0(L) K0(S)', '0.4-1.4 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910057'],"['The current status of experiments with SND detector at VEPP-2M e^+e^- collider in the energy range 2E_0=400-1400 MeV and recent results of data analysis for $\\phi$, $\\omega$ and $\\rho$ decays and e^+e^- annihilation into hadrons are presented.']",['1999-10-28']
1107,['eng'],"['Artuso, M', 'Ayad, R', 'Azfar, F', 'Efimov, A', 'Kopp, S E', 'Mountain, R', 'Majumder, G', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Wang, J C', 'Coan, T E', 'Fadeev, V', 'Volobuev, I', 'Ye, J', 'Anderson, S', 'Kubota, Y', 'Smith, A', 'Lipeles, E']",['Performance of the CLEO III LiF-TEA Ring Imaging Cherenkov Detector in a High Energy Muon Beam'],['Detectors and Experimental Techniques'],"['particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'Cherenkov counter, crystal', 'lithium, fluorine', 'angular resolution', 'optics, absorption', 'proportional chamber, wire', 'organic compounds, gas', 'photoelectron, yield', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910054'],"['The CLEO III Ring Imaging Cherenkov detector uses LiF radiators to generate Cherenkov photons which are then detected by proportional wire chambers using a mixture of CH$_4$ and TEA gases. The first two photon detector modules which were constructed, were taken to Fermilab and tested in a beam dump that provided high momentum muons. We report on results using both plane and ""sawtooth"" shaped radiators. Specifically, we discuss the number of photoelectrons observed per ring and the angular resolution. The particle separation ability is shown to be sufficient for the physics of CLEO III.']",['1999-10-27']
1108,['eng'],"['Dersch, U']","['Total Cross Section Measurements with $\\pi^{-}$, $\\Sigma^{-}$ and Protons on Nuclei and Nucleons around 600 GeV/c']",['Particle Physics - Experimental Results'],"['hadron nucleon, interaction', 'hadron nucleus, nuclear reaction', 'pi-', 'p', 'Sigma-', 'carbon', 'copper', 'organic compounds', 'model, Glauber', 'correction, screening', 'total cross section, momentum dependence', 'energy dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'approx. 600 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910052'],"['Total cross sections for Sigma- and pi- on beryllium, carbon, polyethylene and copper as well as total cross sections for protons on beryllium and carbon have been measured in a broad momentum range around 600GeV/c. These measurements were performed with a transmission technique adapted to the SELEX hyperon-beam experiment at Fermilab. We report on results obtained for hadron-nucleus cross sections and on results for sigma_tot(Sigma- N) and sigma_tot(pi- N), which were deduced from nuclear cross sections.']",['1999-10-26']
1109,['eng'],"['Csilling, Akos']",['Hadron production in two-photon collisions at LEP-L3'],['Particle Physics - Experimental Results'],"['talk, Zagreb 1999/06/17', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'hadron, multiple production', 'cross section, energy dependence', 'parametrization', 'Regge poles', 'rho(770)0, photoproduction', 'mass spectrum, (2rho(770) pi0)', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> (n)hadron positron electron', 'electron positron --> 2rho(770)0 positron electron', 'electron positron --> rho(770)0 positron electron anything']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910051'],"['The reaction e+ e- -> e+ e- gamma* gamma* -> e+ e- hadrons is analysed for quasi-real virtual photons using data collected by the L3 detector during the LEP high energy runs at sqrt(s) = 183 and 189 GeV. Preliminary results on the cross sections sigma(e+e- -> e+e- hadrons) and sigma(gamma gamma -> hadrons) are given in the interval 5 GeV < W_{gamma gamma} < 145 GeV. The centre-of-mass energy dependence of the two-photon cross section is well described by the universal Regge parametrisation, but with a steeper rise with energy as compared to hadron-hadron cross sections. The data are also compared to the expectations of different theoretical models. To investigate diffractive processes, the elastic gamma gamma -> rho0 rho0 process and the inclusive rho0 production gamma gamma -> rho0 X are studied in the W_{gamma gamma} > 3 GeV region. In all channels a comparison is made with the Pythia and Phojet Monte Carlo generators.']",['1999-10-26']
1110,['eng'],[],['Search for Charmless Haadronic Decays of B Mesons with the SLD Detector'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'beautiful meson, hadronic decay', 'beautiful meson, branching ratio', 'upper limit', 'B+', 'B0', 'B/s0', 'final state, (2meson)', 'final state, (0charmed particle)', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910050'],"['Based on a sample of approximately 500,000 hadronic Z0 decays accumulated between 1993 and 1998, the SLD experiment has set limits on 24 fully charged two-body and quasi two-body exclusive charmless hadronic decays of B+, B0, and B0_s mesons. The precise tracking capabilities of the SLD detector provided for the efficient reduction of combinatoric backgrounds, yielding the most precise available limits for ten of these modes.']",['1999-10-26']
1111,['eng'],[],['Search for Scalar Top and Scalar Bottom Quarks in $p\\overline{p}$ collisions at $\\sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'squark, truth', 'squark, beauty', 'squark, pair production', 'squark, decay', 'final state, ((n)jet missing-energy)', 'neutralino, LSP', 'sparticle, mass', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2squark anything', 'squark --> quark neutralino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910049'],"['We have searched for direct pair production of scalar top and scalar bottom quarks in 88 pb$^{-1}$ of $p\\bar{p}$ collisions at $\\sqrt{s}=1.8$ TeV with the CDF detector. We looked for events with a pair of heavy flavor jets and missing energy, consistent with scalar top quark decays to a charm quark and a neutralino, or scalar bottom quark decays to a bottom quark and a neutralino. The numbers of events that pass our selection for each process show no deviation from Standard Model expectations. We compare our results to next-to-leading order calculations for the scalar quark production cross sections to exclude regions in scalar quark-neutralino parameter space.']",['1999-10-25']
1112,['eng'],"['Landsberg, G L']",['The Search for Pentaquark Baryon with Hidden Strangeness'],['Particle Physics - Experimental Results'],"['talk, Batavia 1999/09/27', 'p nucleon, exclusive reaction', 'p nucleus, exclusive reaction', 'carbon', 'diffraction', 'baryon resonance, search for', 'quark, multiquark', 'Sigma0, hadroproduction', 'K, associated production', 'mass spectrum, (Sigma0 K)', 'baryon resonance, mass', 'baryon resonance, width', 'transverse momentum, spectra', 'magnetic spectrometer, experimental results', 'Serpukhov PS', '70 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910048'],"['Evidences for new baryon states with mass >1.8 GeV were obtained in the experiments of the SPHINX Collaboration in studying hyperon-kaon mass spectra in several proton diffractive reactions. The main result of these experiments is the observation of X(2000)->SIGMA K state with unusual dynamical features (narrow width, anomalously large branching ratios for the decay channels with strange particle emission). The possibility of the interpretation of this state as cryptoexotic pentaquark baryon with hidden strangeness is discussed. The additional data which are supported the real existence of X(2000) baryon are also presented.']",['1999-10-25']
1113,['eng'],"['Ma, H', 'Appel, R', 'Atoyan, G S', 'Bassalleck, B', 'Bergman, D', 'Cheung, N', 'Dhawan, S K', 'Do, H', 'Egger, J', 'Eilerts, S W', 'Fischer, H', 'Herold, W D', 'Issakov, V V', 'Kaspar, H', 'Kraus, D E', 'Lazarus, D M', 'Lichard, P', 'Lowe, J', 'Lozano-Bahilo, J', 'Majid, W A', 'Menzel, W', 'Pislak, S', 'Poblaguev, A A', 'Rehak, P', 'Sher, A E', 'Thompson, J A', 'Truöl, P', 'Zeller, M E']",['A New Measurement of the Rare Decay $K^{+}\\to \\pi^{+} \\mu^{+} \\mu^{-}$'],['Particle Physics - Experimental Results'],"['K+, rare decay', 'K+, semileptonic decay', 'K+, branching ratio', 'mass spectrum, (pi+ muon+ muon-)', 'mass spectrum, (muon+ muon-)', 'angular distribution', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ muon+ muon-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910047'],"['More than 400 $K^{+}\\to\\pi^{+}\\mu^+\\mu^-$ events were observed in a rare $K^+$ decay experiment at the AGS. Normalized to the $K^{+}\\to\\pi^{+}\\pi^+\\pi^-$ decay, the branching ratio is determined to be $(9.22 \\pm 0.60 (stat) \\pm 0.49 (syst))\\times 10^{-8}$. This branching ratio and the $\\mu\\mu$ mass spectrum is in very good agreement with the measurement of the $K^{+}\\to\\pi^{+}e^+e^-$ decay, but deviates significantly from the previous measurement.']",['1999-10-22']
1114,['eng'],"['Anderson, S']",['Hadronic Structure in the Decay $\\tau^{-}\\to \\pi^{-}\\pi^{0}\\nu_{\\tau}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'mass spectrum, (pi- pi0)', 'rho(770)-', 'rho(1450)', 'CVC model, validity test', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'bibliography', 'electron positron --> tau+ tau-', 'tau- --> pi- pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910046'],['We report on a study of the invariant mass spectrum of the hadronic system in the decay tau- -> pi- pi0 nu_tau. This study was performed with data obtained with the CLEO II detector operating at the CESR e+ e- collider. We present fits to phenomenological models in which resonance parameters associated with the rho(770) and rho(1450) mesons are determined. The pi- pi0 spectral function inferred from the invariant mass spectrum is compared with data on e+ e- -> pi+ pi- as a test of the Conserved Vector Current theorem. We also discuss the implications of our data with regard to estimates of the hadronic contribution to the muon anomalous magnetic moment.'],['1999-10-22']
1115,['eng'],[],['Measurement of inclusive prompt photon photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'photon, direct production', 'differential cross section, rapidity dependence', 'transverse energy, dependence', 'quantum chromodynamics, perturbation theory', 'showers, parton', 'leading logarithm approximation', 'photon, structure function', 'parametrization', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> photon anything', 'approx. 300 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910045', 'http://www-zeus.desy.de/~schlenst/conf/osaka_paper.html']","['First inclusive measurements of isolated prompt photons in photoproduction at the HERA ep collider have been made with the ZEUS detector, using an integrated luminosity of 38.4 pb$^{-1}$. Cross sections are given as a function of the pseudorapidity and the transverse energy ($\\eta^\\gamma$, \\eTg) of the photon, for $\\eTg > $ 5 GeV in the $\\gamma p$ centre-of-mass energy range 134-285 GeV. Comparisons are made with predictions from Monte Carlo models having leading-logarithm parton showers, and with next-to-leading-order QCD calculations, using currently available parameterisations of the photon structure. For forward $\\eta^\\gamma$ (proton direction) good agreement is found, but in the rear direction all predictions fall below the data.']",['1999-10-21']
1116,['eng'],"['Palla, Fabrizio']",['An investigation on the b quark mass'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, multiple production', 'particle identification, flavor', 'final state, (3jet)', 'mass, beauty', 'event shape analysis', 'correction, hadronization', 'correction, higher-order', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910044'],"['In this article I will review the measurements of the b quark mass performed by ALEPH and DELPHI and presented at the HEP99 Conference in Tampere. Very clean effects of the mass running are observed, even if a wide spread in the results and large systematic errors due to hadronization corrections prevent to extract an average value of the running b quark mass.']",['1999-10-21']
1117,['eng'],[],"['Measurement of the $E_{T}^{2},jet/Q^{2}$ dependence of forward-jet production at HERA']",['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'jet, photoproduction', 'small-angle', 'photon, resolved', 'quantum chromodynamics, perturbation theory', 'showers, parton', 'Altarelli-Parisi equation', 'Lipatov equation', 'color, dipole', 'differential cross section, transverse energy', 'momentum transfer, dependence', 'numerical calculations, Monte Carlo', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> jet anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910043'],"['The forward-jet cross section in deep inelastic ep scattering has been measured using the ZEUS detector at HERA with an integrated luminosity of 6.36 pb^-1. The jet cross section is presented as a function of jet transverse energy squared, E(T,jet)^2, and Q^2 in the kinematic ranges 10^-2<E(T,jet)^2/Q^2<10^2 and 2.5 10^-4<x<8.0 10^-2. Since the perturbative QCD predictions for this cross section are sensitive to the treatment of the log(E_T/Q)^2 terms, this measurement provides an important test. The measured cross section is compared to the predictions of a next-to-leading order pQCD calculation as well as to various leading-order Monte Carlo models. Whereas the predictions of all models agree with the measured cross section in the region of small E(T,Jet)^2/Q^2, only one model, which includes a resolved photon component, describes the data over the whole kinematic range.']",['1999-10-21']
1118,['eng'],"['Mikaelyan, L A']","['Chooz, Palo Verde, Krasnoyarsk']",['Particle Physics - Experimental Results'],"['talk, Paris 1999/09/06', 'neutrino, oscillation', 'fission, particle source', 'antineutrino p, interaction', 'charged current', 'antineutrino/e', 'positron, energy spectrum', 'correlation, (n positron)', 'neutrino, mass difference', 'neutrino, mixing angle', 'scintillation counter, liquid', 'experimental results', 'proposed experiment', 'antineutrino/e p --> n positron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910042'],['This is a short review of the present ~ 1 km baseline oscillation experi-ments at nuclear reactors. An idea of a new search for very small mixing angle oscillations at Krasnoyarsk is also mentioned.'],['1999-10-21']
1119,['eng'],"['Mandelkern, M A', 'Schultz, J']",['The Statistical Analysis of Gaussian and Poisson Signals Near Physical Boundaries'],['Detectors and Experimental Techniques'],['statistical analysis'],['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910041'],"['We propose a construction of frequentist confidence intervals that is effective near unphysical regions and unifies the treatment of two-sided and upper limit intervals. It is rigorous, has coverage, is computationally simple and avoids the pathologies that affect some other constructions. Away from non-physical regions, the results are exactly the usual central two-sided intervals. The construction is based on including the physical constraint in the Likelihood Function, leading to an estimator that is necessarily in the physical domain.']",['1999-10-21']
1120,['eng'],"['Abbott, B']",['Search for Second Generation Leptoquark Pairs in $\\overline{p}p$ Collisions at $\\Sqrt{s} =1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, leptoquark', 'leptoquark, pair production', 'leptoquark, decay', 'final state, ((n)jet dimuon)', 'leptoquark, vector', 'leptoquark, scalar', 'leptoquark, mass', 'lower limit', 'channel cross section, upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910040'],"['We have searched for second generation leptoquark (LQ) pairs in the the D0 experiment at the Fermilab Tevatron during 1993-1996. No evidence for a signal is observed. These results are combined with those from the \\mu\\nu+jets and \\nu\\nu+jets channels to obtain 95% confidence level (C.L.) upper limits on the LQ pair production cross section as a function of mass and $beta, the branching fraction of a LQ decay into a charged lepton and a quark. Lower limits of 200(180) GeV/c^2 for \\beta=1(1/2) are set at the 95% C.L. on the mass of scalar LQ. Mass limits are also set on vector leptoquarks as a function of']",['1999-10-20']
1121,['eng'],"['Iori, M']",['Charm hadroproduction results from Selex'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'p nucleon, inclusive reaction', 'pi- nucleon, inclusive reaction', 'nucleon Sigma, inclusive reaction', 'D, hadroproduction', 'Lambda/c+, hadroproduction', 'particle antiparticle, asymmetry', 'x-dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'hadron nucleon --> charmed particle anything', '650 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910039'],"['The SELEX experiment (E781) is 3-stage magnetic spectrometer for a high statistics study of hadroproduction of charm baryons out to large x_F using 650 Gev Sigma-, pi- and p beams. The main features of the spectrometer are: a high precision silicon vertex system, powerful particle identification provided by TRD and RICH, forward Lambda decay spectrometer and 3-stage lead glass photon detector. An experiment overview and spectrometer features are shown. Reconstructed charm states and results on Lambda_c, D+ particles and antiparticles produced by Sigma-, pi- and p beams at x_F>0.3 and asymmetry for Lambda_c are presented.']",['1999-10-20']
1122,['eng'],[],['Measurement of diffractive photoproduction of vector mesons at large momentum transfer at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'photon p, exclusive reaction', 'vector meson, photoproduction', 'diffraction, dissociation', 'rho(770)0', 'Phi(1020)', 'J/psi(3100)', 'vector meson, hadronic decay', 'angular distribution', 'differential cross section, momentum transfer', 'quantum chromodynamics, perturbation theory', 'mass spectrum, two-pion', 'spin, density matrix', 'energy dependence', 'pomeron, exchange', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> p vector meson positron', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910038'],"['Elastic and proton-dissociative photoproduction of $\\rho^0$, $\\phi$ and $J/\\psi$ vector mesons ($\\gamma p\\to Vp$, $\\gamma p\\to VN$, respectively) have been measured in e^+p interactions at HERA up to -t=3 GeV$^2$, where t is the four-momentum transfer squared at the photon-vector meson vertex. The analysis is based on a data sample in which photoproduction reactions were tagged by detection of the scattered positron in a special-purpose calorimeter. This limits the photon virtuality, Q^2, to values less than 0.01 GeV$^2$, and selects a $\\gamma p$ average center-of-mass energy of <W> = 94 GeV. Results for the differential cross sections, d$\\sigma$/d$t$, for $\\rho^0$, $\\phi$ and $J/\\psi$ mesons are presented and compared to the results of recent QCD calculations. Results are also presented for the t-dependence of the pion-pair invariant-mass distribution in the $\\rho^0$ mass region and of the spin-density matrix elements determined from the decay-angle distributions. The Pomeron trajectory has been derived from measurements of the W dependence of the elastic differential cross sections d$\\sigma$/d$t$ for both $\\rho^0$ and $\\phi$ mesons.']",['1999-10-20']
1123,['eng'],"['Ellison, J']",['W and Z Properties at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'intermediate boson, pair production', 'channel cross section, branching ratio', 'W, width', 'universality, (tau electron)', 'coupling, (3gauge boson)', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910037'],"['We present recent results from CDF and D0 on W and Z production cross sections, the width of the W boson, tau-e universality in W decays, trilinear gauge boson couplings, and on the observation of Z -> b bbar.']",['1999-10-20']
1124,['eng'],"[""D'Agostini, G""]",['Sceptical combination of experimental results'],['Particle Physics - Experimental Results'],"['data analysis method', 'statistical analysis', 'K0, hadronic decay', 'violation, CP', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910036'],"['This paper is meant as a contribution to the often debated subject of how to combine data which appear to be in mutual disagreement. As a practical example, the epsilon-prime/epsilon determinations have been considered.']",['1999-10-19']
1125,['eng'],"['Abbaneo, D']",['Production of excited charmed mesons at LEP'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, semileptonic decay', 'charmed meson, excited state', 'charmed meson, yield', 'D*2(2460), hadronic decay', 'D/s*2(2536), hadronic decay', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'D*2(2460) --> D*(2010) pi-', 'D*(2010) --> D0 pi+', 'D/s*2(2536) --> D0 K', '((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910035'],"['Studies od the production of orbitally excited charmed and charmed strange mesons in e+e- collisions, performed by the LEP collaborations are reviewed. Measurements of the production rates of orbitally excited charmed mesons in semileptonic b decays are presented. Searches for charmed meson radial excitations are also briefly discussed.']",['1999-10-19']
1126,['eng'],"['Landsberg, G L']",['Search for Exotics at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'leptoquark, mass', 'lower limit', 'quark, composite', 'lepton, composite', 'family, 4', 'Higgs particle, radiative decay', 'particle, technicolor', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'proposed experiment', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910034'],"['We present recent results on searches for non-SUSY new physics at the CDF and D0 Collaborations in the 1992-1996 Fermilab Tevatron run. While no compelling evidence for existence of new physics was found, the Tevatron data have excluded a significant region of the theoretically allowed phase space for a variety of non-SUSY extensions of the Standard Model. Tight limits on the existence of the following new phenomena are set: leptoquarks of all three generations, quark-lepton compositeness, 4-th generation quarks, fermiophobic Higgs, technicolor, etc. Prospects of the Tevatron experiments in Run II are discussed.']",['1999-10-19']
1127,['eng'],"['Lykken, J D', 'Matchev, K T']",['Tau Jet Signals for Supersymmetry at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Batavia 1998/11/19', 'talk, Gainesville 1999/03/08', 'talk, Madison 1999/04/14', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'supergravity', 'supersymmetry', 'final state, (tau lepton)', 'sparticle, pair production', 'sparticle, decay modes', 'chargino', 'neutralino', 'slepton', 'final state, (3lepton)', 'tau, semileptonic decay', 'jet', 'sparticle, mass', 'mass, hierarchy', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> chargino neutralino anything']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910033'],"['We present a more detailed account of our study (hep-ph/9903238) for the supersymmetry reach of the Tevatron in channels with isolated leptons and identified tau jets. We review the theoretical motivations for expecting such signatures, and describe the relevant parameter space in the minimal supergravity and the minimal gauge-mediated models. With explicit Monte Carlo simulations we then show that for certain parameter ranges, channels with two leptons and one tau jet offer a better reach in Run II than the clean trilepton signal. We emphasize than improving on tau ID is an important prerequisite for successful searches in multiple tau jet channels. Finally, we discuss some triggering issues.']",['1999-10-18']
1128,['eng'],"['LI, H']",['Recent $N^{*}$ Results From $J/\\psi$ Decays'],['Particle Physics - Experimental Results'],"['talk, Beijing 1999/08/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'J/psi(3100), electroproduction', 'J/psi(3100), hadronic decay', 'mass spectrum, (p pi0)', 'mass spectrum, (p eta)', 'mass spectrum, (anti-p pi0)', 'mass spectrum, (anti-p eta)', 'partial wave analysis', 'N(1535)', 'N(1650)', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> J/psi(3100)', 'J/psi(3100) --> p anti-p pi0', 'J/psi(3100) --> p anti-p eta', '3.1 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910032'],"['Based on 7.8 million J/\\psi events collected at BEPC, the events for J/\\psi peaks are observed around 1480 MeV in p\\pi^0 (\\bar{p}\\pi^0) invariant mass spectrum and near the threshold for $\\eta$ production in p\\eta(\\bar{p}\\eta) invariant mass spectrum. A partial wave analysis of J/\\psi \\to p\\bar{p}\\eta data has been performed. Two J^P={1/2}^- resonances are observed with mass and width (M, \\Gamma) at (1540^{+15}_{-17}, 178^{+20}_{-22}) MeV and (1648^{+18}_{-16}, 150)MeV, and are considered to be the nucleon resonances S_{11}(1535) and S_{11}(1650) respectively.']",['1999-10-18']
1129,['eng'],"['Cerutti, F']",['Is there new physics in the 1999 ALEPH data ?'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'sparticle', 'supersymmetry, symmetry breaking', 'Higgs particle, neutral particle', 'R parity, violation', 'electroweak interaction, validity test', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '192, 196 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910031'],['The first results on searches performed by ALEPH on the 1999 data sample are presented here. They are based on an integrated luminosity of about 54 pb$^-1$ collected at the two centre-of-mass energies of 192 and 196 GeV. Preliminary results on searches for supersymmetric particles and for the neutral Higgs bosons are shown.'],['1999-10-18']
1130,['eng'],[],['Search for the Weak Decay of a Lightly Bound H Dibaryon'],['Particle Physics - Experimental Results'],"['p nucleus, interaction', 'neutral particle, secondary beam', 'baryon resonance, dibaryon', 'H baryon, hadronic decay', 'H baryon, mass', 'channel cross section, branching ratio', 'upper limit', 'dependence, lifetime', 'dependence, mass', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'H baryon --> Lambda p pi-', 'Xi- --> Lambda pi0', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910030'],['5 \\times 10^{-10}$~sec to $\\sim'],['1999-10-18']
1131,['eng'],[],['Recent results from D0 on the top quark'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'spin, correlation', 'quark, decay modes', 'Higgs particle, charged particle', 'final state, (muon electron)', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> Higgs particle beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910029'],"['We describe three recent results from D0 related to the top quark: a preliminary measurement of the t-tbar spin correlation in top quark pair production, a search for top quark decays into charged Higgs bosons, and an improved cross section analysis in the t-tbar -> e mu channel using neural networks.']",['1999-10-18']
1132,['eng'],"['Petroff, P']",['D0 Upgrade for RUN II'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beam detector', 'anti-p p, colliding beams', 'electroweak interaction, validity test', 'quantum chromodynamics, validity test', 'quark, truth', 'quark, beauty', 'four-pi-detector, DZERO', 'upgrade', 'semiconductor detector, microstrip', 'scintillation counter, fibre', 'solenoid, superconducting', 'proportional chamber, drift tube', 'trigger', 'Batavia TEVATRON Coll', 'talk, Mumbai 1999/01/14']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910028'],"['The D0 detector at The Fermilab Tevatron is undergoing a major upgrade to prepare for data taking with luminosities reaching 2 x 10^{32} cm^{-2} s^{-1}. The upgrade includes a new central tracking array, new muon detector components and electronic upgrades to many subsystems. The D0 upgraded detector will be operational for RUN II in spring 2000.']",['1999-10-15']
1133,['eng'],"['Harris, F A']",['Recent Charmonium Results from BES'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'quarkonium, charm', 'quarkonium, electroproduction', 'quarkonium, hadronic decay', 'quarkonium, radiative decay', 'psi(3685), branching ratio', 'psi(3685), decay modes', 'chi mesons, charm', 'eta/c(2980), mass', 'chi/c0(3415), mass', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', '2-5 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910027'],"[""This paper summarizes recent results obtained from the BES psi(2S) data, which with 3.8 M events, is the world's largest data set. Distributions for psi(2S) -> pi^+ pi^- J/psi are fit to the Novikov-Shifman model. Preliminary branching fractions are reported for psi(2S) -> gamma f_2(1270) and gamma f_J(1710), as well as for decays into states containing an omega or phi. Finally recent measurements of the mass of the chi_c0 and eta_c are reported.""]",['1999-10-15']
1134,['eng'],"['Wall, D']",['Search for nucleon decay into lepton + K0 final states using Soudan 2'],['Particle Physics - Experimental Results'],"['nucleon, semileptonic decay', 'search for, decay', 'p, lifetime', 'lower limit', 'supersymmetry', 'grand unified theory', 'deep underground detector, Soudan', 'experimental results', 'p --> K0 lepton+', 'n --> K0 neutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910026'],"['A search for nucleon decay into two-body final states containing K^0 mesons has been conducted using the 963 metric ton Soudan 2 iron tracking calorimeter. The topologies, ionizations, and kinematics of contained events recorded in a 5.52 kiloton-year total exposure (4.41 kton-year fiducial volume exposure) are examined for compatibility with nucleon decays in an iron medium. For proton decay into the fully visible final states \\mu^+K^0_s and e^+K^0_s, zero and one event candidates are observed respectively. The lifetime lower limits (\\tau /B) thus implied are 1.5 \\times 10^{32} years and 1.2 \\times 10^{32} years, respectively. Lifetime lower limits are also reported for proton decay into l^+K^0_l, and for neutron decay into \\nu K^0_s.']",['1999-10-15']
1135,['eng'],"['Ashery, D']",['Diffractive Dissociation of High Momentum Pions'],['Particle Physics - Experimental Results'],"['talk, Bloomington 1999/04/08', 'pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'jet, pair production', 'pi-, diffraction', 'diffraction, dissociation', 'pi, wave function', 'quark, momentum spectrum', 'color, transparency', 'dependence, mass number', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910024'],"['The diffractive dissociation of 500 GeV/c $\\pi^-$ into di-jets is described as a way to measure the momentum distribution of quarks in the pion. The measurements of the pion diffractive dissociation were carried out using data from Fermilab E791. Preliminary results show that the $|q\\bar {q}>$ Asymptotic wave function which was developed using perturbative QCD methods describes the data well for $Q^2 \\sim 10 ~{\\rm (GeV/c)^2}$. At these values signals of color transparency are expected and, indeed, observed through the $A$-dependence of the yield of the diffractive di-jets.']",['1999-10-14']
1136,['eng'],"['Abe, T']",['QCD with SLD'],['Particle Physics - Experimental Results'],"['talk, Providence 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, beauty', 'gluon, associated production', 'gluon, fragmentation', 'beautiful particle, energy spectrum', 'hadron, multiple production', 'correlation, two-particle', 'rapidity, correlation', 'baryon number, conservation law', 'charge, conservation law', 'correlation, long-range', 'dependence, flavor', 'quantum chromodynamics, validity test', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty gluon', 'Z0 --> quark antiquark gluon', 'gluon --> 2beauty', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910023'],"['We present selected new results on strong interaction physics from the SLD experiment at the SLAC Linear Collider (SLC), symmetry tests of b\\bar{b}g vertex, the rate of secondary b\\bar{b} production via gluon splitting, the B hadron energy spectrum and rapidity correlations between identified charged hadrons. The parity violation in Z0 --> b\\bar{b}g decays is consistent with electroweak theory plus QCD. New tests of T- and CP-conservation at the splitting into b\\bar{b} pairs yields g_{b\\bar{b}}=0.00307 +- 0.00071 (stat.) +- 0.00066 (syst.) (Preliminary). The B hadron energy spectrum is measured using a new inclusive technique, allowing tests of predictions for its shape and a measurement of < x_B > = 0.714 +- 0.005 (stat.) +- 0.007 (syst.) (Preliminary). A study of correlations in rapidity between pairs of identified pions, kaons and protons confirms that strangeness and baryon number areconserved locally, and shows local charge conservation between meson-baryon and strange-nonstrange pairs. Flavor-dependent long-range correlations are observed for all combinations of these hadron species. The first study of correlations using signed rapidities is done and find the first direct observation of baryon number ordering along the q\\bar{q} axis.']",['1999-10-13']
1137,['eng'],"['Hawkings, R', 'Mönig, K']",['Electroweak and CP violation physics at a linear collider Z-factory'],['Detectors and Experimental Techniques'],"['electron positron, linear collider', 'linear collider, proposed', 'polarized beam', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'Z0, branching ratio', 'polarization, asymmetry', 'angular distribution, asymmetry', 'electroweak interaction, validity test', 'Kobayashi-Maskawa angle', 'violation, CP', 'B, hadronic decay', 'B/s0, hadronic decay', 'mass spectrum, two-pion', 'numerical calculations, Monte Carlo', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910022'],"['A future linear collider such as TESLA may be able to run on the Z0 resonance with very high luminosity and polarised electron and positron beams. The possibilities of measuring electroweak quantities with high precision are investigated. Huge improvements with respect to the present precision can be expected, especially for the asymmetries A_LR and A_b where beam polarisation can be exploited. The very large sample of Z to bbbar events also allows studies of various CP-violating b decays. The precision achievable on the CKM unitarity triangle angles is comparable to experiments at b factories and future hadron colliders.']",['1999-10-13']
1138,['eng'],"['Bussey, Peter J']",['Photoproduction at low $Q^{2}$'],['Particle Physics - Experimental Results'],"['talk, Ann Arbor 1999/06/24', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'jet, multiple production', 'momentum transfer, low', 'hard scattering', 'photon, resolved', 'final state, (2jet)', 'final state, (3jet)', 'photon, direct production', 'photon, structure function', 'gluon, momentum spectrum', 'energy spectrum, transverse energy', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910018'],['The past year has seen a number of important developments in hard photoproduction physics at the HERA Collider. These are surveyed.'],['1999-10-12']
1139,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bevensee, B', 'Bhatti, A A', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, B S', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chan, A W', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Ciobanu, C I', 'Clark, A G', 'Cobal, M', 'Cocca, E', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Costanzo, D', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Gadomski, S', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Grassmann, H', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incagli, M', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kirk, M', 'Kim, B J', 'Kim, H S', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Knoblauch, D', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Meschi, E', 'Mesropian, C', 'Miao, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Parri, A', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Perazzo, A', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takashima, R', 'Takikawa, K', 'Tanaka, M', 'Takano, T', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Truitt, S', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Production of $\\Upsilon(1S)$ Mesons from $_{\\chi}_{b}$ Decays in $p\\overline{p}$ Collisions at $sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quarkonium, hadroproduction', 'chi mesons, beauty', 'chi mesons, radiative decay', 'upsilon mesons, hadronic decay', 'Upsilon(9460), direct production', 'Upsilon(9460), leptonic decay', 'yield, ratio', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> chi mesons anything', 'chi mesons --> Upsilon(9460) photon', 'Upsilon(9460) --> muon+ muon-', 'anti-p p --> upsilon mesons anything', 'upsilon mesons --> Upsilon(9460) pi+ pi-', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910025'],"['We have reconstructed the radiative decays $\\chi_{b}(1P) \\to \\Upsilon(1S) at $\\sqrt{s} = 1.8$ TeV, and measured the fraction of $\\Upsilon(1S)$ mesons that originate from these decays. For $\\Upsilon(1S)$ mesons with $p^{\\Upsilon}_{T}>8.0$ GeV/$c$, the fractions that come from $\\chi_{b}(1P)$ and $(10.5\\pm4.4(stat)\\pm1.4(s ys))%$, respectively. We have derived the fraction of directly produced $\\Upsilon(1S)$ mesons to be $(50.9\\pm8.2(stat)\\pm9.0(sys)) %$.']",['1999-10-14']
1140,['eng'],[],['Measurement of the Inclusive Charm Cross Section at 4.03 GeV and 4.14 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, inclusive reaction', 'charmed meson, electroproduction', 'D+, hadronic decay', 'D0, hadronic decay', 'channel cross section, branching ratio', 'radiative correction', 'cross section, hadronic', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> D anything', 'D0 --> K- pi+', 'D+ --> K- 2pi+', '4.03, 4.14 GeV-cms, ((2))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910016'],['The cross section for charmed meson production at $\\sqrt{s} = 4.03 $ and 4.14 GeV has been measured with the Beijing Spectrometer. The measurement was made using 22.3 $pb^{-1}$ of $e^+e^-$ data collected at 4.03 GeV and 1.5 $pb^{-1}$ of $e^+e^-$ data collected at 4.14 GeV. Inclusive observed cross sections for the production of charged and neutral D mesons and momentum spectra are presented. Observed cross sections were radiatively corrected to obtain tree level cross sections. Measurements of the total hadronic cross section are obtained from the charmed meson cross section and an extrapolation of results from below the charm threshold.'],['1999-10-11']
1141,['eng'],"['Kulchitskii, Yu A']",['Hadronic Shower Development in Tile Iron-Scintillator Calorimetry'],['Detectors and Experimental Techniques'],"['talk, Lisbon 1999/06/13', 'calorimeter, hadronic', 'iron', 'scintillation counter', 'showers, hadronic', 'showers, parametrization', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910015'],"['The lateral and longitudinal profiles of hadronic showers detected by a prototype of the ATLAS Iron-Scintillator Tile Hadron Calorimeter have been investigated. This calorimeter uses a unique longitudinal configuration of scintillator tiles. Using a fine-grained pion beam scan at 100 GeV, a detailed picture of transverse shower behavior is obtained. The underlying radial energy densities for four depth segments and for the entire calorimeter have been reconstructed. A three-dimensional hadronic shower parametrization has been developed. The results presented here are useful for understanding the performance of iron-scintillator calorimeters, for developing fast simulations of hadronic showers, for many calorimetry problems requiring the integration of a shower energy deposition in a volume and for future calorimeter design.']",['1999-10-08']
1142,['eng'],"['Hou, W S', 'Smith, J G', 'Würthwein, F']",['Determination of the Phase of Vub from Charmless Hadronic B Decay Rates'],['Particle Physics - Experimental Results'],"['B, hadronic decay', 'final state, (0charm)', 'Kobayashi-Maskawa angle', 'decay, form factor', 'mass, strangeness', 'numerical calculations, interpretation of experiments', 'B --> 2pseudoscalar meson']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910014', 'http://arXiv.org/abs/hep-ex/?9910014']","['We perform a model dependent fit to recent data on charmless hadronic B decays and determine $\\gamma$, the phase of $V^*_{ub}$. We find $\\gamma = 114^{+25}_{-21}$ degrees, which disfavors the often quoted $\\gamma \\sim 60^\\circ$ at the two standard deviation level. We also fit for the form factors $F_0^{B\\pi}$ and $A_0^{B\\rho}$, and the strange-quark mass. They are consistent with theoretical expectations, although $m_s$ is somewhat low. Such agreement and the good $\\chi^2$ for the fit may be interpreted as a confirmation of the adequacy of our model assumptions.']",['1999-10-08']
1143,['eng'],"['Geer, S', 'Marriner, J P', 'Martens, M', 'Ray, R E', 'Streets, J', 'Wester, W C', 'Hu, M', 'Snow, G A', 'Armstrong, T A', 'Buchanan, C D', 'Corbin, B', 'Lindgren, M', 'Müller, T', 'Gustafson, R']",['A new limit on CPT violation'],['Particle Physics - Experimental Results'],"['anti-p, decay modes', 'anti-p, lifetime', 'lower limit', 'violation, CPT', 'upper limit', 'baryon number, violation', 'experimental results', 'Fermilab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910013'],['A search for antiproton decay has been made at the Fermilab Antiproton Accumulator. Limits are placed on fifteen antiproton decay modes. The results are used to place limits on the characteristic mass scale Mx that could be associated with CPT-violation accompanied by baryon number violation.'],['1999-10-07']
1144,['eng'],"['Telnov, V I']","['Gamma-gamma, gamma-electron colliders']",['Detectors and Experimental Techniques'],"['talk, Sitges 1999/04/28', 'electron positron, linear collider', 'linear collider, proposed', 'photon photon, colliding beams', 'photon electron, colliding beams', 'beam cooling, laser', 'luminosity', 'beam, width']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910011'],"['In this report on Photon Colliders the following technical aspects are considered: special requirements to an accelerator, new ideas on laser optics, laser cooling, and interaction region layout issues. In fact it is continuation of my first talk at this workshop where physics motivation, possible luminosities and backgrounds were discussed.']",['1999-10-05']
1145,['eng'],"['Telnov, V I']","['Gamma-gamma, gamma-electron colliders']",['Detectors and Experimental Techniques'],"['talk, Sitges 1999/04/28', 'electron positron, linear collider', 'photon photon, colliding beams', 'photon electron, colliding beams', 'backscatter, laser', 'luminosity', 'new particle, search for', 'Higgs particle, decay modes', 'charged particle, pair production', 'supersymmetry', 'quantum gravity, effect', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910010'],"[""This report on Photon Colliders covers the following ``physics'' issues: physics motivation, possible luminosities, backgrounds, plans of works and international cooperation. More technical aspects such as accelerator issues, new ideas on laser optics, laser cooling, and interaction region layout are discussed in my second talk at this Workshop.""]",['1999-10-05']
1146,['eng'],[],['Production of $J\\psi$ Mesons in pBe Collisions at 530 and 800 GeV/c'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'beryllium', 'J/psi(3100), hadroproduction', 'J/psi(3100), leptonic decay', 'differential cross section, x-dependence', 'angular distribution', 'energy dependence', 'transverse momentum, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '530, 800 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910005'],"['We report on the production of J/psi mesons in 530 and 800 GeV/c proton - Be collisions in the Feynman-x range 0.0 < xf < 0.6. The J/psi mesons were detected via decays into opposite sign muon pairs. Differential distributions for J/psi production have been measured as functions of xf, pT^2, and cosine of the Gottfried-Jackson decay angle. These distributions are compared with results on J/psi production obtained in 515 GeV/c pion - Be collisions, measured by the same experiment, as well as with results from other experiments using incident protons.']",['1999-10-04']
1147,['eng'],"['Abe, F']","[""Search for a W' Boson via the Decay Mode $W' \\to \\mu_{\\nu}$ in 1.8 TeV $p\\overline{p}$ Collisions""]",['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', ""W', search for"", ""W', leptonic decay"", 'mass spectrum, (muon neutrino/mu)', 'mass, transverse', ""W', mass"", 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', ""anti-p p --> W' anything"", ""W' --> muon neutrino/mu"", '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910004'],"[""We report the results of a search for a W' boson produced in p-pbar collisions at a center-of-mass energy of 1.8 TeV using a 107 pb-1 data sample recorded by the Collider Detector at Fermilab. We consider the decay channel W' -> mu nu and search for anomalous production of high transverse mass mu-nu lepton pairs. We observe no excess of events above background and set limits on the rate of W' boson production and decay relative to Standard Model W boson production and decay using a fit of the transverse mass distribution observed. If we assume Standard Model strength couplings of the W' boson to quark and lepton pairs, we exclude a W' boson with invariant mass less than 660 GeV/c**2 at 95% confidence level.""]",['1999-10-04']
1148,['eng'],"['Wong, H T']",['Prospects of Scintillating Crystal Detector in Low-Energy Low-Background Experiments'],['Detectors and Experimental Techniques'],"['scintillation counter, crystal', 'cesium, iodine', 'radiation, yield', 'optics, absorption', 'neutrino, magnetic moment', 'astrophysics, missing-mass', 'WIMP', 'neutrino, solar', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910002'],['Scintillating crystal detector offers potential advantages in low-energy (keV-MeV range) low-background experiments for particle physics and astrophysics. The merits are discussed using CsI(Tl) crystal as illustrations. The various physics topics which can be pursued with this detector technology are summarized. A conceptual design for a generic detector is presented.'],['1999-10-04']
1149,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Baru, S E', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Koop, I A', 'Ivanov, P M', 'Korol, A A', 'Koshuba, S V', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V', 'Varganov, A V', 'Velikzhanin, Yu S']",['The process $e^{+}e^{-}\\to\\pi^{+}\\pi^{-}\\pi^{0}$ in the energy range $2E_{0}=1.04-1.38 GeV$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'pi, multiple production', 'mass spectrum, (pi+ pi- pi0)', 'meson resonance, electroproduction', 'meson resonance, mass', 'new particle, omega(1200)', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> pi+ pi- pi0', '1.04-1.38 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910001'],['In the experiment with the SND detector at VEPP-2M e^+e^- collider the process $e^+e^-\\to\\pi^+\\pi^-\\pi^0$ was studied in the energy range 2E_0 from 1.04 to 1.38 GeV. A broad peak was observed with the visible mass $M_{vis}=1220\\pm 20$ MeV and cross section in the maximum $\\sigma_0\\simeq 4$ nb. The peak can be interpreted as a $\\omega$-like resonance $\\omega (1200)$.'],['1999-10-04']
1150,['eng'],"['Schumm, B A']",['Tracking and Vertexing at a High Energy Linear Collider'],['Detectors and Experimental Techniques'],"['talk, Sitges 1999/04/28', 'electron positron, colliding beam detector', 'tracks', 'drift chamber, gas', 'semiconductor detector, pixel', 'semiconductor detector, microstrip', 'drift chamber, semiconductor detector', 'electron positron, linear collider', 'linear collider, proposed', 'semiconductor detector, vertex']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909054'],"['The relative merits and disadvantages of various alternatives for vertexing and central tracking detectors for the Linear Collider detector are presented. Research and development prospects for the various alternatives are also discussed, as well as a preliminary study of the prospects for forward (cos(theta) > 0.9) tracking.']",['1999-10-01']
1151,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for Anomalous Production of Acoplanar Di-lepton Events in $e^{+}e^{-}$ Collisions at $\\sqrt{s}$=183 and 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'event shape analysis, planarity', 'transverse momentum, missing-energy', 'W, pair production', 'W, leptonic decay', 'new particle, search for', 'slepton', 'chargino', 'Higgs particle, charged particle', 'channel cross section, branching ratio', 'upper limit', 'mass, lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '183, 189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909052'],"['A selection of di-lepton events with significant missing transverse momentum has been performed using a total data sample of 237.4 pb-1 at e+e- centre-of-mass energies of 183 GeV and 189 GeV. The observed numbers of events - 78 at 183 GeV and 301 at 189 GeV - are consistent with the numbers expected from Standard Model processes, which arise predominantly from W+W- production with each W decaying leptonically. This topology is also an experimental signature for the pair production of new particles that decay to a charged lepton accompanied by one or more invisible particles. Discrimination techniques are described that optimise the sensitivity to particular new physics channels. No evidence for new phenomena is apparent and model independent limits are presented on the production cross-section times branching ratio squared for sleptons and for leptonically decaying charginos and charged Higgs. Assuming a 100 % branching ratio for the decay of a slepton to a lepton and the lightest neutralino, we exclude at 95 % CL: right-handed smuons with masses below 82.3 GeV for a smuon-neutralino mass difference > 3 Gev and right-handed staus with masses below 81.0 GeV for a stau-neutralino mass difference > 8 GeV. Right-handed selectrons are excluded at 95% CL for masses below 87.1 GeV for a selectron-neutralino mass diffeerence > 5GeV, within the framework of the Minimal Supersymmetric Standard Model assuming mu < -100 GeV and tan{beta} = 1.5. Charged Higgs bosons are excluded at 95% CL for masses below 82.8GeV, assuming a 100% branching ratio for their decay to tau+neutrino.']",['1999-09-30']
1152,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for Chargino and Neutralino Production at $\\sqrt{s} = 189 GeV$ at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'chargino, decay modes', 'neutralino, decay modes', 'sparticle, pair production', 'sparticle, mass', 'lower limit', 'channel cross section, upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909051'],"['A search for charginos and neutralinos, predicted by supersymmetric theories, is performed using a data sample of 182.1 pb-1 taken at a centre-of-mass energy of 189 GeV with the OPAL detector at LEP. No evidence for chargino or neutralino production is found. Upper limits on chargino and neutralino pair production cross-sections are obtained as a function of the chargino mass, the lightest neutralino mass and the second lightest neutralino mass. Within the Constrained Minimal Supersymmetric Standard Model framework, and for a chargino - neutralino mass difference of more than 5 GeV, the 95% confidence level lower limits on the chargino mass are 93.6 GeV for tan{beta} = 1.5 and 94.1 GeV for tan{beta} = 35. These limits are obtained assuming a universal scalar mass m_0 > 500 GeV. The corresponding limits for all m_0 are 78.0 and 71.7 GeV. The 95% confidence level lower limits on the lightest neutralino mass, valid for any value of tan{beta} are 32.8 GeV for m_0 > 500 GeV and 31.6 GeV for all m_0.']",['1999-09-30']
1153,['eng'],"['Bergfeld, T']",['Observation of Radiative Leptonic Decay of the Tau Lepton'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, radiative decay', 'tau-, branching ratio', 'electroweak interaction, validity test', 'angular distribution, (lepton photon)', 'photon, energy spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> muon- neutrino/tau antineutrino/mu photon', 'tau- --> electron neutrino/tau antineutrino/e photon', '10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909050'],"['Using 4.68 fb^{-1} of e^+e^- annihilation data collected with the CLEO II detector we have studied tau radiative decays tau --> mu nu nu gamma and tau --> e nu nu gamma. For a 10 MeV minimum photon energy in the tau rest frame, the branching fraction of a tau radiatively decaying to a muon is measured to be (3.61+-0.16+-0.35)*10^{-3}, and to an electron is (1.75+-0.06+-0.17)*10^{-2}. The branching fractions are in agreement with the Standard Model theoretical predictions. All quoted results are preliminary.']",['1999-09-29']
1154,['eng'],"['Müller, D']",['Recent Tests of QCD at SLD'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1999/07/07', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'final state, (4jet)', 'quark, jet', 'gluon, jet', 'parton, fragmentation', 'angular distribution, asymmetry', 'quark, beauty', 'quark, pair production', 'mass, beauty', 'beautiful particle, energy spectrum', 'hadron, multiple production', 'rapidity, correlation', 'correlation, long-range', 'coupling constant, strong interaction', 'dependence, flavor', 'parity, violation', 'quantum chromodynamics, validity test', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> quark antiquark gluon', 'gluon --> 2beauty', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909049'],"['We present selected results on strong interaction physics from the SLD experiment at the SLAC Linear Collider. We report on several new studies of 3- and 4-jet hadronic Z decays, in which jets are identified as quark, antiquark or gluon. The 3-jet Z^0->b\\bar{b}g rate is sensitive to the b-quark mass; prospects for measuring m_b are discussed. The gluon energy spectrum is measured over the full kinematic range, providing an improved test of QCD and limits on anomalous bbg couplings. The parity violation in Z^0->b\\bar{b}g decays is consistent with electroweak theory plus QCD. New tests of T- and CP-conservation at the bbg vertex are performed. A new measurement of the rate of gluon splitting into b\\bar{b} pairs yields g_{b\\bar{b}}=0.0031+-0.0007(stat.)+-0.0006(syst.) (Preliminary). We also present a number of new results on jet fragmentation into identified hadrons. The B hadron energy spectrum is measured over the full kinematic range using a new, inclusive technique, allowing stringent tests of predictions for its shape and a precise measurement of <x_B>=0.714+-0.005(stat.)+-0.007(syst.) (Preliminary). A detailed study of correlations in rapidity y between pairs of identified pions, kaons and protons confirms that strangeness and baryon number are conserved locally, and shows local charge conservation between meson-baryon and strange-nonstrange pairs. Flavor-dependent long-range correlations are observed for all combinations of these hadron species, yielding new information on leading particle production. The first study of correlations using rapidities signed such that y>0 corresponds to the quark direction provides additional new insights into fragmentation, including the first direct observation of baryon number ordering along the q\\bar{q} axis.']",['1999-09-29']
1155,['eng'],"['Palestini, S']",['Measurement of direct CP violation with the experiment NA48 at CERN'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'K0, hadronic decay', 'K0(L), secondary beam', 'K0(S), secondary beam', 'track data analysis, vertex', 'violation, CP', 'magnetic spectrometer, experimental results', 'CERN SPS', 'K0 --> pi+ pi-', 'K0 --> 2pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909046'],"[""Direct CP violation is studied in two pion decays of the neutral kaon. Using data collected in the first beam period in 1997, the result for the parameter Re(epsilon'/epsilon) is (18.5+/-4.5(stat)+/-5.8(syst))x10^(-4).""]",['1999-09-28']
1156,['eng'],"['Cropp, R']","['Recent results on $J\\psi, \\psi(2S)$ and $\\Upsilon$ production at CDF']",['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quarkonium, hadroproduction', 'quarkonium, polarization', 'J/psi(3100), leptonic decay', 'psi(3685)', 'upsilon mesons', 'chi mesons, beauty', 'chi mesons, radiative decay', 'final state, dimuon', 'channel cross section, branching ratio', 'transverse momentum, dependence', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> quarkonium anything', 'quarkonium --> muon+ muon-', 'chi mesons --> Upsilon(9460) photon', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9910003'],"['CDF has obtained new results on quarkonium production in p\\bar{p} collisions at \\sqrt{s} = 1.8 TeV. We report on measurements of Upsilon meson production, Upsilon(1S) production from Chi_b feeddown, and the production polarization of Upsilon(1S), J/Psi and Psi(2S) mesons.']",['1999-10-04']
1157,['eng'],"['Affolder, T']",['Measurement of the Helicity of W Bosons in Top Quark Decays'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'W, leptonic decay', 'W, helicity', 'lepton, transverse momentum', 'transverse momentum, spectra', 'mass, truth', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909042'],"[""We use the transverse momentum spectrum of leptons in the decay chain t-->bW with W-->l nu to measure the helicity of the W bosons in the top quark rest frame. Our measurement uses a ttbar sample isolated in 106 +/- 4 inverse picobarns of data collected in ppbar collisions at sqrt(s)=1.8 TeV with the CDF detector at the Fermilab Tevatron. Assuming a standard V--A weak decay, we find that the fraction of W's with zero helicity in the top rest frame is F_0 = 0.91 +/- 0.37 (stat) +/- 0.13 (syst), consistent with the standard model prediction of F_0=0.70 for a top mass of 175 GeV/c**2.""]",['1999-09-24']
1158,['eng'],"['Adams, T', 'Alton, A', 'Bolton, T', 'Goldman, J', 'Goncharov, M', 'Naples, D', 'Johnson, R A', 'Vakili, M', 'Wu, V', 'Conrad, J', 'Formaggio, J A', 'Koutsoliotas, S', 'Kim, J H', 'McNulty, C', 'Romosan, A', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Tamminga, B', 'Vaitaitis, A G', 'Zimmerman, E D', 'Bernstein, R H', 'Bugel, L', 'Lamm, M J', 'Marsh, W', 'Nienaber, P', 'Yu, J', 'De Barbaro, L', 'Buchholz, D A', 'Schellman, H', 'Zeller, G P', 'Brau, J E', 'Drucker, R B', 'Frey, R', 'Mason, D', 'Avvakumov, S', 'De Barbaro, P', 'Bodek, Arie', 'Budd, H S', 'Harris, D A', 'McFarland, K S', 'Sakumoto, W K', 'Yang, U K']",['Evidence for Diffractive Charm Production in $\\nu_{\\mu}Fe$ and $\\overline \\nu_{\\mu}Fe$ Scattering at the Tevatron'],['Particle Physics - Experimental Results'],"['neutrino nucleus, interaction', 'antineutrino nucleus, interaction', 'iron', 'diffraction', 'charged current', 'D/s, neutrinoproduction', 'D/s*(2110), neutrinoproduction', 'charmed meson, semileptonic decay', 'mass spectrum, dimuon', 'neutral current', 'J/psi(3100), search for', 'production, upper limit', 'calorimeter, target', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'neutrino iron --> charmed meson anything', '((3))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909041'],['We present evidence for the diffractive processes nu_mu Fe -> mu^- D_s^+ (D_s^*+) Fe and nubar_mu Fe -> mu^+ D_s^- (D_s^*-) Fe using the Fermilab SSQT neutrino beam and the Lab E neutrino detector. We observe the neutrino trident reactions nu_mu Fe -> nu_mu mu^- mu^+ Fe and nubar_mu Fe -> nubar_mu mu^+ mu^- Fe at rates consistent with Standard Model expectations. We see no evidence for neutral-current production of J/psi via either diffractive or deep inelastic scattering mechanisms.'],['1999-09-24']
1159,['eng'],"['Bai, J Z']",['Partial Wave Analysis of $J/\\psi \\rightarrow \\gamma(\\pi^{+} \\pi^{-}\\pi^{+} \\pi^{-})$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'J/psi(3100), electroproduction', 'J/psi(3100), radiative decay', 'J/psi(3100), branching ratio', 'partial wave analysis', 'mass spectrum, (2pi+ 2pi-)', 'meson resonance, mass', 'meson resonance, width', 'meson resonance, hadronic decay', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> J/psi(3100)', 'J/psi(3100) --> 2pi+ 2pi- photon', '3.1 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909040'],"['BES data on $J/\\psi \\to \\gamma \\pi^{+} \\pi^{-} \\pi^{+} \\pi^{-}$ have been analyzed into partial waves. We fit with resonances having $J^{PC}=2^{++}$ at 1275 MeV, $0^{++}$ at 1500 MeV, $2^{++}$ at 1565 MeV, $0^{++}$ at 1740 MeV, $2^{++}$ at 1940 MeV and $0^{++}$ at 2104 MeV, plus a broad $0^-$. The $0^{++}$ resonances decay dominantly to $\\sigma\\sigma$, while $2^{++}$ resonances in the high mass region decay mainly to $f_2(1270)\\sigma$ and $\\sigma\\sigma$; $2^{++}$ resonances from the low mass region decay dominantly to $\\rho\\rho$.']",['1999-09-24']
1160,['eng'],"['Vossebeld, J H']",['The Partonic Structure of the Quasi-Real Photon'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'positron p, colliding beams', 'jet, photoproduction', 'final state, (2jet)', 'photon, structure function', 'gluon, momentum spectrum', 'channel cross section, transverse energy', 'rapidity dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909039'],['New measurements of dijet photoproduction at HERA provide information on the gluon density in the photon and on its quark densities at high x_gamma and high factorisation scales.'],['1999-09-24']
1161,['eng'],"['Bai, J Z']",['$\\Psi(2S)\\rightarrow \\pi^{+}\\pi^{-} J/\\psi$ Decay Distributions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), hadronic decay', 'J/psi(3100), leptonic decay', 'pi, angular distribution', 'mass spectrum, (pi+ pi-)', 'decay, amplitude analysis', 'partial wave analysis', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> psi(3685)', 'psi(3685) --> J/psi(3100) pi+ pi-', 'J/psi(3100) --> lepton+ lepton-', '3.685 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909038'],"['Using a sample of 3.8 M psi(2S) events accumulated with the BES detector, the process psi(2S) -> pi^+ pi^- J/psi is studied. The angular distributions are compared with the general decay amplitude analysis of Cahn. We find that the dipion system requires some D-wave, as well as S-wave. On the other hand, the J/psi-(pi pi) relative angular momentum is consistent with being pure S-wave. The decay distributions have been fit to heavy quarkonium models, including the Novikov-Shifman model. This model, which is written in terms of the parameter kappa, predicts that D-wave should be present. We determine kappa = 0.183 +/- 0.002 +/- 0.003 based on the joint dipion mass - cos theta distribution. The fraction of D-wave as a function of the dipion mass is found to decrease with increasing dipion mass, in agreement with the model. We have also fit the Mannel-Yan model, another model that allows D-wave.']",['1999-09-24']
1162,['eng'],"['Ghete, V M']",['Hadronic final state interactions at ALEPH and OPAL'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1999/07/07', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'W, pair production', 'intermediate boson, hadronic decay', 'correlation, (2Lambda)', 'correlation, (2Antilambda)', 'fermion, statistics', 'boson, statistics', 'color, recombination', 'magnetic detector, ALEPH', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '((4)) ((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909037'],['The studies of Fermi-Dirac correlations of $\\Lambda\\Lambda$ and Bose-Einstein correlations and colour reconnection in $\\mathrm{W}$-pairs decays performed by the ALEPH collaboration in $\\mathrm{e^+e^-}$ annihilation at LEP are presented. The OPAL analysis of Bose-Einstein correlations in'],['1999-09-23']
1163,['eng'],"['Eitel, K']",['Compatibility Analysis of the LSND Evidence and the KARMEN Exclusion for $\\overline {\\nu}_{\\mu}\\rightarrow \\overline{\\nu}_{e}$'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'antineutrino/mu', 'antineutrino/e', 'fission, particle source', 'statistical analysis', 'neutrino, mass difference', 'neutrino, mixing angle', 'experimental results', 'Rutherford ISIS PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909036'],"['A combined statistical analysis of the experimental results of the LSND and KARMEN numubar->nuebar oscillation search is presented. LSND has evidence for neutrino oscillations that is not confirmed by the KARMEN experiment. However, there is a region in the (sin^2(2theta),Dm^2) parameter space where the results of both experiments are statistically compatible. This joint analysis is based on likelihood functions for both data sets. A frequentist approach creating Monte Carlo samples analogous to the experimental outcome is applied to deduce correct confidence limits. Different schemes of combination can be chosen to provide correct coverage which lead to slightly different confidence regions in (sin^2(2theta),Dm^2).']",['1999-09-23']
1164,['eng'],"['Erhan, S', 'Schlein, Peter E']",['Inelastic diffraction data and the Pomeron trajectory'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'anti-p p, inelastic scattering', 'diffraction', 'exchange, pomeron', 'cross section, energy dependence', 'differential cross section, parametrization', 'Regge poles, multi-Regge', 'momentum transfer, dependence', 'numerical calculations, interpretation of experiments', '((4)) ((5)) ((6)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909035'],"['We demonstrate that all available inclusive p-p and pbar-p single diffraction data from ISR to Tevatron require an effective Pomeron trajectory whose intercept, alpha(0), changes with energy; it decreases from 1.10 at low energy to about 1.03 at the SPS and perhaps smaller at the Tevatron. This result, when combined with a relatively s-independent trajectory, alpha(t) ~ 0.92 - 0.95 in the range, 1.0 < |t| < 1.5 GeV^2, specifies a new effective Pomeron trajectory in inelastic diffraction.']",['1999-09-23']
1165,['eng'],[],['High Altitude test of RPCs for the ARGO-YBJ experiment'],['Detectors and Experimental Techniques'],"['photon, cosmic radiation', 'shower detector', 'ionization chamber', 'electrode, impedance', 'performance']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909034'],"['A 50 m**2 RPC carpet was operated at the YangBaJing Cosmic Ray Laboratory (Tibet) located 4300 m a.s.l. The performance of RPCs in detecting Extensive Air Showers was studied. Efficiency and time resolution measurements at the pressure and temperature conditions typical of high mountain laboratories, are reported.']",['1999-09-22']
1166,['eng'],"['Lefebvre, M', 'Keeler, Richard K', 'Sobie, Randall J', 'White, J']",['Propagation of Errors for Matrix Inversion'],['Detectors and Experimental Techniques'],"['statistical analysis, error', 'formula', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909031'],['A formula is given for the propagation of errors during matrix inversion. An explicit calculation for a 2 by 2 matrix using both the formula and a Monte Carlo calculation are compared. A prescription is given to determine when a matrix with uncertain elements is sufficiently nonsingular for the calculation of the covariances of the inverted matrix elements to be reliable.'],['1999-09-20']
1167,['eng'],"['Abbott, B']",['A Measurement of the W Boson Mass Using Electrons at Large Rapidities'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'W, mass', 'mass spectrum, transverse', 'transverse momentum, spectra', 'four-pi-detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'W --> electron neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909030'],"['We report a measurement of the W boson mass based on an integrated luminosity of 82/pb from p-pbar collisions at sqrt(s) = 1.8 TeV recorded in 1994-1995 by the D0 detector at the Fermilab Tevatron. We identify W bosons by their decays to e-nu, where the electron is detected in the forward calorimeters. We extract the mass by fitting the transverse mass and the electron and neutrino transverse momentum spectra of 11,089 W boson candidates. We measure Mw = 80.691 +- 0.227 GeV. By combining this measurement with our previously published central calorimeter results from data taken in 1992-1993 and 1994-1995, we obtain Mw = 80.482 +- 0.091 GeV.']",['1999-09-16']
1168,['eng'],"['Adloff, C']",['Measurement of Open Beauty Production at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'quark, photoproduction', 'beautiful particle, semileptonic decay', 'muon, momentum spectrum', 'transverse momentum, spectra', 'channel cross section, energy dependence', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909029', 'http://arXiv.org/abs/hep-ex/?9909029']","[""The first observation of open b production in ep collisions is reported. An event sample containing muons and jets has been selected which is enriched in semileptonic b quark decays. The visible cross section \\sigma(ep -> b \\bar{b}X -> \\mu X') for Q^2 < 1 GeV^2, 0.1 < y < 0.8 is measured to be 0.176+-0.016(stat.)+0.026-0.017(syst.) nb for the muons to be detected in the range 35 deg < \\theta^\\mu < 130 deg and \\pt^\\mu > 2.0 GeV in the laboratory frame. The expected visible cross section based on a NLO QCD calculation is 0.104+-0.017 nb. The cross sections for electroproduction with Q^2<1 GeV^2 and photoproduction are derived from the data and found to be \\sigma(ep-> e X) = 111+-10(stat.)+23-20(syst.) at an average <W_{\\gamma p}> \\sim 180 GeV, respectively.""]",['1999-09-16']
1169,['eng'],"['Abe, T']",['Current Performance of the SLD VXD3'],['Detectors and Experimental Techniques'],"['talk, Texel 1999/06/20', 'semiconductor detector, vertex', 'spatial resolution', 'alignment', 'track data analysis', 'magnetic detector, SLD', 'SLAC SLC Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909048'],"['During 1996, the SLD collaboration completed construction and began operation of a new charge-coupled device (CCD) vertex detector (VXD3). Since then, its performance has been studied in detail and a new topological vertexing technique has been developed. In this paper, we discuss the design of VXD3, procedures for aligning it, and the tracking and vertexing improvements that have led to its world-record performance.']",['1999-09-29']
1170,['eng'],"['Nelson, H N']",['Search for $D^{0}-\\overline{D}^{0}$ Mixing'],['Particle Physics - Experimental Results'],"['talk, Chicago 1999/06/21', 'electron positron, colliding beams', 'electron positron, annihilation', 'D0 anti-D0, interference', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'particle identification, flavor', 'pi, charge', 'decay, time', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> D*(2010) anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K+ pi-', 'approx. 10 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909028'],"[""We report on a search for D0-D0bar mixing made by a study of the `wrong-sign' process D0 -> K+pi-. The data come from an integrated luminosity of e+e- collisions at sqrt{s} of about 10 GeV consisting of 9.0 1/fb recorded with the CLEO-II.V detector. We measure the time-integrated rate of the `wrong-sign' process D0 -> K+pi-, relative to that of the Cabibbo-favored process D0bar -> K+pi-, to be R_ws=(0.34+-0.07+-0.06)%. We study that rate as a function of the decay time of the D0, to distinguish the rate of direct doubly-Cabibbo-suppressed decay from D0-D0bar mixing. The amplitudes that describe D0-D0bar mixing, x' and y', are consistent with zero. The one-dimensional limits, at the 95% C.L., that we determine are (1/2)x'^2<0.05%, and -5.9% < y' < 0.3%. All results are preliminary.""]",['1999-09-15']
1171,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azfar, F', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bevensee, B E', 'Bhatti, A A', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Ciobanu, C I', 'Clark, A G', 'Cobal, M', 'Cocca, E', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Costanzo, D', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Gadomski, S', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Grassmann, H', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incagli, M', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kirk, M', 'Kim, B J', 'Kim, H S', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Knoblauch, D', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loken, J G', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lyons, L', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Meschi, E', 'Mesropian, C', 'Miao, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Parri, A', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Perazzo, A', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Reher, D', 'Reichold, A', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takashima, R', 'Takikawa, K', 'Tanaka, M', 'Takano, T', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R M', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Truitt, S', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Waters, D', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Search for a Fourth-Generation Quark more Massive than the $Z^{0}$ Boson in $p\\overline{p}$ Collisions at $\\Sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'quark, pair production', 'family, 4', 'quark, decay', 'neutral current, flavor changing', 'quark, beauty', 'Z0, decay modes', 'channel cross section, branching ratio', 'upper limit', 'mass, dependence', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> quark antiquark', 'quark --> Z0 beauty', 'Z0 --> lepton+ lepton-', 'Z0 --> (n)hadron', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909027'],"[""We present the results of a search for pair production of a fourth-generation charge -1/3 quark (b') in sqrt(s)=1.8 TeV ppbar collisions using 88 pb^(-1) of data obtained with the Collider Detector at Fermilab. We assume that both quarks decay via the flavor-changing neutral current process b' -> bZ and that the b' mass is greater than m_Z + m_b. We studied the decay mode b'b'bar -> ZZ b bbar where one Z0 decays into e^+e^- or mu^+ mu^- and the other decays hadronically, giving a signature of two leptons plus jets. An upper limit on the cross section of ppbar -> b'b'bar times [BR (b' -> bZ)]^2 is established as a function of the b' mass. We exclude at 95% confidence level a b' quark with mass between 100 and 199 GeV/c^2 for BR(b' -> bZ) = 100%.""]",['1999-09-15']
1172,['eng'],"['Chekanov, S V', 'Zawiejski, L']",['Short-Range and Long-Range Correlations in DIS at HERA'],['Particle Physics - Experimental Results'],"['talk, Providence 1999/08/09', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'quantum chromodynamics, perturbation theory', 'quark, fragmentation', 'universality, validity test', 'quantum chromodynamics, validity test', 'angular correlation, two-particle', 'kinematics, Breit frame', 'correlation, short-range', 'correlation, long-range', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909026'],['Correlations in deep-inelastic scattering at HERA are investigated in order to test perturbative QCD and quark fragmentation universality. Two-particle correlations at small angular separations are measured in the Breit frame and compared to e+e- collisions. Also presented are the correlations between the current and target regions of the Breit frame.'],['1999-09-15']
1173,['eng'],"['Palestini, S']",['Space charge in ionization detectors and the NA48 calorimeter'],['Detectors and Experimental Techniques'],"['talk, Lisbon 1999/06/13', 'calorimeter, liquid', 'krypton, liquid', 'effect, space charge', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909025'],"['The effects of space charge due to slowly drifting ions can be relevant for detectors operated at high intensity, or for relatively low values of the bias voltage. Accurate measurements have been obtained with the liquid krypton calorimeter of the NA48 experiment, from data collected in 1997. The build-up of space charge takes place during the first part of the beam extraction burst, and causes a dependence of the response on the transverse coordinate of the axis of electromagnetic showers, and a small reduction of average amplitude. The effects are well reproduced by a computation, where the only free parameter is the value of the ion mobility. The model can be applied a wide range of operating conditions, and generalized to detectors with different geometry and active medium.']",['1999-09-15']
1174,['eng'],"['Gary, J W']",['Tests of QCD using differences between gluon and quark jets'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, multiple production', 'quark, jet', 'gluon, jet', 'quantum chromodynamics, validity test', 'color', 'jet, multiplicity', 'jet, fragmentation function', 'parametrization', 'charged particle, multiplicity', 'eta, multiplicity', 'transverse momentum, spectra', 'experimental results', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909024'],"['I present recent results from LEP which utilize differences between gluon and quark jets to make quantitative tests of QCD. The principal topic is a determination of the ratio of QCD color factors, C$_{\\mathrm{A}}$/C$_{\\mathrm{F}}$, using either the multiplicity or fragmentation functions of the jets. In addition, I discuss a recent measurement of the rate of $\\eta$ mesons in gluon jets compared to quark jets.']",['1999-09-15']
1175,['eng'],"['Berns, H G', 'Wilkes, R J']",['GPS Time Synchronization System for K2K'],['Detectors and Experimental Techniques'],"['neutrino, oscillation', 'neutrino, counters and detectors', 'control system, time', 'communications, satellite', 'deep underground detector, KAMIOKANDE', 'KEK Lab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909021'],"['The K2K (KEK E362) long-baseline neutrino oscillations experiment requires synchronization of clocks with ~100 nsec accuracy at the near and far detector sites (KEK and Super-Kamiokande, respectively), which are separated by 250 km. The Global Positioning System (GPS) provides a means for satisfying this requirement at very low cost. In addition to low-resolution time data (day of year, hour, minute, second), commercial GPS receivers output a 1 pulse per sec (1PPS) signal whose leading edge is synchronized with GPS seconds rollovers to well within the required accuracy. For each beam spill trigger at KEK, and each event trigger at Super-Kamiokande, 50 MHz free-running Local Time Clock (LTC) modules at each site provide fractional-second data with 20 nsec ticks. At each site, two GPS clocks run in parallel, providing hardware backup as well as data quality checks.']",['1999-09-14']
1176,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V V', 'Acharya, B S', 'Adam, I', 'Adams, D L', 'Adams, M', 'Ahn, S', 'Akimov, V E', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B Yu', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Belyaev, A', 'Beri, S B', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S K', 'Bloom, P', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F O', 'Boswell, C', 'Brandt, A', 'Breedon, R E', 'Briskin, G M', 'Brock, R L', 'Bross, A D', 'Buchholz, D A', 'Burtovoi, V S', 'Butler, J M', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Chen, W', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cobau, W G', 'Cochran, J', 'Coney, L', 'Cooper, W E', 'Coppage, D', 'Cretsinger, C E', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fatyga, M K', 'Fehér, S', 'Fein, D K', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Forden, G E', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Geld, T L', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Ginther, G', 'Gobbi, B', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, D R', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Guida, J A', 'Guida, J M', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Hernández-Montoya, R', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hsieh, F', 'Hu Tong', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Jun, S Y', 'Kahn, S', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Koltick, D S', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Landry, F J', 'Landsberg, G L', 'Leflat, A', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lu, J G', 'Lucotte, A', 'Lueking, L H', 'Maciel, A K A', 'Madaras, R J', 'Madden, R', 'Magana-Mendoza, L', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Markeloff, R', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McKibben, T', 'McKinley, J', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mostafa, M A', 'Da Motta, H', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Narayanan, A', 'Neal, H A', 'Negret, J P', 'Némethy, P', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Oshima, N', 'Owen, D', 'Padley, P', 'Para, A', 'Parashar, N', 'Park, Y M', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pishchalnikov, Yu', 'Pope, B G', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramírez, O', 'Reay, N W', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Sánchez-Hernández, A', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Scully, J R', 'Shabalina, E', 'Shaffer, C', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Song, X F', 'Sosebee, M', 'Sotnikova, N', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Sznajder, A', 'Tamburello, P D', 'Tarazi, J', 'Tartaglia, M', 'Thomas, T L T', 'Thompson, J', 'Toback, D', 'Trippe, T G', 'Tuts, P M', 'Vaniev, V', 'Varelas, N', 'Varnes, E W', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yepes, P', 'Yip, K', 'Yoshikawa, C', 'Youssef, S', 'Yu, J', 'Yu, Y', 'Zanabria, M E', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Differential Production Cross-Section of $Z$ Bosons as a Function of Transverse Momentum at $\\Sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Z0, hadroproduction', 'differential cross section', 'transverse momentum, spectra', 'quantum chromodynamics, perturbation theory', 'effect, nonperturbative', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909020'],"['We present a measurement of the transverse momentum distribution of Z bosons produced in ppbar collisions at sqrt{s}=1.8 TeV using data collected by the D0 experiment at the Fermilab Tevatron Collider during 1994--1996. We find good agreement between our data and a current resummation calculation. We also use our data to extract values of the non-perturbative parameters for a particular version of the resummation formalism, obtaining significantly more precise values than previous determinations.']",['1999-09-14']
1177,['eng'],"['Sadygov, Z Ya', 'Suleimanov, M K', 'Bokova, T Yu']",['Supersensitive avalanche silicon drift photodetector'],['Detectors and Experimental Techniques'],"['semiconductor, optical', 'silicon, metal', 'photoelectron, avalanche', 'semiconductor detector, drift chamber', 'photoelectron, yield']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909017'],['Physical principles of performance and main characteristics of a novel avalanche photodetector developed on the basis of MOS(metal-oxide-silicon) technology is presented. The photodetector contains a semitransparent gate electrode and a drain contact to provide a drift of multiplicated charge carriers along the semiconductor surface. A high gain(more than 10^4) of photocurrent was achived due to the local negative feedback effect realizied on the Si-SiO_2 boundary. Special attention is paid to the possibilities of development of a supersensitive avalanche CCD (charge coupled device) for detection of individual photons in visible and ultraviolet spectral regions. Experimental results obtained with a two-element CCD prototype are discussed.'],['1999-09-13']
1178,['eng'],"['Barbaro-Galtieri, A']",['Single Top Production and Top Properties at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1999/02/28', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, hadroproduction', 'quark, pair production', 'quark, decay modes', 'quark, branching ratio', 'Kobayashi-Maskawa angle', 'helicity, amplitude analysis', 'spin, correlation', 'search for, rare decay', 'new particle, search for', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'truth --> W beauty', 'truth --> W quark', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909016'],"[""We summarize recent measurements made at the Tevatron Collider using top event candidates. Cross section and mass measurements are discussed in a separate contribution to these Proceedings. Here we report on studies of the top P$_T$ distribution in $\\ttbar$ production and studies of single top production. Properties of top decays examined are: BF($t \\into Wb$)/BF($t \\into Wq$), helicity amplitudes of W's from top decays and correlations of $\\ttbar$ decay products. Searches for new physics in rare top decays and a search for a state X $\\into \\ttbar$ are also reported.""]",['1999-09-13']
1179,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Baru, S E', 'Beloborodov, K I', 'Berdyugin, A V', 'Bogdanchikov, A G', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Drozdetsky, A A', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Koshuba, S V', 'Kukartsev, G A', 'Pakhtusova, E V', 'Popov, V M', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Sidorov, V A', 'Silagadze, Z K', 'Usov, Yu V', 'Velikzhanin, Yu S', 'Zakharov, A C']",['Spherical Neutral Detector for VEPP-2M collider'],['Detectors and Experimental Techniques'],"['calorimeter, energy resolution', 'angular resolution', 'scintillation counter, crystal', 'sodium-iodide', 'drift chamber', 'muon, counters and detectors', 'streamer chamber, drift tube', 'scintillation counter, plastics', 'performance', 'data acquisition', 'four-pi-detector, SND', 'Novosibirsk Stor2', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909015'],"['The Spherical Neutral Detector (SND) operates at VEPP-2M collider in Novosibirsk studying e^+e^- annihilation in the energy range up to 1.4 GeV. Detector consists of a fine granulated spherical scintillation calorimeter with 1632 NaI(Tl) crystals, two cylindrical drift chambers with 10 layers of sense wires, and a muon system made of streamer tubes and plastic scintillation counters. The detector design, performance, data acquisition and processing are described.']",['1999-09-13']
1180,['eng'],"['Barberis, D', 'Binon, Freddy G', 'Close, Francis Edwin', 'Danielsen, K M', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinson, J B', 'Kirk, A', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Minashvili, I A', 'Peigneux, J P', 'Romanovsky, V I', 'Rusakovitch, N', 'Semenov, A A', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Stassinaki, M', 'Stroot, J P', 'Takamatsu, K', 'Tsuru, T', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['Experimental evidence for a vector-like behaviour of Pomeron exchange'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'pomeron, exchange', 'exchange, (2pomeron)', 'current, vector', 'meson, hadroproduction', 'angular distribution, (2p)', 'Delta(1232)', 'mass spectrum, (p pi+)', 'magnetic spectrometer, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p meson', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909013'],"['Evidence is presented that the Pomeron act as a non-conserved vector current. A study has been made of the azimuthal angle phi, which is defined as the angle between the pT vectors of the two outgoing protons, in the reaction pp -> pp(X0) for those resonances (X0) which are compatible with being produced by double Pomeron exchange. These distributions have been compared with a model which describes the Pomeron as a non-conserved vector current and a qualitative agreement is found. In addition, when one of the particles exchanged is known to have spin 0, namely pi-Pomeron exchange, the phi distribution is flat.']",['1999-09-09']
1181,['eng'],"['Giorgini, M']",['Search for magnetic monopoles with nuclear track detectors'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1999/05/17', 'magnetic monopole, search for', 'flux, upper limit', 'plastics, track sensitive', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909012'],"['This paper describes an experimental search for GUT magnetic monopoles in the MACRO experiment using the nuclear track subdetector CR39. After discussing the working principle, the charge resolution and the calibration of the detector, the experimental procedure for searching for magnetic monopoles is described. Since no candidates were found, the upper flux limits obtained by the MACRO CR39 used as a ""stand alone detector"" for magnetic monopoles of different magnetic charges are presented.']",['1999-09-08']
1182,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bevensee, B E', 'Bhatti, A A', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Ciobanu, C I', 'Clark, A G', 'Cobal, M', 'Cocca, E', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Guimarães da Costa, J', 'Costanzo, D', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Gadomski, S', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Grassmann, H', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incagli, M', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kirk, M', 'Kim, B J', 'Kim, H S', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Knoblauch, D', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Meschi, E', 'Mesropian, C', 'Miao, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Parri, A', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Perazzo, A', 'Pescara, L', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Reher, D', 'Riegler, W', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takashima, R', 'Takikawa, K', 'Tanaka, M', 'Takano, T', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R M', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Truitt, S', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Measurement of b Quark Fragmentation Fractions in $p\\overline{p}$ Collisions at $\\sqrt{s}$=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, pair production', 'quark, beauty', 'quark, fragmentation', 'dependence, flavor', 'beautiful particle, hadroproduction', 'B+', 'B0', 'B/s0', 'Lambda/b0', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909011'],"['We have studied the production of B hadrons in 1.8-TeV p-pbar collisions. We present measurements of the fragmentation fractions, f_u, f_d, f_s and f_baryon, of produced b quarks that yield B^+, B^0, B^0_s and Lambda_b hadrons. Reconstruction of several electron-charm final states yields f_s/(f_u+f_d)=0.213+/-0.068 and f_baryon/(f_u+f_d)=0.118+/-0.042, assuming f_u=f_d. If all B hadrons produced in p-pbar collisions cascade to one of these four hadrons, we determine f_u=f_d=0.375+/-0.023, f_s=0.160+/-0.044 and f_baryon=0.090+/-0.029. If we do not assume f_u=f_d, we find f_d/f_u=0.84+/-0.16.']",['1999-09-07']
1183,['eng'],"['Affolder, T', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amaral, P', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bailey, M W', 'Bailey, S', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Bedeschi, F', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bevensee, B E', 'Bhatti, A A', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blumenfeld, B', 'Blusk, S R', 'Bocci, A', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Brandl, A', 'van den Brink, S C', 'Bromberg, C', 'Bruner, N L', 'Buckley-Geer, E', 'Budagov, Yu A', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlson, J', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chang, P S', 'Chang, P T', 'Chapman, J', 'Chen, C', 'Chen, Y C', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chirikov-Zorin, I E', 'Chlachidze, G A', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Ciobanu, C I', 'Clark, A G', 'Cobal, M', 'Cocca, E', 'Connolly, A', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Guimarães da Costa, J', 'Costanzo, D', 'Cranshaw, J', 'Cronin-Hennessy, D', 'Cropp, R', 'Culbertson, R J', 'Dagenhart, D', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Fukui, Y', 'Gadomski, S', 'Galeotti, S', 'Gallinaro, M', 'Gao, T', 'García-Sciveres, M', 'Garfinkel, A F', 'Gatti, P', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giromini, P', 'Glagolev, V V', 'Gold, M', 'Goldstein, J', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Grassmann, H', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Günther, M', 'Guillian, G', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hall, C', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hatakeyama, K', 'Hauser, J', 'Heinrich, J', 'Heiss, A', 'Hinrichsen, B', 'Hoffman, K D', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incagli, M', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Jones, M', 'Joshi, U', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kelly, M', 'Kennedy, R D', 'Kephart, R D', 'Khazins, D M', 'Kikuchi, T', 'Kirk, M', 'Kim, B J', 'Kim, H S', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Knoblauch, D', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korytov, A V', 'Kovacs, E', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lai, N', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Latino, G', 'LeCompte, T J', 'Lee, A M', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Long, O', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lys, J', 'Madrak, R', 'Maeshima, K', 'Maksimovic, P', 'Malferrari, L', 'Mangano, Michelangelo L', 'Mariotti, M', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mazzanti, P', 'McFarland, K S', 'McIntyre, P', 'Mckigney, E A', 'Menguzzato, M', 'Menzione, A', 'Meschi, E', 'Mesropian, C', 'Miao, C', 'Miao, T', 'Miller, R', 'Miller, J S', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Moggi, N', 'Moore, E', 'Moore, R', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Munar, A', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nachtman, J', 'Nahn, S', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, P', 'Nicolaidi, P', 'Niu, H', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Palmonari, F', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Parri, A', 'Partos, D S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Perazzo, A', 'Pescara, L', 'Peters, M D', 'Phillips, T J', 'Piacentino, G', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Pope, G', 'Prokoshin, F', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Reher, D', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Rossin, R', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Savard, P', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schmitt, M', 'Scodellaro, L', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semenov, A A', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Signorelli, G', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Slaughter, A J', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Solodsky, A', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, T', 'Takashima, R', 'Takikawa, K', 'Tanaka, M', 'Takano, T', 'Tannenbaum, B', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thurman-Keup, R M', 'Tipton, P', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Truitt, S', 'Tseng, J', 'Turini, N', 'Ukegawa, F', 'Valls, J', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Volobuev, I', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Watanabe, T', 'Watts, T', 'Webb, R', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolbers, S', 'Wolinski, D', 'Wolinski, J', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Yu, S', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['A Measurement of $sin 2\\beta$ from $B \\to J/\\psi K^{0}_{S}$ with the CDF detector'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B+, hadronic decay', 'B0, hadronic decay', 'J/psi(3100)', 'K*(892)', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'particle identification, flavor', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> B0 anything', 'B0 --> J/psi(3100) K0(S)', 'B+ --> J/psi(3100) K+', 'B0 --> J/psi(3100) K*(892)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909003'],"['This paper reports an updated measurement of the Standard Model CP violation parameter $\\sin2\\beta$ using the CDF Detector at Fermilab. The entire Run I data sample of 110 pb$^{-1}$ of proton antiproton collisions at $\\sqrt{s}=1.8 TeV$ is used to identify a signal sample of $\\sim 400$ $B \\to J/\\psi K^0_S$ events, where $J/\\psi \\to \\mu^+\\mu^-$ and $K_S^0 \\to \\pi^+\\pi^-$. The flavor of the neutral B meson is identified at the time of production by combining information from three tagging algorithms: a same-side tag, a jet-charge tag, and a soft-lepton tag. A maximum likelihood fitting method is used to determine is consistent with the Standard Model prediction, based upon existing measurements, of a large positive CP violating asymmetry in this decay mode.']",['1999-09-06']
1184,['eng'],"['Oreglia, M']",['Searches for Other Higgs Bosons at LEP'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, pair production', 'Higgs particle, multiplet', 'doublet, 2', 'Higgs particle, decay modes', 'photon, pair production', 'sparticle, pair production', 'channel cross section, branching ratio', 'upper limit', 'experimental results', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909002'],"['Recent LEP searches for Higgs bosons in models other than the Minimal Standard Model and the Minimal Supersymetric Standard Model are reviewed. Limits are presented for Higgs bosons decaying into diphotons or invisible particles, and for charged Higgs bosons.']",['1999-09-03']
1185,['eng'],"['Wadhwa, M']",['Two Photon Physics at LEP'],['Particle Physics - Experimental Results'],"['talk, Ann Arbor 1999/06/24', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'hadron, multiple production', 'meson resonance, photoproduction', 'quarkonium, charm', 'photon, structure function', 'glueball, search for', 'cross section, energy dependence', 'jet, photoproduction', 'quark, heavy', 'photon, resolved', 'photon, off-shell', 'quantum electrodynamics, structure function', 'experimental results', 'CERN LEP Stor', 'bibliography', '91, 183, 189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9909001'],"[""LEP offers an excellent opportunity to measure two photon processes over a large kinematical range and thus study the complex nature of the photon. This article reviews the experimental status of ``Two Photon Physics'' at LEP. The recent results on resonances, multi-hadron production and photon structure functions are discussed""]",['1999-09-02']
1186,['eng'],"['Glasman, C']",['QCD Tests at HERA'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'mass spectrum, (2jet)', 'mass spectrum, (3jet)', 'quantum chromodynamics, validity test', 'photon, structure function', 'momentum spectrum, parton', 'jet, multiplicity', 'quark, jet', 'gluon, jet', 'differential cross section', 'angular distribution', 'transverse energy, dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908067'],"['Measurements of inclusive jet, dijet and three-jet cross sections in photon-proton interactions are presented. These measurements provide new tests of QCD, constrain the parton densities of the photon, and allow searches for new physics. Measurements of the mean subjet multiplicity are reported and used to test the differences between quark and gluon jets.']",['1999-09-01']
1187,['eng'],"['Spurio, M']",['Atmospheric Neutrino Physics with the MACRO detector'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1999/05/17', 'neutrino/mu, cosmic radiation', 'cosmic radiation, flux', 'cosmic radiation, angular distribution', 'neutrino nucleon, interaction', 'charged current', 'muon, angular distribution', 'muon, absorption', 'neutrino, oscillation', 'neutrino/tau', 'neutrino, mass difference', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908066'],"['We present the measurement of the the flux and angular distribution of atmospheric muon neutrinos using the MACRO detector. Three different event topologies are detected in two different energy ranges. High energy neutrinos (E~80 GeV) via the identification of upward throughgoing muons. Lower energy neutrinos (E~ 4 GeV) via the upgoing stopping and partially contained downgoing muons (ID+UGS), or via the partially contained upgoing muons (IU). The measured flux is reduced with respect to the predictions. For the high energy sample, globally the flux reduction is $0.74\\pm 0.054_{stat+sys} \\pm 0.12_{th}$ and varies with the zenith angle. The ratio of measured to expected events is almost constant with the zenith angle for the low energy events, and is $0.57 0.09_{stat+sys} \\pm 0.17_{theor}$ for the (ID+UGS). All the data sets are consistent within a scenario of neutrino oscillations, with maximum mixing and']",['1999-09-01']
1188,['eng'],"['García-Abia, P', 'Lohmann, W']",['Measurement of the Higgs Cross Section and Mass with Linear Colliders'],['Detectors and Experimental Techniques'],"['talk, Sitges 1999/04/28', 'electron positron, annihilation', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, mass', 'channel cross section', 'background', 'Z0, leptonic decay', 'recoil, mass', 'resolution', 'numerical calculations', 'proposed experiment, linear collider', '350 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908065'],"['We report on the accuracy of the measurement of the Higgs boson mass and the total cross section of the process e+e- -> ZH that would be achieved in a linear collider operating at a centre-of-mass energy of 350 GeV, assuming an integrated luminosity of 500 (1/fb). For that we have exploited the recoil mass off the Z using its leptonic decays into electron and muon pairs. The Higgs mass is determined with 150 MeV accuracy, the recoil mass resolution is about 1.5 GeV and the cross section is obtained with a statistical error of 3%.']",['1999-08-31']
1189,['eng'],"['Tamminga, B H', 'Adams, T', 'Alton, A', 'Arroyo, C G', 'Avvakumov, S', 'Barbaro, L', 'Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Formaggio, J A', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Koutsoliotas, S', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McFarland, K S', 'McNulty, C', 'Mishra, S R', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Sciulli, F J', 'Seligman, W G', 'Shaevitz, M H', 'Smith, W H', 'Spentzouris, P', 'Stern, E G', 'Vakili, M', 'Vaitaitis, A G', 'Yang, U K', 'Zeller, G P', 'Zimmerman, E D']",['Low $Q^{2}$ low $\\times$ structure function analysis of CCFR data for $F_{2}$'],['Particle Physics - Experimental Results'],"['talk, Uppsala 1999/06/10', 'neutrino nucleus, deep inelastic scattering', 'deuteron', 'iron', 'muon nucleus, deep inelastic scattering', 'nucleon, structure function', 'small-x', 'momentum transfer, low', 'experimental results', 'Batavia TEVATRON PS', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908064'],['Analyses of structure functions (SFs) from neutrino and muon deep inelastic scattering data have shown discrepancies in F2 for x < 0.1. A new SF analysis of the CCFR collaboration data examining regions in x down to x=.0015 and 0.4 < Q^2 < 1.0 is presented. Comparison to corrected charged lepton scattering results for F2 from the NMC and E665 experiments are made. Differences between muon and neutrino scattering allow that the behavior of F2 from muon scattering could be different from F2 from neutrino scattering as Q^2 approaches zero. Comparisons between F2 muon and F2 neutrino are made in this limit.'],['1999-08-31']
1190,['eng'],"['Kroll, I J']",['CP Violation in B Decays at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Chicago 1999/06/21', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0, hadronic decay', 'anti-B0, hadronic decay', 'violation, CP', 'J/psi(3100), leptonic decay', 'Kobayashi-Maskawa angle, unitarity', 'B/s0 anti-B/s0, oscillation', 'B, rare decay', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'proposed experiment', 'Batavia TEVATRON Coll', 'B0 --> J/psi(3100) K0(S)', 'J/psi(3100) --> muon+ muon-', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908062'],"[""Between 1992 to 1996, the CDF and D0 detectors each collected data samples exceeding 100 pb^{-1} of p\\bar{p} collisions at sqrt{s}=1.8 TeV at the Fermilab Tevatron. These data sets led to a large number of precision measurements of the properties of B hadrons including lifetimes, masses, neutral B meson flavor oscillations, and relative branching fractions, and to the discovery of the B_c meson. Perhaps the most exciting result was the first look at the CP violation parameter sin(2beta) using the world's largest sample of fully reconstructed B^0/bar{B}^0 -> J/psi K^0_S decays. A summary of this result is presented here. In the year 2000, the Tevatron will recommence p\\bar{p} collisions with an over order of magnitude expected increase in integrated luminosity (1 fb^{-1} per year). The CDF and D0 detectors will have undergone substantial upgrades, particularly in the tracking detectors and the triggers. With these enhancements, the Tevatron B physics program will include precision measurements of sin(2beta) and B^0_s flavor oscillations, as well as studies of rare B decays that are sensitive to new physics. The studies of B^0_s mesons will be particularly interesting as this physics will be unique to the Tevatron during the first half of the next decade.""]",['1999-08-26']
1191,['eng'],[],['Results from the ARGO-YBJ Test Experiment'],['Detectors and Experimental Techniques'],"['talk, San Miniato 1999/05/17', 'cosmic radiation', 'showers, air', 'angular distribution', 'density, spectra', 'shower detector', 'streamer chamber', 'electrode, impedance', 'efficiency', 'angular resolution']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908060'],"['An RPC carpet covering ~10**4 m**2 (ARGO-YBJ experiment) will be installed in the YangBaJing Laboratory (Tibet, P.R. China) at an altitude of 4300 m a.s.l.. A test-module of ~50 m**2 has been put in operation in this laboratory and about 10**6 air shower events have been collected. The carpet capability of reconstructing the shower features is presented.']",['1999-08-26']
1192,['eng'],"['Adloff, C']",['Measurement of Neutral and Charged Current Cross-Sections in Positron-Proton Collisions at Large Momentum Transfer'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'momentum transfer, high', 'neutral current', 'charged current', 'p, structure function', 'momentum spectrum, parton', 'momentum transfer, dependence', 'x-dependence', 'W, mass', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'tables', '300 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908059', 'http://arXiv.org/abs/hep-ex/?9908059']","['The inclusive single and double differential cross-sections for neutral and charged current processes with four-momentum transfer squared Q^2 between 150 and 30,000 GeV2 and with Bjorken x between 0.0032 and 0.65 are measured in e^+ p collisions. The data were taken with the H1 detector at HERA between 1994 and 1997, and they correspond to an integrated luminosity of 35.6 pb^-1. The Q^2 evolution of the parton densities of the proton is tested, yielding no significant deviation from the prediction of perturbative QCD. The proton structure function F_2(x,Q^2) is determined. An extraction of the u and d quark distributions at high x is presented. At high Q^2 electroweak effects of the heavy bosons Z0 and W are observed and found to be consistent with Standard Model expectation.']",['1999-08-25']
1193,['eng'],"['Abbott, B']",['A measurement of the W boson mass using large rapidity electrons'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'W, mass', 'electron, momentum', 'electron, rapidity', 'rapidity spectrum', 'transverse momentum, spectra', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', 'anti-p p --> W anything', 'W --> electron neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908057'],"['We present a measurement of the W boson mass using data collected by the D0 experiment at the Fermilab Tevatron during 1994--1995. We identify W bosons by their decays to e-nu final states where the electron is detected in a forward calorimeter. We extract the W boson mass, Mw, by fitting the transverse mass and transverse electron and neutrino momentum spectra from a sample of 11,089 W -> e nu decay candidates. We use a sample of 1,687 dielectron events, mostly due to Z -> ee decays, to constrain our model of the detector response. Using the forward calorimeter data, we measure Mw = 80.691 +- 0.227 GeV. Combining the forward calorimeter measurements with our previously published central calorimeter results, we obtain Mw = 80.482 +- 0.091 GeV.']",['1999-08-24']
1194,['eng'],"['Schwartz, A J']",['Recent Charm Results from Fermilab Experiment E791'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'charmed meson, hadroproduction', 'charmed meson, semileptonic decay', 'charmed meson, hadronic decay', 'D+', 'D/s+', 'D0', 'form factor, ratio', 'D0 anti-D0, interference', 'width, difference', 'charmed meson, rare decay', 'final state, dilepton', 'search for, multiquark', 'bound state, (5quark)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> K*(892) lepton+ neutrino', 'D/s+ --> Phi(1020) lepton+ neutrino', 'D0 --> K- lepton+ neutrino', 'D0 --> K- pi+', 'D0 --> K- 2pi+ pi-', 'D0 --> K+ K-', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908054'],"[""Fermilab experiment E791 studied weak decays of D+, D_s, and D^0 mesons produced in collisions of 500 GeV/c negative pions with Pt and C targets. The experiment collected over 200,000 fully reconstructed charm decays. Four recent results are discussed here: (a) measurement of the form factor ratios V/A_1, A_2/A_1, and A_3/A_1 in D->K*-l-nu and Ds->phi-l-nu decays; (b) measurement of the difference in decay widths $\\Delta\\Gamma$ between the two D^0/D^0-bar mass eigenstates; (c) search for rare and forbidden D decays to dilepton final states; and (d) search for a ``Pentaquark,'' a bound state of c-bar-suud.""]",['1999-08-19']
1195,['eng'],"['Bazhutov, Y N']",['Disclosure of New Stable Heavy Charged Particles in Cosmic Rays'],['Particle Physics - Experimental Results'],"['cosmic radiation', 'new particle, search for', 'ionization, high', 'charged particle, heavy', 'charged particle, mass', 'charged particle, lifetime', 'model, mirror', 'scintillation counter, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908053'],"['A telescope of two coaxial scintillation detectors (an upper thin CsJ crystal of d63x0,35mm2 and a lower thick NaJ crystal of d150x100 mm2) located vertically on the surface of the Earth was used to have during T=106 hours 20 events registered with increased specific ionization in each detector that turned out to exceed 10 times the specific ionization caused by cosmic rays. All the events excluding three background events are within two standard deviations from a curve calculated for non-relativistic single charged particles with mass M=(175 +/- 25)GeV/C2, flying vertically along the telescope. Based upon the condition of being non-relativistic and the limitations on the dimentions of the experimental set-up, it follows that their life-time t >1,5*10-9s. Their intensity in cosmic rays on the Earth surface is J=(1,8 +/- 0,4)*10-6cm-2 ster-1 s-1 (at E<6 GeV, P<50 GeV/C). The events disclosed are in full correspondence with our phenomenological predictions, with previous experimental results in the course of searching them for, and with the predictions of the ""mirror model"" which interpreters a possibility of existing hypothetical stable heavy hadrons (Erzions).']",['1999-08-17']
1196,['eng'],"['McIntyre, P', 'Accomando, E', 'Arnowitt, Richard Lewis', 'Dutta, B', 'Kamon, T', 'Sattarov, A']",['The Tevatron Tripler'],['Particle Physics - Experimental Results'],"['anti-p p, storage ring', 'energy, upgrade', 'luminosity, upgrade', 'bending magnet, superconducting', 'Higgs particle, search for', 'quark antiquark, interaction', 'gluon gluon, interaction', 'supersymmetry', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908052'],"[""Recent advances in superconductor properties and superconducting magnet technology have made it possible to build cost-effective, high-performance dipoles with a field of 12 Tesla - 3 times the field strength of the Tevatron. Such magnets could be used to upgrade Fermilab's collider in its existing tunnel to a collision energy $\\sqrt s$= 6 TeV and luminosity {$\\cal L$}$>$ 10$^{33}$ cm$^{-2}$s$^{-1}$. We have calculated the parton luminosities for quark-antiquark and gluon-gluon scattering for the Tevatron, the Tripler, and LHC. In most models of the Higgs field and supersymmetry, the Tripler would have a high likelihood to discover many of the predicted particle states.""]",['1999-08-16']
1197,['eng'],"['Deshpande, A A']",['The Physics Case for Polarized Protons at HERA'],['Particle Physics - Experimental Results'],"['talk, Hamburg 1999/05/17', 'electron p, deep inelastic scattering', 'positron p, deep inelastic scattering', 'p, polarized beam', 'electron, polarized beam', 'electron nucleus, deep inelastic scattering', 'nucleon, structure function', 'structure function, spin', 'gluon, momentum spectrum', 'gluon, polarization', 'quantum chromodynamics, perturbation theory', 'fusion, photon gluon', 'jet, pair production', 'hadron, electroproduction', 'transverse momentum, high', 'photon p, interaction', 'jet, photoproduction', 'quark, momentum spectrum', 'quark, polarization', 'charged current', 'polarization, asymmetry', 'momentum transfer, high', 'fragmentation function', 'numerical calculations', 'interpretation of experiments, DESY HERA Stor', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908051'],"['Several important and unique measurements, within the standard model and of possible physics beyond it, could be made with {\\em polarized HERA} in which both the proton and the electron beams are polarized. With a $\\sim$820 GeV proton beam and a $\\sim$27.6 GeV electron beam, the polarized HERA will enable variables in the kinematic range, $10^{-5} \\le x_{\\rm Bj} \\le 0.6$ and $0 \\le Q^{2} \\le 10^{5}$, using the H1 and ZEUS detectors at DESY. This will be an increase of two orders of magnitude in both $x$ and $Q^{2}$ range compared to the presently explored range from fixed target experiments at CERN, SLAC and DESY. No other approved or planned spin experiment or accelerator facility will access the low $x$ and high $Q^{2}$ regions possible with HERA. Measurements performed with the polarized HERA collider will include the polarized structure function $g_{1}(x,Q^{2})$ at very low $x$, the polarized gluon distribution di-jet events and high-p$_{T}$ hadrons in photon gluon fusion process and in photoproduction, the weak structure functions, the valence quark distribution functions from semi-inclusive asymmetries, parton distributions inside polarized photon, and information on helicity structure of possible new physics beyond the standard model. With such a rich and broad physics program possible for HERA,not polarizing the proton beam would be a great opportunity lost.']",['1999-08-16']
1198,['eng'],"['Rykov, V L']",['How Could CP-Invariance and Physics Beyond SM Be Tested in Polarized Proton Collisions at RHIC?'],['Detectors and Experimental Techniques'],"['p p, interaction', 'p, polarized beam', 'violation, CP', 'quark antiquark, annihilation', 'charged current', 'W, exchange', 'lepton, pair production', 'effective Lagrangian', 'quark, polarization', 'differential cross section', 'spin, asymmetry', 'proposed experiment, Brookhaven RHIC Coll', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908050'],"['Just in months ahead, the first high luminosity collisions of two polarized proton beams are expected to occur at RHIC in BNL at sqrt{s} up to 500 GeV, bringing a new quality to the collider physics. In collisions of polarized particles, the presence of two axial vectors of initial polarizations, fully controlled by experimenters, may dramatically increase the number of available for tests correlations between participating vectors, generating asymmetries that could relatively easily be measured. In frame of Standard Model (SM), many of these asymmetries are either strongly suppressed or strictly prohibited. Therefore, if some of them were found nonzero, this could be an indication of a new physics beyond SM. If certain criteria met, it might be difficult to explain the observed nonzero correlations in theories without CP- and/or T-violation.']",['1999-10-15']
1199,['eng'],[],['Neutrino-induced upward stopping muons in Super-Kamiokande'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'muon, cosmic radiation', 'neutrino nucleon, interaction', 'charged current', 'muon, angular distribution', 'muon, flux', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908049'],"['A total of 137 upward stopping muons of minimum energy 1.6 GeV are observed by Super-Kamiokande during 516 detector live days. The measured muon flux is 0.39+/-0.04(stat.)+/-0.02(syst.)x10^{-13}cm^{-2}s^{-1}sr^{-1} compared to an expected flux of 0.73+/-0.16(theo.)x10^{-13}cm^{-2}s^{-1}sr^{-1}. Using our previously-published measurement of the upward through-going muon flux, we calculate the stopping/through-going flux ratio R}, which has less theoretical uncertainty. The measured value of R=0.22+/-0.02(stat.)+/-0.01(syst.) is significantly smaller than the value 0.37^{+0.05}_{-0.04}(theo.) expected using the best theoretical information (the probability that the measured R is a statistical fluctuation below the expected value is 0.39%). A simultaneous fitting to zenith angle distributions of upward stopping and through-going muons gives a result which is consistent with the hypothesis of neutrino oscillations with the parameters sin^2 2\\theta >0.7 and 1.5x10^{-3} < \\Delta m^2 < 1.5x10^{-2} eV^2 at 90% confidence level, providing a confirmation of the observation of neutrino oscillations by Super-Kamiokande using the contained atmospheric neutrino events.']",['1999-10-15']
1200,['eng'],"['Avakian, R O', 'Dallakian, S K', 'Darbinian, S M']",['The Search of Large Cross Section Asymmetries in the Pair Production Process by Polarized Photons'],['Detectors and Experimental Techniques'],"['photon nucleus, interaction', 'photon nucleus, polarized beam', 'polarization, beam monitoring', 'electron, pair production', 'energy spectrum, (positron electron)', 'angular distribution, asymmetry', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908048'],['The regions of pair particle energies and emergence angles in the process of photoproduction of electron-positron pairs in the coulomb field by polarized photons are found in which a value of cross section asymmetry is essentially large. The distributions of pair particles on energy and on angles are calculated by the Monte-Carlo method. The obtained results for pair particle yield and asymmetry permit us to conclude that on their basis can be developed a new effective method for polarized photon polarimetry.'],['1999-10-15']
1201,['eng'],"['Mikaelyan, L A', 'Sinev, V V']",['Neutrino Oscillations at Reactors'],['Particle Physics - Experimental Results'],"['review, Dubna 1999/06/28', 'neutrino, oscillation', 'fission, particle source', 'antineutrino/e, energy spectrum', 'antineutrino nucleon, interaction', 'charged current', 'positron, energy spectrum', 'neutrino, mass difference', 'neutrino, mixing angle', 'scintillation counter, liquid', 'calibration', 'experimental results', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908047'],['We shortly review past and future experiments at reactors aimed at searches for neutrino masses and mixing. We also consider new idea to search at Krasnoyarsk for small mixing angle oscillations in the atmosheric neutrino mass parameter region.'],['1999-10-15']
1202,['eng'],"['Bai, J Z']",['Measurement of the Total Cross Section for Hadronic Production by $e^+ e^-$ Annihilation at Energies between 2.6-5 Gev'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'cross section, hadronic', 'event shape analysis', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', '2.6-5.0 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908046'],"['Using the upgraded Beijing Spectrometer (BESII), we have measured the total cross section for $e^+e^-$ annihilation into hadronic final states at center-of-mass energies of 2.6, 3.2, 3.4, 3.55, 4.6 and 5.0 GeV. Values of $R$,']",['1999-10-15']
1203,['eng'],"['Bai, J Z']",['Partial Wave Analysis of $J/\\psi \\to \\gamma (K^{+}K^{-}\\pi^{+}\\pi^{-})$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'J/psi(3100), electroproduction', 'J/psi(3100), radiative decay', 'pi, pair production', 'K, pair production', 'partial wave analysis', 'mass spectrum, (2K*(892))', 'meson resonance, quantum number', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'J/psi(3100) --> K+ K- pi+ pi- photon', '3.1 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908045'],"['BES data on $J/\\psi \\to \\gamma (K^+K^-\\pi^+\\pi^-)$ are presented. The $K^*\\bar K^*$ contribution peaks strongly near threshold. It is fitted with a broad $0^{-+}$ resonance with mass $M = 1800 \\pm 100$ MeV, width $\\Gamma = 500 with width $\\sim 500$ MeV. There is further evidence for a $2^{-+}$ component peaking at 2.55 GeV. The non-$K^*\\bar K^*$ contribution is close to phase space; it peaks at 2.6 GeV and is very different to $K^{*}\\bar{K^{*}}$.']",['1999-10-15']
1204,['eng'],"['Kelly, M L']",['Application of Bayesian probability theory to the measurement of binomial data at past and future Tevatron experiments'],['Detectors and Experimental Techniques'],"['statistical analysis', 'background', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'W, hadroproduction', 'W, pair production', 'new particle, search for', 'Higgs particle', 'luminosity, measurement', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908044'],"['The experimental problem of converting a measured binomial quantity, the fraction of events in a sample that pass a cut, into a physical binomial quantity, the fraction of events originating from a signal source, is described as a system of linear equations. This linear system illustrates several familiar aspects of experimental data analysis. Bayesian probability theory is used to find a solution to this binomial measurement problem that allows for the straightforward construction of confidence intervals. This solution is also shown to provide an unbiased formalism for evaluating the behavior of data sets under different choices of cuts, including a cut designed to increase the significance of a possible, albeit previously unseen, signal. Several examples are used to illustrate the features of this method, including the discovery of the top quark and searches for new particles produced in association with $W^{\\pm}$ bosons. It is also demonstrated how to use this method to make projections for the potential discovery of a Standard Model Higgs boson at a Tevatron Run 2 experiment, as well as the utility of measuring the integrated luminosity through inclusive $p\\bar{p} \\to W^{\\pm}$ production.']",['1999-10-15']
1205,['eng'],"['Jannakos, T E']",['Search for neutrino oscillations with KARMEN'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'neutrino, oscillation', 'antineutrino/mu', 'antineutrino/e', 'fission, particle source', 'muon, leptonic decay', 'pi, leptonic decay', 'antineutrino p, interaction', 'charged current', 'n, radiative capture', 'energy spectrum, (positron photon)', 'neutrino, mass difference', 'neutrino, mixing angle', 'calorimeter, experimental results', 'Rutherford ISIS PS', '0.8 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908043'],['Results from the search for muon anti neutrino to electron anti neutrino oscillations with the karmen experiment. Results are based on the data taken from Feb.97 to Feb.99.'],['1999-10-15']
1206,['eng'],"['King, B J']",['Muon Colliders'],['Detectors and Experimental Techniques'],"['talk, New York 1999/03/29', 'muon+ muon-, storage ring', 'neutrino, secondary beam', 'muon, leptonic decay', 'neutrino, flux', 'neutrino, interaction', 'numerical calculations', 'proposed experiment']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908042', 'http://documents.cern.ch/archive/electronic/other/uploader/PAC99/thp36.pdf']",['It is shown that muon decays in straight sections of muon collider rings will naturally produce highly collimated neutrino beams that can be several orders of magnitude stronger than the beams at existing accelerators. We discuss possible experimental setups and give a very brief overview of the physics potential from such beamlines. Formulae are given for the neutrino event rates at both short and long baseline neutrino experiments in these beams.'],['1999-10-15']
1207,['eng'],[],['Search for $D^{0}-\\overline{D^{0}}$ Mixing'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'D0, hadronic decay', 'anti-D0, hadronic decay', 'D0 anti-D0, interference', 'upper limit', 'width, ratio', 'time dependence', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D*(2010) --> D0 pi+', 'D0 --> K+ pi-', 'anti-D0 --> K+ pi-', 'approx. 10 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908040'],"[""We report on a search for D0-D0bar mixing made by a study of the `wrong-sign' process D0 -> K+pi-. The data come from 9.0 fb^-1 of integrated luminosity of e+e- collisions at sqrt{s} approximately 10 GeV produced by CESR and accumulated with the CLEO II.V detector. We measure the time-integrated rate of the `wrong-sign' process D0 -> K+pi-, relative to that of the Cabibbo-favored D0bar -> K+pi-, to be R_ws=(0.34+-0.07+-0.06)%. By a study of the rate as a function of the decay time of the D0, we measure the rate of direct, doubly Cabibbo suppressed decay D0 -> K+pi- relative to D0bar -> K+pi-, to be R_D=(0.50+0.11-0.12+-0.08)%. The amplitudes that describe D0-D0bar mixing, x' and y' are consistent with zero. The one-dimensional limits, at the 95% C.L., that we determine are (1/2)x^'2<0.05%, and -5.9%<y'<0.3%. All results are preliminary.""]",['1999-10-15']
1208,['eng'],[],"['Study of charmless hadronic B decays into the final states $K\\pi,\\pi\\pi$, and KK, with the first observation of $B \\to \\pi^{+} \\pi^{-}$ and $B \\to K^{0}\\pi^{0}$']",['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, branching ratio', 'final state, (0charm)', 'Kobayashi-Maskawa angle', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> K pi', 'B --> pi+ pi-', 'B0 --> K0 pi0', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908039'],"['We have studied charmless hadronic decays of B mesons into two-body final states with kaons and pions. We present preliminary results based on 9.66 million $B\\bar{B}$ pairs collected with the CLEO detector. We have made the first observation of the decay $B \\to \\pi^+\\pi^-$, with the branching fraction of $Br(B \\to \\pi^+ \\pi^-) = (4.7^{+1.8}_{-1.5} \\pm 0.6) \\times 10^{-6}$. We have also observed for the first time the decay $B \\to K^0\\pi^0$ with the branching fraction of $Br(B \\to K^0 \\pi^0) = (14.8^{+5.9+2.4}_{-5.1-3.3}) measurements. We present improved measurements for the decays $B\\to K^{\\pm}\\pi^{\\mp}$, $B^{\\pm}\\to K^0\\pi^{\\pm}$, and $B^{\\pm}\\to K^{\\pm}\\pi^0$. We use these and other charmless hadronic B decays to make a first determination of the value of the weak phase ${\\rm Arg}(V^*_{ub})=\\gamma = {113^\\circ}^{+25^\\circ}_{-23^\\circ}$.']",['1999-10-15']
1209,['eng'],"['Anikeev, V B', 'Borisov, A', 'Chernichenko, S K', 'Goryachev, V N', 'Kirsanov, M M', 'Kononov, A I', 'Kozhin, A S', 'Kravtsov, V I', 'Lipaev, V V', 'Mukhin, A I', 'Mukhin, S A', 'Salomatin, Yu I', 'Spiridonov, A A', 'Sviridov, Yu M', 'Tumakov, V L', 'Batusov, Yu A', 'Bunyatov, S A', 'Klimov, O L', 'Krasnoperov, A V', 'Kuznetsov, V E', 'Nefedov, Y A', 'Popov, B A', 'Sidorov, A V', 'Snyatkov, V I', 'Tereshchenko, V V', 'Valuev, V Yu', 'Vovenko, A S']",['Measurement of F2 and xF3 Structure Functions in Low $Q^{2}$ Region with the IHEP-JINR Neutrino Detector'],['Particle Physics - Experimental Results'],"['neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'nucleon, structure function', 'momentum transfer, dependence', 'momentum transfer, low', 'quantum chromodynamics, Lambda parameter', 'coupling constant, strong interaction', 'calorimeter, experimental results', 'Serpukhov PS', '3-30 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908037'],['Preliminary results on the measurements of F2 and xF3 structure functions with the IHEP-JINR Neutrino Detector in a wide band neutrino beam at the U-70 accelerator are presented.'],['1999-10-15']
1210,['eng'],"['Geer, S']",['Search for antiproton decay at the Fermilab Antiproton Accumulator'],['Particle Physics - Experimental Results'],"['anti-p, accumulator', 'anti-p, decay modes', 'anti-p, lifetime', 'lower limit', 'experimental results', 'Fermilab', 'anti-p --> electron 2photon', 'anti-p --> rho(770) electron', 'anti-p --> omega(783) electron', 'anti-p --> K*(892) electron', 'anti-p --> muon- photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908036'],"['A search for antiproton decay has been made at the Fermilab Antiproton Accumulator. Limits are placed on fifteen antiproton decay modes. The results include the first explicit experimental limits on the muonic decay modes of the antiproton, and the first limits on the decay modes e- gamma gamma, e- rho, e- omega, and e- K0*. The most stringent limit is for the decay mode pbar-> e- gamma. At 90% C.L. we find that tau/B(pbar-> e- gamma) > 7 x 10^5 yr. The most stringent limit for decay modes with a muon in the final state is for the decay pbar-> mu- gamma. At 90% C.L. we find that tau/B(pbar-> mu- gamma) > 5 x 10^4 yr.']",['1999-10-15']
1211,['eng'],"['Landsberg, G L']",['Study of the Primakoff Reactions at High Energy'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'pi- nucleus, coherent interaction', 'Sigma nucleus, coherent interaction', 'hadron, hadroproduction', 'effect, Coulomb', 'Primakoff effect', 'b1(1235), radiative decay', 'a2(1320), radiative decay', 'Sigma(1385), radiative decay', 'new particle, search for', 'meson, exotic', 'quark, multiquark', 'spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> nucleus pi+ 2pi-', 'pi- nucleus --> nucleus pi+ 2pi- pi0', 'b1(1235) --> pi- photon', 'a2(1320) --> pi- photon', 'Sigma(1385) --> Sigma- photon', '600 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908034'],['In this talk the Coulomb production reactions at high energy are discussed as well as the study of electromagnetic properties of hadrons (mesons and hyperons) in these processes. The results of previous investigations are summed together with some recent data of SELEX(Fermilab) and SPHINX(IHEP) experiments.'],['1999-10-15']
1212,['eng'],"['Browder, T E']",['Structure Functions in the Decay $\\tau^{\\mp}\\to \\tau^{\\mp}\\pi^{0}\\pi^{0}\\nu_{\\tau}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'decay, structure function', 'vector', 'axial-vector', 'scalar', 'mass spectrum, (3pi)', 'Dalitz plot', 'tau-, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> pi- 2pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908030'],"['Using the CLEO II detector operating at the CESR e+e- collider, we have measured the structure functions in the decay tau+/- --> pi+/- pi0 pi0 nu, based on a sample corresponding to 4*10E6 produced tau-pair events. We determine the integrated structure functions, which depend only on the three pion invariant mass, as well as the structure functions differential in the Dalitz plot. We extract model independent limits on non-axial-vector contributions from the measured structure functions as less than 16.6% of the total branching fraction, at the 95% confidence level. Separating the non-axial-vector contributions into scalar and vector contributions, we measure that scalars (vectors) contribute with less than 9.4% (7.3%) to the total branching ratio, at the 95% confidence level.']",['1999-10-15']
1213,['eng'],"['Coan, T E']",['Measurement of Charge Asymmetries in Charmless Hadronic B Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'charge, asymmetry', 'violation, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> K pi', 'B --> K eta(958)', 'B --> omega(783) pi', 'approx. 10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908029'],['We search for CP violating asymmetries in five charmless hadronic B meson decays using the full CLEO II and CLEO II.V data samples totalling 9.7 million BBbar events. The resulting Acp measurements have a precision that varies from +-0.12 to +-0.25 (absolute) depending on mode. No significant nonzero asymmetry is observed in any mode but 90% CL limits are strong and rule out some estimates of Acp.'],['1999-10-15']
1214,['eng'],[],['Measurement of the Spin-Density Matrix Elements in Exclusive Electroproduction of $\\rho^{0}$ Mesons at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, exclusive reaction', 'rho(770)0, electroproduction', 'rho(770)0, hadronic decay', 'angular distribution', 'spin, density matrix', 'helicity, violation', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> p rho(770)0 positron', 'rho(770)0 --> pi+ pi-', 'approx. 300 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908026', 'http://www-zeus.desy.de/~schlenst/conf/osaka_paper.html']","['Exclusive electroproduction of rho^0 mesons has been measured using the ZEUS detector at HERA in two Q^2 ranges, 0.25<Q^2<0.85 GeV^2 and 3<Q^2<30 GeV^2. The low-Q^2 data span the range 20<W<90 GeV; the high-Q^2 data cover the 40<W<120 GeV interval. Both samples extend up to four-momentum transfers of |t|=0.6 GeV^2. The distribution in the azimuthal angle between the positron scattering plane and the rho^0 production plane shows a small but significant violation of s-channel helicity conservation, corresponding to the production of longitudinally polarised (i.e. helicity zero) rho^0 mesons from transverse photons. Measurements of the 15 combinations of spin-density matrix elements which completely define the angular distributions are presented and discussed.']",['1999-10-15']
1215,['eng'],"['Anastassov, A']",['Update of the Search for the Neutrinoless Decay $\\tau \\to \\mu \\gamma$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, radiative decay', 'violation, flavor', 'tau, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau --> muon photon', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908025'],"['We present an update of the search for the lepton family number violating decay $\\tau \\to \\mu\\gamma$ using a complete CLEO II data sample of 12.6 million corresponding upper limit is $ \\BR(\\tau \\to \\mu\\gamma) < 1.0 \\times 10^{-6} $ at 90% CL, significantly smaller than previous limits. All quoted results are preliminary.']",['1999-10-15']
1216,['eng'],"['Edwards, K W']",['Resonant Structure of $\\tau \\to 3\\pi\\pi^{0}\\nu_{\\tau}$ and $\\tau \\to \\omega\\pi\\nu_{\\tau}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'final state, (3pi pi0)', 'second-class current, search for', 'partial wave analysis', 'spectral representation', 'meson resonance, mass', 'meson resonance, width', 'rho(1700)', 'a1(1260)', 'current, hadronic', 'parametrization', 'CVC model', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau --> 3pi pi0 neutrino/tau', 'tau --> omega(783) pi neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908024'],['The resonant structure of the four pion final state in the decay $\\tau \\to collected by the CLEO II experiment. We search for second class currents in the decay $\\tau \\to ømega\\pi\\nu_\\tau$ using spin-parity analysis and establish an upper limit on the non-vector current contribution. The mass and width of the spectral function. A partial wave analysis of the resonant structure of the the four pion system is dominated by the $ømega\\pi$ and $a_1 \\pi$ final states.'],['1999-10-15']
1217,['eng'],"['Crittenden, J A']",['Results on Diffractive Processes from the HERA Collider Experiments'],['Particle Physics - Experimental Results'],"['talk, Bloomington 1999/04/08', 'positron p, colliding beams', 'photon p, interaction', 'diffraction', 'rapidity, gap', 'vector meson, photoproduction', 'vector meson, electroproduction', 'rho(770)0', 'omega(783)', 'Phi(1020)', 'J/psi(3100)', 'cross section, energy dependence', 'momentum transfer, dependence', 'rapidity spectrum', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908023'],['We review topical results on diffractive processes from the experiments H1 and ZEUS at the HERA electron-proton collider. Emphasis is placed on the phenomenological and experimental consequences of the discoveries at HERA for the proposed electron/polarized-ion collider EPIC.'],['1999-10-15']
1218,['eng'],"['Ahmed, S']",['$b\\to s\\gamma$ Branching Fraction and CP Asymmetry'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'quark, beauty', 'quark, pair production', 'quark, radiative decay', 'quark, branching ratio', 'asymmetry, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'beauty --> strangeness photon', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908022'],['We present preliminary results on $b \\to s \\gamma$ from the CLEO experiment. An updated result on the branching fraction is reported at $\\cal{B}'],['1999-10-15']
1219,['eng'],"['Nelson, H N']",['Compilation of $D^{0} \\to \\overline{D^{0}}$ Mixing Predictions'],['Particle Physics - Experimental Results'],"['review, Stanford 1999/08/09', 'data compilation', 'D0 anti-D0, interference', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908021'],['We present a compilation of predictions for the amplitudes of D0-D0bar mixing.'],['1999-10-15']
1220,['eng'],[],['Observation of CP Violation in $K(L)\\to\\pi^{+}\\pi^{-}e^{+}e^{-}$ Decays'],['Particle Physics - Experimental Results'],"['K0(L), semileptonic decay', 'violation, CP', 'mass spectrum, (pi+ pi- positron electron)', 'decay, angular distribution', 'asymmetry', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi+ pi- positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908020'],"['We report the first observation of a manifestly CP violating effect in the K(L)->pi+pi-e+e- decay mode. A large asymmetry was observed in the distribution of these decays in the CP-odd and T-odd angle phi between the decay planes of the e+e- and pi+pi- pairs in the K(L) center of mass system. After acceptance corrections, the overall asymmetry is found to be 13.6+-2.5 (stat) +-1.2 (syst)%. This is the largest CP-violating effect yet observed integrating over the entire phase space of a mode and the first such effect observed in an angular variable.']",['1999-10-15']
1221,['eng'],"['Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Dambasuren, E', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chan, S', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, T K', 'Richman, J D', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A E']","[""Two-body B Meson Decays to $\\eta$ and $\\eta^{'}$- Observation of $B \\to \\eta K^{*}$""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'eta', 'eta(958)', 'K*(892)', 'B, branching ratio', 'final state, (0strangeness)', 'branching ratio, upper limit', 'tables', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> K*(892) eta', 'B --> eta(958) K0', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908019'],"['We present the first observation of the decay B->J/psi phi K. Using 9.6 million B meson pairs collected with the CLEO detector, we have observed 10 fully reconstructed B->J/psi phi K candidates, whereas the estimated mean background is 0.5 events. We obtained Br(B->J/psi phi K) = (8.8+3.5/-3.0(stat)+/-1.3(syst))*10^-5. This observation serves as the first conclusive evidence for the $s \\bar{s}$ pair popping in the B meson decays.']",['1999-08-06']
1222,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V V', 'Acharya, B S', 'Adam, I', 'Adams, D L', 'Adams, M', 'Ahn, S', 'Akimov, V E', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B Yu', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Belyaev, A', 'Beri, S B', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Blazey, G C', 'Blessing, S K', 'Bloom, P', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F O', 'Boswell, C', 'Brandt, A', 'Breedon, R E', 'Briskin, G M', 'Brock, R L', 'Bross, A D', 'Buchholz, D A', 'Burtovoi, V S', 'Butler, J M', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chan, K M', 'Chekulaev, S V', 'Chen, W', 'Cho, D K', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cobau, W G', 'Cochran, J', 'Coney, L', 'Cooper, W E', 'Coppage, D', 'Cretsinger, C E', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Estrada, J K', 'Evans, H', 'Evdokimov, V N', 'Fahland, T', 'Fatyga, M K', 'Fehér, S', 'Fein, D K', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Forden, G E', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Geld, T L', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Ginther, G', 'Gobbi, B', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, D R', 'Green, J A', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Guida, J A', 'Guida, J M', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hays, C', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Hernández-Montoya, R', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hsieh, F', 'Hu Tong', 'Ito, A S', 'Jaques, J', 'Jerger, S A', 'Jesik, R', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Jun, S Y', 'Kahn, S', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Knuteson, B', 'Ko, W', 'Kohli, J M', 'Koltick, D S', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kubantsev, M A', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Landry, F J', 'Landsberg, G L', 'Leflat, A', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lu, J G', 'Lucotte, A', 'Lueking, L H', 'Maciel, A K A', 'Madaras, R J', 'Madden, R', 'Magana-Mendoza, L', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Markeloff, R', 'Marshall, T', 'Martin, M I', 'Martin, R D', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McKibben, T', 'McKinley, J', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mostafa, M A', 'Da Motta, H', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Narayanan, A', 'Neal, H A', 'Negret, J P', 'Némethy, P', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Oshima, N', 'Owen, D', 'Padley, P', 'Para, A', 'Parashar, N', 'Park, Y M', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pishchalnikov, Yu', 'Pope, B G', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramírez, O', 'Reay, N W', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Sánchez-Hernández, A', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Scully, J R', 'Shabalina, E', 'Shaffer, C', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Sidwell, R A', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Slattery, P', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Song, X F', 'Sosebee, M', 'Sotnikova, N', 'Souza, M', 'Stanton, N R', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Sznajder, A', 'Tamburello, P D', 'Tarazi, J', 'Tartaglia, M', 'Thomas, T L T', 'Thompson, J', 'Toback, D', 'Trippe, T G', 'Tuts, P M', 'Vaniev, V', 'Varelas, N', 'Varnes, E W', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yepes, P', 'Yip, K', 'Yoshikawa, C', 'Youssef, S', 'Yu, J', 'Yu, Y', 'Zanabria, M E', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Evidence of Color Coherence Effects in $W+$ Jets Events from $p\\overline{p}$ Collisions at $\\Sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'jet, associated production', 'color, coherence', 'quantum chromodynamics, perturbation theory', 'leading logarithm approximation', 'duality, parton hadron', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W (n)jet anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908017'],"['We report the results of a study of color coherence effects in ppbar collisions based on data collected by the D0 detector during the 1994-1995 run of the Fermilab Tevatron Collider, at a center of mass energy sqrt(s) = 1.8 TeV. Initial-to-final state color interference effects are studied by examining particle distribution patterns in events with a W boson and at least one jet. The data are compared to Monte Carlo simulations with different color coherence implementations and to an analytic modified-leading-logarith m perturbative calculation based on the local parton-hadron duality hypothesis.']",['1999-08-06']
1223,['eng'],"['Barate, R']",['Search for neutral Higgs bosons in $e^{+}e^{-}$ collisions at $\\sqrt{s} \\leq$ 196 GeV'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, neutral particle', 'Higgs particle, electroproduction', 'Higgs particle, mass', 'lower limit', 'Z0, associated production', 'Higgs particle, pair production', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'electron positron --> 2Higgs particle Z0', '191.6, 195.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908016'],"['A preliminary search for neutral Higgs bosons is performed in the data collected by ALEPH in 1999, corresponding to integrated luminosities of 29.0 and 69.5 pb^-1 at centre-of-mass energies of 191.6 and 195.6 GeV respectively. No evidence for a signal is found. Combined with the lower energy ALEPH data, this observation leads to a 95% confidence level lower mass limit of 98.8 GeV/c^2 for the Standard Model Higgs boson. In the MSSM, the lower limit for the mass of the lightest CP-even Higgs boson h, is found to be 85.2 GeV/c^2 for all values of tan(beta)>=1.']",['1999-08-06']
1224,['eng'],"['Burrows, P N']",['QCD and $\\gamma-\\gamma$ interactions at a high-energy linear $e^{+}e^{-}$ collider'],['Particle Physics - Experimental Results'],"['talk, Sitges 1999/04/28', 'electron positron, linear collider', 'photon photon, interaction', 'quantum chromodynamics, validity test', 'strong interaction, coupling constant', 'momentum transfer, dependence', 'event shape analysis', 'quark, truth', 'quark, pair production', 'threshold', 'gluon, radiation', 'Z0', 'color, recombination', 'polarized beam', 'multiplicity', 'dependence, flavor', 'photon, structure function']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908015'],"['A summary is presented of the key strong-interaction measurements that could be made at a high-energy, high-luminosity e+e- collider']",['1999-08-06']
1225,['eng'],"['Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Dambasuren, E', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chan, S', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, T K', 'Richman, J D', 'Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A E', 'Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H']",['First Observation of the Decay $B \\to J/\\psi\\phi K$'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'J/psi(3100), leptonic decay', 'Phi(1020), hadronic decay', 'Dalitz plot', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> J/psi(3100) Phi(1020) K', 'J/psi(3100) --> lepton+ lepton-', 'Phi(1020) --> K+ K-', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908014'],"['We present the first observation of the decay B->J/psi phi K. Using 9.6 million B meson pairs collected with the CLEO detector, we have observed 10 fully reconstructed B->J/psi phi K candidates, whereas the estimated mean background is 0.5 events. We obtained Br(B->J/psi phi K) = (8.8+3.5/-3.0(stat)+/-1.3(syst))*10^-5. This observation serves as the first conclusive evidence for the $s \\bar{s}$ pair popping in the B meson decays.']",['1999-08-06']
1226,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A Study of Three-Prong $\\tau$ Decays with Charged Kaons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau-, semileptonic decay', 'final state, (3charged particle)', 'K1(1270)', 'K1(1400)', 'tau-, branching ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau- --> K- pi+ pi- neutrino/tau', 'tau- --> K+ K- pi- neutrino/tau', 'tau- --> 3charged particle pi0 neutrino/tau', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908013'],"['From an analysis of the ionisation energy loss of charged particles selected from a sample of 147926 e+e- -> tau+tau- candidates recorded in the OPAL detector at e+e- centre-of-mass energies near the Z0 resonance, we determine the branching ratios: BR(tau- -> nu_tau K- pi- pi+ (pi0)) = 0.343 +- 0.073 +- 0.031 % BR(tau- -> nu_tau K- pi- K+ (pi0)) = 0.159 +- 0.053 +- 0.020 % where the (pi0) notation refers to decay modes with or without an accompanying pizero. The tau- -> nu_tau K- pi- pi+ (pi0) final states occurring through tau- -> nu_tau K- K_s (pi0) are treated as background in this analysis. We also examine the resonant structure of tau- -> nu_tau K- pi- pi+ candidates. Under the assumption that the resonant structure is dominated by the K_1 resonances, we determine the ratio of the BR (tau- -> K_1(1270)) to the sum of the BRs (tau -> K_1(1270) and (tau -> K_1(1400)) to be 0.71 +- 0.16 +- 0.11. In all results, the first uncertainties are statistical and the second are systematic.']",['1999-08-06']
1227,['eng'],[],['Measurement of $D^{*\\pm}$ production and the charm contribution to $F_{2}$ in deep inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'p, structure function', 'structure function, charm', 'channel cross section', 'differential cross section, transverse momentum', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'quantum chromodynamics, validity test', 'quark, charm', 'quark, fragmentation', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> D*(2010) anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K- 2pi+ pi-', 'approx. 300 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908012', 'http://www-zeus.desy.de/~schlenst/conf/osaka_paper.html']","['The production of D*+-(2010) mesons in deep inelastic scattering has been measured in the ZEUS detector at HERA using an integrated luminosity of 37 pb^-1. The decay channels D*+ -> D0 pi+(+c.c.), with D0 -> K- pi+ or D0 ->K- pi- pi+ pi+, have been used to identify the D mesons. The e+p cross section for inclusive D*+- production with 1<Q^2<600 GeV^2 and 0.02<y<0.7 is 8.31 +- 0.31(stat.) +0.30-0.50(syst.) nb in the kinematic region 1.5< pT(D*+-)<15 GeV and |eta(D*+-)|<1.5. Differential cross sections are consistent with a next-to-leading-order perturbative-QCD calculation when using charm-fragmentation models which take into account the interaction of the charm quark with the proton remnant. The observed cross section is extrapolated to the full kinematic region in pT(D*+-) and eta(D*+-) in order to determine the charm contribution, F^ccbar_2(x,Q^2), to the proton structure function. The ratio F^ccbar_2/F_2 rises from ~10% at Q^2 ~1.8 GeV^2 to ~30% at Q^2 ~130 GeV^2 for x values in the range 10^-4 to 10-3.']",['1999-08-05']
1228,['eng'],"['Vaitaitis, A G']",['Search for Neutral Heavy Leptons in a High-Energy Neutrino Beam'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'beryllium, oxygen', 'heavy lepton, search for', 'heavy lepton, neutral particle', 'interference, (heavy lepton neutrino/mu)', 'heavy lepton, decay', 'production, upper limit', 'calorimeter, experimental results', 'Batavia TEVATRON PS', 'heavy lepton --> muon electron neutrino', 'heavy lepton --> 2muon neutrino', 'heavy lepton --> rho(770) muon', 'heavy lepton --> pi muon', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908011'],"['A search for neutral heavy leptons (NHLs) has been performed using an instrumented decay channel at the NuTeV (E-815) experiment at Fermilab. The decay channel was composed of helium bags interspersed with drift chambers, and was used in conjunction with the NuTeV neutrino detector to search for NHL decays. The data were examined for NHLs decaying into muonic final states (mu mu nu, mu e nu, mu pi, and mu rho); no evidence has been found for NHLs in the 0.25 - 2.0 GeV mass range. This analysis places limits on the mixing of NHLs with standard light neutrinos at a level up to an order of magnitude more restrictive than previous search limits in this mass range.']",['1999-08-04']
1229,['eng'],[],['Hadroproduction of the $\\chi1$ and $\\chi2$ States of Charmonium in 800 GeV/c Proton-Silicon Interactions'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'silicon', 'chi/c1(3510), hadroproduction', 'chi/c2(3555), hadroproduction', 'chi mesons, radiative decay', 'channel cross section, ratio', 'energy dependence', 'J/psi(3100), leptonic decay', 'mass spectrum, dimuon', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'p silicon --> chi mesons anything', 'chi mesons --> J/psi(3100) photon', '800 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908010'],"['The cross sections for the hadroproduction of the Chi1 and Chi2 states of charmonium in proton-silicon collisions at sqrt{s}=38.8 GeV have been measured in Fermilab fixed target Experiment 771. The Chi states were observed via their radiative decay to J/psi+gamma, where the photon converted to e+e- in the material of the spectrometer. The measured values for the Chi1 and Chi2 cross sections for x_F>0 are 263+-69(stat)+-32(syst) and 498+-143(stat)+-67(syst) nb per nucleon respectively. The resulting sigma(Chi1}/sigma(Chi2) ratio of 0.53+-0.20(stat)+-0.07(syst), although somewhat larger than most theoretical expectations, can be accomodated by the latest theoretical estimates.']",['1999-08-04']
1230,['eng'],"['Anderson, S']",['Observation of a Broad L=1 $c\\overline{q}$ State in $B^{-}\\rightarrow D^{*+}\\pi^{-}\\pi^{-}$ at CLEO'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B-, hadronic decay', 'charmed meson, new particle', 'new particle, D1(2460)', 'charmed meson, mass', 'charmed meson, width', 'angular momentum', 'mass spectrum, (D*(2010) pi)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B- --> D*(2010) 2pi-', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908009'],"['Using 4.7 fb^-1 of data taken at CESR at energies at and near the Upsilon(4S) we have studied the decay B- -> D{*+}pi-pi- (and its conjugate). We observe a new, broad charmed meson state, which we interpret as D_J(j=1/2), in its decay to D{*+}pi-. Our preliminary results indicate the mass and width of this L=1 state to be m = (2461 +41/-3} +/-10 +/-32) MeV and Gamma = (290 +101/-79 +/-26 +/-36) MeV, with the third uncertainty associated with the parameterization of the relative strong phases. In addition we have measured several new branching fractions of charged B mesons. All quoted results are preliminary.']",['1999-08-04']
1231,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Tests of the Standard Model and Constraints on New Physics from Measurements of Fermion-pair Production at 189 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'fermion, pair production', 'electron', 'muon', 'tau', 'quark', 'hadron, multiple production', 'new particle, search for', 'new interaction, search for', 'four-fermion interaction', 'coupling constant, electromagnetic interaction', 'energy dependence', 'gravitation, higher-dimensional', 'graviton', 'sneutrino, exchange', 'R parity, violation', 'electroweak interaction, validity test', 'angular distribution, asymmetry', 'cross section, energy dependence', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908008'],"['Cross-sections and angular distributions for hadronic and lepton pair final states in e+e- collisions at a centre-of-mass energy near 189 GeV, measured with the OPAL detector at LEP, are presented and compared with the predictions of the Standard Model. The results are used to measure the energy dependence of the electromagnetic coupling constant alpha_em, and to place limits on new physics as described by four-fermion contact interactions or by the exchange of a new heavy particle such as a sneutrino in supersymmetric theories with R-parity violation. A search for the indirect effects of the gravitational interaction in extra dimensions on the mu+mu- and tau+tau- final states is also presented.']",['1999-08-04']
1232,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for pair-produced leptoquarks in $e^{+}e^{-}$ interactions at $\\sqrt{s} \\simeq$ 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'search for, leptoquark', 'leptoquark, pair production', 'leptoquark, semileptonic decay', 'leptoquark, scalar', 'leptoquark, vector', 'leptoquark, coupling', 'leptoquark, quantum number', 'leptoquark, mass', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2leptoquark', 'leptoquark --> quark lepton', 'leptoquark --> quark neutrino', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908007'],['A search for pair-produced leptoquarks has been performed using a sample of e+e- collision events collected by the OPAL detector at LEP at e+e- centre-of-mass energies of about 183 GeV. The data sample corresponds to an integrated luminosity of 55.9 pb-1. The leptoquarks were assumed to be produced via couplings to the photon and the Z0 and then to decay within a single fermion generation. No evidence for contributions from leptoquark pair production processes was observed. Lower limits on scalar and vector leptoquark masses are obtained. The existing limits are improved in the region of large decay branching ratio to quark-neutrino.'],['1999-08-04']
1233,['eng'],"['Abe, K']",['An Improved Direct Measurement of Leptonic Coupling Asymmetries with Polarized $Z^{0}s*$'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, leptonic decay', 'coupling, (Z0 lepton)', 'coupling, asymmetry', 'angular distribution, asymmetry', 'polarization, asymmetry', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908006'],"[""We report new direct measurements of the $Z^0$-lepton coupling asymmetry parameters $A_e$, $A_{\\mu}$ and $A_{\\tau}$, with polarized $Z^0$'s collected by the SLD detector at the SLAC Linear Collider. The parameters are extracted from the measurement of the left-right-forward-backward asymmetries for each lepton species. The 1996, 1997 and 1998 SLD runs are included in this analysis and combined with published data from the 1993-95 runs. Preliminary results are $A_e = 0.1558 \\pm 0.0064$, $A_{\\mu}=0.137 \\pm 0.016 $ and $A_{\\tau}=0.142 \\pm 0.016$. If lepton universality is assumed, a combined asymmetry parameter $A_{l} = 0.1523 \\pm 0.0057$ results. This translates into an effective weak mixing angle $\\sin^2\\theta^{eff}_W = 0.23085 \\pm 0.00073$ at the $Z^0$ resonance.""]",['1999-08-04']
1234,['eng'],"['Telnov, V I']","['Status of $\\gamma-\\gamma$, $\\gamma$-electron colliders']",['Particle Physics - Experimental Results'],"['talk, Freiburg 1999/05/23', 'electron positron, linear collider', 'linear collider, proposed', 'photon photon, colliding beams', 'photon electron, colliding beams', 'backscatter, laser', 'luminosity', 'beam optics', 'Higgs particle, search for', 'charged particle, pair production', 'W', 'quark, truth', 'sparticle', 'quantum gravity, higher-dimensional', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908005'],"['This report on Photon Colliders briefly reviews three main issues: physics motivation, possible parameters and technical feasibility, plans of works and international cooperation. New scheme of laser optics at the interaction region is described which can drastically (at least by one order) reduce the cost of the laser system.']",['1999-08-03']
1235,['eng'],"['Burrows, P N']",['A CCD vertex detector for a high-energy linear $e^{+}e^{-}$ collider'],['Detectors and Experimental Techniques'],"['talk, Texel 1999/06/20', 'magnetic detector, SLD', 'semiconductor detector, vertex', 'semiconductor detector, pixel', 'particle identification, flavor', 'background', 'readout', 'radiation, damage']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908004'],"['I present a summary of the experience with CCD-based vertex detectors at the SLD experiment at SLAC, and discuss their advantages for use at a future high-energy e+e- collider. The extensive R+D programme to improve further the vertexing capabilities of CCD detectors is also outlined.']",['1999-08-03']
1236,['eng'],"['Redondo, I']",['Measurement of $D^{*\\pm}$ Cross Sections and the Charm Contribution to the Structure Function of the Proton in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'p, structure function', 'structure function, charm', 'quantum chromodynamics, validity test', 'differential cross section, transverse momentum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> D*(2010) anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K- 2pi+ pi-', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908003'],['We present measurements on D*+- production cross sections in deep inelastic e+p scattering with 1<Q^2<600 GeV^2 and 0.02<y<0.7 in two restricted kinematic regions in p_t(D*) and eta(D*). The decay channels D*+ -> D0 pi+ with subsequent decay D0 -> K- pi+ or D0 -> K- pi+ pi+ pi- (+c.c) are used. The cross sections are extrapolated to the full kinematic region to determine the charm contribution to the proton structure function.'],['1999-08-03']
1237,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for Neutral Higgs Bosons in $e^{+}e^{-}$ Collisions at $\\sqrt{s} \\sim$ 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, neutral particle', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, pair production', 'supersymmetry', 'Higgs particle, decay modes', 'Higgs particle, mass', 'lower limit', 'squark, truth', 'squark, interference', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', 'electron positron --> Higgs particle Z0', 'electron positron --> 2Higgs particle Z0', 'Higgs particle --> 2Higgs particle', 'Higgs particle --> 2beauty', 'Higgs particle --> tau+ tau-', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908002'],"['A search for neutral Higgs bosons has been performed with the OPAL detector at LEP, using approximately 170 pb-1 of e+e- collision data collected at sqrt(s)~189GeV. Searches have been performed for the Standard Model (SM) process e+e- to H0Z0 and the MSSM processes e+e- to H0Z0, A0h0. The searches are sensitive to the b b-bar and tau antitau decay modes of the Higgs bosons, and also to the MSSM decay mode h0 to A0A0. OPAL search results at lower centre-of-mass energies have been incorporated in the limits we set, which are valid at the 95% confidence level. For the SM Higgs boson, we obtain a lower mass bound of 91.0 GeV. In the MSSM, our limits are mh>74.8GeV and mA>76.5GeV, assuming tan(beta)>1, that the mixing of the scalar top quarks is either zero or maximal, and that the soft SUSY-breaking masses are 1 TeV. For the case of zero scalar top mixing, we exclude values of tan(beta) between 0.72 and 2.19.']",['1999-08-03']
1238,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the Production Rate of Charm Quark Pairs from Gluons in Hadronic $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'gluon, fragmentation', 'quark, charm', 'quark, pair production', 'yield, charm', 'particle identification, (D*(2010) muon electron)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'Z0 --> quark antiquark gluon', 'gluon --> 2charm', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908001'],"['The rate of secondary charm-quark-pair production has been measured in 4.4 million hadronic Z0 decays collected by OPAL. By selecting events with three jets and tagging charmed hadrons in the gluon jet candidate using leptons and charged D* mesons, the average number of secondary charm-quark pairs per hadronic event is found to be (3.20+-0.21+-0.38)x10-2.']",['1999-08-03']
1239,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Boeriu, O', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Dallison, S', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Donkers, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Ferrari, P', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'Lillich, J', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Marchant, T E', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Meyer, I', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trefzger, T M', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Waller, D', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Multi-photon production in $e^{+}e^{-}$ collisions at $\\sqrt{s}$ = 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'photon, multiple production', 'mass spectrum, two-photon', 'quantum electrodynamics, validity test', 'angular distribution', 'electron, excited state', 'heavy lepton, mass', 'lower limit', 'exchange, graviton', 'resonance, search for', 'resonance, radiative decay', 'channel cross section, branching ratio', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2photon', 'electron positron --> 3photon', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907064'],"['The process e+e- to 2 (or 3) gammas is studied using data recorded with the OPAL detector at LEP. The data sample taken at a centre-of-mass energy of 189 GeV corresponds to a total integrated luminosity of 178 pb-1. The measured cross-section agrees well with the expectation from QED. A fit to the angular distribution is used to obtain improved limits at 95% CL on the QED cut-off parameters: Lambda+ > 304 GeV and Lambda- > 295 GeV as well as a mass limit for an excited electron, Me* > 306 GeV assuming equal e*egamma and eegamma couplings. Graviton exchange in the context of theories with higher dimensions is excluded for scales G+ < 660 GeV and G- < 634 GeV. No evidence for resonance production is found in the invariant mass spectrum of photon pairs. Limits are obtained for the cross-section times branching ratio for a resonance decaying into two photons and produced in association with another photon.']",['1999-08-02']
1240,['eng'],"['Abe, K', 'Adam, I', 'Akagi, T', 'Akimoto, H', 'Allen, N J', 'Ash, William W', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barakat, M B', 'Bardon, O', 'Barklow, T L', 'Bashindzhagian, G L', 'Bauer, J M', 'Bellodi, G', 'Benvenuti, Alberto C', 'Bilei, G M', 'Bisello, D', 'Blaylock, G', 'Bogart, J R', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Byrne, R M', 'Calcaterra, A', 'Calloway, D H', 'Camanzi, B', 'Carpinelli, M', 'Cassell, R', 'Castaldi, R', 'Castro, A', 'Cavalli-Sforza, M', 'Chou, A', 'Church, E', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cowan, R F', 'Coyne, D G', 'Crawford, G', 'Damerell, C J S', 'Danielson, M N', 'Daoudi, M', 'De Groot, N', ""Dell'Orso, R"", 'Dervan, P J', 'De Sangro, R', 'Dima, M', 'Dong, D N', 'Doser, M', 'Dubois, R', 'Eisenstein, B I', 'Erofeeva, I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fan, C', 'Fernández, J P', 'Fero, M J', 'Flood, K', 'Frey, R', 'Gifford, J A', 'Gillman, T', 'Gladding, G E', 'González, S', 'Goodman, E R', 'Hart, E L', 'Harton, J L', 'Hasuko, K', 'Hedges, S J', 'Hertzbach, S S', 'Hildreth, M D', 'Huber, J', 'Huffer, M E', 'Hughes, E W', 'Huynh, X', 'Hwang, H', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Johnson, R A', 'Junk, T R', 'Kajikawa, R', 'Kalelkar, M S', 'Kamyshkov, Yu A', 'Kang, H J', 'Karliner, I', 'Kawahara, H', 'Kim, Y D', 'King, M E', 'King, R', 'Kofler, R R', 'Krishna, N M', 'Kroeger, R S', 'Langston, M', 'Lath, A', 'Leith, D W G S', 'Lia, V', 'Lin, C', 'Liu, M X', 'Liu, X', 'Loreti, M', 'Lu, A', 'Lynch, H L', 'Ma, J', 'Mahjouri, M', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'Masuda, H', 'Mazzucato, E', 'McKemey, A K', 'Meadows, B T', 'Menegatti, G', 'Messner, R', 'Mockett, P M', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Nagamine, T', 'Narita, S', 'Nauenberg, U', 'Neal, H A', 'Nussbaum, M', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, C H', 'Pavel, T J', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Pitts, K T', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Punkar, G D', 'Quigley, J', 'Ratcliff, B N', 'Reeves, T W', 'Reidy, J', 'Reinertsen, P L', 'Rensing, P E', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schindler, R H', 'Schumm, B A', 'Schwiening, J', 'Sen, S', 'Serbo, V V', 'Shaevitz, M H', 'Shank, J T', 'Shapiro, G', 'Sherden, D J', 'Shmakov, K D', 'Simopoulos, C', 'Sinev, N B', 'Smith, S R', 'Smy, M B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, H', 'Steiner, R', 'Strauss, M G', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Szumilo, A', 'Takahashi, T', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Toumbas, N K', 'Usher, T', 'Vannini, C', 'Vavra, J', 'Vella, E N', 'Venuti, J P', 'Verdier, R', 'Verdini, P G', 'Wagner, D L', 'Wagner, S R', 'Waite, A P', 'Walston, S', 'Watts, S J', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'White, S L', 'Wickens, F J', 'Williams, B', 'Williams, D C', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Word, G B', 'Wright, T R', 'Wyss, J', 'Yamamoto, R K', 'Yamartino, J M', 'Yang, X', 'Yashima, J', 'Yellin, S J', 'Young, C C', 'Yuta, H', 'Zapalac, G H', 'Zdarko, R W', 'Zhou, J']",['Combined SLD Measurement of $A_{b}$ at the $Z^{0}$ Resonance using Various Techniques'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'asymmetry', 'quark, decay modes', 'track data analysis, vertex', 'jet, charge', 'particle identification, (K lepton)', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907063'],"['We present a new preliminary combination of measurements of the parity-violation parameter Ab made by the SLD collaboration using various experimental techniques. The techniques differ in detail, but in general a sample of bb events is selected or enhanced by using the topologically reconstructed mass of the separated vertices formed by decaying B hadrons. The direction of the b(bbar) quark is signed by one of four final state tags: jet charge, vertex charge, leptons, or identified K+- from the b vertex. We account for statistical and systematic correlations between the four analyses to arrive at our combined result: Ab=0.905 +/- 0.017 {stat} +/- 0.020 (syst).']",['1999-07-30']
1241,['eng'],"['Jun, S Y', 'Akchurin, N', 'Andreev, V A', 'Atamanchuk, A G', 'Aykac, M', 'Balats, M Ya', 'Bondar, N F', 'Bravar, A', 'Cooper, P S', 'Dauwe, L J', 'Davidenko, G V', 'Dersch, U', 'Dolgolenko, A G', 'Dreossi, D', 'Dzyubenko, G B', 'Edelstein, R M', 'Emediato, L', 'Endler, A M F', 'Engelfried, J', 'Eschrich, I', 'Escobar, C O', 'Evdokimov, A V', 'Filimonov, I S', 'García, F G', 'Gaspero, M', 'Gerzon, S', 'Giller, I', 'Golovtsov, V L', 'Goncharenko, Yu M', 'Gottschalk, E E', 'Gouffon, P', 'Grachov, O A', 'Gülmez, E', 'Iori, M', 'Kamenskii, A D', 'Kangling, H', 'Kaya, M', 'Kilmer, J', 'Kim, V T', 'Kochenda, L M', 'Königsmann, Kay C', 'Konorov, I', 'Kozhevnikov, A P', 'Krivshich, A G', 'Krüger, H', 'Kubantsev, M A', 'Kubarovskii, V P', 'Kulyavtsev, A I', 'Kuropatkin, N P', 'Kurshetsov, V F', 'Kushnirenko, A', 'Kwan, S', 'Lach, J', 'Lamberto, A', 'Landsberg, G L', 'Larin, I', 'Leikin, E M', 'Luksys, M', 'Lungov, T', 'Magarrel, D', 'Maleev, V P', 'Mao, D', 'Masciocchi, S', 'Mathew, P', 'Mattson, M E', 'Matveev, V', 'McCliment, E', 'McKenna, S L', 'Moinester, M A', 'Molchanov, V V', 'Morelos, A', 'Mukhin, V A', 'Nelson, K D', 'Nemitkin, A V', 'Neoustroev, P V', 'Newsom, C R', 'Nilov, A P', 'Nurushev, S B', 'Ocherashvili, A I', 'Oleynik, G A', 'Önel, Y M', 'Ozel, E', 'Ozkorucuklu, S', 'Patrichev, S', 'Penzo, Aldo L', 'Petrenko, S I', 'Pogodin, P I', 'Povh, B', 'Procario, M', 'Prutskoi, V A', 'Ramberg, E', 'Rappazzo, G F', 'Razmyslovich, B V', 'Rud, V I', 'Russ, J', 'Schiavon, R P', 'Semyatchkin, V K', 'Simón, J', 'Sitnikov, A I', 'Skow, D', 'Smith, V J', 'Srivastava, M', 'Steiner, V', 'Stepanov, V', 'Stutte, L', 'Svoiski, M', 'Terentyev, N K', 'Thomas, G P', 'Uvarov, L N', 'Vasilev, A N', 'Vavilov, D V', 'Verebryusov, V S', 'Victorov, V A', 'Vishniakov, V V', 'Vorobyov, A A', 'Vorwalter, K', 'Wenheng, Z', 'You, J', 'Yunshan, L', 'Zhen Lin M', 'Zhigang, L', 'Zukanovich-Funchal, R']",['Observation of the Cabibbo-suppressed decay $\\Xi_{c}^{+} \\to p K^{-} \\pi^{+}$'],['Particle Physics - Experimental Results'],"['hadron nucleon, inclusive reaction', 'Xi/c+, hadroproduction', 'Xi/c+, hadronic decay', 'Xi/c+, branching ratio', 'mass spectrum, (p K- pi+)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'Xi/c+ --> p K- pi+', 'Xi/c+ --> Sigma+ K- pi+', 'Xi/c+ --> Xi- pi+ pi-', '600 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907062'],"['We report the first observation of the Cabibbo-suppressed charm baryon decay Xi_c+ -> p K- pi+. We observe 150 +- 22 events for the signal. The data were accumulated using the SELEX spectrometer during the 1996-1997 fixed target run at Fermilab, chiefly from a 600 GeV/c Sigma- beam. The branching fractions of the decay relative to the Cabibbo-favored Xi_c+ -> Sigma+ K- pi+ and Xi_c+ -> X- pi+ pi+ are measured to be B(Xi_c+ -> p K- pi+)/B(Xi_c+ -> Sigma+ K- pi+) = 0.22 +- 0.06 +- 0.03 and B(Xi_c+ -> p K- pi+)/B(Xi_c+ -> X- pi+ pi+) = 0.20 +- 0.04 +- 0.02, respectively.']",['1999-07-30']
1242,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A study of $B^{0}_{s}$ meson oscillation using hadronic $Z^{0}$ decays containing leptons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B/s0 anti-B/s0, oscillation', 'B/s0, mass difference', 'lower limit', 'particle identification, flavor', 'lepton, charge', 'jet, charge', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907061'],"['A sample of Z decays containing b-flavoured hadrons is tagged using leptons, and events having precise proper time measurements are selected. These events are used to study Bs oscillations. using the lepton to tag the decay b-flavour and jet charge or a second lepton, where available, to determine the produced b-flavour. The flavour (b or b-bar) at decay is determined from the lepton charge while the flavour at production is determined from jet charge or the charge of a second lepton, where available. The experiment was not able to resolve the oscillatory behaviour, and we deduce that the Bs oscillation frequency Delta(ms)> 5.2ps-1 at the 95% confidence level.']",['1999-07-30']
1243,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for Higgs Bosons and Other Massive States decaying into two Photons in $e^{+}e^{-}$ Collisions at 189 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'boson, pair production', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, radiative decay', 'mass spectrum, two-photon', 'photon, energy spectrum', 'Higgs particle, branching ratio', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'Higgs particle --> 2p photon', 'Z0 --> 2fermion', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907060'],"['A search is described for the generic process e+e- to X Y, where X is a neutral heavy scalar boson decaying into a pair of photons, and Y is a neutral heavy boson (scalar or vector) decaying into a fermion pair. The search is motivated mainly by the cases where either X, or both X and Y, are Higgs bosons. In particular, we investigate the case where X is the Standard Model Higgs boson and Y the Z0 boson. Other models with enhanced Higgs boson decay couplings to photon pairs are also considered. The present search combines the data set collected by the OPAL collaboration at 189 GeV collider energy, having an integrated luminosity of 182.6pb-1, with data samples collected at lower energies. The search results have been used to put 95% confidence level bounds, as functions of the mass of X, on the product of the cross-section and the relevant branching ratios, both in a model independent manner and for the particular models considered.']",['1999-07-30']
1244,['eng'],"['Bland, L C']",['Plans for Spin Physics at RHIC'],['Detectors and Experimental Techniques'],"['talk, Bloomington 1999/04/08', 'p p, interaction', 'p, polarized beam', 'p, structure function', 'spin, dependence', 'gluon, momentum spectrum', 'photon, direct production', 'jet, associated production', 'magnetic detector, PHENIX', 'magnetic detector, STAR', 'numerical calculations', 'proposed experiment, Brookhaven RHIC Coll', 'p p --> jet photon anything', '500 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907058'],"[""Polarized proton collisions will be studied at RHIC up to a total center of mass energy of 500 GeV, starting in 2002. An overview of the RHIC-spin program, and the critical components of the PHENIX and STAR detectors for spin experiments, is presented. The premier experiment within the RHIC-spin program is the determination of the fraction of the proton's spin carried by gluons. A detailed analysis of how accurately this fraction can be determined by the STAR experiment at RHIC is presented.""]",['1999-07-29']
1245,['eng'],"['Brandenburg, G']",['Charged Track Multiplicity in B Meson Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, semileptonic decay', 'charged particle, multiplicity', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907057'],"['We have used the CLEO II detector to study the multiplicity of charged particles in the decays of B mesons produced at the $\\Upsilon(4S)$ resonance. Using a sample of 1.5 x 10^6 B meson pairs, we find the mean inclusive charged particle multiplicity to be 10.71 +- 0.02 +0.21/-0.15 for the decay of the pair. This corresponds to a mean multiplicity of 5.36 +- 0.01 +0.11/-0.08 for a single B meson. Using the same data sample, we have also extracted the mean multiplicities in semileptonic and nonleptonic decays. We measure a mean of 7.82 +- 0.05 +0.21/-0.19 charged particles per $B\\bar{B}$ decay when both mesons decay semileptonically. When neither B meson decays semileptonically, we measure a mean charged particle multiplicity of 11.62 +- 0.04 +0.24/-0.18 per $B\\bar{B}$ pair.']",['1999-07-29']
1246,['eng'],"['Bergfeld, T']",['Observeration of Radiative Leptonic Decay of the $\\tau$ Lepton'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, radiative decay', 'tau, branching ratio', 'electroweak interaction, validity test', 'angular distribution, (lepton photon)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> muon- neutrino/tau antineutrino/mu photon', 'tau- --> electron neutrino/tau antineutrino/e photon', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907056'],"['Using 4.68 fb^{-1} of e^+e^- annihilation data collected with the CLEO II detector we have studied tau radiative decays tau --> mu nu nu gamma and tau --> e nu nu gamma. For a 10 MeV minimum photon energy in the tau rest frame, the branching fraction of a tau radiatively decaying to a muon is measured to be (3.61+-0.16+-0.35)*10^{-3}, and to an electron is (1.75+-0.06+-0.17)*10^{-2}. The branching fractions are in agreement with the Standard Model theoretical predictions. All quoted results are preliminary.']",['1999-07-29']
1247,['eng'],"['Barberis, D']",['A coupled channel analysis of the centrally produced $K^{+}K^{-}$ and $\\pi^{+}\\pi^{-}$ final states in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'K, pair production', 'pi, pair production', 'mass spectrum, (pi+ pi-)', 'mass spectrum, (K+ K-)', 'partial wave analysis, coupled channel', 'mass, pole', 'f0(975)', 'f0(1370)', 'f0(1500)', 'f0(1710)', 'experimental results', 'CERN SPS', 'p p --> pi+ pi- anything', 'p p --> K+ K- anything', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907055'],"['A coupled channel analysis of the centrally produced K+K- and pi+pi- final states has been performed in pp collisions at an incident beam momentum of 450 GeV/c. The pole positions and branching ratios to pipi and KK of the f0(980), f0(1370), f0(1500) and f0(1710) have been determined. A systematic study of the production properties of all the resonances observed in the pi+pi- and K+K- channels has been performed.']",['1999-07-29']
1248,['eng'],"['Sakamura, Y', 'Hemmi, Y', 'Matsuo, H', 'Sakai, H', 'Sasao, N', 'Higashi, Y', 'Korhonen, T T', 'Taniguchi, T', 'Urakawa, J']","['Development of a Laser Wire Beam Profile Monitor, 1']",['Accelerators and Storage Rings'],"['electron, storage ring', 'storage ring, beam damping', 'beam monitoring, wire', 'Compton scattering', 'radiation, laser', 'electron positron, linear collider', 'linear collider, proposed', 'KEK Lab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907054'],"['A conceptual design work and a basic experimental study of a new beam profile monitor have been performed. The monitor will be used to measure emittance of an electron beam in the ATF damping ring at KEK, in which the transverse beam size of about 10 micron is expected. It utilizes a CW laser and an optical cavity, instead of a material wire, to minimize interference with an electron beam. A laser beam with a very thin waist is realized by employing the cavity of nearly concentric mirror configuration while the intensity is amplified by adjusting the cavity length to a Fabry-Perot resonance condition. We built a test cavity to establish a method to measure important parameters such as a laser beam waist and a power enhancement factor. Three independent methods were examined for the measurement of the beam waist. It was found that the cavity realized the beam waist of 20 micron with the power enhancement factor of 50.']",['1999-07-29']
1249,['eng'],"['Affolder, T']",['Measurement of the $B^{0}\\overline{B}^{0}$ oscillation frequency using $l^{-} D^{*+}$ pairs and lepton flavor tags'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B0 anti-B0, interference', 'B0, mass difference', 'anti-B0, semileptonic decay', 'decay, inclusive reaction', 'D*(2010)', 'decay, path length', 'decay, time', 'momentum spectrum', 'lepton, charge', 'charge, asymmetry', 'particle identification, flavor', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-B0 --> D*(2010) lepton antineutrino anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907053'],"['The oscillation frequency Delta-md of B0 anti-B0 mixing is measured using the partially reconstructed semileptonic decay anti-B0 -> l- nubar D*+ X. The data sample was collected with the CDF detector at the Fermilab Tevatron collider during 1992 - 1995 by triggering on the existence of two lepton candidates in an event, and corresponds to about 110 pb-1 of pbar p collisions at sqrt(s) = 1.8 TeV. We estimate the proper decay time of the anti-B0 meson from the measured decay length and reconstructed momentum of the l- D*+ system. The charge of the lepton in the final state identifies the flavor of the anti-B0 meson at its decay. The second lepton in the event is used to infer the flavor of the anti-B0 meson at production. We measure the oscillation frequency to be Delta-md = 0.516 +/- 0.099 +0.029 -0.035 ps-1, where the first uncertainty is statistical and the second is systematic.']",['1999-07-29']
1250,['eng'],"['Bai, J Z']",['Direct Measurement of $B(D^{0}\\rightarrow \\phi X^{0})$ and $B(D^{+}\\rightarrow\\phi X^{+})$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, pair production', 'D0, hadronic decay', 'D+, semileptonic decay', 'D0, branching ratio', 'D+, branching ratio', 'Phi(1020)', 'recoil, charge', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'D0 --> Phi(1020) anything0', 'D+ --> Phi(1020) anything+', 'D+ --> Phi(1020) positron anything0', '4.03 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907052'],"['The first measurement of B(0->phi X0) and an upper limit for B(D+->phi X+) are determined from 22.3 pb-1 of e+e- annihilation data at a C. M. energy of 4.03 GeV. The data were recorded by the Beijing Spectrometer (BES) at BEPC. A recoil charge method is applied for the first time to charm threshold data to determine the charge of the D meson in the recoil from 9054+-309+-416 reconstructed D0, D+ mesons. The branching fractions B(D->phiX0) =(1.71+0.76-0.71+-0.17)%, and B(D+->phiX+) <1.8% are determined from 10 events with a reconstructed D and a recoiling phi. In addition, a 90% C.L. upper limit of B(D+->phi e+X0)<1.6% is determined from a search for semileptonic decays of the D+.']",['1999-07-28']
1251,['eng'],"['Felcini, Marta']",['The search for Higgs particles at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'electron positron, colliding beams', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'photon, associated production', 'Higgs particle, pair production', 'supersymmetry', 'Higgs particle, decay modes', 'channel cross section, branching ratio', 'upper limit', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907049'],"['The results of the experimental searches for Higgs particles at LEP, using the data collected at centre-of-mass energies up to 189 GeV, are reviewed and the prospects for the near future outlined.']",['1999-07-28']
1252,['eng'],"['Abbott, B']",['A Search for Dilepton Signatures from Minimal Low Energy Supergravity in $\\overline{p}p$ Collisions at $\\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'sparticle, search for', 'squark', 'gluino', 'gaugino', 'final state, dilepton', 'jet, multiplicity', 'transverse energy, missing-energy', 'supergravity', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907048', 'http://arXiv.org/abs/hep-ex/?9907048']","['We report on a search for supersymmetry using the DØ detector. The 1994-96 data sample of $\\sqrt{s}=1.8$ TeV $\\bar{p}p$ collisions was analyzed for events containing two leptons ($e$ or $\\mu$), two or more jets, and missing transverse energy. Assuming minimal supergravity, with free parameters $m_0$, $m_{1/2}$ and $\\tan\\beta$, various thresholds were employed to optimize the search. No excess of events was observed. We present exclusion contours in the $(m_0, m_{1/2})$ plane for $\\tan\\beta=2-6$.']",['1999-07-27']
1253,['eng'],"['Neyret, D', 'Pussieux, T']",['A photon calorimeter using lead tungstate crystals for the CEBAF Hall A Compton polarimeter'],['Detectors and Experimental Techniques'],"['electron, polarized beam', 'polarization, beam monitoring', 'Compton scattering', 'photon, calorimeter', 'scintillation counter, crystal', 'lead, tungsten', 'Newport News CEBAF Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907047'],['The performances of the calorimeter of the Jlab Hall A Compton Polarimeter have been measured using the Mainz tagged photon beam.'],['1999-07-27']
1254,['eng'],"['Briere, R A', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Blanc, F', 'Boisvert, V', 'Cassel, David G', 'Dickson, M', 'Von Dombrowski, S', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Galik, R S', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Jones, C D', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Avery, P', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Coppage, D', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Ahmed, S', 'Alam, M S', 'Athar, S B', 'Jian, L', 'Ling, L', 'Mahmood, A H', 'Saleem, M', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Schwarthoff, H', 'Spencer, M B', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A E', 'Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Dambasuren, E', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Wolf, A', 'Wu, J', 'Csorna, S E', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chan, S', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, T K', 'Richman, J D', 'Roberts, D']","[""Rare Decays of the $\\eta^{'}$""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'eta(958), rare decay', 'eta(958), branching ratio', 'upper limit', 'eta(958), hadronic decay', 'Dalitz plot', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'eta(958) --> eta positron electron', 'eta(958) --> pi0 positron electron', 'eta(958) --> positron electron photon', 'eta(958) --> eta pi+ pi-', 'eta(958) --> muon electron', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907046'],"['We have searched for the rare decays of the eta prime meson to e+ e- eta, e+ e- pizero, e+ e- gamma, and e mu in hadronic events at the CLEO II detector. The search is conducted on 4.80 fb^-1 of e+ e- collisions at the Cornell Electron Storage Ring. We find no signal in any of these modes, and set 90% confidence level upper limits on their branching fractions of 2.4 X 10^-3, 1.4 X 10^-3, 0.9 X 10^-3, and 4.7 X 10^-4, respectively. We also investigate the Dalitz plot of the common decay of the eta prime to pi+ pi- eta. We fit the matrix element with the Particle Data Group parameterization and find Re(alpha) = -0.021 +- 0.025, where alpha is a linear function of the kinetic energy of the eta.']",['1999-07-26']
1255,['eng'],"['Abe, K']",['New Measurement of $A_{b}$ at the Z Resonance using a Vertex-Charge Technique'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'angular distribution, asymmetry', 'violation, CP', 'polarization, asymmetry', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907050'],"['We present a new preliminary measurement of the parity-violation parameter Ab using a self-calibrating vertex-charge technique. In the SLD experiment we observe hadronic decays of polarized Z bosons produced in collisions between longitudinally polarized electrons and unpolarized positrons at the SLAC Linear Collider. A sample of bb events is selected using the topologically reconstructed mass of B hadrons. From out 1996-8 data sample of approximately 400,000 hadronic Z decays, we obtain Ab = 0.897 +/- 0.027 (stat) +0.036/-0.034 (syst).']",['1999-07-28']
1256,['eng'],"['Appel, R', 'Atoyan, G S', 'Bassalleck, B', 'Bergman, D R', 'Brown, D N', 'Cheung, N', 'Dhawan, S K', 'Do, H', 'Egger, J', 'Eilerts, S W', 'Felder, C', 'Fischer, H', 'Gach, M', 'Herold, W D', 'Issakov, V V', 'Kaspar, H', 'Kraus, D E', 'Lazarus, D M', 'Leipuner, L', 'Lichard, P', 'Lowe, J', 'Lozano-Bahilo, J', 'Ma, H', 'Majid, W A', 'Menzel, W', 'Pislak, S', 'Poblaguev, A A', 'Postoev, V E', 'Proskuryakov, A L', 'Rehak, P', 'Robmann, P', 'Sher, A E', 'Thomas, T L', 'Thompson, J A', 'Truöl, P', 'Weyer, H', 'Zeller, M E']",['A new measurement of the properties of the rare decay $K \\to \\pi^{+} e^{+} e^{-}$'],['Particle Physics - Experimental Results'],"['K+, rare decay', 'K+, branching ratio', 'mass spectrum, (positron electron)', 'angular distribution', 'form factor, decay', 'parametrization', 'perturbation theory, chiral', 'quantum chromodynamics, perturbation theory', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907045'],"['A large low-background sample of events (10300) has been collected for the rare decay of kaons in flight K+ -> pi+ e+ e- by experiment E865 at the Brookhaven AGS. The decay products were accepted by a broad band high-resolution charged particle spectrometer with particle identification. The branching ratio (2.94 +- 0.05(stat.) +- 0.13(syst.) +- 0.05(model))*10**{-7} was determined normalizing to events from the decay chain K+ -> pi+ pi0; pi0 -> e+ e- gamma. From the analysis of the decay distributions the vector nature of this decay is firmly established now, and limits on scalar and tensor contributions are deduced. From the (e+ e-) invariant mass distribution the decay form factor f(z)=f0(1+ delta*z) (z=M(ee)**2/m(K)**2) is determined with delta=2.14 +- 0.13 +- 0.15. Chiral QCD perturbation theory predictions for the form factor are also tested, and terms beyond leading order O(p**4) are found to be important.']",['1999-07-23']
1257,['eng'],"['Abbott, B']",['Measurement of the Transverse Momentum Distributions of W and Z Bosons Produced in pbar p Collisions at $ \\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'differential cross section, transverse momentum', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907044'],['We present measurements of the transverse momentum distribution of W and Z bosons produced in pbar p collisions at sqrt(s) = 1.8 TeV. The data were collected with the D0 detector at Fermilab during 1994-1996 Tevatron run. The results are in good agreement with theoretical predictions based on the perturbative QCD and soft gluon resummation combined calculation over the entire measured pt range p_T = 0-200 GeV/c).'],['1999-07-22']
1258,['eng'],"['Dittmar, Michael']",['Status and Prospects of Supersymmetry Searches at Colliders'],['Particle Physics - Experimental Results'],"['review, Paris 1999/06/07', 'electron positron, annihilation', 'anti-p p, interaction', 'p p, interaction', 'supersymmetry', 'sparticle, search for', 'Higgs particle, search for', 'Higgs particle, mass', 'W, pair production', 'strong interaction, coupling constant', 'energy dependence', 'mass, truth', 'W, mass', 'sparticle, mass', 'mass, hierarchy', 'experimental results', 'proposed experiment', 'CERN LEP Stor', 'Batavia TEVATRON Coll', 'CERN LHC Coll', '((5)) ((7)) ((8))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907042'],"[""Experiments at particle colliders have reached center of mass energies well above 100 GeV, equivalent to temperatures which existed shortly after the big bang. These experiments, testing the initial conditions of the universe have, with great precision, established the Standard Model of Particle Physics. In contrast, the existence of the Higgs boson and perhaps Supersymmetry remain speculative, as todays searches have failed to find signs of their existence. However, the next generation of high energy collider experiments and especially CERN's 14 TeV LHC, expected to start operation in the year 2005, should lead either to the discovery of the Higgs and Supersymmetry or disprove todays theoretical ideas.""]",['1999-07-22']
1259,['eng'],"['Klapdor-Kleingrothaus, H V']",['Perspectives of Double $\\beta$ and Dark Matter Search as Windows to New Physics'],['Particle Physics - Experimental Results'],"['review, experimental results', 'double-beta decay, (0neutrino)', 'neutrino, mass', 'supersymmetry', 'model, composite', 'Majoron', 'neutrino, sterile', 'leptoquark', 'W, right-handed', 'relativity theory', 'equivalence principle', 'astrophysics, missing-mass', 'neutrino, oscillation', 'neutrino, solar', 'electron electron, interaction', 'W-, pair production', 'neutrino, mass difference', 'semiconductor detector, germanium', 'proposed experiment', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907040'],"['Nuclear double beta decay provides an extraordinarily broad potential to search for beyond Standard Model physics, probing already now the TeV scale, on which new physics should manifest itself. These possibilities are reviewed here.']",['1999-07-21']
1260,['eng'],"['Abe, K']",['Measurement of $A_c$ with charmed mesons at SLD'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, charm', 'quark, pair production', 'particle identification, charm', 'D*(2010), hadronic decay', 'D+, hadronic decay', 'D0, decay modes', 'pi, transverse momentum', 'polarization, asymmetry', 'angular distribution, asymmetry', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'D*(2010) --> D0 pi+', 'D+ --> K- 2pi+', 'D0 --> K (n)pi', 'D0 --> K- lepton+ neutrino', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907039'],"['We present a direct measurement of the parity-violation parameter A_c. The measurement is based on 550k Z^0 decays collected by the SLD detector. The mean electron-beam polarization is |P_e| = 73 %. The tagging of c-quark events was performed using two methods: The exclusive reconstruction of D^*+, D^+, and D^0 mesons, and the inclusive P_T spectrum of soft-pions (pi_s) in the decay of D^*+ -> D^0 pi_s^+. The results of these two methods are combined to give A_c = 0.688 +- 0.035(stat.) +- 0.025(sys.) (preliminary).']",['1999-07-21']
1261,['eng'],"['Apollonio, M', 'Baldini, A', 'Bemporad, C', 'Caffau, E', 'Cei, F', 'Déclais, Y', 'De Kerret, H', 'Dieterle, B D', 'Etenko, A', 'Foresti, L', 'George, J', 'Giannini, G', 'Grassi, M', 'Kozlov, Yu Z', 'Kropp, W R', 'Kryn, Didier', 'Laiman, M', 'Lane, C E', 'Lefièvre, B', 'Machulin, I N', 'Martemyanov, A N', 'Martemyanov, B V', 'Mikaelyan, L A', 'Nicolo, D', 'Obolensky, M', 'Pazzi, R', 'Pieri, G', 'Price, L', 'Riley, S', 'Reeder, R', 'Sabelnikov, A A', 'Santin, G', 'Skorokhvatov, M', 'Sobel, H', 'Steele, J', 'Steinberg, R', 'Sukhotin, S V', 'Tomshaw, S', 'Véron, D', 'Vyrodov, V']",['Limits on Neutrino Oscillations from the CHOOZ Experiment'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'upper limit', 'fission, particle source', 'antineutrino p, exclusive reaction', 'antineutrino/e, flux', 'charged current', 'neutrino, mass difference', 'neutrino, mixing angle', 'positron, energy spectrum', 'positron, yield', 'scintillation counter, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907037'],"['We present new results based on the entire CHOOZ data sample. We find (at 90% confidence level) no evidence for neutrino oscillations in the anti_nue disappearance mode, for the parameter region given by approximately Delta m**2 > 7 x 10**-4 eV^2 for maximum mixing, and sin**2(2 theta) = 0.10 for large Delta m**2. Lower sensitivity results, based only on the comparison of the positron spectra from the two different-distance nuclear reactors, are also presented; these are independent of the absolute normalization of the anti_nue flux, the cross section, the number of target protons and the detector efficiencies.']",['1999-10-22']
1262,['eng'],"['Hadig, T']",['Issues on NLO pQCD Programs'],['Detectors and Experimental Techniques'],"['talk, Durham 1998/09/20', 'quantum chromodynamics', 'perturbation theory, higher-order', 'programming', 'electron p, deep inelastic scattering', 'jet, electroproduction', 'jet, pair production', 'transverse momentum, spectra', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907036'],"[""This paper summarizes a talk presented at the Durham HERA '98 Workshop. We compare the features that are available in NLO pQCD programs and demonstrate that understanding where in phase space NLO calculations are accurate is vital for extracting information from measurements at the HERA experiments.""]",['1999-10-22']
1263,['eng'],"['King, B J']",['Neutrino Physics at Muon Colliders'],['Detectors and Experimental Techniques'],"['talk, San Francisco 1997/12/10', 'muon+ muon-, storage ring', 'neutrino, secondary beam', 'muon, leptonic decay', 'neutrino nucleon, interaction', 'charged current', 'neutral current', 'calorimeter, target', 'drift chamber, time projection', 'magnetic field', 'nucleon, structure function', 'Kobayashi-Maskawa angle', 'Weinberg angle', 'neutrino, oscillation', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907035'],"['An overview is given of the neutrino physics potential of future muon storage rings that use muon collider technology to produce, accelerate and store large currents of muons.']",['1999-10-22']
1264,['eng'],"['King, B J']",['Momentum Resolution Studies for a large TPC-Based Central Tracker'],['Detectors and Experimental Techniques'],"['talk, Hamburg 1996/11/20', 'electron positron, linear collider', 'linear collider, proposed', 'electron positron, colliding beam detector', 'semiconductor detector, microstrip', 'momentum resolution', 'drift chamber, time projection', 'spatial resolution']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907032'],"['This note describes a study on the momentum resolution of the TPC-based central tracker design which will be included in the ECFA/DESY conceptual design report (CDR) for the proposed DESY 500 GeV electron-positron linear collider. The study found it to be likely that the central tracker could achieve a momentum resolution of approximately 10^{-4} (GeV/c)^{-1}, particularly if a layer of silicon microstrip detectors were to be added just inside the TPC.']",['1999-10-22']
1265,['eng'],"['King, B J']",['An All-Solid State Central Tracker for the Proposed DESY Electron-Positron Linear Collider'],['Detectors and Experimental Techniques'],"['talk, Hamburg 1996/11/20', 'electron positron, linear collider', 'linear collider, proposed', 'electron positron, colliding beam detector', 'semiconductor detector, position sensitive', 'momentum resolution', 'semiconductor detector, pixel', 'semiconductor detector, microstrip', 'costs']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907031'],['This report describes an all-solid state central tracker which is intended for use in a detector at the proposed DESY 500 GeV electron-positron linear collider or a similar accelerator. The precise position measurements from position-sensitive silicon detectors give the tracker an outstanding momentum resolution for high momentum tracks: sigma_p/p^2 = 3.6 x 10^{-5} (GeV/c)^{-1} for tracks perpendicular to the beam-line. The report concludes with an example layout for a detector which uses this central tracker.'],['1999-10-22']
1266,['eng'],"['Adloff, C']",['Forward Pi0-Meson Production at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'pi0, electroproduction', 'small-angle', 'small-x', 'transverse momentum, high', 'differential cross section, x-dependence', 'momentum transfer, dependence', 'transverse momentum, dependence', 'rapidity dependence', 'photon, resolved', 'Lipatov equation', 'Altarelli-Parisi equation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> pi0 anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907030'],"['High transverse momentum pi0-mesons have been measured with the H1 detector at HERA in deep-inelastic ep scattering events at low Bjorken-x, down to x <~ 4.10^{-5}. The measurement is performed in a region of small angles with respect to the proton remnant in the laboratory frame of reference, namely the forward region, and corresponds to central rapidity in the centre of mass system of the virtual photon and proton. This region is expected to be particularly sensitive to QCD effects in hadronic final states. Differential cross-sections for inclusive pi0-meson production are presented as a function of Bjorken-x and the four-momentum transfer Q^2, and as a function of transverse momentum and pseudorapidity. A recent numerical BFKL calculation and predictions from QCD models based on DGLAP parton evolution are compared with the data.']",['1999-10-22']
1267,['eng'],[],['A Study of Correlations between Identified Charged Hadrons in Hadronic $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'charged particle, multiple production', 'rapidity spectrum', 'rapidity, correlation', 'correlation, two-particle', 'correlation, short-range', 'correlation, long-range', 'quark, fragmentation', 'particle identification, flavor', 'quantum number', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908035'],"['We present a preliminary study of correlations in rapidity between pairs of identified charged pions, kaons and protons using the entire SLD data sample of 550,000 hadronic Z^0 decays. Short range charge correlations are observed between all combinations of these hadron species, indicating local conservation of quantum numbers and charge ordering in the jet fragmentation process. The rapidity range of this effect is found to be independent of particle momentum. A strong long-range K^+K^- correlation is observed at high-momentum and weaker long-range pi^+pi^-, pi^+K^-, pK^- and pp-bar correlations are observed in light flavor events, providing new information on leading particle production in u, d and s jets. The long-range correlations observed in c-cbar and bb-bar events are markedly different and consistent with expectations based on known decay properties of the leading heavy hadrons. In addition, the SLC electron beam polarization is used to tag the quark hemisphere in each event, allowing the first study of rapidities signed such that positive rapidity is along the quark rather than antiquark direction. Distributions of ordered differences in signed rapidity between pairs of particles provide a direct probe of quantum number ordering along the quark-antiquark axis and other new insights into the fragmentation process.']",['1999-10-15']
1268,['eng'],"['Abbott, B']",['Small Angle Muon and Bottom Quark Production in pbarp Collisions at $sqrt(s)$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'muon, production', 'small-angle', 'cross section, transverse momentum', 'quantum chromodynamics, perturbation theory', 'validity test', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907029'],['This Letter describes a measurement of the muon cross section originating from b quark decay in the forward rapidity range 2.4 < y(mu) <3.2 in pbarp collisions at sqrt(s) = 1.8 TeV. The data used in this analysis were collected by the D0 experiment at the Fermilab Tevatron. We find that NLO QCD calculations underestimate b quark production by a factor of four in the forward rapidity region.'],['1999-10-22']
1269,['eng'],"['Adloff, C']",['Measurements of Transverse Energy Flow in Deep-Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'neutral current', 'transverse energy, energy flow', 'momentum transfer, dependence', 'x-dependence', 'energy dependence', 'rapidity dependence', 'quantum chromodynamics', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907027'],"['Measurements of transverse energy flow are presented for neutral current deep-inelastic scattering events produced in positron-proton collisions at HERA. The kinematic range covers squared momentum transfers Q^2 from 3.2 to 2,200 GeV^2, the Bjorken scaling variable x from 8.10^{-5} to 0.11 and the hadronic mass W from 66 to 233 GeV. The transverse energy flow is measured in the hadronic centre of mass frame and is studied as a function of Q^2, x, W and pseudorapidity. A comparison is made with QCD based models. The behaviour of the mean transverse energy in the central pseudorapidity region and an interval corresponding to the photon fragmentation region are analysed as a function of Q^2 and W.']",['1999-10-22']
1270,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Koop, I A', 'Korol, A A', 'Koshuba, S V', 'Pakhtusova, E V', 'Salnikov, A A', 'Shary, V V', 'Serednyakov, S I', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Valishev, A A']",['Investigation of the $e^{+}e^{-} \\to \\omega \\pi^{0} \\to \\pi^{0} \\pi^{0} \\gamma$ reaction in the energy domain near the $\\phi$-meson'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'omega(783), electroproduction', 'pi0, associated production', 'omega(783), radiative decay', 'Phi(1020), radiative decay', 'interference, (Phi(1020) omega(783) rho(770))', 'amplitude analysis', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'bibliography', 'electron positron --> omega(783) pi0', 'omega(783) --> pi0 photon', 'Phi(1020) --> 2pi0 photon', 'approx. 1.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907026'],"['The $e^+e^- \\to \\omega \\pi^0 \\to \\pi^0 \\pi^0 \\gamma$ process was investigated in the SND experiment at the VEPP-2M collider. A narrow energy interval near the $\\phi$-meson was scanned. The observed cross-section reveals, at the level of three standard deviation, the interference effect caused by $\\phi \\to imaginary parts of the $\\phi$-meson related amplitude, were measured.']",['1999-10-22']
1271,['eng'],"['Landsberg, G L']",['Search for Exotic Baryons with Hidden Strangeness in the Experiments of the Sphinx Collaboration in Diffractive and Coulomb Production Processes'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'p nucleon, exclusive reaction', 'diffraction, production', 'Sigma, hadroproduction', 'K, associated production', 'mass spectrum, (Sigma0 K+)', 'mass spectrum, (Sigma(1385) K+)', 'mass enhancement, (1989)', 'mass enhancement, (1810)', 'baryon resonance, exotic', 'quark, multiquark', 'transverse momentum, spectra', 'effect, Coulomb', 'magnetic spectrometer, experimental results', 'Serpukhov PS', 'bibliography', 'p nucleon --> Sigma0 K+', '70 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907025'],"['Experimental results of the SPHINX Collaboration on studying proton diffractive production processes are presented. Evidences for new baryon states with masses >1.8 GeV were obtained in hyperon-kaon effective mass spectra in several reactions. New data for the diffractive reaction p+N->[Sigma0 K+]+N at Ep=70 GeV were obtained with partially upgraded SPHINX setup. The data are in a good agreement with the results of our previous study of this reaction. In the mass spectrum M(Sigma0 K+) a structure at the threshold region with a mass about 1800 MeV and a distinct X(2000) peak with M=1989+/-6 MeV and Gamma=91+/-20 MeV are observed. Unusual features of the massive X(2000) state (narrow decay width, anomalously large branching ratio for the decay channel with strange particle emission) make it a serious candidate for a cryptoexotic pentaquark baryon with hidden strangeness |qqqs sbar>. We also present new results on the narrow threshold structure X(1810) with M=1807+/-7 MeV and Gamma=62+/-19 MeV which is produced in the region of very small pt**2<0.01 GeV**2. The possibility of the Coulomb production mechanism for X(1810) is discussed.']",['1999-10-22']
1272,['eng'],[],"['Production of Charged $\\pi$, $K$ and $p$ in Hadronic $Z^{0}$ Decays']",['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'charged particle, multiple production', 'charged particle, yield', 'pi', 'K', 'p', 'anti-p', 'momentum spectrum', 'dependence, flavor', 'quantum chromodynamics, perturbation theory', 'model, fragmentation', 'validity test', 'effect, leading particle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908033'],"['We have updated our results on identified charged hadron production using the full SLD data sample of 550,000 hadronic Z^0 decays taken between 1993 and 1998. The SLD Cherenkov Ring Imaging Detector allows the identification of clean samples of charged pions, kaons and protons over a wide momentum range, providing precise tests of perturbative QCD calculations and of fragmentation models. We have studied flavor-inclusive Z^0 decays, as well as decays into light, c and b flavors, selected using the SLD vertex detector. In addition we have updated our comparison of hadron and antihadron production in light quark (rather than antiquark) jets, selected using the high SLC electron beam polarization. Differences between hadron and antihadron production at high momentum fraction provide precise measurements of leading particle production and new, stringent tests of fragmentation models.']",['1999-10-15']
1273,['eng'],"['Abe, K']",['Measurement of the probability for gluon splitting into $b\\overline{b}$ in $Z^{0}$ decays'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (4jet)', 'gluon, fragmentation', 'quark, beauty', 'quark, pair production', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'gluon --> 2beauty', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908028'],"['We present a preliminary measurement of the rate of gluon splitting into bottom quarks, g -> b bbar, in hadronic Z0 decays collected by SLD between 1996 and 1998. The analysis was performed by looking for secondary bottom production in 4-jet events of any primary flavour. 4-jet events were identified, and a topological vertex-mass technique was applied to each jet in order to identify b or bbar jets. The upgraded CCD based vertex detector gives very high B-tagging efficiency, especially for B hadrons of the low energies typical of this process. The two most nearly collinear b/bbar jets were tagged as originating from g -> b bbar. We measured the rate of secondary b/bbar production per hadronic event, g_bb, to be (3.07+-0.71(stat.)+-0.66(syst.)) * 10**-3.']",['1999-10-15']
1274,['eng'],[],['W Production and the Search for Events with an Isolated High-Energy Lepton and Missing Transverse Momentum at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'W, photoproduction', 'W, leptonic decay', 'cross section, transverse momentum', 'coupling, (2W photon)', 'momentum, missing-energy', 'electroweak interaction, validity test', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> W positron anything', 'W --> electron neutrino', 'W --> muon neutrino', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907023'],"['A search for the leptonic decays of W bosons produced in the reaction e^+ the ZEUS detector at HERA using an integrated luminosity of 47.7 pb^-1 . Three events consistent with W\\to e\\nu decay are found, giving a cross section of 0.9 +1.0 -0.7 \\pm 0.2 pb, in good agreement with the Standard Model prediction. The corresponding 95% C.L. upper limit on the cross section is 3.3 pb. A search for the decay W\\to \\mu\\nu has a smaller selection efficiency and yields no candidate events. Limits on the cross section for W production with large hadronic transverse momentum have been used to constrain the anomalous couplings \\Delta\\kappa and \\lambda at the WW\\gamma vertex. A search for high-transverse-momentum isolated tracks in events with large missing transverse momentum yields results in good agreement with Standard Model expectations, in contrast to a recent report by the H1 collaboration of the observation of an excess of such events.']",['1999-10-22']
1275,['eng'],"['Airapetian, A']",['Measurement of the Spin Asymmetry in the Photoproduction of Pairs of High-pT Hadrons at HERMES'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron, polarized beam', 'polarized target, internal', 'hadron, pair production', 'polarization, longitudinal', 'polarization, asymmetry', 'gluon, polarization', 'magnetic detector, HERMES', 'experimental results', 'DESY HERA Stor', 'positron p --> hadron+ hadron- positron anything', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907020'],"['We present a measurement of the longitudinal spin asymmetry A_|| in photoproduction of pairs of hadrons with high transverse momentum p_T. Data were accumulated by the HERMES experiment using a 27.5 GeV polarized positron beam and a polarized hydrogen target internal to the HERA storage ring. For h+h- pairs with p_T^h_1 > 1.5 GeV/c and p_T^h_2 > 1.0 GeV/c, the measured asymmetry is A_|| = -0.28 +/- 0.12 (stat.) +/- 0.02 (syst.). This negative value is in contrast to the positive asymmetries typically measured in deep inelastic scattering from protons, and is interpreted to arise from a positive gluon polarization.']",['1999-10-22']
1276,['eng'],"['Abe, K']",['Symmetry Tests in Polarized $Z^{0}$ Decays to $bbg$'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'gluon, associated production', 'angular distribution, asymmetry', 'parity, violation', 'electroweak interaction, validity test', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty gluon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908031'],"['Angular asymmetries have been measured in polarized Z0 decays to bbg collected by the SLD experiment at the SLC. A high purity bbg event sample is selected by utilizing B lifetime information given by the SLD CCD pixel vertex detector and the stable micron-size SLC beams, and the b- and bbar-jets are identified using lifetime information and momentum-weighted track charge. The forward-backward asymmetry is observed in the b-quark polar angle distribution, and the parity-violation parameter is measured to test the Standard Model. Two angular correlations between the three-jet plane and the Z0 polarization are studied. The CP-even and T-odd, and the CP-odd and T-odd, angular asymmetries are sensitive to physics beyond the Standard Model. The latter requires tagging both the b- and bbar-jet. We measure the expectation values of these quantities to be consistent with zero and set limits on the correlations at the 5% level.']",['1999-10-15']
1277,['eng'],"['Abe, K']",['Study of the structure of $e^{+}e^{-}\\to bb\\overline{g}$ events and improved limits on the anomalous chromomagnetic coupling of the b-quark'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'gluon, associated production', 'gluon, energy spectrum', 'gluon, angular distribution', 'magnetic moment, color', 'quark, magnetic moment', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty gluon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908027'],"['The structure of e+e- -> bbg events was studied using Z0 decays recorded in the SLD experiment at SLAC. Three-jet final states were selected and the CCD-based vertex detector was used to identify two of the jets as b or bbar. Distributions of the gluon energy and polar angle were measured over the full kinematic range, and compared with perturbative QCD predictions. The energy distribution is potentially sensitive to an anomalous b chromomagnetic moment kappa. We measured kappa to be consistent with zero and set limits on its value, -0.11 < kappa < 0.08 at 95% c.l. (preliminary).']",['1999-10-15']
1278,['eng'],"['Abbott, B']",['Search for R-parity Violating Supersymmetry in the Dielectron Channel'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, annihilation', 'supersymmetry, search for', 'R parity, violation', 'electron, pair production', 'jet, multiple production', 'final state, (4jet 2electron)', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907019'],"[""We report on a search for R-parity violating supersymmetry in p-pbar collisions at sqrt(s) = 1.8 TeV using the D0 detector at Fermilab. Events with at least two electrons and four or more jets were studied. We observe 2 events in 99 +- 4.4 pb-1 of data, consistent with the expected background of 1.8 +- 0.4 events. This result is interpreted within the framework of minimal low-energy supergravity supersymmetry models. Squarks with mass below 243 GeV/c^2 and gluinos with mass below 227 GeV/c^2 are excluded at the 95% confidence level (C. L.) for A_0=0, mu < 0$, tan beta=2 and a finite value for R-parity violating Yukawa coupling lambda'_1jk (j=1, 2 and k=1, 2, 3). For equal squark and gluino masses, the corresponding mass limit is 277 GeV/c^2.""]",['1999-07-15']
1279,['eng'],"['Field, J H', 'Sciarrino, D']",['A Study of the LEP and SLD Measurements of $A_{b}$'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Z0, leptonic decay', 'quark, beauty', 'quark, pair production', 'angular distribution, asymmetry', 'measurement, error', 'SLAC SLC Linac', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907018'],"['A systematic study is made of the data dependence of the parameter $A_b$, that, since 1996, has shown a deviation from the Standard Model prediction of between 3.3 and 2.5 standard deviations. Issues addressed include: the effect of particular measurements, values found by individual experiments, LEP/SLD comparison, and the treatment of systematic errors. The effect, currently at the 2.5$\\sigma$ level, is found to vary in the range from 1.7$\\sigma$ to 2.9$\\sigma$ by excluding marginal or particularly sensitive data. Since essentially the full LEP1 and SLD data sets are now analysed the meaning of the deviation, (new physics, or marginal statistical fluctuation) is unlikely to be given by the present generation of colliders.']",['1999-07-15']
1280,['eng'],"['Abe, K']",['A Preliminary Direct Measurement of the s-Quark Coupling'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, strangeness', 'quark, pair production', 'coupling, (Z0 strangeness)', 'parity, violation', 'particle identification, strangeness', 'angular distribution, asymmetry', 'polarization, asymmetry', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2strangeness', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908038'],"['We present an updated direct measurement of the parity-violating coupling of the Z boson to strange quarks, A_s, derived from the full SLD data sample of approximately 550,000 hadronic decays of Z bosons produced with a polarized electron beam and recorded by the SLD experiment at SLAC between 1993 and 1998. Events with primary strange quarks are tagged by the presence in each event hemisphere of a high-momentum charged K meson, neutral K meson or Lambda hyperon identified using the Cherenkov Ring Imaging Detector and/or a mass tag. The CCD vertex detector is used to suppress the background from heavy flavor events. The strangeness of the tagged particle is used to sign the event thrust axis in the direction of the initial strange quark. The coupling A_s is obtained directly from a measurement of the left-right-forward-backward production asymmetry in polar angle of the tagged strange quark. The background from primary up and down events is measured from the data, as is the analyzing power of the method for primary strange events. We measure: A_s = 0.85 +- 0.06(stat.) +- 0.07(syst.) (preliminary).']",['1999-10-15']
1281,['eng'],"['Achard, P']",['Double-tag events study with the L3 detector at $\\sqrt{s}$ = 189 GeV'],['Particle Physics - Experimental Results'],"['talk, Freiburg 1999/05/23', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'hadron, multiple production', 'quantum chromodynamics, perturbation theory', 'photon, structure function', 'model, quark parton', 'Lipatov equation', 'cross section', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907016'],"['A preliminary study of double tag events using the L3 detector at center of mass energy sqrt{s}=189 GeV has been performed. The cross-section of gamma* gamma* collisions is measured at average <Q2>=14.5 GeV2. The results are in agreement with predictions based on perturbative QCD, while the Quark Parton Model alone is insufficient to describe the data. The measurements lie below the LO and above the NLO BFKL calculations.']",['1999-07-14']
1282,['eng'],[],['New results on the $\\nu_{\\mu} \\rightarrow\\nu_{\\tau}$ oscillation search with the CHORUS detector'],['Particle Physics - Experimental Results'],"['talk, Stanford 1999/08/09', 'neutrino, oscillation', 'upper limit', 'neutrino/mu, beam', 'neutrino/tau, search for', 'neutrino/e', 'neutrino nucleon, interaction', 'charged current', 'tau-, semileptonic decay', 'nuclear emulsion, target', 'experimental results', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907015'],"['The present results on the $\\numtonut$ oscillation search by the CHORUS experiment at CERN are summarized. A fraction of the neutrino interactions collected in 1994-1997 has been analysed, searching for $\\nu_{\\tau}$ charged current interactions followed by the $\\tau$ lepton decay into a negative hadron, electron, or into a muon. A sample of 126,229 events with an identified muon in the final state and 19,436 events without an identified muon in the final state have been located in the emulsion target. Within the applied cuts, no $\\nu_{\\tau}$ candidate has been found. This result leads to a 90% C.L. limit $P(\\numtonut)< 4.0\\cdot 10^{-4}$ on the mixing probability. A $\\nuetonut$ exclusion plot is also presented corresponding to 90% C.L. limit on the mixing probability of $P(\\nuetonut)<~3.0\\cdot~10^{-2}$.']",['1999-07-14']
1283,['eng'],"['Alavi-Harati, A']",['Search for the Decay $K_{L}\\rightarrow\\pi^{0}\\nu \\overline{\\nu}$ using $\\pi^{0}\\rightarrow e^{+} e^{-}\\gamma$'],['Particle Physics - Experimental Results'],"['K0(L), secondary beam', 'K0(L), semileptonic decay', 'K0(L), rare decay', 'pi0, radiative decay', 'pi0, electromagnetic decay', 'violation, CP', 'Kobayashi-Maskawa angle, parametrization', 'K0(L), branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON Coll', 'K0(L) --> pi0 neutrino antineutrino', 'pi0 --> positron electron photon', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907014'],"['We report on a search for the decay K_L -> pi^0 nu nubar, carried out as a part of E799-II, a rare K_L decay experiment at Fermilab. Within the Standard Model, the K_L -> pi^0 nu nubar decay is dominated by direct CP violating processes, and thus an observation of the decay implies confirmation of direct CP violation. Due to theoretically clean calculations, a measurement of B(K_L -> pi^0 nu nubar) is one of the best ways to determine the CKM parameter eta. No events were observed, and we set an upper limit B(K_L -> pi^0 nu nubar) < 5.9 times 10^-7 at the 90% confidence level.']",['1999-07-14']
1284,['eng'],[],['Measurement of the $b$ Quark Fragmentation Function in $Z^{0}$ Decay'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'talk, Stanford 1999/08/09', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, fragmentation function', 'particle identification, beauty', 'beautiful particle, energy spectrum', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908032'],"['We present preliminary results of a new measurement of the inclusive b quark fragmentation function in Z0 decays using a novel kinematic B hadron energy reconstruction technique. The measurement is performed using 150,000 hadronic Z0 events recorded in the SLD experiment at SLAC between 1996 and 1997. The small and stable SLC beam spot and the CCD-based vertex detector are used to reconstruct topological B-decay vertices with high efficiency and purity, and to provide precise measurements of the kinematic quantities used in this technique. We measure the B energy with good efficiency and resolution over the full kinematic range. We compare the measured scaled B hadron energy distribution with several functional forms of the B hadron energy distribution and predictions of several models of b quark fragmentation. Several functions are excluded by the data. The average scaled energy of the weakly decaying B hadron is measured to be xB = 0.714 +/- 0.005 (stat) +/- 0.007 (syst) +/- 0.002 (model) (preliminary).']",['1999-10-15']
1285,['eng'],"['Meyer, V', 'Bagayev, S N', 'Baird, P', 'Bakule, P', 'Boshier, M G', 'Breitrück, A', 'Cornish, S L', 'Dychkov, S', 'Eaton, G H', 'Grossmann, A', 'Hübl, D', 'Hughes, V W', 'Jungmann, K', 'Lane, I C', 'Liu Yu Wei', 'Lucas, D', 'Matyugin, Y', 'Merkel, J', 'zu Putlitz, G', 'Reinhard, I', 'Sandars, P G H', 'Santra, R', 'Schmidt, P', 'Scott, C A', 'Toner, W T', 'Towrie, M', 'Träger, K', 'Willmann, L', 'Yakhontov, V']",['Measurement of the 1s-2s energy interval in muonium'],['Other Fields of Physics'],"['muonium, energy levels', 'mass ratio, (muon electron)', 'charge, ratio', 'experimental methods, laser', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907013'],['The 1s-2s interval has been measured in the muonium ({$\\mu^+e^-$}) atom by Doppler-free two-photon laser spectroscopy. The frequency separation of the states was determined to be 2 455 528 941.0(9.8)~MHz in good agreement with quantum electrodynamics. The muon-electron mass ratio can be extracted and is found to be 206.768 38(17). The result may be interpreted as measurement of the muon-electron charge ratio as $-1- 1.1(2.1)\\cdot 10^{-9}$.'],['1999-07-13']
1286,['eng'],"['Nisius, R']",['The Structure of Quasi-Real and Virtual Photons'],['Particle Physics - Experimental Results'],"['review, Freiburg 1999/05/23', 'electron positron, inelastic scattering', 'exchange, two-photon', 'photon photon, interaction', 'photon, structure function', 'quantum electrodynamics', 'quantum chromodynamics', 'momentum transfer, dependence', 'angular correlation', 'cross section', 'hadron, multiple production', 'photon, off-shell', 'Lipatov equation', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907012'],['This review covers the measurements of the QED and QCD structure of quasi-real and virtual photons from the reaction ee --> ee gamma* gamma(*) --> ee X.'],['1999-07-13']
1287,['eng'],"['Cacciari, M', 'Chlebana, F S', 'Sinclair, L', 'Weber, M']",['Progress and Problems in QCD'],['Particle Physics - Experimental Results'],"['conference, review', 'Zeuthen 1999/04/19', 'lepton nucleon, deep inelastic scattering', 'anti-p p, interaction', 'hadron, multiple production', 'quantum chromodynamics', 'Lipatov equation', 'small-x', 'quark, heavy', 'event shape analysis', 'jet, fragmentation', 'strong interaction, coupling constant', 'photon, structure function', 'photon, direct production', 'model, composite', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907011'],"['We present a summary of the Hadronic Final States parallel sessions of the DIS99 Workshop. Topics were presented over two days and included both theoretical and experimental talks. Recent progress in the understanding of QCD in deep inelastic scattering, e^+e^- collisions, and in gamma and p collisions was discussed.']",['1999-07-12']
1288,['eng'],"['Breitweg, J']",['Measurement of High-$Q^{2}$ Charged-Current $e^{+}p$ Deep Inelastic Scattering Cross Sections at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'charged current', 'momentum transfer, high', 'differential cross section, momentum transfer', 'x-dependence', 'nucleon, structure function', 'quark, sea', 'electroweak interaction, validity test', 'coupling constant', 'W, mass', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> antineutrino/e anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907010'],"['The e^+p charged-current deep inelastic scattering cross sections, $d\\sigma/dQ^2$ for Q^2 between 200 and 60000 GeV^2, and $d\\sigma/dx$ and $d\\sigma/dy$ for Q^2 > 200 GeV^2, have been measured with the ZEUS detector at HERA. A data sample of 47.7 pb^-1, collected at a center-of-mass energy of 300 GeV, has been used. The cross section $d\\sigma/dQ^2$ falls by a factor of about 50000 as Q^2 increases from 280 to 30000 GeV^2. The double differential cross section $d^2\\sigma/dxdQ^2$ has also been measured. A comparison between the data and Standard Model (SM) predictions shows that contributions from antiquarks ($\\bar{u}$ and $\\bar{c}$) and quarks (d and s) are both required by the data. The predictions of the SM give a good description of the full body of the data presented here. A comparison of the charged-current cross section $d\\sigma/dQ^2$ with the recent ZEUS results for neutral-current scattering shows that the weak and electromagnetic forces have similar strengths for Q^2 above $M^2_W, M^2_Z$. A fit to the data for $d\\sigma/dQ^2$ with the Fermi constant $G_F$ and $M_W$ as free parameters yields $G_F = (1.171 \\pm 0.034 (stat.) ^{+0.026}_{-0.032} (syst.) ^{+0.016}_{-0.015} (PDF)) \\times 10^{-5} GeV^{-2}$ and $M_W = 80.8 ^{+4.9}_{-4.5} (stat.) ^{+5.0}_{-4.3} (syst.) ^{+1.4}_{-1.3} (PDF) GeV$. Results for $M_W$, where the propagator effect alone or the SM constraint between $G_F$ and $M_W$ have been considered, are also presented.']",['1999-07-12']
1289,['eng'],"['Abbott, B']",['Measurement of the inclusive differential cross section for Z bosons as a function of transverse momentum in $\\overline{p}p$ collisions at $\\sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Z0, hadroproduction', 'Z0, leptonic decay', 'differential cross section, transverse momentum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', 'anti-p p --> Z0 anything', 'Z0 --> positron electron', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907009'],['We present a measurement of the differential cross section as a function of transverse momentum of the Z boson in ppbar collisions at sqrt{s}=1.8 TeV using data collected by the D0 experiment at the Fermilab Tevatron Collider during 1994--1996. We find good agreement between our data and the NNLO resummation prediction and extract values of the non-perturbative parameters for the resummed prediction from a fit to the differential cross section.'],['1999-07-09']
1290,['eng'],"['Baurov, Yu A', 'Sobolev, Yu G', 'Kushniruk, V F', 'Kuznetzov, A N', 'Konradov, A A']",['Experimental investigation of changes in $\\beta$-decay count rate of radioactive elements'],['Particle Physics - Experimental Results'],"['nucleus, semileptonic decay', 'radioactivity', 'cobalt', 'cesium', 'strontium', 'time variation', 'scintillation counter, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907008'],"['The experimental data on continuous investigation of changes in beta-decay count rate of Cs-137 and Co-60 from 9.12.98 till 30.04.99, are presented. The 27-day and 24-hour periods in these changes, inexplicable by traditional physics, have been found.']",['1999-07-09']
1291,['eng'],"['Murakami, K', 'Hemmi, Y', 'Kurashige, H', 'Matono, Y', 'Nomura, T', 'Sakamoto, H', 'Sasao, N', 'Suehiro, M', 'Takeuchi, Y', 'Fukushima, Y', 'Ikegami, Y', 'Nakamura, T T', 'Taniguchi, T', 'Asai, M']",['Experimental search for the decay mode $K_{L} \\to \\pi^{0} \\gamma e^{+} e^{-}$'],['Particle Physics - Experimental Results'],"['K0(L), radiative decay', 'K0(L), branching ratio', 'upper limit', 'K0(L), secondary beam', 'magnetic spectrometer, experimental results', 'KEK PS', 'K0(L) --> pi0 positron electron photon', '12 GeV/c (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907007'],['We report on results of a search for the decay mode K_L -> pi^0 gamma e^+ e^- conducted by the E162 experiment at KEK. We observed no events and set a 90% confidence level upper limit of Br(K_L -> pi^0 gamma e^+ e^-)< 7.1x10^{-7} for its branching ratio. This is the first published experimental result on this decay mode.'],['1999-07-09']
1292,['eng'],[],['Study of the $\\phi$ decays into $\\pi^{0}\\pi^{0} \\gamma$ and $\\eta\\pi^{0}\\gamma$ final states'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'pseudoscalar meson, pair production', 'eta, hadronic decay', 'eta, branching ratio', 'upper limit', 'Phi(1020), branching ratio', 'f0(975), intermediate state', 'parity, violation', 'violation, CP', 'photon, angular distribution', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> 2pi0 photon', 'Phi(1020) --> eta pi0 photon', 'eta --> 2pi0', 'approx. 10.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907006'],"['Radiative decays of the $\\phi$ meson have been studied using a data sample of about 19 million $\\phi$ decays collected by the CMD-2 detector at VEPP-2M collider in Novosibirsk. From selected $e^+e^-\\to\\pi^{0}\\pi^{0}\\gamma$ and $e^+e^-\\to\\eta\\pi^{0}\\gamma$ events the following model independent results have been obtained: \\par $Br(\\phi\\to\\pi^{0}\\pi^{0}\\gamma) = (0.92\\pm 0.08\\pm0.06)\\times10^{-4}$ for $M_{\\pi^{0}\\pi^{0}}>700$ MeV, \\par $Br(\\phi\\to\\eta\\pi^{0}\\gamma) = (0.90\\pm 0.24\\pm 0.10)\\times10^{-4}$. It is shown that the intermediate mechanism $f_{0}(980)\\gamma$ dominates in the $\\phi\\to\\pi^{0}\\pi^{0}\\gamma$ decay and the corresponding branching ratio is \\par $Br(\\phi\\to f_{0}(980)\\gamma)=(2.90\\pm 0.21\\pm1.54)\\times10^{-4}$. The systematic error is dominated by the possible model uncertainty. \\par Using the same data sample the upper limit has been obtained for the P- and CP-violating decay of $\\eta$ at 90% CL: \\par $Br(\\eta\\to\\pi^{0}\\pi^{0}) < 4.3\\times10^{-4}$ >.']",['1999-07-08']
1293,['eng'],[],['First observation of the $\\phi\\rightarrow \\pi^{+} \\pi^{-}\\gamma$ decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'pi, pair production', 'f0(975)', 'rho(770)', 'eta', 'Phi(1020), branching ratio', 'upper limit', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> pi+ pi- photon', 'Phi(1020) --> muon+ muon- photon', 'Phi(1020) --> rho(770) photon', 'Phi(1020) --> f0(975) photon', 'Phi(1020) --> eta photon', 'approx. 10.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907005'],"['Radiative decays of the $\\phi$ meson have been studied using a data sample of about 20 million $\\phi$ decays collected by the CMD-2 detector at VEPP-2M collider in Novosibirsk. From selected $e^+e^-\\to\\pi^{+}\\pi^{-}\\gamma$ events the $\\phi\\to\\pi^{+}\\pi^{-}\\gamma$ decay has been observed for the first time. dominates in the $\\phi \\to \\pi^+\\pi^-\\gamma$ decay, the corresponding branching ratio is $Br(\\phi\\to f_{0}(980)\\gamma)=(1.93\\pm 0.46\\pm 0.50)\\times10^{-4}$. $Br(\\phi\\to\\mu^+\\mu^-\\gamma) =(1.43\\pm 0.45\\pm 0.14)\\times10^{-5}$ for $E_{\\gamma}>20$ MeV. \\par Using the same data sample, upper limits at 90% CL have been obtained for the C-violating decay of the $\\phi$: $Br(\\phi\\to\\rho\\gamma) < 1.2\\times10^{-5}$; and for the P- and CP-violating decay of the $\\eta$: \\par $Br(\\eta\\to\\pi^+\\pi^-) < 3.3\\times10^{-4}$.']",['1999-07-08']
1294,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Koop, I A', 'Korol, A A', 'Koshuba, S V', 'Nesterenko, I N', 'Pakhtusova, E V', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Usov, Yu V']",['Upper limit on the $K_{S} \\rightarrow 3\\pi^{0}$ decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'K0(S), pair production', 'K0(S), hadronic decay', 'K0(S), branching ratio', 'upper limit', 'final state, (3pi0)', 'pi0, radiative decay', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'K0(S) --> 3pi0', 'approx. 10.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907004'],"['The search for CP-violating K_S\\to3\\pi^0 decay was performed with SND detector at VEPP-2M e^+e^- collider. The total amount of data corresponding to 7 million produced K_S mesons was analyzed. No candidate events were found, giving an upper limit of the decay branching ratio: Br(K_S\\to3\\pi^0) < 1.4\\cdot10^{-5} at 90% confidence level.']",['1999-07-08']
1295,['eng'],[],['Study of the radiative decay $\\phi \\rightarrow \\eta \\gamma$ with CMD-2 detector'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'eta, hadronic decay', 'Phi(1020), branching ratio', 'Phi(1020), mass', 'photon, angular distribution', 'channel cross section, energy dependence', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> eta photon', 'eta --> pi+ pi- pi0', 'approx. 10.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907003'],"['Using the $1.9 pb^{-1}$ of data collected with the CMD-2 detector at VEPP-2M the decay mode $\\phi \\to \\eta \\gamma$, $\\eta \\to \\pi^+\\pi^-\\pi^0$ has been studied. The obtained branching ratio is B($\\phi \\to \\eta \\gamma) = (1.18 \\pm 0.03 \\pm 0.06) %$.']",['1999-07-07']
1296,['eng'],"['Adloff, C']",['A Search for Leptoquark Bosons and Lepton Flavor Violation in $e^{+} p$ Collisions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'leptoquark, search for', 'leptoquark, decay', 'leptoquark, mass', 'violation, flavor', 'neutral current', 'charged current', 'momentum transfer, spectra', 'coupling, Yukawa', 'mass, dependence', 'muon, transverse momentum', 'tau, transverse momentum', 'transverse momentum, high', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907002'],"['A search for new bosons possessing couplings to lepton-quark pairs is performed in the H1 experiment at HERA using 1994 to 1997 data corresponding to an integrated luminosity of 37pb^-1. First generation leptoquarks (LQs) are searched in very high Q^2 neutral (NC) and charged (CC) current data samples. The measurements are compared to Standard Model (SM) expectations from deep-inelastic scattering (DIS). A deviation in the Q^2 spectrum previously observed in the 1994 to 1996 dataset at Q^2 \\gsim 15000GeV^2 remains, though with less significance. This deviation corresponded to a clustering in the invariant mass spectrum at M \\simeq 200 GeV which is not observed with the 1997 dataset alone. The NC DIS data is used to constrain the Yukawa couplings lambda of first generation scalar and vector LQs in the Buchmueller-Rueckl-Wyler effective model. Scalar LQs are excluded for masses up to 275GeV for a coupling of electromagnetic strength, lambda=0.3. A sensitivity to coupling values \\lsim 1 is established for masses up to 400GeV for any LQ type. The NC and CC DIS data are combined to constrain lambda for arbitrary branching ratios of the LQ into eq in a generic model. For a decay branching ratio into e^+ u pairs as small as 10%, LQ masses up to 260 GeV are ruled out for lambda=0.3. LQs possessing couplings to mixed fermion generations, which could lead to signals of lepton flavor violation (LFV), are searched in events with a high transverse momentum mu or tau. No mu+X or tau+X event candidate is found that is compatible with LQ kinematics. Constraints are set on the Yukawa coupling involving the mu and tau lepton in a yet unexplored mass range.']",['1999-07-05']
1297,['eng'],"['Migliore, E']",['Heavy quark asymmetries with DELPHI'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, charm', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'angular distribution, asymmetry', 'Weinberg angle', 'jet, charge', 'lepton, charge', 'charge, correlation', 'D, particle identification', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907001'],['The measurements of the forward-backward asymmetry in Z -> c cbar and Z -> b bbar decays are among the most precise determinations of sin^2(theta)_W. In this paper the results obtained by the DELPHI experiment at LEP with three different analyses are reviewed together with the impact of the combined LEP result on the global Electroweak fit.'],['1999-07-02']
1298,['eng'],"['Aitala, E M']","['Search for Rare and Forbidden Dilepton Decays of the $D^{+}, D^{+}_{s}$ and $D^{0}$ Charmed Mesons']",['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'charmed meson, hadroproduction', 'charmed meson, rare decay', 'final state, dilepton', 'D+, semileptonic decay', 'D/s+, semileptonic decay', 'D0, leptonic decay', 'charmed meson, branching ratio', 'upper limit', 'neutral current, flavor changing', 'violation, flavor', 'lepton number, violation', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906045'],"['We report the results of a search for flavor-changing neutral current, lepton-flavor violating, and lepton-number violating decays of D+, Ds, and D0 mesons (and their antiparticles) into modes containing muons and electrons. Using data from Fermilab charm hadroproduction experiment E791, we examine the pi,l,l and K,l,l decay modes of D+ and Ds and the l+l- decay modes of D0. No evidence for any of these decays is found. Therefore, we present branching-fraction upper limits at 90% confidence level for the 24 decay modes examined. Eight of these modes have no previously reported limits, and fourteen are reported with significant improvements over previously published results.']",['1999-07-01']
1299,['eng'],"['Baudis, L', 'Klapdor-Kleingrothaus, H V']",['Detection of low energy solar neutrinos with HPGermanium'],['Detectors and Experimental Techniques'],"['neutrino, solar', 'neutrino, energy spectrum', 'neutrino electron, elastic scattering', 'germanium', 'background', 'deep underground detector, Gran Sasso']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906044'],"['The potential of the GENIUS proposal to measure the spectrum of low energy solar neutrinos in real time is studied. The detection reaction is elastic neutrino-electron scattering. The energy resolution for detecting the recoil electrons is about 0.3 %, the energy threshold is a few keV. The expected number of events for a target of one ton of natural germanium is 3.6 events/day for pp-neutrinos and 1.3 events/day for 7Be-neutrinos, calculated in the standard solar model (BP98). It should be feasible to achieve a background low enough to measure the low energy solar neutrino spectrum.']",['1999-07-01']
1300,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['A Study of Spin Alignment of $\\rho(770)^{\\pm}$ and $\\omega(782)$ Mesons in Hadronic $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'vector meson, production', 'rho(770), hadronic decay', 'omega(783), hadronic decay', 'spin, alignment', 'helicity, density matrix', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'Z0 --> vector meson anything', 'rho(770) --> pi pi0', 'omega(783) --> pi+ pi- pi0', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906043'],"['The helicity density matrix elements rho[00] of rho(770)+- and omega(782) mesons produced in Z decays have been measured using the OPAL detector at LEP. Over the measured meson energy range, the values are compatible with 1/3, corresponding to a statistical mix of helicity -1, 0 and +1 states. For the highest accessible scaled energy range 0.3 < x_E < 0.6, the measured rho[00] values of the rho(770)+- and the omega are 0.373 +- 0.052 and 0.142 +- 0.114, respectively. These results are compared to measurements of other vector mesons.']",['1999-07-01']
1301,['eng'],"['Yang, U K']",['A Measurement of $xF_{3}^{\\nu}- xF_{3}^{\\overline{\\nu}}$ and R with the CCFR Detector'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'neutrino nucleon, interaction', 'antineutrino nucleon, interaction', 'nucleon, structure function', 'structure function, longitudinal', 'structure function, transverse', 'structure function, ratio', 'differential cross section', 'nucleon, charm', 'nucleon, strangeness', 'quark, sea', 'quark, massive', 'quantum chromodynamics, perturbation theory', 'momentum transfer, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906042'],['We report on a measurement of the neutrino-nucleon and antineutrino-nucleon differential cross sections in the CCFR detector. The measurement of the differential cross sections over a wide range of energies allows Delta xF_3 = xF_3(nu)-xF_3(anti-nu) and R to be extracted. Delta xF_3 is related to the difference between the contributions of the strange and charm seas in the nucleon to production of massive charm quark. The results for Delta xF_3 are compared to various massive charm NLO QCD models. The Q^2 dependence of R for x<0.1 has been measured for the first time.'],['1999-06-30']
1302,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Measurements of inclusive semileptonic branching fractions of b hadrons in $Z^{0}$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'beautiful particle, semileptonic decay', 'beautiful particle, branching ratio', 'quark, fragmentation function', 'model, fragmentation', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906041'],"['A measurement of inclusive semileptonic branching fractions of b hadrons produced in Z decays is presented. An enriched Z -> bbbar sample is obtained with a lifetime flavour-tagging technique. The leptonic events are then selected from this sample, and classified according to their origin, which is determined by comparing the distribution of several kinematic variables using artificial neural network techniques. Using 3.6 million multihadronic events collected with the OPAL detector at energies near the Z resonance, the values BR(b->lX) =(10.83 +- 0.10(stat.) +- 0.20(syst.) +0.20 -0.13(model)) % BR(b->c->lX) = (8.40 +- 0.16(stat.) +- 0.21(syst.) +0.33 -0.29 (model)) % are measured, where b denotes all weakly decaying b hadrons and l represents either e or mu. The second error includes all experimental systematic uncertainties whereas the last error is due to uncertainties in modelling of the lepton momentum spectrum in semileptonic decays and b quark fragmentation. The average fraction of the beam energy carried by the weakly decaying b hadron, xe, is measured to be <xe> = 0.709 +- 0.003(stat.) +- 0.003 (syst.) +- 0.013(model) where the modelling error is dominated by the choice of b fragmentation model. The agreement between data and various semileptonic decay models and fragmentation functions is also investigated.']",['1999-06-30']
1303,['eng'],"['Glasman, C']",['Inclusive hard processes in photon-photon and photon-proton interactions'],['Particle Physics - Experimental Results'],"['review, Freiburg 1999/05/23', 'photon photon, inclusive reaction', 'photon p, inclusive reaction', 'jet, photoproduction', 'photon, direct production', 'photon, structure function', 'photon, off-shell', 'hadron, photoproduction', 'transverse momentum, high', 'quark, charm', 'quark, pair production', 'quantum chromodynamics, perturbation theory', 'correction, higher-order', 'event shape analysis', 'transverse energy, energy flow', 'experimental results', 'CERN LEP Stor', 'DESY HERA Stor', 'bibliography', '((5)) ((6))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906040'],"['Measurements of jet, prompt photon, high-pT hadron and heavy quark production in photon-induced processes provide tests of QCD and are sensitive to the photon parton densities. A review of the latest experimental results in photon-photon and photon-proton interactions is presented. Next-to-leading-order QCD calculations for these measurements are discussed.']",['1999-06-29']
1304,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barillari, T', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Total Hadronic Cross-Section of Photon-Photon Interactions at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'hadron, photoproduction', 'charged particle, multiplicity', 'cross section, energy dependence', 'factorization', 'Regge poles', 'photon p, interaction', 'p p, interaction', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161, 172, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906039'],"['The total hadronic cross-section sigma_gg(W) for the interaction of real photons, gg->hadrons, is measured for gg centre-of-mass energies 10<W<110 GeV. The cross-section is extracted from a measurement of the process e+e- -> e+e-g*g* -> e+e- hardrons, using a luminosity function for the photon flux together with form factors for extrapolating to real photons (Q^2=0 GeV^2). The data were taken with the OPAL detector at LEP at e+e- centre-of-mass energies 161, 172 and 183 GeV. The cross-section sigma_gg(W) is compared with Regge factorisation and with the energy dependence observed in gp and pp interactions. The data are also compared to models which predict a faster rise of sigma_gg(W) compared to gp and pp interactions due to additional hard gg interactions not present in hadronic collisions.']",['1999-06-29']
1305,['eng'],"['Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Frey, R', 'Formaggio, J A', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Koutsoliotas, S', 'Kim, J H', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McNulty, C', 'McFarland, K S', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Tamminga, B', 'Vakili, M', 'Vaitaitis, A G', 'Wu, V', 'Yang, U K', 'Yu, J', 'Zeller, G P']",['Strange Content of the Nucleon (NuTeV)'],['Particle Physics - Experimental Results'],"['talk, Bloomington 1999/04/08', 'neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'neutrino/mu', 'nucleon, structure function', 'nucleon, strangeness', 'nucleon, charm', 'quark, sea', 'charged current', 'neutral current', 'production, charm', 'muon, charge', 'final state, dimuon', 'quark, momentum spectrum', 'asymmetry', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'neutrino nucleon --> charm anything', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906038'],['The NuTeV experiment uses neutrino deep-inelastic scattering from separate neutrino and anti-neutrino beams to study the structure of the nucleon. Charged-current production of charm is sensitive to the strange content of the nucleon while neutral-current charm production probes the charm content. Preliminary analyses of both topics are presented along with discussion of possible momentum asymmetry in the strange sea.'],['1999-06-29']
1306,['eng'],"['Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Frey, R', 'Formaggio, J A', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Koutsoliotas, S', 'Kim, J H', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McNulty, C', 'McFarland, K S', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Tamminga, B', 'Vakili, M', 'Vaitaitis, A G', 'Wu, V', 'Yang, U K', 'Yu, J', 'Zeller, G P']",['Charm Production at NuTeV'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/20', 'neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'neutrino/mu', 'charged current', 'neutral current', 'production, charm', 'nucleon, structure function', 'nucleon, charm', 'nucleon, strangeness', 'quark, sea', 'muon, charge', 'final state, dimuon', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'neutrino nucleon --> charm anything', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906037'],['Neutrino deep-inelastic scattering provides a means to study both the strange and charm content of the nucleon. The NuTeV experiment (Fermilab E-8Neutrino deep-inelastic scattering provides a means to study both the strange and charm content of the nucleon. The NuTeV experiment (Fermilab E-815) takes full advantage of separated neutrino and anti-neutrino beams to probe the nucleon. The strange sea is studied with charged-current charm production resulting in an opposite-signed two muon final state. The charm content of the nucleon is probed via neutral-current charm production creating an event with a single wrong-signed muon. Preliminary results are presented for both analyses.'],['1999-06-29']
1307,['eng'],"['Saeki, T']",['W mass measurement at LEP'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/20', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, leptonic decay', 'W, hadronic decay', 'W, mass', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906036'],"['In 1998, the four experiments of LEP, i.e. ALEPH, DELPHI, L3 and OPAL, collected data of about 175 /pb per experiment at the center-of-mass energy of 189 GeV. Using these data, the mass of W boson was directly measured by reconstructing the decay products of two W bosons from the e+e- collisions. The W mass measurement was combined personally with the results obtained from data at 161, 172, and 183 GeV. This yielded the private LEP2 average of Mw = 80.350 +/- 0.056 GeV.']",['1999-06-25']
1308,['eng'],"['Ackerstaff, K']",['Flavor Decomposition of the Polarized Quark Distributions in the Nucleon from Inclusive and Semi-inclusive Deep-inelastic Scattering'],['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'p nucleus, inclusive reaction', 'helium, nuclide', 'p, polarized beam', 'polarized target, longitudinal', 'charged particle, hadroproduction', 'hadron, multiple production', 'cross section, x-dependence', 'momentum transfer, dependence', 'spin, asymmetry', 'nucleon, structure function', 'quark, polarization', 'quark, valence', 'quark, sea', 'quark, momentum spectrum', 'moment', 'sum rule, Bjorken', 'symmetry, SU(3)', 'symmetry, flavor', 'quantum chromodynamics', 'lattice field theory', 'magnetic detector, HERMES', 'experimental results', 'DESY HERA Stor', 'bibliography', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906035'],"['Spin asymmetries of semi-inclusive cross sections for the production of positively and negatively charged hadrons have been measured in deep-inelastic scattering of polarized positrons on polarized hydrogen and 3He targets, in the kinematic range 0.023<x<0.6 and 1 GeV^2<Q^2<10 GeV^2. Polarized quark distributions are extracted as a function of x for up $(u+u_bar) and down (d+d_bar) flavors. The up quark polarization is positive and the down quark polarization is negative in the measured range. The polarization of the sea is compatible with zero. The first moments of the polarized quark distributions are presented. The isospin non-singlet combination Delta_q_3 is consistent with the prediction based on the Bjorken sum rule. The moments of the polarized quark distributions are compared to predictions based on SU(3)_f flavor symmetry and to a prediction from lattice QCD.']",['1999-06-25']
1309,['eng'],"['Aitala, E M']",['Total Forward and Differential Cross Sections of Neutral D Mesons Produced in 500 GeV/c $\\pi^{-}$-Nucleon Interactions'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D0, hadroproduction', 'production, small-angle', 'D0, hadronic decay', 'mass spectrum, (K (n)pi)', 'channel cross section', 'differential cross section, x-dependence', 'transverse momentum, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON Coll', 'pi- nucleon --> D0 anything', 'D0 --> K pi', 'D0 --> K 3pi', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906034'],"['We measure the neutral D total forward cross section and the differential cross sections as function of Feynman-x ($x_F$) and transverse momentum squared for 500 GeV/c $\\pi^-$-nucleon interactions. The results are obtained from 88990+-460 reconstructed neutral D mesons from Fermilab experiment E791 using the decay channels $D\\to K^-\\pi^+$ and $D\\to K^-\\pi^+\\pi^-\\pi^+$ (and charge conjugates). We extract fit parameters from the differential cross sections and provide the first direct measurement of the turnover point in the $x_F$ distribution, 0.0131+-0.0038. We measure an absolute $D^0 + \\bar{D^0}$ ($x_F > 0$) cross section of 15.4+1.8-2.3 microbarns/nucleon (assuming a linear A dependence). The differential and total forward cross sections are compared to theoretical predictions and to results of previous experiments.']",['1999-06-24']
1310,['eng'],"['Movilla-Fernández, P A', 'Biebel, O', 'Bethke, Siegfried']",['Tests of Power Corrections to Event Shape Distributions from $e^{+}e^{-}$ Annihilation'],['Particle Physics - Experimental Results'],"['talk, Tampere 1999/07/15', 'review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'jet, electroproduction', 'event shape analysis', 'quantum chromodynamics, perturbation theory', 'effect, nonperturbative', 'correction', 'strong interaction, coupling constant', 'bibliography', '35-183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906033'],"['A study of differential event shape distributions using e+e- data at centre-of-mass energies of 35 to 183 GeV is presented. We investigated non-perturbative power corrections for the thrust, C-parameter, total and wide jet broadening observables. We observe a good description of the distributions by the combined resummed QCD calculations plus power corrections from the dispersive approach. The single non-perturbative parameter \\alpha_0 is measured to be \\alpha_0 (2 GeV) = 0.502 +- 0.013 (stat.) ^{+0.046)_{-0.032} (exp. syst.) ^{+0.074}_{-0.053} (theo. syst.) and is found to be universal for the observables studied within the given systematic uncertainties. Using revised calculations of the power corrections for the jet broadening variables, improved consistency of the individual fit results is obtained. Agreement is also found with results extracted from the mean values of event shape distributions.']",['1999-06-24']
1311,['eng'],[],['Measurement of the $\\phi$ meson parameters with CMD-2 detector at VEPP-2M Collider'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), hadronic decay', 'Phi(1020), mass', 'K0, pair production', 'K0(L)', 'K0(S)', 'width, branching ratio', 'channel cross section', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> K0(L) K0(S)', '0.984-1.040 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906032'],['About 300 000 $e^+e^-\\to \\phi\\to K^0_L K^0_S$ events in the center of mass energy range from 984 to 1040 MeV were used for the measurement of the $\\phi$ meson parameters. The following results have been obtained: $\\sigma_0 = (1367 K^0_L K^0_S) = (4.364 \\pm 0.048 \\pm 0.065)\\cdot 10^{-4}$ MeV.'],['1999-06-24']
1312,['eng'],"['Hapke, M']",['QCD at LEP 2 and WW Final State Interactions'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'final-state interaction', 'charged particle, multiplicity', 'event shape analysis', 'color, recombination', 'correlation function, two-particle', 'boson, statistics', 'quantum chromodynamics', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', 'W --> quark antiquark', '133-189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906031'],['A short overview of the QCD program at LEP~2 is given. Studies of final state interactions in e+e- -> WW -> qqqq decays are discussed.'],['1999-06-24']
1313,['eng'],"['Warburton, A']",['CKM Physics from B Decays using the CLEO Experiment'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'B, hadronic decay', 'Kobayashi-Maskawa angle', 'HQET model', 'parametrization', 'mass, recoil', 'lepton, energy spectrum', 'moment', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'beauty --> charm lepton neutrino', 'beauty --> up lepton neutrino', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906030'],"['We report on studies of three types of B-meson decay that can contribute to an understanding of fundamental intergenerational quark mixing, charge-conjugation--parity violation, and long-distance quantum chromodynamics. Specifically, we discuss a selection of analyses related to the Cabibbo-Kobayashi-Maskawa (CKM) parameters Vcb, Vub, alpha, and gamma, and the nonperturbative heavy quark effective theory quantities lambda_1 and lambda_bar. We first describe an examination of the first and second moments of the hadronic-recoil mass and charged-lepton energy spectra in inclusive b -> c l nu decays. We also report on the reconstruction, using similar experimental techniques, of the CKM-suppressed decay B -> rho l nu and the extraction of its branching fraction, Br(B0 -> rho- l+ nu) = (2.57 +- 0.29 +0.33/-0.46 +- 0.41) x 10E-4, as well as the value |Vub| = (3.25 +- 0.14 +0.21/-0.29 +- 0.55) x 10E-3, where the uncertainties are statistical, systematic, and due to model dependence, respectively. Finally, we present results on rare two-body charmless hadronic B -> K pi, pi pi, and K K decays and comment briefly on their implications to the geometry of the CKM unitarity triangle, including a bound on gamma.']",['1999-06-21']
1314,['eng'],"['Kabuss, E M']",['Future Polarised DIS Fixed Target Experiments'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'lepton nucleon, deep inelastic scattering', 'lepton nucleon, inclusive reaction', 'nucleon, polarized target', 'lepton, polarized beam', 'charmed particle, hadroproduction', 'quark, charm', 'quark, pair production', 'hadron, pair production', 'transverse momentum, high', 'polarization, asymmetry', 'helicity', 'flavor', 'polarization, transverse', 'structure function, spin', 'gluon, polarization', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906028'],"['New experiments in polarised deep inelastic scattering will mainly concentrate on the measurement of semi-inclusive asymmetries. Especially, the upgraded HERMES experiment at DESY and the newly built COMPASS experiment at CERN will investigate the gluon polarisation via open charm and high p_T hadron pair production, study in detail the flavour decomposition of the quark helicity distributions and measure the tranversity distributions with tranversely polarised targets.']",['1999-06-17']
1315,['eng'],"['Bassler, U', 'Laenen, E', 'Quadt, A', 'Schellman, H']","[""Summary of the Structure Function Working Group at DIS '99""]",['Particle Physics - Experimental Results'],"['review, Zeuthen 1999/04/19', 'lepton nucleon, deep inelastic scattering', 'hadron hadron, interaction', 'nucleon, structure function', 'momentum spectrum, parton', 'quark, sea', 'asymmetry, (up down)', 'momentum transfer, dependence', 'x-dependence', 'gluon', 'differential cross section', 'photon, direct production', 'pi0, direct production', 'structure function, charm', 'quantum chromodynamics, perturbation theory', 'Lipatov equation', 'unitarity', 'lattice field theory', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906027'],"[""We summarize the experimental and theoretical results presented in the ``Structure Function Working Group - WG1'' at DIS'99.""]",['1999-06-17']
1316,['eng'],"['Brooks, T C', 'Convery, M E', 'Davis, W L', 'Signore, K W D', 'Jenkins, T L', 'Kangas, E', 'Knepley, M G', 'Kowalski, K L', 'Taylor, C C', 'Oh, S H', 'Walker, W D', 'Colestock, P L', 'Hanna, B', 'Martens, M', 'Streets, J', 'Ball, R C', 'Gustafson, H R', 'Jones, L W', 'Longo, M J', 'Bjorken, James D', 'Abashian, A', 'Morgan, N', 'Pruneau, C A']",['A Search for Disoriented Chiral Condensate at the Fermilab Tevatron'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'pi, multiple production', 'production, small-angle', 'condensation, chiral', 'search for, condensation', 'charged particle, multiplicity', 'photon, multiplicity', 'correlation', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906026'],"['We present results from MiniMax (Fermilab T-864), a small test/experiment at the Tevatron designed to search for the production of disoriented chiral condensate (DCC) in $p - \\bar p$ collisions at $\\sqrt{s} = 1.8$ TeV in the forward direction, $\\sim 3.4 < \\eta < \\sim 4.2$. Data, consisting of $1.3 earlier paper. The results are consistent with generic, binomial-distribution partition of pions into charged and neutral species. Limits on DCC production in various models are presented.']",['1999-06-16']
1317,['eng'],"['Zeller, G P', 'Adams, T', 'Alton, A', 'Avvakumov, S', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Formaggio, J A', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Koutsoliotas, S', 'Kim, J H', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McNulty, C', 'McFarland, K S', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Tamminga, B', 'Vakili, M', 'Vaitaitis, A G', 'Yang, U K']",['A Measurement of the Weak Mixing Angle in Neutrino-Nucleon Scattering at NuTeV'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'neutrino nucleon, interaction', 'antineutrino nucleon, interaction', 'charged current', 'neutral current', 'Weinberg angle', 'W, mass', 'scintillation counter, target', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906024'],"['The NuTeV experiment at Fermilab presents a determination of the electroweak mixing angle. High purity, large statistics samples of muon-neutrino and muon-antineutrino events allow the use of the Paschos-Wolfenstein relation. This considerably reduces systematic errors associated with charm production and other sources. With Standard Model assumptions, this measurement of sin2thw indirectly determines the W boson mass to a precision comparable to direct measurements from high energy e+e- and p-pbar colliders. NuTeV measures sin^2theta_W (on-shell) = 0.2253 +/- 0.0019(stat) +/- 0.0010(syst) which implies M_W = 80.26 +/- 0.11 GeV.']",['1999-06-15']
1318,['eng'],"['Pripstein, D A', 'Brown, C N', 'Carey, T A', 'Chen, Y C', 'Childers, R L', 'Cooper, W E', 'Darden, C W', 'Gidal, G', 'Gounder, K N', 'Ho, P M', 'Isenhower, L D', 'Jansen, D M', 'Jeppesen, R G', 'Kaplan, D M', 'Kapustinsky, J S', 'Kiang, G C', 'Kowitt, M S', 'Lane, D W', 'Lederman, L M', 'Leitch, M J', 'Lillberg, J W', 'Luebke, W R', 'Luk, K B', 'McGaughey, P L', 'Mishra, C S', 'Moss, J M', 'Peng, J C', 'Preston, R S', 'Sá, J', 'Sadler, M E', 'Schnathorst, R G', 'Schub, M H', 'Tanikella, V', 'Teng, P K', 'Wilson, J R']",['Search for Flavor-Changing Neutral Currents and Lepton-Family-Number Violation in Two-Body $D^{0}$ Decays'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'gold', 'beryllium', 'D0, hadroproduction', 'D0, leptonic decay', 'D0, branching ratio', 'upper limit', 'neutral current, flavor changing', 'violation, flavor', 'mass spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> muon electron', 'D0 --> positron electron', 'D0 --> muon+ muon-', '800 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906022'],"['Results of a search for the three neutral charm decays, D0 -> mu e, D0 -> mu mu, and D0 -> e e, are presented. This study was based on data collected in Experiment 789 at the Fermi National Accelerator Laboratory using 800 GeV/c proton-Au and proton-Be interactions. No evidence is found for any of the decays. Upper limits on the branching ratios, at the 90% confidence level, are obtained.']",['1999-06-15']
1319,['eng'],[],['Upper Limit on the Prompt Muon Flux Derived from the LVD Underground Experiment'],['Particle Physics - Experimental Results'],"['cosmic radiation, nuclear reaction', 'charmed particle, decay', 'muon, multiplicity', 'muon, direct production', 'hadron, decay', 'muon, flux', 'upper limit', 'angular distribution', 'spatial distribution', 'muon, energy spectrum', 'parametrization', 'pi, flux', 'flux, ratio', 'deep underground detector, Gran Sasso', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906021'],"['We present the analysis of the muon events with all muon multiplicities collected during 21804 hours of operation of the first LVD tower. The measured depth-angular distribution of muon intensities has been used to obtain the normalization factor, A, the power index, gamma, of the primary all-nucleon spectrum and the ratio, R_c, of prompt muon flux to that of pi-mesons - the main parameters which determine the spectrum of cosmic ray muons at the sea level. The value of gamma = 2.77 +/- 0.05 (68% C.L.) and R_c < 2.0 x 10^-3 (95% C.L.) have been obtained. The upper limit to the prompt muon flux favours the models of charm production based on QGSM and the dual parton model.']",['1999-06-14']
1320,['eng'],"['Elvira, V D']",['Inclusive Jet Cross Sections in $\\overline{p}p$ Collisions at $\\sqrt{s}$ = 630 and 1800 GeV'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'cross section, transverse energy', 'rapidity dependence', 'energy dependence', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> jet anything', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906020'],"['We have made a precise measurement of the inclusive jet cross section at 1800 GeV. The result is based on an integrated luminosity of 92 pb**-1 collected at the Fermilab Tevatron pbarp Collider with the DO detector. The measurement is reported as a function of jet transverse energy (60 GeV < ET < 500 GeV), and in the pseudorapidity intervals |eta|<0.5 and 0.1<eta<0.7. A preliminary measurement of the pseudorapidity dependence of inclusive jet production (eta<1.5) is also discussed. The results are in good agreement with predictions from next-to-leading order (NLO) quantum chromodynamics (QCD). DØ has also determined the ratio of jet cross sections at $\\sqrt{s}$=630 GeV and from NLO QCD predictions.']",['1999-06-11']
1321,['eng'],"['Bernardini, P']",['Measurement of the Atmospheric Muon Neutrinos with the MACRO Detector'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1999/02/28', 'neutrino/mu, cosmic radiation', 'cosmic radiation, flux', 'neutrino nucleon, interaction', 'charged current', 'muon, angular distribution', 'neutrino, oscillation', 'neutrino/tau', 'neutrino, mixing angle', 'neutrino, mass difference', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906019'],"['The flux of muons induced by atmospheric neutrinos has been measured with the MACRO detector. Different event topologies have been detected, due to neutrino interactions in the apparatus and in the rock below it. The upward-throughgoing muon sample is the larger one and is generated by neutrinos with a peak energy of ~100 GeV. The observed upward-throughgoing muons are 26 % fewer than expected and the zenith angle distribution does not fit with the expected one. Assuming \\mutau neutrino oscillation, the angular shape and the normalization factor suggest maximal mixing and \\Delta m^2 of a few times 10^{-3} eV^2. Also the other event categories induced by low-energy neutrinos (peak energy ~ 4 GeV) show a deficit of observed events. The value of this deficit and its uniformity with respect to the angular bins are in agreement with the oscillation parameters suggested by the analysis of the upward-throughgoing muon sample.']",['1999-06-11']
1322,['eng'],"['Meyer, P O']",['Internal Jet Structure in Dijet Production in Deep-Inelastic Scattering'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, pair production', 'jet, event shape analysis', 'multiplicity', 'quantum chromodynamics', 'kinematics, Breit frame', 'transverse energy, dependence', 'rapidity dependence', 'photon photon, interaction', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906018'],"['The internal jet structure in dijet production in deep-inelastic scattering is measured with the H1 detector at HERA. Jets with transverse energies E(T,breit) > 5 GeV are selected in the Breit frame employing kt and cone jet algorithms in the kinematic region of squared momentum transfers of 10 < Q^2 < 120 GeV^2 and x-Bjorken values of 0.0002 < x < 0.008. Jet shapes and subjet multiplicities are measured as functions of a resolution parameter. The corrected data are well described by QCD models. It is observed that jets are more collimated with increasing transverse jet energies and decreasing pseudo-rapidities, i.e. towards the photon direction. Comparisons with OPAL data show that jet shapes of jets measured in photon-photon collisions are very similar to those measured in ep collisions.']",['1999-06-11']
1323,['eng'],"['Mari, S M']",['Performance of RPCs operated at the YangBaJing Laboratory'],['Detectors and Experimental Techniques'],"['talk, Salt Lake City 1999/08/17', 'photon, cosmic radiation', 'drift chamber', 'electrode, impedance', 'efficiency', 'time resolution']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906017', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h6_1_17.pdf']","['The ARGO-YBJ experiment will be installed at YangBaJing Cosmic Ray Laboratory (Tibet, P.R. China), 4300 m a.s.l. . It consists of a full coverage of about 10^4 m^2 realized with RPC chambers. A small carpet of about 50 m^2 has been operated at YangBaJing in order to check the RPC performance in these high altitude conditions. Results concerning efficiency and time resolution are reported.']",['1999-06-11']
1324,['eng'],"['Gerber, C E']",['Recent Results from the Tevatron Fixed Target and Collider Experiments'],['Particle Physics - Experimental Results'],"['review, Zeuthen 1999/04/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'p nucleon, inclusive reaction', 'jet, hadroproduction', 'final state, (2jet)', 'diffraction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'differential cross section, transverse momentum', 'photon, hadroproduction', 'muon, associated production', 'muon, pair production', 'Drell-Yan process', 'W, mass', 'mass, truth', 'quark, beauty', 'quark, pair production', 'B0, hadronic decay', 'K0, hadronic decay', 'violation, CP', 'experimental results', 'Batavia TEVATRON Coll', 'Batavia TEVATRON PS', '800 GeV, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906016'],"['We present a review of recent QCD related results from the Fermilab Tevatron fixed target and collider experiments. Topics include jet and boson production, W boson and top quark mass measurements, and studies of CP violation.']",['1999-06-10']
1325,['eng'],"['Athanas, M']",['Limit on $\\tau$ Neutrino Mass from $\\tau ^{-}\\rightarrow \\pi^{-}\\pi^{+}\\pi^{-} \\pi^{0}\\nu_{\\tau}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'neutrino/tau, mass', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> tau+ tau-', 'tau- --> pi+ 2pi- pi0 neutrino/tau', '10.52, 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906015'],['From a data sample of 29058 $\\tau^\\pm\\to\\pi^\\pm\\pi^+\\pi^-\\pi^0\\nu_\\tau$ decays observed in the CLEO detector we derive a 95% confidence upper limit on the tau neutrino mass of 28 MeV.'],['1999-06-10']
1326,['eng'],"['Söldner-Rembold, S']",['Jet and hadron production in photon-photon collisions'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'jet, hadroproduction', 'final state, (2jet)', 'charged particle, multiple production', 'differential cross section, transverse energy', 'photon, direct production', 'quantum chromodynamics, perturbation theory', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161-172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906014'],"['Di-jet and inclusive charged hadron production cross-sections measured in photon-photon collisions by OPAL are compared to NLO pQCD calculations. Jet shapes measured in photon-photon scattering by OPAL, in deep-inelastic ep scattering by H1 and in photon-proton scattering by ZEUS are shown to be consistent in similar kinematic ranges. New results from TOPAZ on prompt photon production in photon-photon interactions are presented.']",['1999-06-10']
1327,['eng'],"['Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Boisvert, V', 'Cassel, David G', 'Crowcroft, D S', 'Dickson, M', 'Von Dombrowski, S', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Meyer, T O', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Ogg, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Thayer, J G', 'Thies, P G', 'Valant-Spaight, B L', 'Warburton, A', 'Ward, C', 'Athanas, M', 'Avery, P', 'Jones, C D', 'Lohner, M', 'Prescott, C', 'Rubiera, A I', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Briere, R A', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Plager, C', 'Sedlack, C', 'Selen, M', 'Thaler, J J', 'Williams, J', 'Edwards, K W', 'Janicek, R', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Coppage, D', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhao, X', 'Zhou, L', 'Anderson, S', 'Frolov, V V', 'Kubota, Y', 'Lee, S J', 'Mahapatra, R', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Alam, M S', 'Athar, S B', 'Mahmood, A H', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Gan, K K', 'Gwon, C', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lorenc, J', 'Schwarthoff, H', 'von Törne, E', 'Zoeller, M M', 'Richichi, S J', 'Severini, H', 'Skubic, P L', 'Undrus, A E', 'Bishai, M', 'Chen, S', 'Fast, J', 'Hinson, J W', 'Lee, J', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Glenn, S', 'Kwon, Y', 'Lyon, A L', 'Thorndike, E H', 'Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Stroynowski, R', 'Ye, J', 'Wlodek, T', 'Artuso, M', 'Ayad, R', 'Dambasuren, E', 'Kopp, S E', 'Majumder, G', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Titov, A', 'Viehhauser, G', 'Wang, J C', 'Csorna, S E', 'McLean, K W', 'Marka, S', 'Xu, Z', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chan, S', 'Eigen, G', 'Lipeles, E', 'Schmidtler, M', 'Shapiro, A', 'Sun, W M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Jaffe, D E', 'Masek, G E', 'Paar, H P', 'Potter, E M', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Eppich, A', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, H N', 'Nelson, T K', 'Richman, J D', 'Roberts, D', 'Behrens, B H', 'Ford, W T', 'Gritsan, A', 'Krieg, H', 'Roy, J D', 'Smith, J G']",['Evidence of New States Decaying into $\\Xi_{c}^{*}\\pi$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, electroproduction', 'charmed baryon, hadronic decay', 'postulated particle, Xi/c1', 'final state, (Xi/c0 pi+ pi-)', 'final state, (Xi/c+ pi+ pi-)', 'charmed baryon, hadronic decay', 'mass spectrum, mass difference', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906013'],"['Using data recorded by the CLEO II detector at CESR, we report evidence for two new charmed baryons, one decaying into $\\Xi_c^+\\pi^+\\pi^-$ via an intermediate $\\Xi_c^{*0}$, and its isospin partner decaying into differences of the two states to be $M(\\Xi_c^+\\pi^+\\pi^-)-M(\\Xi_c^+)=$ $348.6\\pm0.6\\pm1.0$ MeV, and $M(\\Xi_c^0\\pi^+\\pi^-)-M(\\Xi_c^0)=$ $347.2\\pm0.7\\pm2.0$ MeV. We interpret these new states as the $J^P = {3/2}^-']",['1999-06-09']
1328,['eng'],"['Cvach, J']",['Real and virtual photon structure from dijet events'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'final state, (2jet)', 'jet, transverse momentum', 'photon, structure function', 'momentum transfer, dependence', 'gluon, momentum spectrum', 'small-x', 'photon, off-shell', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906012'],"['Jet production in $ep$ collisions is sensitive to the partonic structure of photon. The latest measurements of dijet production from the H1 experiment provide new results of the gluon density of real photons at low $x$ and, for the first time, on the partonic density of virtual photons. Properties of the photon remnant were measured as a function of the hard scale defined by the $p_T$ of the jets. The comparison of dijet cross sections with the NLO QCD calculation shows the non-triviality of the concept of virtual photon structure.']",['1999-06-09']
1329,['eng'],"['Apollonio, M', 'Baldini, A', 'Bemporad, C', 'Caffau, E', 'Cei, F', 'Déclais, Y', 'De Kerret, H', 'Dieterle, B D', 'Etenko, A', 'Foresti, L', 'George, J', 'Giannini, G', 'Grassi, M', 'Kozlov, Yu Z', 'Kropp, W R', 'Kryn, Didier', 'Laiman, M', 'Lane, C E', 'Lefièvre, B', 'Machulin, I N', 'Martemyanov, A N', 'Martemyanov, B V', 'Mikaelyan, L A', 'Nicolo, D', 'Obolensky, M', 'Pazzi, R', 'Pieri, G', 'Price, L', 'Riley, S', 'Reeder, R', 'Sabelnikov, A A', 'Santin, G', 'Skorokhvatov, M', 'Sobel, H', 'Steele, J', 'Steinberg, R', 'Sukhotin, S V', 'Tomshaw, S', 'Véron, D', 'Vyrodov, V']",['Determination of neutrino incoming direction in the CHOOZ experiment and Supernova explosion location by scintillator detectors'],['Particle Physics - Experimental Results'],"['antineutrino/e, flux', 'antineutrino/e, energy spectrum', 'fission, particle source', 'antineutrino nucleon, interaction', 'charged current', 'particle identification, (n positron)', 'n, path length', 'supernova, particle source', 'scintillation counter, liquid', 'experimental results', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906011'],"['The CHOOZ experiment measured the antineutrino flux at a distance of about 1 Km from two nuclear reactors in order to detect possible neutrino oscillations with squared mass differences as low as 10**-3 eV**2 for full mixing. We show that the data analysis of the electron antineutrino events, collected by our liquid scintillation detector, locates the antineutrino source within a cone of half-aperture of about 18 degrees at the 68% C.L.. We discuss the implications of this experimental result for tracking down a supernova explosion.']",['1999-06-08']
1330,['eng'],"['Heinson, A P']",['Recent Results on the Top Quark from the Tevatron Collider Experiments'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay modes', 'mass spectrum, (2truth)', 'mass, truth', 'W, helicity', 'spin, correlation', 'Higgs particle, search for', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906023'],"['This paper presents the latest measurements of the properties of the top quark as determined by the DZero and CDF collaborations at the Fermilab Tevatron ppbar collider. Both experiments have studied the all-hadronic decay mode of ttbar events. The top quark measurement has been refined over the past year, with the addition of new channels and a re-evaluation of some of the earlier ones. There are recent studies of the mass of the ttbar system, the helicity of the W bosons in the top quark decays, and of the correlation of the spins of the top and antitop quarks. New results are also reported on searches for charged Higgs bosons in top quark decay, and for electroweak production of single top quarks.']",['1999-06-15']
1331,['eng'],"['Schmidt, M P']",['Two Recent Results on B Physics from CDF'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, interference', 'B0, hadronic decay', 'anti-B0, hadronic decay', 'B/s0, hadronic decay', 'J/psi(3100)', 'Phi(1020)', 'K*(892)', 'decay, asymmetry', 'violation, CP', 'polarization', 'amplitude analysis', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B0 --> J/psi(3100) K0(S)', 'B0 --> J/psi(3100) K*(892)', 'B/s0 --> J/psi(3100) Phi(1020)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906029'],"['Preliminary results from two recent CDF b physics analysis are presented. The first obtains sin(2beta) = 0.79 + 0.41 -0.44 from a measurement of the asymmetry in B0, B0bar to J/psi K_short decays, providing the best direct indication so far that CP invariance is violated in the b sector. The second obtains new results on the parity even (A_0 and A_par) and odd (A_perp) polarization amplitudes from full angular analyses of B0 to J/psi K*0 and B_s to J/psi J/psi phi decays.']",['1999-06-17']
1332,['eng'],"['Vasilev, M A', 'Beddo, M E', 'Brown, C N', 'Carey, T A', 'Chang, T H', 'Cooper, W E', 'Gagliardi, C A', 'Garvey, G T', 'Geesaman, D F', 'Hawker, E A', 'He Xiao Chun', 'Isenhower, L D', 'Kaplan, D M', 'Kaufman, S B', 'Koetke, D D', 'Lee, W M', 'Leitch, M J', 'McGaughey, P L', 'Moss, J M', 'Müller, B A', 'Papavassiliou, V', 'Peng, J C', 'Petitt, G', 'Reimer, P E', 'Sadler, M E', 'Sondheim, W E', 'Stankus, P W', 'Towell, R S', 'Tribble, R E', 'Webb, J C', 'Willis, J L', 'Young, G R']",['Parton Energy-Loss Limits and Shadowing in Drell-Yan Dimuon Production'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'beryllium', 'iron', 'tungsten', 'muon, pair production', 'Drell-Yan process', 'energy loss, parton', 'channel cross section, ratio', 'shadowing', 'dependence, mass number', 'x-dependence', 'transverse momentum, dependence', 'mass, dimuon', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'p nucleus --> muon+ muon- anything', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906010'],"['A precise measurement of the ratios of the Drell-Yan cross section per nucleon for an 800 GeV/c proton beam incident on Be, Fe and W targets is reported. The behavior of the Drell-Yan ratios at small target parton momentum fraction is well described by an existing fit to the shadowing observed in deep-inelastic scattering. The cross section ratios as a function of the incident parton momentum fraction set tight limits on the energy loss of quarks passing through a cold nucleus.']",['1999-06-07']
1333,['eng'],"['Krane, J']",['The Ratio of Dimensionless Jet Cross Sections at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'anti-p p, colliding beams', 'anti-p p, inelastic scattering', 'jet, hadroproduction', 'channel cross section, transverse energy', 'cross section, ratio', 'error', 'momentum spectrum, parton', 'renormalization, dependence', 'four-pi-detector, DZERO', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906009'],"['Several sources, both experimental and theoretical, subject inclusive jet cross section measurements to large uncertainties. On the experimental side, the energy scale contributes between 10% and 30% uncertainties. On the theoretical side, choice of parton distribution function introduces a 20% variation in the prediction; freedom in renormalization scale provides another uncertainty of up to 30%. The ratio of inclusive jet cross sections reduces the uncertainty from these major sources, permitting a very precise test of next-to-leading order QCD. The preliminary results from DØ and CDF differ from simple QCD predictions in normalization and differ from each other at small values of jet $x_T$.']",['1999-06-07']
1334,['eng'],"['Tripet, A']",['Exclusive $\\rho^{0}$ Production in Polarized DIS at SMC'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'muon nucleon, deep inelastic scattering', 'muon, polarized beam', 'nucleon, polarized target', 'rho(770)0, electroproduction', 'rho(770)0, photoproduction', 'rho(770)0, hadronic decay', 'mass spectrum, (pi+ pi-)', 'transverse momentum, dependence', 'momentum transfer, dependence', 'energy dependence', 'polarization, asymmetry', 'magnetic spectrometer, experimental results', 'CERN SPS', 'muon nucleon --> nucleon rho(770) muon', '190 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906008'],"[""Preliminary spin cross section asymmetries for exclusive $\\rho^{0}$ lepto-production, $\\vec{\\mu} + \\vec{N} \\to \\mu' + N + \\rho^{0} (\\rho^{0} \\to first time by the Spin Muon Collaboration (SMC) at low Q^2 (photoproduction) and at large Q^2 (DIS) for different $p_T^2$ intervals in the kinematic range $0.01 <Q^2< 60 GeV^2$ and $140 < W^2 < 310 GeV^2$ (<W> \\simeq 15 GeV) for the full SMC data set. About 100 K $\\rho^{0}$'s have been selected for $0.62 < m precision, no significant asymmetries have been observed at low $Q^{2}$ in the preliminary results.""]",['1999-06-07']
1335,['eng'],"['Leonidopoulos, C', 'Lu, C', 'Schwartz, A J']",['Development of a Straw Tube Chamber with Pickup-Pad Readout'],['Detectors and Experimental Techniques'],"['talk, Los Angeles 1999/01/05', 'tracks', 'trigger', 'drift chamber', 'argon, organic compounds', 'electrode', 'magnetic detector, HERA-B', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906007'],"['We have developed a straw tube chamber with pickup-pad readout. The mechanism for signal pickup, the size of the pickup signal, and the distribution of signals among neighboring pads are discussed. We have tested a prototype chamber in a beamtest at Brookhaven National laboratory and have measured chamber efficiencies in excess of 99%.']",['1999-06-07']
1336,['eng'],"['Hughes, V W', 'Deshpande, A A']",['A Polarized HERA Collider'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'electron p, storage ring', 'electron, polarized beam', 'p, polarized beam', 'particle source, polarized beam', 'beam monitoring, polarization', 'nucleon, structure function', 'structure function, spin', 'gluon, polarization', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906006'],"['A brief review is given of the status of nucleon spin structure functions as determined from polarized deep inelastic lepton-nucleon scatttering, including current outstanding problems. The characteristics of a polarized HERA collider, some of the particle physics topics it could address, and the accelerator physics challenges it must meet are discussed.']",['1999-06-04']
1337,['eng'],"['Crittenden, J A']",['Recent Results from Decay-Angle Analyses of $\\rho^{0}$ Photoproduction at High Momentum Transfer from ZEUS'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, inclusive reaction', 'momentum transfer, high', 'rho(770)0, photoproduction', 'rho(770)0, hadronic decay', 'angular distribution', 'quantum chromodynamics, perturbation theory', 'spin, density matrix', 'helicity', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906005'],['Recent results from decay-angle analyses of rho^0 photoproduction are presented and discussed in the context of earlier measurements at lower energy and lower momentum transfer.'],['1999-06-04']
1338,['eng'],"['Giacomelli, Giorgio', 'Patrizii, L']",['Magnetic monopoles'],['Particle Physics - Experimental Results'],"['lectures, Trieste 1998/06/29', 'magnetic monopole, search for', 'grand unified theory', 'dyon', 'energy loss', 'bound state, (nucleus magnetic monopole)', 'magnetic monopole, mass', 'scintillation counter', 'radiation, yield', 'streamer chamber, drift tube', 'plastics, track sensitive', 'photon photon, interaction', 'coupling, (magnetic monopole photon)', 'nuclear matter, strangeness', 'flux, upper limit', 'experimental results']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002032'],"['The main aim of this lecture is to give an update on the lectures on MagneticMonopoles (MMs) of the 1995 Trieste School. The update concerns theoreticaldevelopments, searches for GUT monopoles in the penetrating cosmic radiation atever lower fluxes, study of the energy losses of MMs in the Earth and indetectors,searches for low mass monopoles, and finally mention byproducts of MMsearches.']",['2000-02-15']
1339,['eng'],"['Bertram, I A']",['Uncertainties in the measurements of the Inclusive Jet Cross Section at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'cross section, error', 'transverse energy, dependence', 'magnetic detector, CDF', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906004'],['The systematic uncertainties of the measurements of the Inclusive Jet Cross Section at the Tevatron and their effect on the chi^2 comparisons between data and theoretical predictions are discussed.'],['1999-06-03']
1340,['eng'],"['King, B J']",['Muon Colliders'],['Detectors and Experimental Techniques'],"['talk, San Juan 1998/04/01', 'talk, San Juan 1998/04/08']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908041'],['An overview is given of muon collider technology and of the current status of the muon collider research program. The exciting potential of muon colliders for both neutrino physics and collider physics studies is then described and illustrated using self-consistent collider parameter sets at 0.1 TeV to 100 TeV center-of-mass energies.'],['1999-10-15']
1341,['eng'],"['Bazarko, A O']",['MiniBooNE'],['Detectors and Experimental Techniques'],"['talk, Los Angeles 1999/01/05', 'neutrino, oscillation', 'neutrino, counters and detectors', 'organic compounds', 'radiation, Cherenkov', 'scintillation counter', 'proton synchrotron', 'Fermilab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906003'],"[""The Booster Neutrino Experiment at Fermilab is preparing to search for muon to electron neutrino oscillations. The experiment is designed to make a conclusive statement about LSND's neutrino oscillation evidence. The experimental prospects are outlined in light of the current results from LSND and KARMEN.""]",['1999-06-02']
1342,['eng'],"['Rabbertz, K']",['Event Shapes and Power Corrections in e p DIS'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'event shape analysis', 'parametrization', 'quantum chromodynamics, nonperturbative', 'correction, higher-order', 'strong interaction, coupling constant', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906002'],"[""Deep-inelastic ep scattering data, taken with the H1 detector at HERA, are used to study the event shape variables thrust, jet broadening, jet mass, C parameter, and two kinds of differential two-jet rates over a large range of ``relevant energy'' Q between 7 GeV and 100 GeV. The Q dependence of the mean values is fit to second order calculations of perturbative QCD applying power law corrections proportional to 1/Q^p to account for hadronization effects. The concept of these power corrections is tested by a systematic investigation in terms of a non-perturbative parameter alpha_{p-1} and the strong coupling constant.""]",['1999-06-02']
1343,['eng'],"['Thomson, G']",['The CP/T Experiment'],['Detectors and Experimental Techniques'],"['talk, Moscow 1998/11/16', 'K+, separated beam', 'K+ nucleus, charge exchange', 'K0, secondary beam', 'interference, (K0(L) K0(S))', 'invariance, CPT', 'validity test', 'K0, hadronic decay', 'proposed experiment, Fermilab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9906001'],"['In this talk I describe a proposed Fermilab Main Injector experiment to carry out a program of measurements on the physics of K^0 mesons. The experiment is designed to maximize the interference between K_L and K_S mesons near their production target, and hence have excellent sensitivity to CP violation in many decay modes. The extremely accurate CP violation measurements we will be able to make will allow us to test CPT symmetry violation with sensitivity at the Planck scale. The experiment will use an RF-separated K^+ beam striking a target at the entrance to a hyperon magnet to make the K^0 beam by charge exchange. The decay region, magnetic spectrometer, electromagnetic calorimeter, and muon detector follow immediately to observe interference between K_L and K_S near the target.']",['1999-06-02']
1344,['eng'],"['Wengler, T']",['Forward $\\pi^{0}$-meson production at HERA'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'pi0, electroproduction', 'transverse momentum, high', 'production, small-angle', 'differential cross section, x-dependence', 'momentum transfer, dependence', 'transverse momentum, dependence', 'Altarelli-Parisi equation', 'Lipatov equation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> pi0 anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905062'],"['The production of high transverse momentum piz^0-mesons has been measured in deep-inelastic e-p scattering events at low Bjorken-$x$ taken with the H1 detector at HERA. The production of high p_T particles is strongly correlated to the emission of hard partons in QCD and is therefore sensitive to the dynamics of the strong interaction. For the first time the measurement of single particles has been extended to the region of small angles w.r.t. the proton remnant (forward region) and down to very low values of x ~ 5x10^-5. This region is expected to be particularly sensitive to QCD evolution effects in final states. Differential cross sections of inclusive pi^0-meson production have been measured as a function of Bjorken-x and the four-momentum transfer Q^2, and also as a function of the transverse momentum and the polar angle of the pi^0-mesons. A recent BFKL calculation and QCD models based on the DGLAP splitting functions are compared to the data. The best description of the data is achieved by the BFKL calculation.']",['1999-06-01']
1345,['eng'],"['Zawiejski, L']",['Fragmentation in DIS'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'kinematics, Breit frame', 'momentum spectrum', 'angular correlation, two-particle', 'transverse momentum, spectra', 'multiplicity, spectra', 'quark, fragmentation', 'universality', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905061'],['The fragmentation properties in deep-inelastic scattering (DIS) at HERA are investigated in order to test perturbative QCD and quark fragmentation universality. Selected results for the inclusive single particle distributions and the angular two-particle correlations in the current region of the Breit frame are presented and compared to results from $e^{+}e^{-}$ collisions. The extension of the DIS fragmentation studies to the target region of the Breit frame are also reported.'],['1999-06-01']
1346,['eng'],"['Alavi-Harati, A']","['Observation of Direct CP Violation in $K_{S,L} \\to \\pi\\pi$ Decays']",['Particle Physics - Experimental Results'],"['K0, hadronic decay', 'pi, pair production', 'K0(L), secondary beam', 'K0(S), secondary beam', 'violation, CP', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0 --> pi+ pi-', 'K0 --> 2pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905060'],['We have compared the decay rates of K_L and K_S to \\pi^+ \\pi^- and \\pi^0 at Fermilab. We find that the direct-CP-violation parameter Re(\\epsilon^\\prime/\\epsilon) is equal to (28.0 \\pm 3.0 (stat) \\pm 2.8 (syst)) violation in a decay process.'],['1999-06-01']
1347,['eng'],"['Nisius, R']",['The QED Structure of the Photon'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'muon, pair production', 'quantum electrodynamics', 'photon, structure function', 'x-dependence', 'momentum transfer, dependence', 'angular correlation', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> muon+ muon- positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905059'],"['Measurements of the QED structure of the photon based on the reaction ee --> ee \\gamma(*)(P^2)\\gamma*(Q^2) --> ee mumu are discussed. This review is an update of the discussion of the results on the QED structure of the photon presented in Refs.[1], and covers the published measurements of the photon structure functions F_2, F_A nd F_B and of the differential cross-section dsig/dx for the exchange of two virtual photons.']",['1999-06-01']
1348,['eng'],"['Abe, T']",['A preliminary measurement of the gluon splitting rate into $b\\overline{b}$ pairs in hadronic $Z^{0}$ decays'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'gluon, fragmentation', 'quark, beauty', 'quark, pair production', 'final state, (4jet)', 'track data analysis, vertex', 'magnetic detector, SLD', 'SLAC SLC Linac', 'Z0 --> 4jet', 'gluon --> 2beauty', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905057'],"['We present a measurement of the rate of gluon splitting into bottom quarks, $g \\to b\\bar{b}$, in hadronic $Z^0$ decays collected by SLD from 1996 to 1998. The analysis was performed by looking for secondary bottom production in 4-jet events of any primary flavor. A topological vertex mass technique was used to tag the two jets with the smallest angle between them as $b/\\bar{b}$. We obtained a rate of $g \\to b\\bar{b}$ per hadronic event to be $(3.07 \\pm 0.71']",['1999-05-31']
1349,['eng'],"['Behrens, B H']",['Measurement of $B \\to \\rho\\ell\\nu$ Decay and $|V_{ub}|$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'rho(770)', 'Kobayashi-Maskawa angle', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> rho(770) lepton neutrino', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905056'],"['Using a sample of 3.3 million Upsilon(4S) -> BBbar events collected with the CLEO II detector at the Cornell Electron Storage Ring (CESR), we measure the branching fraction for B -> rho l nu, |V_ub|, and the partial rate (Delta Gamma) in three bins of q^2 = (p_B-p_rho)^2. We find B(B^0 -> rho^- l^+ nu)=(2.69 +- 0.41^+0.35_-0.40 +- 0.50) 10^-4, |V_ub|=(3.23 +- 0.24^+0.23_-0.26 +- 0.58) 10^-3, Delta Gamma (0 < q^2 < 7 GeV^2/c^4) =(7.6 +- 3.0 ^+0.9_-1.2 +- 3.0) 10^-2 ns^-1, Delta Gamma (7 < q^2 < 14 GeV^2/c^4) =(4.8 +- 2.9 ^+0.7_-0.8 +- 0.7) 10^-2 ns^-1, and Delta Gamma (14 < q^2 < 21 GeV^2/c^4) = (7.1 +- 2.1^+0.9_-1.1 +- 0.6)10^-2 ns^-1. The quoted errors are statistical, systematic, and theoretical. The method is sensitive primarily to B -> rho l nu decays with leptons in the energy range above 2.3 GeV. Averaging with the previously published CLEO results, we obtain B(B^0 -> rho^- l^+ nu) = (2.57 +- 0.29^+0.33_-0.46 +- 0.41) 10^-4 and |V_{ub}| = (3.25 +- 0.14 ^+0.21_-0.29 +- 0.55) 10^-3.']",['1999-05-31']
1350,['eng'],"['Amelung, C']",['Measurement of the Proton Structure Function $F_{2}$ and of the Total Photon-Proton Cross Section $\\sigma_{tot}^{\\gamma p}$ at very low $Q^{2}$ and very low x'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'p, structure function', 'photon p, interaction', 'total cross section', 'momentum transfer, low', 'small-x', 'hadron, multiple production', 'diffraction', 'nondiffractive', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905055'],"['The proton structure function F2 has been measured in the range 0.045 GeV2 < Q2 < 0.65 GeV2 and 6*10**-7 < x < 1*10**-3 using 3.9 pb-1 of ep->eX reactions recorded with the ZEUS detector in 1997. The analysis is based on data from the Beam Pipe Calorimeter (BPC) and the Beam Pipe Tracker (BPT). Compared to our previous analysis, the BPT permits improved background suppression and better control of systematic uncertainties, allowing the extension of the kinematic region of the measurement towards lower Q2 as well as higher and lower y. Significant improvements have also been achieved in the simulation of the hadronic final state via a mixture of samples of non-diffractive and diffractive Monte Carlo events, generated by the programs DJANGO and RAPGAP.']",['1999-05-31']
1351,['eng'],"['Dong, D', 'Abe, K', 'Abe, T', 'Adam, I', 'Akagi, T', 'Allen, N J', 'Arodzero, A', 'Ash, William W', 'Aston, D', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barakat, M B', 'Bardon, O', 'Barklow, T L', 'Bauer, J M', 'Bellodi, G', 'Ben-David, R', 'Benvenuti, Alberto C', 'Bilei, G M', 'Bisello, D', 'Blaylock, G', 'Bogart, J R', 'Bolen, B D', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Calcaterra, A', 'Caldwell, D O', 'Calloway, D H', 'Camanzi, B', 'Carpinelli, M', 'Cassell, R', 'Castaldi, R', 'Castro, A', 'Cavalli-Sforza, M', 'Chou, A', 'Church, E', 'Cohn, H O', 'Coller, J A', 'Convery, M R', 'Cook, V', 'Cotton, R', 'Cowan, R F', 'Coyne, D G', 'Crawford, G', 'Damerell, C J S', 'Danielson, M N', 'Daoudi, M', 'De Groot, N', ""Dell'Orso, R"", 'Dervan, P J', 'De Sangro, R', 'Dima, M', 'de Oliveira, A', 'Dong, D N', 'Du, P Y C', 'Dubois, R', 'Eisenstein, B I', 'Eschenburg, V', 'Etzion, E', 'Fahey, S', 'Falciai, D', 'Fan, C', 'Fernández, J P', 'Fero, M J', 'Flood, K', 'Frey, R', 'Gillman, T', 'Gladding, G E', 'González, S', 'Hart, E L', 'Harton, J L', 'Hasan, A', 'Hasuko, K', 'Hedges, S J', 'Hertzbach, S S', 'Hildreth, M D', 'Huber, J', 'Huffer, M E', 'Hughes, E W', 'Huynh, X', 'Hwang, H', 'Iwasaki, M', 'Jackson, D J', 'Jacques, P', 'Jaros, J A', 'Jiang, Z Y', 'Johnson, A S', 'Johnson, J R', 'Johnson, R A', 'Junk, T R', 'Kajikawa, R', 'Kalelkar, M S', 'Kamyshkov, Yu A', 'Kang, H J', 'Karliner, I', 'Kawahara, H', 'Kim, Y D', 'King, R', 'King, M E', 'Kofler, R R', 'Krishna, N M', 'Kroeger, R S', 'Langston, M', 'Lath, A', 'Leith, D W G S', 'Lia, V', 'Lin, C J S', 'Liu, X', 'Liu, M X', 'Loreti, M', 'Lu, A', 'Lynch, H L', 'Ma, J', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'Masuda, H', 'Mazzucato, E', 'McKemey, A K', 'Meadows, B T', 'Menegatti, G', 'Messner, R', 'Mockett, P M', 'Moffeit, K C', 'Moore, T B', 'Morii, M', 'Müller, D', 'Murzin, V', 'Nagamine, T', 'Narita, S', 'Nauenberg, U', 'Neal, H A', 'Nussbaum, M', 'Oishi, N', 'Onoprienko, D V', 'Osborne, L S', 'Panvini, R S', 'Park, H', 'Park, C H', 'Pavel, T J', 'Peruzzi, I', 'Piccolo, M', 'Piemontese, L', 'Pieroni, E', 'Pitts, K T', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Punkar, G D', 'Quigley, J', 'Ratcliff, B N', 'Reeves, T W', 'Reidy, J', 'Reinertsen, P L', 'Rensing, P E', 'Rochester, L S', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schindler, R H', 'Schumm, B A', 'Schwiening, J', 'Sen, S', 'Serbo, V V', 'Shaevitz, M H', 'Shank, J T', 'Shapiro, G', 'Sherden, D J', 'Shmakov, K D', 'Simopoulos, C', 'Sinev, N B', 'Smith, S R', 'Smy, M B', 'Snyder, J A', 'Stängle, H', 'Stahl, A', 'Stamer, P E', 'Steiner, R', 'Steiner, H', 'Strauss, M G', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Szumilo, A', 'Takahashi, T', 'Taylor, F E', 'Thom, J', 'Torrence, E', 'Toumbas, N K', 'Trandafir, A I', 'Turk, J', 'Usher, T', 'Vannini, C', 'Vavra, J', 'Vella, E N', 'Venuti, J P', 'Verdier, R', 'Verdini, P G', 'Wagner, S R', 'Wagner, D L', 'Waite, A P', 'Walston S', 'Wang, J', 'Ward, C', 'Watts, S J', 'Weidemann, A W', 'Weiss, E R', 'Whitaker, J S', 'White, S L', 'Wickens, F J', 'Williams, B', 'Williams, D C', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Wittlin, J L', 'Woods, M', 'Word, G B', 'Wright, T R', 'Wyss, J', 'Yamamoto, R K', 'Yamartino, J M', 'Yang, X', 'Yashima, J', 'Yellin, S J', 'Young, C C']",['An Improved Measurement of the b Quark Fragmentation Function in $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, fragmentation function', 'beautiful particle, energy spectrum', 'beautiful particle, decay', 'model, fragmentation', 'track data analysis, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905054', 'http://www-sld.slac.stanford.edu/sldwww/physics/dropbox/ich00bfra.ps']","['We present a new preliminary measurement of the b quark fragmentation function in Z0 decays using a novel kinematic B hadron energy reconstruction technique. The measurement is performed using 150,000 hadronic Z0 events recorded in the SLD experiment at SLAC between 1996 and 1997. The small and stable SLC beam spot and the CCD-based vertex detector are used to reconstruct topological B-decay vertices with high efficiency and purity, and to provide precise measurements of the kinematic quantities used in this technique. We measure the B energy with good efficiency and resolution over the full kinematic range. We compare the scaled B hadron energy distribution with several functional forms of the B hadron energy distribution and models of b quark fragmentation. Several functions including JETSET + Peterson are excluded by the data. The average scaled energy of the weakly decaying B hadron is measured to be XB = 0.719 +/- 0.005 (stat) +/- 0.007 (syst) +/- 0.001 (model) (preliminary).']",['1999-05-31']
1352,['eng'],"['Düren, M']",['Polarized lepton nucleon scattering'],['Particle Physics - Experimental Results'],"['conference, review', 'Zeuthen 1999/04/19', 'lepton nucleon, deep inelastic scattering', 'lepton, polarized beam', 'nucleon, polarized target', 'nucleon, structure function', 'spin, dependence', 'spin, asymmetry', 'quark, polarization', 'quark, flavor', 'quark, sea', 'gluon, polarization', 'hadron, electroproduction', 'rho(770)0, photoproduction', 'difference', 'sum rule', 'Lambda, polarization', 'polarization, transverse', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905053'],"['This paper summarizes the contributions to the experimental sessions on polarized lepton nucleon scattering at the DIS 99 workshop. Results are reported about the flavor decomposition of the quark polarization, a first direct measurement of a positive gluon polarization, the observation of a double-spin asymmetry in diffractive rho production, the polarization of lambda hyperons, the observation of transverse single-spin asymmetries and the measurement of the Gerasimov-Drell-Hearn sum rule. Prospects of future fixed target and collider facilities are discussed.']",['1999-05-31']
1353,['eng'],"['Vakili, M', 'Arroyo, C G', 'Auchincloss, P S', 'De Barbaro, P', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Budd, H S', 'Conrad, J', 'De Barbaro, L', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Koizumi, G', 'Koutsoliotas, S', 'Lamm, M J', 'Lefmann, W C', 'Marsh, W', 'McFarland, K S', 'McNulty, C', 'Mishra, S R', 'Naples, D', 'Nienaber, P', 'Oreglia, M J', 'Perera, L P', 'Quintas, P Z', 'Romosan, A', 'Sakumoto, W K', 'Schumm, B A', 'Sciulli, F J', 'Seligman, W G', 'Shaevitz, M H', 'Smith, W H', 'Spentzouris, P', 'Steiner, R', 'Stern, E G', 'Yang, U K', 'Yu, J']",['Nuclear Structure Functions in the Large $X$ Large $Q^{2}$ Kinematic Region in Neutrino Deep Inelastic Scattering'],['Particle Physics - Experimental Results'],"['neutrino nucleus, deep inelastic scattering', 'nucleon, structure function', 'nuclear properties, effect', 'correlation, ((n)nucleon)', 'cluster, multiquark', 'spectra, x-dependence', 'momentum transfer, high', 'experimental results', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905052'],"[""Data from the CCFR E770 Neutrino Deep Inelastic Scattering (DIS) experiment at Fermilab contain events with large Bjorken x (x>0.7) and high momentum transfer (Q^2>50 (GeV/c)^2). A comparison of the data with a model based on no nuclear effects at large x, shows a significant excess of events in the data. Addition of Fermi gas motion of the nucleons in the nucleus to the model does not explain the excess. Adding a higher momentum tail due to the formation of ``quasi-deuterons'' makes some improvement. An exponentially falling F_2 ``few-nucleon correlations'', can describe the data. A value of s=8.3 \\pm 0.7(stat.)\\pm 0.7(sys.) yields the best agreement with the data.""]",['1999-05-28']
1354,['eng'],"['Wing, M']",['Semi-leptonic Decays of Heavy Quarks in Dijet Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'final state, (2jet electron)', 'transverse energy, high', 'quark, beauty', 'electron, transverse momentum', 'differential cross section, transverse momentum', 'differential cross section, x-dependence', 'magnetic detector, ZEUS', 'DESY HERA Stor', 'positron p --> 2jet electron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905051'],"['The production of heavy quarks has been studied in photoproduction processes with the ZEUS detector at HERA using an integrated luminosity of $36.9 pb^{-1}$. Events with a photon virtuality, $Q^2<1 GeV^2$, were selected with two jets of high transverse energy and an electron in the final state. Consideration of the distribution in $p_T^{rel}$ - the momentum of the electron transverse to the axis of the jet to which the electron is closest - allows a measurement of the beauty cross-section in a restricted region of phase space.']",['1999-05-28']
1355,['eng'],"['Kulchitskii, Yu A', 'Kuzmin, M V']",['Non-compensation of the Barrel Combined Calorimeter Prototype'],['Detectors and Experimental Techniques'],"['talk, Geneva 1998/06']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9911007'],"['The e/$\\pi$ ratio for the Barrel Combined Calorimeter Prototype, composed from electromagnetic LAr calorimeter and hadronic Tile calorimter was investigated. Response of Combined Calorimeter on pions and electrons in the energy region 20 - 300 GeV was studied. Found $e/h = 1.37\\pm0.01\\pm0.02$ is in good agreement with results from previous Combined Calorimeter test but has more precisions.']",['1999-11-08']
1356,['eng'],[],['Angular and Current-Target Correlations in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'correlation, (2charged particle)', 'multiplicity, correlation', 'kinematics, Breit frame', 'correlation, short-range', 'correlation, long-range', 'angular correlation, two-particle', 'momentum transfer, high', 'electron positron, annihilation', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905050'],"['Correlations between charged particles in deep inelastic ep scattering have been studied in the Breit frame with the ZEUS detector at HERA using an integrated luminosity of 6.4 pb-1. Short-range correlations are analysed in terms of the angular separation between current-region particles within a cone centred around the virtual photon axis. Long-range correlations between the current and target regions have also been measured. The data support predictions for the scaling behaviour of the angular correlations at high Q2 and for anti-correlations between the current and target regions over a large range in Q2 and in the Bjorken scaling variable x. Analytic QCD calculations and Monte Carlo models correctly describe the trends of the data at high Q2, but show quantitative discrepancies. The data show differences between the correlations in deep inelastic scattering and e+e- annihilation.']",['1999-05-27']
1357,['eng'],"['Ginsburg, C M']",['Deep-Inelastic $e^{+}p$ Scattering at Very High $Q^{2}$ from ZEUS at HERA'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'momentum transfer, high', 'neutral current', 'charged current', 'differential cross section, momentum transfer', 'x-dependence', 'electroweak interaction, validity test', 'Z0, mass', 'W, mass', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905049'],['Neutral-current and charged-current deep-inelastic scattering at very high four-momentum transfer squared (Q^2) have been studied in positron-proton collisions at center-of-mass energy 300 GeV using the ZEUS detector at HERA. An integrated luminosity of 47.7 $pb^{-1}$ was collected in the years 1994-1997. Differential cross sections are presented for $Q^2 > 400 GeV^2$ and compared to Standard Model predictions.'],['1999-05-26']
1358,['eng'],[],['Muon Astronomy with LVD Detector'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'muon, cosmic radiation', 'angular distribution', 'shadowing, lunar', 'cosmic radiation, particle source', 'astrophysics', 'cosmic radiation, flux', 'upper limit', 'deep underground detector, Gran Sasso', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905048', 'http://krusty.physics.utah.edu/~icrc1999/root/vol7/s3_2_40.pdf']","['We analysed the arrival directions of single muons detected by the first LVD tower from November, 1994 till January, 1998. The moon shadowing effect has been observed. To search for point sources of high energy photons we have analysed muons crossing the rock thickness greater than 3, 5 and 7 km w.e., which corresponds to the mean muon energies 1.6, 3.9 and 8.4 TeV at the surface, respectively. Upper limits on steady muon fluxes for selected astrophysical sources for different muon energies are presented.']",['1999-05-26']
1359,['eng'],[],['Measurement of the Neutron Flux Produced by Cosmic-Ray Muons with LVD at Gran Sasso'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'muon, cosmic radiation', 'muon nucleus, interaction', 'n, electroproduction', 'cascade', 'n, flux', 'spatial distribution', 'deep underground detector, Gran Sasso', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905047', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h3_1_15.pdf']","['The flux of muon-produced neutrons far away from the muon track may constitute a background for the underground detectors searching for rare events. The muon events collected by the first LVD tower from March, 1996, to February, 1998, (1.56 years of live time) were used to estimate the neutron flux at various distances from the muon track or muon-produced cascade.']",['1999-05-26']
1360,['eng'],"['Dong, D']",['Tests of QCD using Heavy Flavors at SLD'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/20', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'quark, beauty', 'quark, pair production', 'quark, coupling', 'gluon, associated production', 'gluon, energy spectrum', 'beautiful particle, energy spectrum', 'quark, fragmentation function', 'gluon, fragmentation', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty gluon', 'gluon --> 2beauty', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905058'],"['We present preliminary results on three SLD analyses: the gluon energy spectrum in 3-jet bbg events, the rate of g->bb, and the b fragmentation function in Z0 decays. The gluon energy spectrum, measured over the full kinematic range, is compared with perturbative QCD predictions. We set new 95% C.L. limits on the anomalous chromomagnetic coupling of the b quark: -0.09<kappa<0.06. The rate of g->bb is measured to be (3.07 +/- 0.71(stat) +/- 0.66(syst)) X 10^-3. The inclusive B hadron energy distribution in Z0 decays is measured for the first time over the full kinematic range, using a novel B hadron energy reconstruction technique. Several models of b fragmentation including JETSET + Peterson are excluded by the data. The average scaled B hadron energy of the weakly decaying B hadron is measured to be XB = 0.713 +/- 0.005(stat) +/- 0.007(syst) +/- 0.002 (model). All three measurements take advantage of the small and stable SLC interaction point as well as the excellent vertexing and tracking capabilities of the upgraded CCD-pixel vertex detector.']",['1999-05-31']
1361,['eng'],"['Breitweg, J']",['Measurement of Dijet Photoproduction at High Transverse Energies at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'jet, photoproduction', 'jet, pair production', 'transverse energy, high', 'channel cross section, transverse energy', 'rapidity dependence', 'track data analysis, cluster', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'tables', 'bibliography', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905046'],"['The cross section for dijet photoproduction at high transverse energies is presented as a function of the transverse energies and the pseudorapidities of the jets. The measurement is performed using a sample of ep-interactions corresponding to an integrated luminosity of 6.3 pb^(-1), recorded by the ZEUS detector.Jets are defined by applying a k_T-clustering algorithm to the hadrons observed in the final state. The measured cross sections are compared to next-to-leading order QCD calculations. In a kinematic regime where theoretical uncertainties are expected to be small, the measured cross sections are higher than these calculations.']",['1999-05-25']
1362,['eng'],"['Allison, W W M', 'Alner, G J', 'Ayres, D S', 'Barrett, W L', 'Bode, C', 'Border, P M', 'Brooks, C B', 'Cobb, J H', 'Cotton, R J', 'Courant, H', 'Demuth, D M', 'Fields, T H', 'Gallagher, H R', 'Goodman, M C', 'Gran, R', 'Joffe-Minor, T M', 'Kafka, T', 'Kasahara, S M', 'Leeson, W', 'Lichtfield, P J', 'Longley, N P', 'Mann, W A', 'Marshak, M L', 'Milburn, R H', 'Miller, W H', 'Mualem, L M', 'Napier, A', 'Oliver, W P', 'Pearce, G F', 'Peterson, E A', 'Petyt, D A', 'Price, L E', 'Ruddick, K', 'Sánchez, M', 'Schneps, J', 'Schub, M H', 'Seidlein, R', 'Stassinakis, A', 'Thron, J L', 'Vasilev, V', 'Villaume, G', 'Wakely, S P', 'West, N', 'Wall, D']",['Cygnus X-3 Revisited'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'muon, cosmic radiation', 'photon, cosmic radiation', 'cosmic radiation, particle source', 'cosmic radiation, flux', 'shadowing, lunar', 'deep underground detector, Soudan', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905045'],"['The Soudan 2 deep underground tracking calorimeter has recorded cosmic ray muon tracks from the direction of the galactic x-ray binary Cygnus X-3 on most transits during the interval 1989-1998. We analyze these events in the context of previous reports of Cygnus X-3-related muon flux during major radio flares of that source. We find some evidence for excess flux during a small number of transits coincident with major radio flares. We also find an indication that these events may be distributed around the source with a Gaussian point spread function with $\\sigma = 1.3^{\\circ}$, larger than the instrumental angular spread of $\\le 0.3^{\\circ}$, verified by observation of the shadow of the moon.']",['1999-05-25']
1363,['eng'],"['Cobb, J H', 'Marshak, M L', 'Allison, W W M', 'Alner, G J', 'Ayres, D S', 'Barrett, W L', 'Bode, C', 'Border, P M', 'Brooks, C B', 'Cotton, R J', 'Courant, H', 'Demuth, D M', 'Fields, T H', 'Gallagher, H R', 'García-García, C', 'Goodman, M C', 'Gran, R', 'Joffe-Minor, T M', 'Kafka, T', 'Kasahara, S M', 'Leeson, W', 'Lichtfield, P J', 'Longley, N P', 'Mann, W A', 'Milburn, R H', 'Miller, W H', 'Moon, C', 'Mualem, L M', 'Napier, A', 'Oliver, W P', 'Pearce, G F', 'Peterson, E A', 'Petyt, D A', 'Price, L E', 'Ruddick, K', 'Sánchez, M', 'Sankey, P', 'Schneps, J', 'Schub, M H', 'Seidlein, R', 'Stassinakis, A', 'Thron, J L', 'Vasilev, V', 'Villaume, G', 'Wakely, S P', 'West, N', 'Wall, D']",['Observation of the Moon Shadow in Deep Underground Muon Flux'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'cosmic radiation, flux', 'shadowing, lunar', 'deep underground detector, Soudan', 'angular resolution', 'alignment', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905044'],"['A shadow of the moon, with a statistical significance of $5\\sigma$, has been observed in the underground muon flux at a depth of 2090 mwe using the Soudan 2 detector. The angular resolution of the detector is well described by a Gaussian with $\\sigma \\le 0.3^{\\circ}$. The position of the shadow confirms the alignment of the detector to better than $0.15^{\\circ}$. This alignment has remained stable during 10 years of data taking from 1989 through 1998.']",['1999-05-25']
1364,['eng'],"['Allison, W W M', 'Alner, G J', 'Ayres, D S', 'Barrett, W L', 'Bode, C', 'Border, P M', 'Brooks, C B', 'Cobb, J H', 'Cotton, R J', 'Courant, H', 'Demuth, D M', 'Fields, T H', 'Gallagher, H R', 'García-García, C', 'Goodman, M C', 'Gran, R', 'Joffe-Minor, T M', 'Kafka, T', 'Kasahara, S M', 'Leeson, W', 'Lichtfield, P J', 'Longley, N P', 'Mann, W A', 'Marshak, M L', 'Milburn, R H', 'Miller, W H', 'Mualem, L M', 'Napier, A', 'Oliver, W P', 'Pearce, G F', 'Peterson, E A', 'Petyt, D A', 'Price, L E', 'Ruddick, K', 'Sánchez, M', 'Schneps, J', 'Schub, M H', 'Seidlein, R', 'Stassinakis, A', 'Thron, J L', 'Vasilev, V', 'Villaume, G', 'Wakely, S P', 'West, N', 'Wall, D']",['Cosmic Ray Sun Shadow in Soudan 2 Underground Muon Flux'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'muon, cosmic radiation', 'cosmic radiation, flux', 'flux, time variation', 'shadowing, solar', 'magnetic field', 'deep underground detector, Soudan', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905043'],"['The absorption of cosmic rays by the sun produces a shadow at the earth. The angular offset and broadening of the shadow are determined by the magnitude and structure of the interplanetary magnetic field (IPMF) in the inner solar system. We report the first measurement of the solar cosmic ray shadow by detection of deep underground muon flux in observations made during the entire ten-year interval 1989 to 1998. The sun shadow varies significantly during this time, with a $3.3\\sigma$ shadow observed during the years 1995 to 1998.']",['1999-05-25']
1365,['eng'],"['González-Mestres, L']",['The Luminescent Bolometer As a Dark Matter Detector'],['Detectors and Experimental Techniques'],"['talk, Salt Lake City 1999/08/17', 'astrophysics, missing-mass', 'WIMP, particle identification', 'bolometer', 'superconducting, tunneling', 'neutrino, solar', 'double-beta decay']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905042', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h6_4_04.pdf']","['Direct detection of WIMP dark matter candidates has to face many difficult challenges. In particular, it requires an extremely high level of background rejection. The only way out seems to be particle identification which, for experiments based on nucleus recoil, is most efficiently performed by simultaneously detecting ionization or light and phonons. When comparing different approaches, it is necessary to keep in mind the potential requirement of building large detectors and the difficulties that this condition may raise for some cryogenic devices. It is claimed that the luminescent bolometer (simultaneous detection of light and phonons) red by arrays of superconducting tunnel junctions, as proposed by the author some years ago, ultimately provides the most appropriate WIMP detector. Solar neutrino detection and other applications are also briefly discussed.']",['1999-05-25']
1366,['eng'],"['Iwasaki, M']",['Measurements of $Z^{0}$ to Heavy-quark couplings at SLD'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, charm', 'quark, beauty', 'coupling, (Z0 quark)', 'Z0, branching ratio', 'asymmetry', 'parity, violation', 'particle identification, flavor', 'particle identification, charge', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905040'],"['We present measurements of $Z^0$ to heavy-quark coupling electroweak parameters, $R_b$, $R_c$, and parity-violation parameter $A_c$, from SLD. The measurements are based on approximately 550k hadronic $Z^0$ events collected in 1993-98. Obtained preliminary results of $R_b$ and $R_c$ measurements are $R_b = 0.2159 \\pm 0.0014 \\pm 0.0014$ and $R_c = 0.1685 \\pm 0.0047 \\pm 0.0043$. In the $A_c$ measurement, we use four methods to determine the initial-quark charge: combined Kaon charge and Vertex charge, lepton, exclusively reconstructed D*, D-mesons, and a new method using inclusive soft-pion from D*. The preliminary results of these four methods were combined to give $A_c = 0.634 \\pm 0.027$.']",['1999-05-25']
1367,['eng'],"['Sidorov, A V', 'Anykeyev, V B', 'Batusov, Yu A', 'Bunyatov, S A', 'Borisov, A', 'Bozhko, N', 'Chukin, G L', 'Denisov, O Yu', 'Fachrutdinov, R M', 'Goryachev, V N', 'Kazarinov, Yu M', 'Kirsanov, M M', 'Klimov, O L', 'Kononov, A I', 'Kozhin, A S', 'Krasnoperov, A V', 'Kravtsov, V I', 'Kusnetsov, V E', 'Lipajev, V V', 'Mukhin, A I', 'Nefedov, Y A', 'Popov, B A', 'Prakhov, S N', 'Salomatin, Yu I', 'Snyatkov, V I', 'Sviridov, Yu M', 'Tereshchenko, V V', 'Tumakov, V L', 'Valuev, V Yu', 'Vovenko, A S']",['Measurement of $xF_{3}$ and $F_{2}$ Structure Functions in Low $Q^{2}$ Region with the IHEP-JINR Neutrino Detector'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'neutrino nucleon, interaction', 'antineutrino nucleon, interaction', 'neutrino/mu', 'charged current', 'target, isoscalar', 'momentum transfer, low', 'nucleon, structure function', 'x-dependence', 'quantum chromodynamics, Lambda parameter', 'strong interaction, coupling constant', 'experimental results', 'Serpukhov PS', '6-28 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905038'],['The isoscalar structure functions $xF_3$ and $F_2$ are measured as functions of $x$ averaged over all $Q^2$ permissible for the range of 6 to 28 GeV of incident neutrino (anti-neutrino) energy at the IHEP-JINR Neutrino Detector. The QCD analysis of $xF_3$ structure function provides validity in the region of low $Q^2$. The corresponding value of the strong interaction constant $\\alpha_S (M_Z) = 0.123^{+0.010}_{-0.013}$ agrees with the recent result of the CCFR collaboration and with the combined LEP/SLC result.'],['1999-05-21']
1368,['eng'],"['De Carvalho, L A', 'Dobrigkeit, C']",['A method to estimate primary composition with the Auger Observatory'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'cosmic radiation, primary', 'elements, cosmic radiation', 'showers, air', 'showers, density', 'showers, spatial distribution', 'muon, cosmic radiation', 'electron, cosmic radiation', 'photon, cosmic radiation', 'numerical calculations, Monte Carlo', 'experimental methods, proposed']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905037', 'http://krusty.physics.utah.edu/~icrc1999/root/vol1/h2_5_06.pdf']","['We explore the feasibility of estimating primary cosmic ray composition at ultra high energies from the sum of muon, electron and photon densities and the depth of maximum of extensive air showers detected by the Auger Observatory. From the information of the Fluorescence ($X_{max}$) and water Cerenkov detectors ($\\rho(1000)$) we infere the most probable type of primary which originated the shower. The method is tested simulating Extensive Air Showers (EAS) at energies up to $10^{20}$ eV using a version of MOCCA/Sibyll adapted for Dec Alpha Servers. We also discuss some results on the mass composition using the depth of the shower maximum and the lateral distribution of showers in the energy range $10^{18}$-$10^{20}$ eV.']",['1999-05-21']
1369,['eng'],"['Cobb, J H', 'Marshak, M L', 'Allison, W W M', 'Alner, G J', 'Ayres, D S', 'Barrett, W L', 'Bode, C', 'Border, P M', 'Brooks, C B', 'Cotton, R J', 'Courant, H', 'Demuth, D M', 'Fields, T H', 'Gallagher, H R', 'Goodman, M C', 'Gran, R', 'Joffe-Minor, T M', 'Kafka, T', 'Kasahara, S M', 'Leeson, W', 'Lichtfield, P J', 'Longleym N P', 'Mann, W A', 'Milburn, R H', 'Miller, W H', 'Moon, C', 'Mualem, L M', 'Napier, A', 'Oliver, W P', 'Pearce, G F', 'Peterson, E A', 'Petyt, D A', 'Price, L E', 'Ruddick, K', 'Sánchez, M', 'Sankey, P', 'Schneps, J', 'Schub, M H', 'Seidlein, R', 'Stassinakis, A', 'Thron, J L', 'Vasilev, V', 'Villaume, G', 'Wakely, S P', 'West, N', 'Wall, D']",['The Observation of a Shadow of the Moon in the Underground muon flux in the Soudan 2 detector'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'flux', 'shadowing, lunar', 'angular resolution', 'alignment', 'track data analysis', 'deep underground detector, Soudan', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905036'],"['A shadow of the moon, with a statistical significance of 5 sigma, has been observed in the underground muon flux at a depth of 2090 mwe using the Soudan 2 detector. The angular resolution of the detector is well described by a Gaussian with a sigma of less than 0.3 degrees. The position of the shadow confirms that the alignment of the detector is known to better than 0.15 degrees and has remained stable during ten years of data taking.']",['1999-05-21']
1370,['eng'],"['Campanelli, M']",['Review on new Neutrino Oscillation Experiments'],['Particle Physics - Experimental Results'],"['review, Les Arcs 1999/03/13', 'neutrino, oscillation', 'neutrino, cosmic radiation', 'neutrino, solar', 'neutrino/mu, beam', 'neutrino nucleon, interaction', 'charged current', 'ratio, (neutrino/mu neutrino/e)', 'neutrino, mass difference', 'neutrino/tau', 'neutrino, sterile', 'experimental results', 'counters and detectors, proposed']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905035'],"['Driven by new experimental results, in the latest period several new neutrino oscillation experiments have been proposed. I will outline the main ideas behind the different proposals, in particular concerning atmospheric neutrinos and neutrinos from accelerated beams.']",['1999-05-20']
1371,['eng'],"['Vigdor, S E']",['The RHIC Spin Program'],['Particle Physics - Experimental Results'],"['talk, Protvino 1998/09/08', 'p p, interaction', 'p, polarized beam', 'polarization, longitudinal', 'polarization, transverse', 'p, structure function', 'structure function, spin', 'quantum chromodynamics, validity test', 'new interaction, search for', 'quark, polarization', 'quark, sea', 'gluon, helicity', 'spin, correlation', 'photon, direct production', 'quark gluon, Compton scattering', 'quark quark, interaction', 'W, hadroproduction', 'W, leptonic decay', 'parity, violation', 'jet, hadroproduction', 'Lambda, hadroproduction', 'Lambda, polarization', 'fragmentation function', 'p, charm', 'magnetic detector, STAR', 'magnetic detector, PHENIX', 'numerical calculations, Brookhaven RHIC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905034'],"['I review progress toward the experimental study of polarized proton collisions at RHIC, at center-of-mass energies of several hundred GeV. The tools under development for these experiments are summarized, with emphasis on the complementarity for the spin program of the two major detectors, PHENIX and STAR. The proposed research program includes measurements of the spin structure of hadrons, tests of QCD predictions for spin observables, and polarization searches for interactions beyond the Standard Model. I argue, in particular, that RHIC should provide the best determination of the gluonic contribution to proton spin foreseen for the coming decade.']",['1999-05-20']
1372,['eng'],"['Hayes, M']",['Heavy Flavours in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/13', 'positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'final state, (2jet)', 'quark, beauty', 'quark, charm', 'quark, photoproduction', 'D*(2010), particle identification', 'differential cross section, x-dependence', 'muon, transverse momentum', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905033'],"['Differential cross sections, $d\\sigma/d x_\\gamma^{\\rm OBS}$, for dijet photoproduction events with a tagged $D^*$ meson are presented, where $x_\\gamma^{\\rm OBS}$ is the fraction of the photon energy contributing to the two highest transverse energy jets. Results on open beauty cross sections (from semileptonic decays) compared to LO Monte Carlo predictions are also presented.']",['1999-05-20']
1373,['eng'],[],['Measurement of High-$Q^{2}$ Neutral-Current $e^{+}p$ Deep Inelastic Scattering Cross-Sections at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'momentum transfer, high', 'neutral current', 'differential cross section, momentum transfer', 'rapidity dependence', 'electroweak interaction, validity test', 'Z0, exchange', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905032'],"['The e^+p neutral-current deep inelastic scattering differential cross-sections $d\\sigma/dQ^2$, for Q^2 > 400 GeV^2, $d\\sigma/dx$ and $d\\sigma/dy$, for Q^2 > 400, 2500 and 10000 GeV^2, have been measured with the ZEUS detector at HERA. The data sample of 47.7 pb^-1 was collected at a center-of-mass energy of 300 GeV. The cross-section, $d\\sigma/dQ^2$, falls by six orders of magnitude between Q^2 = 400 and 40000 GeV^2. The predictions of the Standard Model are in very good agreement with the data. Complementing the observations of time-like Z^0 contributions to fermion-antifermion annihilation, the data provide direct evidence for the presence of Z^0 exchange in the space-like region explored by deep inelastic scattering.']",['1999-05-20']
1374,['eng'],"['Satriano, C']","['Search for Steady, Modulated, and Variable Cosmic Ray Sources Using Underground Muons in MACRO']",['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'muon, cosmic radiation', 'flux, upper limit', 'cosmic radiation, particle source', 'deep underground detector, MACRO', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905031', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h3_1_02.pdf']",['Using a sample of 38.5 million underground muons collected by the MACRO detector we have performed an all-sky search for pointlike sources producing excesses of muons above the expected background. The d.c. muon flux upper limit at the Earth coming from selected sources is of the order of 10^-13 cm^-2 s^-1 or less. Futhermore we discuss searches for possible modulated and variable sources of muons using different techniques.'],['1999-05-20']
1375,['eng'],"['Achasov, M N', 'Baru, S E', 'Bozhenok, A V', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P I', 'Korol, A A', 'Koshuba, S V', 'Perevedentsev, E A', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Usov, Yu V']",['Measurement of the decay $\\phi\\rightarrow \\mu^{+} \\mu^{-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'muon, pair production', 'Phi(1020), electroproduction', 'Phi(1020), leptonic decay', 'Phi(1020), branching ratio', 'Phi(1020), electromagnetic decay', 'channel cross section, energy dependence', 'experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> muon+ muon-', '0.984-1.020 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905030'],['The process e^+e^- ->mu^+mu^- has been studied with SND detector at VEPP-2M e^+e^- collider in the vicinity of phi(1020) resonance. The product of branching ratios of phi meson into leptons \\sqrt{B(phi->mu^+mu^-) B(phi-> e^+e^-)}=(3.14+-0.22+-0.14)x10^{-4} was measured from the interference in the cross section of the process e^+e^- ->mu^+mu^-. The branching ratio B(phi->mu^+mu^-)=(3.30+-0.45+-0.32)x10^{-4} was obtained.'],['1999-05-20']
1376,['eng'],"['Surdo, A']",['Low Energy Atmospheric Neutrino Events in MACRO'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'neutrino, cosmic radiation', 'neutrino, flux', 'neutrino nucleon, interaction', 'charged current', 'muon, angular distribution', 'neutrino, oscillation', 'deep underground detector, MACRO', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905028', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h4_1_06.pdf']","['The flux of low energy atmospheric neutrinos (E_nu ~ 4 GeV) has been studied with the MACRO detector at Gran Sasso by detecting nu_mu interactions inside the apparatus, and by upward-going stopping muons. The updated analysis of the data collected until now with the complete apparatus will be presented. The results show a deficit of the measured number of events in an uniform way over the whole zenith angle with respect to Monte Carlo predictions. The deficit and the angular distributions, when interpreted in terms of neutrino oscillations, are consistent with the MACRO results on the much higher energy upward throughgoing muons (E_nu ~ 100 GeV).']",['1999-05-19']
1377,['eng'],"['Vannerem, P', 'Müller, K R', 'Schölkopf, B', 'Smola, A J', 'Söldner-Rembold, S']",['Classifying LEP Data with Support Vector Algorithms'],['Particle Physics - Experimental Results'],"['talk, Heraklion 1999/04/12', 'data analysis method, efficiency', 'neural network', 'mathematical methods, support vector machine', 'electron positron, annihilation', 'quark, pair production', 'particle identification, charm', 'quark, fragmentation', 'hadron, multiple production', 'muon, particle identification', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905027'],"['We have studied the application of different classification algorithms in the analysis of simulated high energy physics data. Whereas Neural Network algorithms have become a standard tool for data analysis, the performance of other classifiers such as Support Vector Machines has not yet been tested in this environment. We chose two different problems to compare the performance of a Support Vector Machine and a Neural Net trained with back-propagation: tagging events of the type e+e- -> ccbar and the identification of muons produced in multihadronic e+e- annihilation events.']",['1999-05-18']
1378,['eng'],"['Giglietto, N']",['Moon and Sun Shadowing Observed by the MACRO Detector'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'muon, cosmic radiation', 'shadowing, lunar', 'shadowing, solar', 'cosmic radiation, primary', 'magnetic field, effect', 'angular resolution', 'deep underground detector, MACRO', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905026', 'http://krusty.physics.utah.edu/~icrc1999/root/vol7/s3_2_38.pdf']","[""Using over 40 million muons collected since 1989 by the MACRO detector we have searched for a depletion of muons coming from the direction of the Moon due to primary cosmic rays striking the Moon. We observe this Moon shadow in the expected position with a statistical significance of more than 5 standard deviations. We have analyzed the same data for an analogous Sun shadow, and have found a signal with a significance of about 4 standard deviations. The Sun shadow is displaced from the Sun's position by about 0.6 degrees North in ecliptic coordinates. This displacement is compatible with a deflection of primary cosmic rays due to the Interplanetary Magnetic Field in the 10-20 TeV primary energy range which is relevant to the underground muons observed by MACRO.""]",['1999-05-18']
1379,['eng'],"['Ronga, F']",['Neutrino Oscillations at High Energy by MACRO'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'neutrino nucleon, interaction', 'charged current', 'muon, angular distribution', 'neutrino/mu', 'neutrino/tau', 'neutrino, sterile', 'deep underground detector, MACRO', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905025', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h4_1_07.pdf']","[""We present updated results of the measurement of upward-going muons produced by neutrino interactions in the rock below the MACRO detector. These data support MACRO's previously published results. They favor a neutrino oscillation explanation of the atmospheric neutrino anomaly.""]",['1999-05-18']
1380,['eng'],"['Abbott, B']",['The $b\\overline{b}$ Production Cross Section and Angular Correlations in $p\\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1999/03/20', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'angular correlation, (quark antiquark)', 'quantum chromodynamics, perturbation theory', 'muon, transverse momentum', 'final state, dimuon', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905024'],"['We present measurements of the b-bbar production cross section and angular correlations using the D0 detector at the Fermilab Tevatron p-pbar Collider operating at sqrt(s) = 1.8 TeV. The b quark production cross section for |y(b)|<1.0 and p_T(b)>6 GeV/c is extracted from single muon and dimuon data samples. The results agree in shape with the next-to-leading order QCD calculation of heavy flavor production but are greater than the central values of these predictions. The angular correlations between b and bbar quarks, measured from the azimuthal opening angle between their decay muons, also agree in shape with the next-to-leading order QCD prediction.']",['1999-05-17']
1381,['eng'],"['Choudhary, B C', 'Ambrosio, M']",['Search for Magnetic Monopoles with MACRO'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'search for, magnetic monopole', 'flux, upper limit', 'velocity, dependence', 'search for, Q-ball', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905023'],"['Data from the complete MACRO detector have been used to search for magnetic monopoles (MMs) of all expected velocities. Scintillator, streamer tube (instrumented with specialized electronics) and nuclear track detectors have been used to search for signatures coming from MMs; the scintillator and nuclear track subdetectors were used also for searches for other rare particles (nuclearites, charged Q-balls). Based on no observation of such signals, we establish strigent flux limits, for MMs as slow as a few 10^-5c.']",['1999-05-17']
1382,['eng'],"['Akhmetshin, R R', 'Anashkin, E V', 'Arpagaus, M', 'Aulchenko, V M', 'Banzarov, V S', 'Barkov, L M', 'Baru, S E', 'Bashtovoy, N S', 'Bondar, A E', 'Bondarev, D V', 'Bragin, A V', 'Chernyak, D V', 'Chertovskikh, A G', 'Dvoredsky, A P', 'Eidelman, S I', 'Fedotovich, G V', 'Gabyshev, N I', 'Grigoriev, D N', 'Ivanov, P M', 'Karpov, S V', 'Khazin, B I', 'Koop, I A', 'Kurdadze, L M', 'Kuzmin, A S', 'Logashenko, I B', 'Lukin, P A', 'Mikhailov, Yu K', 'Nesterenko, I N', 'Okhapkin, V S', 'Perevedentsev, E A', 'Popov, A S', 'Purlatz, T A', 'Root, N I', 'Ruban, A A', 'Ryskulov, N M', 'Shamov, A G', 'Shatunov, Yu M', 'Shekhtman, A I', 'Shwartz, B A', 'Sidorov, V A', 'Skrinsky, A N', 'Smakhtin, V P', 'Snopkov, I G', 'Solodov, E P', 'Stepanov, P Yu', 'Sukhanov, A Yu', 'Titov, V M', 'Yudin, Yu V', 'Zverev, S G', 'Thompson, J A']",['Observation of $K_{S}^{0}$ semileptonic decays with CMD-2 detector'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'K0, pair production', 'K0(S), semileptonic decay', 'K0(S), branching ratio', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> K0(L) K0(S)', 'K0(S) --> pi electron neutrino', '1.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905022'],"['The decay $K_S^0 \\to \\pi e \\nu$ has been observed by the CMD-2 detector at the e^+e^- collider VEPP-2M at Novosibirsk. Of 6 million produced $K_L^0K_S^0$ pairs, $75 \\pm 13$ events of the $K_S^0 \\to \\pi e \\nu$ decay were selected. The corresponding branching ratio is $B(K_S^0 \\to \\pi e \\nu)=(7.2 \\pm 1.4)\\times10^{-4}$. This result is consistent with the evaluation of $B(K_S^0 assuming $\\Delta S=\\Delta Q$ .']",['1999-05-17']
1383,['eng'],"['Montaruli, T', 'Ambrosio, M']",['Search for WIMPS using Upward-Going Muons in MACRO'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'WIMP, search for', 'supersymmetry', 'neutralino, annihilation', 'neutrino, production', 'neutrino nucleon, interaction', 'meson, angular distribution', 'neutrino, background', 'flux, upper limit', 'mass, dependence', 'deep underground detector, MACRO', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905021', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h5_1_03.pdf']",['We present updated results on the search for a neutrino signal from the core of the Earth and of the Sun induced by Weakly Interacting Massive Particles (WIMPs). In this paper we concentrate on neutralinos as WIMP candidates. The 971 and 642 events used respectively for the search from the Sun and from the Earth are compatible with the background of atmospheric neutrinos. Consequently we calculate flux limits for various search cones around these sources. Limits as a function of the neutralino mass are given and compared to the supersymmetric (SUSY) models.'],['1999-05-14']
1384,['eng'],"['Montaruli, T', 'Ambrosio, M']",['MACRO as a Telescope for Neutrino Astronomy'],['Particle Physics - Experimental Results'],"['talk, Salt Lake City 1999/08/17', 'neutrino, cosmic radiation', 'cosmic radiation, particle source', 'astrophysics', 'neutrino nucleon, interaction', 'muon, angular distribution', 'photon, showers', 'correlation, space-time', 'flux, upper limit', 'deep underground detector, MACRO', 'deep underground detector, Gran Sasso', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905020', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h4_2_03.pdf']","['We use a sample of 990 upward-going muons, induced primarily by atmospheric neutrinos, to search for neutrinos of astrophysical origin. No evidence has been found using the event direction information. Flux limits of the order of 10^-15 cm^-2 s^-1 are imposed on current models for candidate point-sources. A space-time correlation search has been undertaken between 2328 BATSE gamma ray bursts (GRBs) and MACRO upward-going muons.']",['1999-05-14']
1385,['eng'],"['Montaruli, T', 'Ambriola, M']",['Capabilities of an Underwater Detector as a Neutrino Telescope and for the Neutrino Oscillation Search'],['Detectors and Experimental Techniques'],"['talk, Salt Lake City 1999/08/17', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'Cherenkov counter, water', 'deep underground detector, water']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905019', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h6_3_06.pdf']",['We report on the results of a Monte Carlo simulation study of a km^3 scale deep underwater Cherenkov detector aimed at detecting neutrinos of astrophysical origin. This analysis has been undertaken as part of the NEMO R&D project to develop such an experiment close to the Southern Italian coasts. We have studied the reconstruction capabilities of various arrays of phototubes in order to determine the detector geometries which optimize performance and cost. We have also investigated the possibility of designing a detector with characteristics suited to an experiment on atmospheric neutrino oscillations.'],['1999-05-14']
1386,['eng'],"['Mazziotta, M N']",['Transition Radiation Detector in MACRO'],['Detectors and Experimental Techniques'],"['talk, Salt Lake City 1999/08/17', 'cosmic radiation', 'showers, air', 'muon, counters and detectors', 'muon, energy spectrum', 'transition radiation detector', 'deep underground detector, MACRO']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905018', 'http://krusty.physics.utah.edu/~icrc1999/root/vol2/h3_2_13.pdf']","[""The MACRO detector is located in the Gran Sasso Laboratory. MACRO's overburden varies from 3150 to 7000 hg/cm^2. A transition radiation detector (TRD) has been added to the MACRO detector in order to measure the residual energy of muons entering MACRO, i.e. the energy they have after passing through the Gran Sasso's rock overburden. The TRD consists of three identical modules with a total horizontal area of 36 m^2. The results presented here are referred to single and double events in MACRO with one muon crossing one of the TRD modules. Our data show that double muons are more energetic than single ones, as predicted by the interaction models of primary cosmic rays with the atmosphere.""]",['1999-05-14']
1387,['eng'],"['Palla, Fabrizio']",['Recent Results on Heavy Flavours with ALEPH'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'quark, radiative decay', 'Kobayashi-Maskawa angle', 'B/s0, mass difference', 'B/s0, hadronic decay', 'D/s, hadronic decay', 'D/s*(2110), hadronic decay', 'final state, (2Phi(1020))', 'B/s0, lifetime', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'beauty --> up lepton neutrino anything', 'beauty --> strangeness photon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905017'],"['The latest ALEPH measurements on heavy flavours are presented. In particular the measurements of V_ub, the B(b -> s gamma) and a study on the width difference between mass eigenstates in the B_s system are presented.']",['1999-05-12']
1388,['eng'],"['Scholberg, K']",['Atmospheric Neutrinos at Super-Kamiokande'],['Particle Physics - Experimental Results'],"['talk, Venice 1999/02/23', 'neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino, flux', 'neutrino nucleon, interaction', 'charged current', 'neutrino/mu', 'neutrino/tau', 'neutrino, sterile', 'neutrino, mass difference', 'neutrino, mixing angle', 'muon, angular distribution', 'electron, angular distribution', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905016'],"['In 1998, the Super-Kamiokande announced evidence for the observation of neutrino oscillations based on measurements of the atmospheric neutrino flux. This paper presents the updated results for fully and partially-contained events with 736 days of data, as well as upward-going muon results and a global analysis. Preliminary interpretations of the results in terms of various two-flavor oscillation hypotheses are presented.']",['1999-05-12']
1389,['eng'],"['Komatsubara, T K']",['Status of the Study of the Rare Decay $K^{+} \\to \\pi^{+} \\nu \\overline{\\nu}$ at BNL'],['Particle Physics - Experimental Results'],"['talk, Cape Town 1999/01/24', 'K+, rare decay', 'neutrino, pair production', 'neutral current, flavor changing', 'K+, branching ratio', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905014'],['The current status of the experimental study of the rare kaon decay K^+ \\to collaborations is reported.'],['1999-05-11']
1390,['eng'],"['Woods, M']",['Electroweak Results from the SLD Experiment'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 1999/02/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, leptonic decay', 'Z0, hadronic decay', 'fermion, pair production', 'quark, beauty', 'Weinberg angle', 'correction, oblique', 'angular distribution, asymmetry', 'polarization, asymmetry', 'semiconductor detector, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905015'],"['We present an overview of the electroweak physics program of the SLD experiment at the Stanford Linear Accelerator Center (SLAC). A data sample of 550K Z0 decays has been collected. This experiment utilizes a highly polarized electron beam, a small interaction volume, and a very precise pixel vertex detector. We present a preliminary result for the weak mixing angle, sin2(thetaw)=0.23110 +- 0.00029. We also present a preliminary result for the parity violating parameter, A_b = 0.898 +- 0.029. These measurements are used to test for physics beyond the Standard Model.']",['1999-05-11']
1391,['eng'],"['Brooks, M L', 'Chen Young Kai', 'Cooper, M D', 'Cooper, P S', 'Dzemidzic, M', 'Empl, A', 'Gagliardi, C A', 'Hogan, G E', 'Hughes, E B', 'Hungerford, E V', 'Jui, C', 'Knott, J E', 'Koetke, D D', 'Lan, K A', 'Manweiler, R', 'Mayes, B', 'Mischke, R E', 'Piilonen, L E', 'Stanislaus, T D S', 'Stantz, K M', 'Szymanski, J J', 'Tribble, R E', 'Tu, X L', 'Van Ausdeln, L A', 'Von Witsch, W H', 'Wright, S C', 'Ziock, K O H', 'Kroupa, M A']",['New Limit for the Family-Number Non-conserving Decay $\\mu^{+} \\to e^{+}_{\\gamma}$'],['Particle Physics - Experimental Results'],"['muon+, radiative decay', 'violation, flavor', 'photon, energy spectrum', 'positron, energy spectrum', 'muon+, branching ratio', 'upper limit', 'experimental results', 'LAMPF Linac', 'muon+ --> positron photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905013'],['An experiment has been performed to search for the muon- and electron-number non-conserving decay mu+ to e+_gamma. The upper limit for the branching ratio to be GAMMA(mu+ to e+_gamma)/GAMMA(mu+ to e+_nu_nubar) < 1.2e-11 with 90% confidence.'],['1999-05-10']
1392,['eng'],"['Bellotti, R', 'Cafagna, F', 'Circella, M', 'De Marzo, C', 'Golden, R L', 'Stochaj, S J', 'De Pascale, M P', 'Morselli, A', 'Picozza, P', 'Stephens, S A', 'Hof, M', 'Menn, W', 'Simon, M', 'Mitchell, J W', 'Ormes, J F', 'Streitmatter, R E', 'Finetti, N', 'Grimani, C', 'Papini, P', 'Piccardi, S', 'Spillantini, P', 'Basini, G', 'Ricci, M']",['Balloon Measurements of Cosmic Ray Muon Spectra in the Atmosphere along with those of Primary Protons and Helium Nuclei over Mid-Latitude'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'cosmic radiation, energy spectrum', 'cosmic radiation, primary', 'p, cosmic radiation', 'helium, cosmic radiation', 'cosmic radiation, flux', 'muon+ muon-, ratio', 'muon-, momentum spectrum', 'magnetic field, geophysics', 'counters and detectors, satellite', 'magnetic spectrometer, experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905012'],"['We report here the measurements of the energy spectra of atmospheric muons and of the cosmic ray primary proton and helium nuclei in a single experiment. These were carried out using the MASS superconducting spectrometer in a balloon flight experiment in 1991. The relevance of these results to the atmospheric neutrino anomaly is emphasized. In particular, this approach allows uncertainties caused by the level of solar modulation, the geomagnetic cut-off of the primaries and possible experimental systematics to be decoupled in the comparison of calculated fluxes of muons to measured muon fluxes. The muon observations cover the momentum and depth ranges of 0.3-40 GeV/c and 5-886 g/cmsquared, respectively. The proton and helium primary measurements cover the rigidity range from 3 to 100 GV, in which both the solar modulation and the geomagnetic cut-off affect the energy spectra at low energies.']",['1999-05-10']
1393,['eng'],"['Alves, G A']",['Diffractive Results from the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'final state, (2jet)', 'diffraction', 'rapidity, gap', 'pomeron, exchange', 'color, singlet', 'exchange, (2pomeron)', 'rapidity dependence', 'transverse energy, dependence', 'energy dependence', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905009'],"['Hard diffraction in events with dijets and rapidity gaps has been studied by diffraction, and hard double pomeron exchange, using Tevatron $\\bar pp$ data at several models.']",['1999-05-07']
1394,['eng'],"['Eisenberg, Y']",['Charm Photoproduction in e-p Collisions at HERA'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'D*(2010), photoproduction', 'D*(2010), hadronic decay', 'quantum chromodynamics, perturbation theory', 'color, singlet', 'color, octet', 'differential cross section, transverse momentum', 'differential cross section, rapidity dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> D*(2010) positron anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K- pi+ 2pi-', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905008'],"['We report the latest results of the ZEUS collaboration on the photoproduction of D* mesons in a wide W range. The results are compared with several recent NLO pQCD calculations. The differential cross-sections in a restricted kinematical region are higher then the NLO calculations, in particular in the forward (proton) direction. A recent pQCD model (BKL) describes the data reasonably well.']",['1999-05-06']
1395,['eng'],"['Tanimori, T', 'Nishi, Y', 'Ochi, A', 'Nishi, Y']",['Imaging Gaseous Detector based on Micro Processing Technology'],['Particle Physics - Experimental Results'],"['talk, Nara 1998/12/04', 'counters and detectors, gas', 'counters and detectors, imaging', 'readout, microstrip']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905006'],"['The development of gaseous detectors has been exciting again since the appearance of a MicroStrip Gas Chamber(MSGC) in 1988, which is made using a micro-electronics technology. These days lots of variations of the advanced gaseous detectors are being intensively studied in the world. We have developed the two-dimensional MSGC having a 10 cm square detection area and the ultra fast readout system for a real time X-ray imaging. The MSGC was made using Multi-Chip Module (MCM) technology, and has a very thin substrate of 17 $\\mu$m, lots of thin anodes and back strips both with 200 both the timing and an energy of each X-ray photon. In addition, an intermediate gas multiplier has been realized using a capillary plate having a conductive surface of a capillary. The MSGC combined with the conductive capillary plate can be steadily operated with a high gain under intense irradiation. Here we also report new approaches of X-ray crystal structure analyses using timing information obtained by the MSGC.']",['1999-05-06']
1396,['eng'],[],['Studies of WW and WZ Production and Limits on Anomalous WW$\\gamma$ and WWZ Couplings'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, pair production', 'coupling, (Z0 2W)', 'coupling, (2W photon)', 'intermediate boson, leptonic decay', 'intermediate boson, hadronic decay', 'final state, (3lepton neutrino)', 'final state, (2jet muon neutrino)', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', 'anti-p p --> Z0 W anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905005'],"['Evidence of anomalous WW and WZ production was sought in pbar{p} collisions at a center-of-mass energy of sqrt(s) = 1.8 TeV. The final states $WW (WZ) to mu-nu-jet-jet + X, WZ to mu-nu-e-e + X and WZ to e-nu-e-e + X were studied using a data sample corresponding to an integrated luminosity of approximately 90 pb-1. No evidence of anomalous diboson production was found. Limits were set on anomalous WWgamma and WWZ couplings and were combined with our previous results. The combined 95% confidence level anomalous coupling limits for Lambda=2 TeV are -0.25 LE Delta-kappa LE 0.39 (lambda=0) and -0.18 LE lambda LE 0.19 (Delta \\kappa = 0), assuming the WWgamma couplings are equal to the WWZ couplings.']",['1999-05-05']
1397,['eng'],[],['Search for the Flavor-Changing Neutral Current Decays $B^{+} \\rightarrow \\mu^{+}\\mu^{-} K^{+}$ and $B^{0}\\rightarrow \\mu^{+}\\mu^{-} K^{*0}$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B, hadroproduction', 'B, semileptonic decay', 'K*(892)', 'neutral current, flavor changing', 'B+, branching ratio', 'B0, branching ratio', 'upper limit', 'mass spectrum, (K*(892) muon+ muon-)', 'mass spectrum, (K+ muon+ muon-)', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B+ --> K+ muon+ muon-', 'B0 --> K*(892) muon+ muon-', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905004'],"['We report on a search for the flavor-changing neutral current decays B^+ -> mu^+ mu^- K^+ and B^0 -> mu^+ mu^- K^{*0} using 88 pb^{-1} of data from p-pbar collisions at \\sqrt{s}=1.8 TeV, collected with the Collider Detector at Fermilab. Finding no evidence for these decays, we set upper limits on the branching fractions B(B^+ -> mu^+ mu^- K^+) < 5.2x10^{-6} and B(B^0 -> mu^+ mu^-K^{*0}) < 4.0x10^{-6} at the 90% confidence level.']",['1999-05-05']
1398,['eng'],"['Dorofeev, V']",['New results from VES'],['Particle Physics - Experimental Results'],"['talk, Rome 1999/03/08', 'pi- nucleus, nuclear reaction', 'beryllium', 'final state, (pi+ 2pi-)', 'final state, (omega(783) pi- pi0)', 'omega(783), hadroproduction', 'partial wave analysis', 'f2(1270)', 'pi2(1670)', 'a3(2050)', 'a4(2040)', 'magnetic spectrometer, experimental results', 'Serpukhov PS', 'pi- beryllium --> beryllium pi+ 2pi-', 'pi- beryllium --> beryllium omega(783) pi- pi0', 'omega(783) --> pi+ pi- pi0', '37 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905002'],"[""The results of the patial wave analysis(PWA) of the pi+pi-pi- and omegapi-pi0 systems are presented. The a3 and a4(2040) signals are observed in the rho(770)pi and f2(1270)pi channels. Indications of the a1' meson existence was found in the 1+0+ rhopi S-wave. The decay branching ratio of the a2(1320)- to omegapi-pi0 was measured. The 2+1+ wave shows a broad bump at M~1.7GeV. The decays of the pi2(1670), a4(2040) and pi(1740) into omegarho- were found. The resonance in the b1(1235)pi wave with exotic quantum numbers jpc=1-+ at M~1.6 is observed and the simultaneous analysis of the 1-+ wave in the b1(1235)pi, etha'pi and rhopi final states is presented.""]",['1999-05-04']
1399,['eng'],"['Dorofeev, V', 'Bugg, D V']",['Natural parity resonances in the $\\eta \\pi^{+} \\pi^{-}$ and $\\omega \\omega$'],['Particle Physics - Experimental Results'],"['talk, Rome 1999/03/08', 'pi- p, charge exchange', 'meson, multiple production', 'pi', 'eta', 'omega(783)', 'mass spectrum, (eta pi+ pi-)', 'mass spectrum, (2omega(783))', 'partial wave analysis', 'new particle, f2(1565)', 'f4(2050)', 'new particle, f2(1950)', 'f4(2300)', 'meson resonance, mass', 'meson resonance, width', 'magnetic spectrometer, experimental results', 'Serpukhov PS', '37 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905001'],"['Results of the ethapi+pi- and omegaomega final state partial wave analysis(PWA) are presented. The mass-independent and the mass-dependent PWA were performed. The ethapi+pi- system PWA results in the observation of the resonances in the JPC=1--,3--,2++ and 4++ waves. The results of the omegaomega system PWA confirms the existence of the f2(1565) and f4(2050). The f2(1950) is observed. There is evidence for a f4(2300) meson.']",['1999-05-04']
1400,['eng'],"['Ootani, W', 'Minowa, M', 'Miuchi, K', 'Inoue, Y', 'Watanabe, T', 'Yoshida, M', 'Ito, Y', 'Ootuka, Y']",['First Results from Dark Matter Search Experiment in the Nokogiriyama Underground Cell'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'WIMP, search for', 'scattering, neutralino p', 'neutralino, mass', 'channel cross section, upper limit', 'energy spectrum', 'bolometer, experimental results', 'lithium, fluorine']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904034'],"['An experiment to search for hypothetical particle dark matter using cryogenic thermal detector, or bolometer is ongoing. The bolometer consists of eight pieces of 21 g LiF absorbers and sensitive NTD germanium thermistors attached to them and is installed in the Nokogiriyama underground cell which is a shallow depth site ($\\sim 15$ m w.e.). We report on the results from the first running for about ten days using this arrayed bolometer system together with appropriate shieldings and muon veto counters. From the obtained energy spectra the exclusion limits for the cross section of the elastic neutralino-proton scattering are derived under commonly accepted astrophysical assumptions. The sensitivity for the light neutralino with a mass below 5 GeV is improved by this work.']",['1999-05-03']
1401,['eng'],"['Gratta, Giorgio']",['Neutrino Oscillation Experiments at Nuclear Reactors'],['Particle Physics - Experimental Results'],"['talk, Cape Town 1999/01/24', 'neutrino, oscillation', 'fission, particle source', 'neutrino, cosmic radiation', 'neutrino, mass difference', 'neutrino, mixing angle', 'antineutrino p, interaction', 'antineutrino/e', 'charged current', 'MSW effect', 'scintillation counter, liquid', 'deep underground detector', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905011'],"['In this paper I give an overview of the status of neutrino oscillation experiments performed using nuclear reactors as sources of neutrinos. I review the present generation of experiments (Chooz and Palo Verde) with baselines of about 1 km as well as the next generation that will search for oscillations with a baseline of about 100 km. While the present detectors provide essential input towards the understanding of the atmospheric neutrino anomaly, in the future, the KamLAND reactor experiment represents our best opportunity to study very small mass neutrino mixing in laboratory conditions. In addition KamLAND with its very large fiducial mass and low energy threshold, will also be sensitive to a broad range of different physics.']",['1999-05-07']
1402,['eng'],"['Dissertori, G']",['Event shapes and power corrections in $e^{+}e^{-}$ annihilations'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1999/04/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'hadron, multiple production', 'event shape analysis', 'correction, nonperturbative', 'jet, thrust', 'jet, mass', 'c-parameter', 'correction, Monte Carlo', 'energy dependence', 'experimental results', 'CERN LEP Stor', '14-189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904033'],['Hadronic final states in e+e- annihilitions at centre-of-mass energies from 14GeV up to 189GeV are studied in order to test recent predictions for power corrections to the mean values as well as the distributions of event shape variables.'],['1999-04-30']
1403,['eng'],[],['Nuclearite search with the MACRO detector at Gran Sasso'],['Particle Physics - Experimental Results'],"['nuclear matter, strangeness', 'cosmic radiation, flux', 'upper limit', 'scintillation counter, liquid', 'plastics, track sensitive', 'experimental results', 'deep underground detector, MACRO']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904031'],"['In this paper we present the results of a search for nuclearites in the penetrating cosmic radiation using the scintillator and track-etch subdetectors of the MACRO apparatus. The analyses cover the beta =v/c range at the detector depth (3700 hg/cm^2) 10^-5 < beta < 1; for beta = 2 x 10^-3 the flux limit is 2.7 x 10^-16 cm^-2 s^-1 sr^-1 for an isotropic flux of nuclearites, and twice this value for a flux of downgoing nuclearites.']",['1999-04-29']
1404,['eng'],"['Maxfield, S J', 'Pötter, B', 'Sinclair, L']",['Jet Cross Sections at HERA'],['Particle Physics - Experimental Results'],"['talk, Durham 1998/09/20', 'positron p, colliding beams', 'positron p, inclusive reaction', 'jet, electroproduction', 'jet, photoproduction', 'final state, (2jet)', 'final state, (3jet)', 'photon, structure function', 'momentum spectrum, parton', 'differential cross section, mass', 'momentum transfer, dependence', 'transverse momentum, dependence', 'color, coherence', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904030'],['Since the start of HERA operation there has been considerable progress in the understanding of jet production in e p collisions. QCD calculations are now able to accommodate the hadronic structure of the virtual photon. The luminosities delivered by HERA are now sufficient to allow studies of final states in which more than two high transverse energy jets are produced. The transition between jet processes in photoproduction and in deep inelastic scattering has been studied in some detail. These advances are highlighted here.'],['1999-04-29']
1405,['eng'],"['Maisheev, V A']",['Birefringence of high-energy $\\Gamma$ - quanta in the single crystals'],['Detectors and Experimental Techniques'],"['photon nucleus, interaction', 'silicon, crystal', 'polarization', 'birefringence', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904029'],['Problems of the experimental observation of the birefringence of high-energy gamma-quanta propagating in single crystals are discussed.'],['1999-04-29']
1406,['eng'],"['Johnson, R A', 'Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bguel, L', 'Conrad, J', 'Drucker, R B', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Koutsoliotas, S', 'Kim, J H', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McNulty, C', 'McFarland, K S', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Vakili, M', 'Vaitaitis, A G', 'Wu, V', 'Yang, U K', 'Yu, J', 'Zeller, G P']",['Measurement of $sin^{2} \\theta_{W}$ in $\\nu N$ Scattering from NuTeV'],['Particle Physics - Experimental Results'],"['talk, Cape Town 1999/01/24', 'neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'Weinberg angle', 'W, mass', 'experimental results', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904028'],"['We report the measurement of sin^2 theta_W in nu N deep inelastic scattering from the NuTeV experiment. By using separate neutrino and anti-neutrino beams, NuTeV is able to determine sin^2 theta_W with smaller systematic and similar or smaller statistical errors when compared to previous neutrino experiments. NuTeV measures sin^2 theta_W (on-shell) = 0.2253 +/- 0.0019(stat.) +/- 0.0010(sys.), which implies M_W = 80.26 +/- 0.11 GeV/c^2.']",['1999-04-27']
1407,['eng'],"['Akhmetshin, R R']",['Measurement of $e^{+}e^{-} \\to \\pi^{+}\\pi^{-}$ cross section with CMD-2 around $\\rho(770)$ meson'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'pi, pair production', 'pi, form factor', 'rho(770), mass', 'rho(770), width', 'interference, (omega(783) rho(770))', 'omega(783), hadronic decay', 'omega(783), branching ratio', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> pi+ pi-', '0.61-0.96 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904027'],"['In experiments with the CMD-2 detector at the VEPP-2M electron-positron collider at Novosibirsk about 150000 $e^+e^-\\to\\pi^+\\pi^-$ events were recorded in the center-of-mass energy range from 0.61 up to 0.96 GeV. The result of the pion form factor measurement with a 1.4% systematic error is presented. The following values of the $\\rho$-meson and $\\rho-\\omega$ interference parameters were found: $M_\\rho=(775.28\\pm 0.61\\pm 0.20) MeV, \\Gamma_\\rho=(147.70\\pm 1.29 Br(\\omega\\to\\pi^+\\pi^-) = (1.32\\pm 0.23)%$.']",['1999-04-27']
1408,['eng'],"['Thompson, J A']",['$K^{+}\\to\\pi^{+}\\mu^{+}\\mu^{-}$ in E865 at BNL'],['Particle Physics - Experimental Results'],"['talk, Cape Town 1999/01/24', 'K+, semileptonic decay', 'K+, branching ratio', 'form factor, slope', 'perturbation theory, chiral', 'validity test', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ muon+ muon-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904026'],"['Preliminary values for the K+ -> pi+ mu+ mu- branching ratio and form factor are reported, based on 400 events, a factor of 2 more in total events and 100 times the present world sample of fully reconstructed events. The results are consistent with previous results on the pi+ e+ e- mode. However, the relatively large slope of the form factor in q^2, lambda = 0.182+/-0.01+/-0.007, required to fit the pi+ e+ e- data and to give consistency between the pi+ e+ e- and pi+ mu+ mu- branching ratios, is larger than expected in simple models of the decays. The K+ -> pi+ mu+ mu- branching ratio we find, (9.23 +/- 0.6 stat +/- 0.58 syst)x10^-8, is the most precise measurement of this mode and is approximately 3.2 sigma larger than the previous measurement. These pi+ l+ l- results are inconsistent with O(p^4) Chiral Perturbation Theory but compatible with O(p^6). Systematic studies for both modes are still in progress.']",['1999-04-27']
1409,['eng'],"['Narsky, I']",['Estimation of Upper Limits Using a Poisson Statistic'],['Detectors and Experimental Techniques'],"['statistical analysis', 'upper limit', 'tau, radiative decay', 'tau, branching ratio', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904025'],"['Bayesian, classical, and extended maximum likelihood approaches to estimation of upper limits in experiments with small numbers of signal events are surveyed. The discussion covers only experiments whose outcomes are well described by a Poisson statistic. A new approach, based on the statistical significance of a signal rather than on the number of events in the signal region, is proposed. A toy model and an example of a recent search for the lepton number violating decay $\\tau\\to\\mu\\gamma$ are used to illustrate application of the discussed techniques.']",['1999-04-26']
1410,['eng'],"['Akhmetshin, R R']",['$a_{1}(1260)\\pi$ dominance in the process $e^{+} e^{-} \\to 4\\pi$ at energies 1.05-1.38 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'pi, multiple production', 'final state, (4pi)', 'channel cross section, energy dependence', 'intermediate state, (a1(1260) pi)', 'intermediate state, (omega(783) pi)', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> pi+ pi- 2pi0', 'electron positron --> 2pi+ 2pi-', '1.05-1.38 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904024'],"['First results of the study of the process e+e- \\to 4\\pi by the CMD-2 collaboration at VEPP-2M are presented for the energy range 1.05-1.38 GeV. Using an integrated luminosity of 5.8 pb^{-1}, energy dependence of the processes e+e- \\to \\pi^+\\pi^-2\\pi^0 and e+e- \\to 2\\pi^+2\\pi^- has been measured. Analysis of the differential distributions demonstrates the dominance of the a_1\\pi and ømega\\pi intermediate states. Upper limits for the contributions of other alternative mechanisms are also placed.']",['1999-04-23']
1411,['eng'],"['Abbott, B']",['Search for Second Generation Leptoquark Pairs Decaying to $\\mu\\nu + jets$ in $p-\\overline{p}$ Collisions at $sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, leptoquark', 'leptoquark, pair production', 'leptoquark, decay modes', 'final state, ((n)jet muon neutrino)', 'channel cross section, branching ratio', 'leptoquark, mass', 'lower limit', 'leptoquark, scalar', 'leptoquark, vector', 'leptoquark, coupling', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2leptoquark anything', 'leptoquark --> quark lepton', 'leptoquark --> quark neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904023'],"['We report on a search for second generation leptoquarks (LQ) produced in $p\\bar{p}$ collisions at sqrt{s} = 1.8 TeV using the D0 detector at Fermilab. Second generation leptoquarks are assumed to be produced in pairs and to decay to either \\mu or \\nu and either a strange or a charm quark (q). Limits are placed on \\sigma(p-pbar -> LQ-LQbar -> \\mu\\nu + jets) as a function of the mass of the leptoquark. For equal branching ratios to \\mu q and \\nu q, second generation scalar leptoquarks with a mass below 160 GeV/c^2, vector leptoquarks with anomalous minimal vector couplings with a mass below 240 GeV/c^2, and vector leptoquarks with Yang-Mills couplings with a mass below 290 GeV/c^2, are excluded at the 95% confidence level.']",['1999-10-22']
1412,['eng'],"['Bodek, Arie', 'Fan, Q', 'Lancaster, M', 'McFarland, K S', 'Yang, U K']",['Implication of W-boson Charge Assymmetry Measurements in $p\\overline{p}$ Collisions to Models for Charge Symmetry Violations in Parton Distributions'],['Particle Physics - Experimental Results'],"['anti-p p, inclusive reaction', 'W, hadroproduction', 'charge, asymmetry', 'p, structure function', 'quark, momentum spectrum', 'quark, sea', 'charge, symmetry breaking', 'neutrino nucleon, interaction', 'Weinberg angle', 'numerical calculations', 'interpretation of experiments, CDF']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904021'],"['A surprisingly large charge symmetry violation of the sea quarks in the nucleon has been proposed in a recent article by Boros et al. as an explanation of the discrepancy between neutrino (CCFR) and muon (NMC) nucleon structure function data at low x. We show that these models are ruled out by the published CDF W charge asymmetry measurements, which strongly constrain the ratio of d and u quark momentum distributions in the proton over the x range of 0.006 to 0.34. This constraint also limits the systematic error from possible charge symmetry violation in the determination of sin^2(theta) from nu-N scattering experiments.']",['1999-04-22']
1413,['eng'],"['Hayato, Y', 'Earl, M A']",['Search for proton decay through $p\\rightarrow \\overline{\\nu} K^{+}$ in a large water Cherenkov detector'],['Particle Physics - Experimental Results'],"['p, semileptonic decay', 'K+, decay modes', 'neutrino, cosmic radiation', 'background', 'p, lifetime', 'lower limit', 'Cherenkov counter, water', 'experimental results', 'deep underground detector, KAMIOKANDE', 'p --> K+ antineutrino', 'K+ --> muon+ neutrino/mu', 'K+ --> pi+ pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904020'],"['We present results of a search for proton decays, $p \\to \\bar{\\nu} K^+$, using data from a 33 kton$\\cdot$year exposure of the Super-Kamiokande detector. Two decay modes of the kaon, $K^+ \\to \\mu^+ \\nu_{\\mu}$ and $K^+ \\to \\pi^+ from atmospheric neutrinos; therefore a lower limit on the partial lifetime of the proton $\\tau / B(p \\to \\bar{\\nu} K^+)$ was found to be $6.7 \\times 10^{32}$ years at 90% confidence level.']",['1999-04-22']
1414,['eng'],"['Montgomery, H E']",['Physics with the Main Injector'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'proton synchrotron', 'p nucleus, inclusive reaction', 'nickel', 'anti-p, hadroproduction', 'neutrino, secondary beam', 'neutrino, oscillation', 'neutrino, mass difference', 'K0, decay modes', 'violation, CP', 'Kobayashi-Maskawa angle, unitarity', 'anti-p p, colliding beams', 'quark, beauty', 'quark, pair production', 'B, decay modes', 'electroweak interaction, symmetry breaking', 'W, mass', 'mass, truth', 'Higgs particle, mass', 'Higgs particle, search for', 'search for, technicolor', 'supersymmetry', 'numerical calculations', 'proposed experiment, Fermilab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904019'],"['The Main Injector is a new rapid cycling accelerator at Fermilab which is a source of protons to be used in antiproton production to enhance the luminosity of the Tevatron Collider and to provide extracted beams for use in a range of fixed target experiments. We discuss the current status of the accelerator and the physics which it enables. The physics ranges broadly over the standard model and beyond, from the search for neutrino mass to collider physics at the highest energy available today.']",['1999-04-21']
1415,['eng'],"['Campanelli, M']",['Physics of W bosons at LEP2'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, leptonic decay', 'W, hadronic decay', 'channel cross section, branching ratio', 'W, mass', 'channel cross section, energy dependence', 'Kobayashi-Maskawa angle', 'unitarity, validity test', 'coupling, (3gauge boson)', 'angular distribution', 'correlation, two-particle', 'boson, statistics', 'color, recombination', 'production, charm', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, OPAL', 'magnetic detector, L3', 'CERN LEP Stor', 'bibliography', '161, 172, 183, 189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904018'],"['After the first observations of W bosons in leptonic interactions, about 4000 WW candidate events per experiment have been collected at LEP2. This data allows the measurement of the WW production cross section at different centre-of-mass energies, as well as W decay branching fractions. The W hadronic branching fraction can be converted into a test of the unitarity of the CKM matrix, or into an indirect determination of the matrix element $|V_{cs}|$. A more direct measurement coming from charm tagging is also performed. The W mass has been measured via the cross section (in the threshold region) and the direct reconstruction of the W decay products, using different techniques to account for the distortions due to experimental effects. The main systematic error to the mass reconstruction in the fully hadronic channel comes from QCD effects like Color reconnections and Bose-Einstein correlations, extensively studied in WW events. In $e^+e^-$ collisions W pairs can be produced in s-channel via a three vector boson vertex, so a direct study of the trilinear gauge boson couplings is possible. Modification of WW cross section and distributions of W production and decay angles would be an indication of non-standard couplings, thus a first hint for the presence of new physics.']",['1999-04-20']
1416,['eng'],"['Rowson, P C']",['Precision Electroweak Measurements at the SLC'],['Particle Physics - Experimental Results'],"['talk, Cape Town 1999/01/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, leptonic decay', 'Z0, hadronic decay', 'angular distribution, asymmetry', 'polarization, asymmetry', 'quark, charm', 'quark, beauty', 'quark, pair production', 'Z0, branching ratio', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904016'],"['Preliminary SLD electroweak results based on essentially the complete 550K Z dataset are presented and interpreted, and some historical background is provided.']",['1999-04-20']
1417,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Search for R-Parity Violating Decays of Scalar Fermions at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'supersymmetry', 'sfermion, pair production', 'sfermion, decay modes', 'slepton', 'sneutrino', 'squark, truth', 'R parity, violation', 'LSP, decay', 'lepton, multiple production', 'jet, multiple production', 'sparticle, mass', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904015'],"['A search for pair produced scalar fermions with couplings that violate R-parity has been performed using a data sample corresponding to an integrated luminosity of 56 pb-1 at a centre-of-mass energy of sqrt{s}= 183 GeV collected with the OPAL detector at LEP. An important consequence of R-parity breaking interactions is that the lightest supersymmetric particle is expected to be unstable. Searches for R-parity violating decays of charged sleptons, sneutrinos and stop quarks have been performed under the assumptions that the lightest supersymmetric particle decays promptly and that only one of the R-parity violating couplings is dominant for each of the decay modes considered. Such processes would yield multi-leptons, jets plus leptons or multi-jets, with or without missing energy, in the final state. No significant excess of such events has been observed. Limits on the production cross-sections of scalar fermions in R-parity violating scenarios are obtained. Mass exclusion regions are also presented in the framework of the Constrained Minimal Supersymmetric Standard Model.']",['1999-04-20']
1418,['eng'],"['Appelshäuser, H']",['Event-by-event fluctuations of average transverse momentum in central Pb + Pb collisions at 158 GeV per nucleon'],['XX'],"['scattering, heavy ion', 'lead', 'charged particle, multiple production', 'transverse momentum, fluctuation', 'quantum chromodynamics', 'critical phenomena, chiral', 'model, nuclear reaction', 'model, thermodynamical', 'magnetic spectrometer, experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904014'],['We present first data on event-by-event fluctuations in the average transverse momentum of charged particles produced in Pb+Pb collisions at the CERN SPS. This measurement provides previously unavailable information allowing sensitive tests of microscopic and thermodynamic collision models and to search for fluctuations expected to occur in the vicinity of the predicted QCD phase transition. We find that the observed variance of the event-by-event average transverse momentum is consistent with independent particle production modified by the known two-particle correlations due to quantum statistics and final state interactions and folded with the resolution of the NA49 apparatus. For two specific models of non-statistical fluctuations in transverse momentum limits are derived in terms of fluctuation amplitude. We show that a significant part of the parameter space for a model of isospin fluctuations predicted as a consequence of chiral symmetry restoration in'],['1999-04-14']
1419,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couchman, J', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Harin-Dirac, M', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanaya, N', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lawson, I', 'Layter, J G', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Méndez-Lorenzo, P', 'Merritt, F S', 'Mes, H', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Okpara, A N', 'Oreglia, M J', 'Orito, S', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Quadt, A', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'Wetterling, D', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Zacek, V', 'Zer-Zion, D']",['Test of the Flavour Independence of $\\alpha_{s}$ using Next-to-Leading Order Calculations for Heavy Quarks'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'hadron, multiple production', 'particle identification, flavor', 'strong interaction, coupling constant', 'dependence, flavor', 'event shape analysis', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904013'],"['We present a test of the flavour independence of the strong coupling constant for charm and bottom quarks with respect to light (uds) quarks, based on a hadronic event sample obtained with the OPAL detector at LEP. Five observables related to global event shapes were used to measure alpha_s in three flavour tagged samples (uds, c and b). The event shape distributions were fitted by Order(alpha_s**2) calculations of jet production taking into account mass effects for the c and b quarks. We find: = 0.997 +- 0.038(stat.) +- 0.030(syst.) +- 0.012(theory) and = 0.993 +- 0.008(stat.) +- 0.006(syst.) +- 0.011(theory) for the ratios alpha_s(charm)/alpha_s(uds) and alpha_s(b)/alpha_s(uds) respectively.']",['1999-04-14']
1420,['eng'],"['Nodulman, L']",['Summary of Experimental Electroweak Physics'],['Particle Physics - Experimental Results'],"['review, Cape Town 1999/01/24', 'electroweak interaction, symmetry breaking', 'electron positron, annihilation', 'hadron hadron, interaction', 'lepton nucleon, interaction', 'Higgs particle, search for', 'muon, magnetic moment', 'Z0, mass', 'Z0, decay modes', 'angular distribution, asymmetry', 'tau, polarization', 'tau, decay modes', 'Weinberg angle', 'W, mass', 'W, decay modes', 'mass, truth', 'Higgs particle, mass', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904012'],"['Progress continues on many fronts of experimental testing of electroweak symmetry breaking. Updates were presented on LEP, SLC, Brookhaven g-2 ring, Tevatron Collider, HERA, CESR and Tevatron neutrino experiments. Perhaps most exciting is the Higgs search at LEP2, complementing the indirect constraints. However, the standard model with one Higgs doublet remains viable.']",['1999-04-13']
1421,['eng'],"['Kopp, S E']",['Studies of $B^{0}$ Decays for Measuring $sin(2\\beta)$'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'B0, branching ratio', 'Kobayashi-Maskawa angle', 'B0 anti-B0, interference', 'violation, CP', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> psi mesons K0', 'B0 --> psi mesons K*(892)', 'B0 --> J/psi(3100) pi0', 'B0 --> J/psi(3100) eta', 'B0 --> 2D*(2010)', 'B0 --> chi/c1(3510) K0(S)', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904009'],"['Future asymmetric e+e- --> Upsilon(4S) B factories are being constructed to search for CP violation in B0 decays. It is hoped that a CP asymmetry may be observed in B0-B0bar mixing in analogy with that found in neutral kaons. In this mixing measurement, B0 decays to CP eigenstates, such as the rare decay B0 psi Kshort, may provide information on the CKM angle sin(2beta). I discuss decay additional CP eigenstate branching ratios measured by the CLEO experiment that may be used by future B factories to measure sin(2beta).']",['1999-04-08']
1422,['eng'],"['Gao, Y', 'Würthwein, F']",['Charmless Hadronic B Decays at CLEO'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charm)', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> 2pseudoscalar meson', 'B --> vector meson pseudoscalar meson', 'B --> rho(770) pi', 'B --> K*(892) pi', 'B --> K pi0', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904008'],"['The CLEO collaboration has studied two-body charmless hadronic decays of $B$ mesons into final states containing two pseudo-scalar mesons, or a pseudo-scalar and a vector meson. We summarize and discuss results presented during the winter/spring 1999 conference season, and provide a brief outlook towards future attractions to come. In particular, CLEO presented preliminary results on the decays $B^\\pm \\to 10^{-5}$), $B\\to \\pi^\\pm\\rho^\\mp$ ($Br(B\\to K^{\\star\\mp}$ ($Br(B\\to \\pi^\\pm K^{\\star\\mp}) = (2.2^{+0.8+0.4}_{-0.6-0.5})\\times 10^{-5}$), and $B^\\pm \\to K^\\pm \\pi^0$ ($Br(B^\\pm \\to K^\\pm \\pi^0) = (1.5 \\pm 0.4 \\pm 0.3) \\times 10^{-5}$) at DPF99, APS99, APS99, and ICHEP98 respectively. None of these decays had been observed previously. The first two of these constitute the first observation of hadronic $b\\to u$ transitions. In addition, CLEO presented preliminary updates on a large number of previously published branching fractions and upper limits.']",['1999-04-08']
1423,['eng'],"['Tournefier, E']",['Electroweak results from the Z resonance cross-sections and leptonic forward-backward asymmetries with the ALEPH detector'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 1999/02/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'fermion, pair production', 'Z0, hadronic decay', 'Z0, leptonic decay', 'Z0, mass', 'Z0, width', 'channel cross section', 'angular distribution, asymmetry', 'coupling constant, vector', 'coupling constant, axial-vector', 'coupling constant, strong interaction', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904007'],['The measurement of the Z resonance parameters and lepton forward-backward asymmetries are presented. These are determined from a sample of 4.5 million Z decays accumulated with the ALEPH detector at LEP1.'],['1999-04-08']
1424,['eng'],"['Pepé-Altarelli, M']",['Higgs Searches and Prospects from LEP2'],['Particle Physics - Experimental Results'],"['talk, Cape Town 1999/01/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, mass', 'lower limit', 'Higgs particle, neutral particle', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, pair production', 'Higgs particle, hadronic decay', 'Higgs particle, leptonic decay', 'quark, beauty', 'tau', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904006'],"['The status of the search at LEP2 for the Higgs in the Standard Model (SM) and in the minimal supersymmetric extension of the Standard Model MSSM) is reviewed. A preliminary lower limit of 95.5/c^2 at 95% C.L. on the SM Higgs is obtained after a preliminary analysis of the data collected at sqrt(s)= 189 GeV. For standard choices of MSSM parameter sets, the search for the neutral Higgs bosons h and A leads to preliminary 95% C.L. exclusion lower limits of 83.5GeV/c^2 and 84.5 GeV/c^2, respectively.']",['1999-04-08']
1425,['eng'],"['Bravin, M', 'Bruckmayer, M', 'Bucci, C']",['The CRESST Dark Matter Search'],['Detectors and Experimental Techniques'],"['astrophysics, missing-mass', 'WIMP, search for', 'WIMP, mass', 'scattering, WIMP nucleon', 'channel cross section, mass', 'counters and detectors, superconducting', 'deep underground detector, Gran Sasso', 'numerical calculations', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904005'],"['The current status of CRESST (Cryogenic Rare Event Search using Superconducting Thermometers) and new results concerning the detector development are presented. The basic technique of CRESST is to search for particle Dark Matter (WIMPS, Weakly Interacting Massive particles) by the measurement of non-thermal phonons as created by WIMP-induced nuclear recoils. Combined with the newly developed method of simultaneous measurement of scintillation light, strong background discrimination is possible, resulting in a substantial increase in WIMP detection sensitivity. The short and long term perspectives of CRESST are discussed.']",['1999-04-07']
1426,['eng'],"['Connolly, A']",['Search for Long-lived Charged Massive Particles at CDF'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'anti-p p, colliding beams', 'new particle, search for', 'charged particle, massive', 'ionization', 'quark, postulated particle', 'flavor, 4', 'color, triplet', 'mass, lower limit', 'slepton, pair production', 'Drell-Yan process', 'supersymmetry, symmetry breaking', 'production, upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904010'],"[""A search for long-lived charged massive particles in CDF's Run1b data sample is presented. The search looks for highly ionizing tracks which would result from slowly moving massive particles. We search for strongly produced particles using a stable color triplet quark as a reference model, and a separate search was performed for weakly produced particles using long-lived sleptons in Gauge Mediated Supersymmetry Breaking as a reference model. No excess over background was observed, and we derive limits on the cross-sections for production of these particles. Prospects for RunII are also discussed.""]",['1999-04-09']
1427,['eng'],"['Halley, A W']",['Heavy Quark Asymmetries at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'quark, charm', 'quark, beauty', 'quark, pair production', 'angular distribution, asymmetry', 'radiative correction', 'Higgs particle, mass', 'quark, decay modes', 'particle identification, flavor', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904004'],"['Measurements of b and c quark asymmetries using data collected at LEP 1 are described. The relative merits of each of the individual techniques used is emphasised as is the most profitable way of combining them. Effects of radiative corrections are discussed, together with the impact of these measurements on global electroweak fits used to estimate the expected mass of the Higgs boson.']",['1999-04-06']
1428,['eng'],"['Filkov, L V', 'Kashevarov, V L', 'Konobeevski, E S', 'Mordovskoy, M V', 'Potashev, S Yu', 'Skorkin, V M']",['Search for Supernarrow Dibaryons in pd-Interaction'],['Particle Physics - Experimental Results'],"['p deuteron, inclusive reaction', 'baryon resonance, search for', 'baryon resonance, mass', 'baryon resonance, width', 'narrow resonance, dibaryon', 'dibaryon, hadronic decay', 'p, spectator', 'mass spectrum, missing-mass', 'p, angular distribution', 'spectrometer, experimental results', 'Moscow ITEF PS', 'p deuteron --> 2p anything', 'p deuteron --> deuteron p anything', 'p deuteron --> p anything', '0.305 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904003'],['The reaction pd-->pX at 305 MeV is studied with aim to search for supernarrow dibaryons a decay of which into two nucleons suppressed by the Pauli principle. The experiment was carried out at Moscow Meson Factory using the spectrometer TAMS which detected the proton spectator in coincidence with another charged particle (either p or d) from a decay of X. A detection of the second charged particle at angles closed to an emission angle of the particle X with the mass M allows to suppress essentially a contribution of background processes and to increase a relative contribution from a possible production of the dibaryon under consideration. Narrow structures in missing mass spectra at 1905 and 1924 MeV with the statistical significance of ~4.5 S.D. have been observed. Widths of both peaks are smaller than the experimental resolution (3 MeV). A comparison of the obtained data with the theoretical predictions leads to a conclusion that most likely the found structure at 1905 MeV corresponds to the supernarrow dibaryon with the isotopic spin equal to 1. The possible origin of the structure at 1924 MeV is also discussed.'],['1999-04-06']
1429,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for Scalar Top and Scalar Bottom Quarks at $\\sqrt{s}$ = 189 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'squark, pair production', 'squark, truth', 'squark, beauty', 'squark, mass', 'lower limit', 'squark, decay modes', 'mass difference, (squark neutralino)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'squark --> charm neutralino', 'squark --> beauty neutralino', 'squark --> beauty lepton sneutrino', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903070'],"['Searches for a scalar top quark and a scalar bottom quark have been performed using a data sample of 182 pb-1 at a centre-of-mass energy of 189 GeV collected with the OPAL detector at LEP. No evidence for a signal was found. The 95% confidence level lower limit on the scalar top quark mass is 90.3 GeV if the mixing angle between the supersymmetric partners of the left- and right-handed states of the top quark is zero. In the worst case, when the scalar top quark decouples from the Z boson, the lower limit is 87.2 GeV. These limits were obtained assuming that the scalar top quark decays into a charm quark and the lightest neutralino, and that the mass difference between the scalar top quark and the lightest neutralino is larger than 10 GeV. The complementary decay mode of the scalar top quark decaying into a bottom quark, a charged lepton and a scalar neutrino has also been studied. From a search for the scalar bottom quark, a mass limit of 88.6 GeV was obtained if the mass difference between the scalar bottom quark and the lightest neutralino is larger than 7 GeV. These limits significantly improve the previous OPAL limits.']",['1999-04-01']
1430,['eng'],"['Tesarek, R J']",['Scalar and Tensor Couplings in Kaon Decays'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'K0, semileptonic decay', 'coupling, tensor', 'coupling, scalar', 'upper limit', 'Dalitz plot', 'neutrino, angular distribution', 'magnetic detector, experimental results', 'Batavia TEVATRON PS', 'K0 --> pi electron neutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903069'],"['In the past few years charged kaon experiments have indicated possible scalar and tensor couplings in semileptonic kaon decays(K --> pi e nu). These couplings, if correct, are not predicted by the Standard Model and may indicate the onset of new physics. We present a summary of the existing data and a new, precision measurement of these couplings in the neutral kaon system based on a 3% subset of the data taken by the KTeV (E799) experiment at Fermilab.']",['1999-03-31']
1431,['eng'],"['Yao, W M']",['Standard Model Higgs and Top Mass Measurements at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'mass, truth', 'Higgs particle, search for', 'Higgs particle, mass', 'intermediate boson, associated production', 'intermediate boson, leptonic decay', 'quark, beauty', 'Higgs particle, hadronic decay', 'channel cross section, branching ratio', 'mass, dependence', 'particle identification, beauty', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> Higgs particle W anything', 'anti-p p --> Higgs particle Z0 anything', 'Higgs particle --> 2beauty', 'W --> lepton neutrino', 'Z0 --> lepton+ lepton-', 'Z0 --> neutrino antineutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903068'],"['A summary of the present Standard Model Higgs search and measurement of top quark mass at the Tevatron are presented. The sensitivity of the present Higgs search at the Tevatron is limited by statistics to a cross section approximately two orders of magnitude higher than the predicted cross section for Standard Model Higgs production. With 30/fb of integrated luminosity, the Tevatron offers an unique potential discovery window for the Standard Model Higgs mass up to 130 GeV before LHC era. The study of top at the Tevatron has moved from discovery phase to one of characterizing its properties. The combined result of top quark mass is 174.3+- 5.1 GeV.']",['1999-03-31']
1432,['eng'],"['Sanders, D A']",['Recent Results from Fermilab Charm Experiment E791'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'charmed meson, hadroproduction', 'charmed meson, branching ratio', 'upper limit', 'charmed meson, rare decay', 'charmed meson, semileptonic decay', 'charmed meson, hadronic decay', 'charmed meson, leptonic decay', 'D+', 'D/s+, lifetime', 'D0, lifetime', 'lifetime, difference', 'form factor, decay', 'D0 anti-D0, interference', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> K*(892) lepton+ neutrino', 'D/s+ --> Phi(1020) lepton+ neutrino', 'D0 --> K- pi+', 'D0 --> K+ K-', '500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903067'],"['We report the results of some recent E791 charm analyses. They include: 1) a search for rare and forbidden decays, 2) measurements of form factors for D+ --> K*,l,nu and Ds --> phi,l,nu, and 3) Ds and D0 lifetime measurements including the lifetime difference between D0-->Kpi and D0-->KK. The latter is the first direct search for a possible lifetime difference that could contribute to D0-D0bar mixing.']",['1999-03-31']
1433,['eng'],"['Wang, J C', 'Artuso, M', 'Ayad, R', 'Azfar, F', 'Dambasuren, E', 'Efimov, A', 'Kopp, S E', 'Majumder, G', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Anderson, S', 'Smith, A', 'Kubota, Y', 'Lipeles, E', 'Coan, T E', 'Staeck, J', 'Fadeev, V', 'Volobuev, I']",['The CLEO-III RICH Detector and Beam Test Results'],['Detectors and Experimental Techniques'],"['talk, Los Angeles 1999/01/05', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'Cherenkov counter, crystal', 'lithium, fluorine', 'proportional chamber, wire', 'organic compounds', 'electronics, readout', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903066'],"['We are constructing a Ring Imaging Cherenkov detector (RICH) for the CLEO III upgrade for precision charged hadron identification. The RICH uses plane and sawtooth LiF crystals as radiators, MWPCs as photon detectors with TEA as the photo-sensitive material, and low-noise Viking readout electronics. Results of a beam test of the first two out of total 30 sectors are presented.']",['1999-03-30']
1434,['eng'],"['Kinoshita, K']",['Probing CKM via Semileptonic B Decays at the $\\Upsilon(4S)$'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'Kobayashi-Maskawa angle', 'unitarity', 'B0 anti-B0, interference', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D lepton neutrino', 'B --> D*(2010) lepton neutrino', 'B --> rho(770) lepton neutrino', 'B --> omega(783) lepton neutrino', 'B --> pi lepton neutrino', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903065'],"['Semileptonic decays of B mesons may be used in many different ways to probe the CKM matrix. Presented here are several recent results from the CLEO II experiment, all involving the analysis or utilization of semileptonic B decays.']",['1999-03-29']
1435,['eng'],"['Brigljevic, V']",['Measurement of the Spectroscopy of Orbitally Excited B Mesons with the L3 detector'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'beautiful meson, hadron spectroscopy', 'B, excited state', 'angular momentum, 1', 'beautiful meson, mass', 'beautiful meson, width', 'B*2(5732)', 'mass spectrum, (B pi)', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903064'],"['We measure the mass, decay width and production rate of orbitally excited B mesons in 1.25 million hadronic Z decays registered by the L3 detector in 1994 and 1995. B meson candidates are inclusively reconstructed and combined with charged pions produced at the event primary vertex. An excess of events above the expected background is observed in the B\\pi mass spectrum near 5.7 GeV. These events are interpreted as resulting from the decay B^** -> B^(*)pi, where B^** denotes a mixture of L=1 B meson spin states. The masses and decay widths of the B^*_2 (j_q = 3/2) and B^*_1 (j_q = 1/2) resonances and the relative production rate for the combination of all spin states are extracted from a fit to the mass spectrum.']",['1999-03-29']
1436,['eng'],"['Parodi, F', 'Roudeau, Patrick', 'Stocchi, A']",['Constraints on the parameters of the CKM matrix by End 1998'],['Particle Physics - Experimental Results'],"['review, experimental results', 'Kobayashi-Maskawa angle, parametrization', 'B, semileptonic decay', 'charmed meson, decay', 'decay constant', 'branching ratio', 'B0, mass difference', 'B/s0, mass difference', 'mass, truth', 'quantum chromodynamics, nonperturbative', 'lattice field theory', 'unitarity', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903063'],"['A review of the current status of the Cabibbo-Kobayashi-Maskawa matrix (CKM) is presented. This paper is an update of the results published in [1]. The experimental constraints imposed by the measurements of \\epsilon_K, V_{ub}/V_{cb}, \\Delta m_d and from the limit on \\Delta m_d are used. Values of the constraints and of the parameters entering into the constraints, which restrict the range of the \\bar{\\rho} and \\bar{\\eta} parameters, include recent measurements presented at 1998 Summer Conferences and progress obtained by lattice QCD collaborations. The results are: \\bar{\\rho}=0.202 ^{+0.053}_{-0.059},\\bar{\\eta}=0.340 \\pm 0.035, from which the angles \\alpha, ^{+ 0.29}_{-0.28} ,\\sin 2 \\beta = 0.725 ^{+0.050}_{-0.060} ,\\gamma= (59.5^{+8.5}_{-7.5})^{\\circ}. Without using the constraint from \\epsilon_K, external measurements or theoretical inputs have been removed, in turn, from the constraints and their respective probability density functions have been obtained. Central values and uncertainties on these quantities have been compared with actual measurements or theoretical evaluations. In this way it is possible to quantify the importance of the different measurements and the coherence of the Standard Model scenario for CP violation. An important result is that \\Delta m_s is expected to be between [12.0-17.6] ps^{-1} with 68% C.L. and <20 ps^{-1} at 95% C.L. Finally relations between the CKM parameters and the quark masses are examined within a given model.']",['1999-03-29']
1437,['eng'],"['Cerutti, F']",['Determination of the upper limit on $m_{\\nu_{\\tau}}$ from LEP'],['Particle Physics - Experimental Results'],"['review, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'mass spectrum, ((n)pi)', 'energy spectrum', 'neutrino/tau, mass', 'upper limit', 'magnetic detector, ALEPH', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau --> 5pi neutrino/tau', 'tau --> 3pi neutrino/tau']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903062'],"['A review of the direct determinations of the upper limit on the tau-neutrino mass from the LEP experiments is given. The experimental methods, the results and the comparison with non LEP measurements are also discussed. The study of the systematic errors shows that the LEP results are statistically limited so that their combination will improve the sensitivity to a massive tau-neutrino. An unofficial combination of the ALEPH and OPAL measurements gives a 95% confidence level upper limit of 15 MeV on the tau-neutrino mass.']",['1999-03-29']
1438,['eng'],"['Holck, C']",['Search for Scalar Top'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'anti-p p, colliding beams', 'new particle, search for', 'squark, truth', 'squark, decay', 'quark, truth', 'quark, decay', 'mass spectrum, transverse', 'channel cross section, mass', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> squark anything', 'squark --> beauty neutralino', 'squark --> beauty chargino', 'truth --> squark neutralino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903060'],"['We report results of three searches for scalar top quark. Two of the searches look for direct production of scalar top quark followed by the decay of the scalar quark to charm quark and neutralino or bottom and chargino. The third search looks for top quark decaying to scalar top and neutralino followed by the decay of scalar top to bottom quark and neutralino. We find no evidence for the presence of scalar top quark in any of the searches. Therefore, depending on the search we set limits on the production cross-section, $BR(t \\to $m_{\\tilde{\\chi}_{1}^{0}}$.']",['1999-03-25']
1439,['eng'],"['Lou, X C']",['BES Results on Inclusive D Meson Decays'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, pair production', 'D', 'D*(2010)', 'charmed meson, decay modes', 'Phi(1020), production', 'D0, branching ratio', 'D+, branching ratio', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> 2D*(2010)', 'electron positron --> D*(2010) D', 'D --> Phi(1020) anything', 'D+ --> Phi(1020) positron neutrino', '4.03 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903059'],"['A preliminary measurement of branching fractions of the D0 and D+ mesons into the phi meson is reported. The result is based on a data sample of 22.3 pb-1 collected at the CM energy of 4.03 GeV with the BES detector operated at the BEPC e+e- storage ring. From tagged D\\bar{D} pair events the average branching fraction for a mixture of D0 and D+ is determined to be B(D->phiX)= (1.29+-0.51+-0.12)%. Upper limits at 90% confidence level are set to be B(D0->phiX)<2.5%, B(D+->phiX)<5.0%, and B(D+->phie+X)<1.6%.']",['1999-03-25']
1440,['eng'],"['Blazey, G C', 'Flaugher, B L']",['Inclusive Jet and Dijet Production at the Tevatron'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'mass spectrum, (2jet)', 'angular distribution, (2jet)', 'channel cross section', 'differential cross section, transverse energy', 'scaling', 'quark, composite', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> jet anything', 'anti-p p --> 2jet anything', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903058'],"['High energy jet distributions measured since 1992 at the Fermilab Tevatron proton--antiproton collider are presented and compared to theoretical predictions. The statistical uncertainties on these measurements are significantly reduced relative to previous results. The systematic uncertainties are comparable in size to the uncertainty in the theoretical predictions. Although some discrepancies between theory and measurements are noted, the inclusive jet and dijet cross sections can be described by quantum chromodynamics. Prospects for reducing the uncertainty in the theoretical predictions by incorporating Tevatron measurements into the proton parton distributions are discussed. Dijet distributions, in excellent agreement with quantum chromodynamics, set a 2.5 TeV limit on the mass of quark constituents.']",['1999-03-25']
1441,['eng'],"['Bauer, G']",['Mixing and CP Violation Measurements of $B^{0}$ Mesons from the Tevatron Collider'],['Particle Physics - Experimental Results'],"['talk, Mumbai 1999/01/14', 'anti-p p, polarized beam', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'time dependence', 'B0, mass difference', 'B/s0, mass difference', 'B0, hadronic decay', 'Kobayashi-Maskawa angle', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B0 --> J/psi(3100) K0(S)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904017'],['$B^0$ mixing measurements from the Tevatron Run I data are reported. These include time-integrated measurements of the average mixing parameter a time-dependent limit on $\\Delta m_s$. Such measurements provide constraints on CKM matrix elements. A sample of $B^0/\\bar{B}{^0} \\to J/\\psi K^0_S$ decays is used to directly measure the CP-violation parameter $\\sin(2\\beta)$. This value agrees well with indirect constraints on the CKM matrix.'],['1999-04-20']
1442,['eng'],[],['Measurement of multiplicity and momentum spectra in the current and target regions of the Breit frame in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'kinematics, Breit frame', 'target, fragmentation', 'current, fragmentation', 'charged particle, multiplicity', 'momentum spectrum', 'transverse momentum, spectra', 'momentum transfer, dependence', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'duality, parton hadron', 'validity test', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903056'],"['Charged particle production in neutral current deep inelastic scattering (DIS) has been studied using the ZEUS detector.The evolution of the mean multiplicities, scaled momenta and transverse momenta in Q^2 and x for $10 < Q^2 < 5120 GeV^2$ and $x > 6\\times 10^{-4}$ has been investigated in the current and target fragmentation regions of the Breit frame. Distributions in the target region, using HERA data for the first time, are compared to distributions in the current region. Predictions based on MLLA and LPHD are inconsistent with the data.']",['1999-03-24']
1443,['eng'],"['Mitchell, G S']",['Spin Structure Functions $g_{1}$ and $g_{2}$ for the Proton and Deuteron'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron p, deep inelastic scattering', 'electron deuteron, deep inelastic scattering', 'electron, polarized beam', 'polarized target', 'polarization, longitudinal', 'polarization, transverse', 'p, structure function', 'deuteron, structure function', 'structure function, spin', 'x-dependence', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'magnetic spectrometer, experimental results', 'SLAC Lab', '48.3 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903055'],"['The experiment E155 at SLAC measured the spin structure functions g_1 and g_2 of the proton and deuteron. The experiment used deep inelastic scattering of 48.3 GeV longitudinally polarized electrons incident on polarized solid ^{15}NH_3 and ^{6}LiD targets. The data taken by three independent spectrometers covered a kinematic range of 0.014 < x < 0.9 and 1 (GeV/c)^2 < Q^2 < 40 (GeV/c)^2. Due to the high luminosity and polarization available at SLAC the data on g_1 are to date the most precise in this kinematic range. The x and Q^2 dependence of g_1 has been studied using NLO PQCD fits, allowing extraction of values for the Bjorken sum rule and quark and gluon spin contributions to the nucleon. Results are presented for g_1 and g_2 for the proton and deuteron.']",['1999-03-23']
1444,['eng'],"['Kulchitskii, Yu A', 'Vinogradov, V B']",['Non-Compensation of the Barrel Tile Hadron Module-0 Calorimeter'],['Detectors and Experimental Techniques'],"['calorimeter, hadronic', 'talk, Geneva 1998/11', 'iron', 'scintillation counter', 'energy resolution', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903054'],"['The detailed experimental information about the electron and pion responses, the electron energy resolution and the e/h ratio as a function of incident energy E, impact point Z and incidence angle $\\Theta$ of the Module-0 of the iron-scintillator barrel hadron calorimeter with the longitudinal tile configuration is presented. The results are based on the electron and pion beams data for E = 10, 20, 60, 80, 100 and 180 GeV at $\\eta$ = -0.25 and -0.55, which have been obtained during the test beam period in 1996. The results are compared with the existing experimental data of TileCal 1m prototype modules, various iron-scintillator calorimeters and with some Monte Carlo calculations.']",['1999-03-23']
1445,['eng'],"['Kulchitskii, Yu A']",['Effect on a Hadron Shower Leakage on the Energy Response and Resolution of Hadron Tile Calorimeter'],['Detectors and Experimental Techniques'],"['calorimeter, hadronic', 'iron', 'scintillation counter', 'energy resolution', 'showers, hadronic', 'statistical analysis', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903051'],['The hadronic shower longitudinal and lateral leakages and its effect on the pion response and energy resolution of iron-scintillator barrel hadron prototype calorimeter with longitudinal tile configuration with a thickness of 9.4 nuclear interaction lengths have been investigated. The results are based on 100 GeV pion beam data at incidence angle $\\Theta = 10^o$ at impact point Z in the range from - 36 to 20 cm which were obtained during test beam period in May 1995 with setup equipped scintillator detector planes placed behind and back of the calorimeter. The fraction of the energy of 100 GeV pions at $\\Theta = 10^o$ leaking out at the back of this calorimeter amounts to 1.8 % and agrees with the one for a conventional iron-scintillator calorimeter. Unexpected behaviour of the energy resolution as a function of leakage is observed: 6 % lateral leakage lead to 18 % improving of energy resolution in compare with the showers without leakage. The measured values of longitudinal punchthrough probability $(18 \\pm 1) %$ and $(20 \\pm 1) %$ for two different hit definitions of leaking events agree with the earlier measurement for our calorimeter and with the one for a conventional iron-scintillator calorimeter with the same nuclear interaction length thickness respectively. Due to more soft cut for hit definition in the leakage detectors the measured value of longitudinal punchthrough probability more corresponds to the calculated iron equivalent length $L_{Fe} = 158 cm$.'],['1999-03-23']
1446,['eng'],"['Kulchitskii, Yu A']",['Electron Response and e/h Ratio of Iron-Scintillator Hadron Prototype Calorimeter with Longitudinal Tile Configuration'],['Detectors and Experimental Techniques'],"['calorimeter, hadronic', 'iron', 'scintillation counter', 'energy resolution', 'calibration', 'particle identification, (pi electron)', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903050'],"['The detailed information about electron response, electron energy resolution and e/h ratio as a function of incident energy E, impact point Z and incidence angle $\\Theta$ of iron-scintillator hadron prototype calorimeter with longitudinal tile configuration is presented. These results are based on electron and pion beams data of E = 20, 50, 100, 150, 300 GeV at $\\Theta = 10^o, 20^o, 30^o$, which were obtained during test beam period in July 1995. The obtained calibration constant is used for muon response converting from pC to GeV. The results are compared with existing experimental data and with some Monte Carlo calculations.']",['1999-03-23']
1447,['eng'],"['Terrón, J']",['Jet shapes in ep collisions at HERA'],['Particle Physics - Experimental Results'],"['talk, Durham 1998/09/20', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'jet, pair production', 'event shape analysis', 'track data analysis, cluster', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903049'],['New measurements of the jet shape in ep collisions at HERA using the k_T-cluster jet algorithm are presented.'],['1999-03-23']
1448,['eng'],"['Alavi-Harati, A']",['Light Gluino Search for Decays Containing $\\pi^{+} \\pi^{-}$ or $\\pi^{0}$ from a Neutral Hadron Beam at Fermilab'],['Particle Physics - Experimental Results'],"['neutral particle, secondary beam', 'gluino, search for', 'bound state, (gluon gluino)', 'bound state, decay', 'pi, pair production', 'mass spectrum, (pi+ pi-)', 'pi0', 'photino', 'bound state, mass', 'bound state, lifetime', 'transverse momentum, spectra', 'quantum chromodynamics, perturbation theory', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903048'],"['We report on two null searches, one for the spontaneous appearance of a long-lived neutral particle into hadrons and an unseen neutral particle. For the lowest level gluon-gluino bound state, known as the $R^0$, we exclude the decays $R^0\\to \\pi^+\\pi^-\\tilde{\\gamma}$ and $R^0\\to \\pi^0\\tilde{\\gamma}$ for the masses of $R^0$ and $\\tilde{\\gamma}$ in the theoretically allowed range. In the most interesting $R^0$ mass range, $\\leq 3 GeV/c^2$, we exclude $R^0$ lifetimes from $3\\times 10^{-10}$ seconds to as high as $10^{-3}$ seconds, assuming perturbative QCD production for the $R^0$.']",['1999-03-23']
1449,['eng'],"['Abbott, B']",['Search for Charged Higgs Bosons in Decays of Top Quark Pairs'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'Higgs particle, search for', 'Higgs particle, charged particle', 'Higgs particle, mass', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> Higgs particle beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902028'],"['We present a search for charged Higgs bosons in decays of pair-produced top quarks using 109.2 +- 5.8 pb^-1 of data recorded from ppbar collisions at sqrt{s} = 1.8 TeV by the D0 detector during 1992-96 at the Fermilab Tevatron. No evidence is found for charged Higgs production, and most parts of the [m(H+),tan(beta)] parameter space where the decay t -> bH+ has a branching fraction close to or larger than that for t -> bW+ are excluded at 95% confidence level. Assuming m(t) = 175 GeV and sigma(ppbar -> ttbar) = 5.5 pb, for m(H+) = 60 GeV, we exclude tan(beta) < 0.97 and tan(beta) > 40.9.']",['1999-02-23']
1450,['eng'],"['Fernández, J P']","['Measurements of $A_{LR}$, $A_{lepton}$ and $A_{b}$ from SLD']",['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, leptonic decay', 'electron, pair production', 'muon, pair production', 'tau, pair production', 'Z0, hadronic decay', 'quark, pair production', 'quark, beauty', 'angular distribution, asymmetry', 'polarization, asymmetry', 'Z0, branching ratio', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903040'],"['We present the measurements of the leptonic asymmetries in $Z^0$ decays measured by the SLD experiment at SLAC. A data sample of approximately 550,000 $Z^0$ bosons are used for the preliminary measurement of $A_{LR}(A_{e})$ and the leptonic final state measurements of $A_{e}$, $A_{\\mu}$ and $A_{\\tau}$, representing the entire set of 1992-1998 SLD runs. When combining all results, a preliminary value for the effective weak mixing angle is obtained: ${\\sin}^2{\\theta}_{W}^{eff} = 0.23109 \\pm 0.00029$. We also present the direct measurements of $A_{b}$ from left-right forward-backward asymmetries, using partial data samples from 1993-1998 SLD runs. The preliminary value combines jet charge, cascade kaon and semileptonic decay analyses to obtain $A_{b} = 0.866 \\pm 0.036$.']",['1999-03-18']
1451,['eng'],"['Convery, M R']",['B Decay Studies at SLD'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'quark, beauty', 'quark, pair production', 'quark, hadronic decay', 'B, hadronic decay', 'B+, lifetime', 'B0, lifetime', 'lifetime, ratio', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'beauty --> strangeness gluon', 'B --> D anti-D anything', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903061'],"['We present three preliminary results from SLD on B decays: an inclusive search for the process b-> s gluon, a measurement of the branching ratio for the process B -> D D-bar X, and measurements of the charged and neutral B lifetimes. All three measurements make use of the excellent vertexing efficiency and resolution of the CCD Vertex Detector and the first two make use of the excellent particle identification capability of the Cherenkov Ring Imaging Detector. The b->sg analysis searches for an enhancement of high momentum charged kaons produced in B decays. Within the context of a simple, Jetset-inspired model of b->sg, a limit of BR(b->sg) < 7.6% is obtained. The B -> D D-bar X analysis reconstructs two secondary vertices and uses identified charged kaons to determine which of these came from charm decays. The result of the analysis is BR(B -> D D-bar X) = (16.2 +/- 1.9 +/- 4.2)%. The results of lifetime analysis are: \\tau_{B^+} = 1.686 +/-0.025 +/- 0.042 ps, \\tau_{B^0} = 1.589 +/- 0.026 +/- 0.055 ps and $\\tau_{B^+}/\\tau_{B^0} = 1.061 +/- ^{0.031}_{0.029} +/- 0.027.']",['1999-03-26']
1452,['eng'],"['Habig, A']",['Neutrino-induced upward-going muons in Super-Kamiokande'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'neutrino, cosmic radiation', 'neutrino nucleon, interaction', 'charged current', 'muon, angular distribution', 'muon, flux', 'neutrino, energy', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, mixing angle', 'Cherenkov counter, water', 'experimental results', 'deep underground detector, KAMIOKANDE']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903047'],"['Upward-going muons observed by the Super-Kamiokande detector are produced by high-energy atmospheric neutrinos which interact in rock around the detector. Those which pass completely through the detector have a mean parent neutrino energy of ~100 GeV, while those which range out inside the detector come from neutrinos of mean energy ~10 GeV. The neutrino baseline varies with the observed muon zenith angle, allowing for an independent test via nu-mu disappearance of the neutrino oscillations observed in the Super-Kamiokande contained events. 614 upward through-going and 137 upward stopping muons were observed over 537 (516) live days, resulting in a flux of Phi_t=1.74\\pm0.07(stat.)\\pm0.02(sys.), Phi_s=0.380\\pm0.038(stat.)^{+0.019}_{-0.016}(sys.) x10^{-13}cm^{-2}s^{-1}sr^{-1}. The observed stopping/through-going ratio R=0.218\\pm0.023(stat.)^{+0.014}_{-0.013}(syst.) is 2.9 sigma lower than the expectation of 0.368^{+0.049}_{-0.044}(theo.). Both the shape of the zenith angle distribution of the observed flux and this low ratio are inconsistent with the null oscillation hypothesis, but are compatible with the previously observed nu-mu <-> nu-tau oscillations. Taken as a whole, the addition of these higher energy nu-mu data to the contained neutrino events provides a better measurement of the oscillation parameters, narrowing the allowed parameter range to sin^22theta >~0.9 and 1.5x10^{-3}eV^2 <~ \\Delta m^2 <~6x10^{-3} at 90% confidence.']",['1999-03-22']
1453,['eng'],"['Cross, R']","['Structure Functions, the Gluon Density, and PQCD Tests']",['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'p, structure function', 'momentum transfer, dependence', 'x-dependence', 'gluon, momentum spectrum', 'quark, sea', 'quantum chromodynamics, perturbation theory', 'nonperturbative', 'validity test', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903046'],"['Measurements of the proton structure function F_2 for 0.11 < Q^2 < 20000 GeV^2 and 1.2 X 10^-5 < x < 0.65 from ZEUS 1994-1997 measurements are presented. From ZEUS 1994 and 1995 F_2 data the slopes d(F_2)/d(ln Q^2) at fixed x and d(ln F_2)/d(ln(1/x)) for x < 0.01 at fixed Q^2 are derived. For the latter E665 data are also used. The transition region in Q^2 is explored using the simplest non-perturbative models and NLO QCD. The data at very low Q^2 <= 0.65 GeV^2 are described successfully by Regge theory. From a NLO QCD fit to ZEUS data the gluon density in the proton is extracted in the range 3 X 10^-5 < x < 0.7. Data from NMC and BCDMS constrain the fit at large x. Assuming the NLO QCD description to be valid down to Q^2 of 1 GeV^2, it is found that the qqbar sea distribution is still rising at small x and the lowest Q^2 values whereas the gluon distribution is strongly suppressed. Preliminary ZEUS 1996-1997 $F_2$ measurements are also presented.']",['1999-03-19']
1454,['eng'],"['Satpathy, A']",['Particle Identification with BELLE'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'particle identification, (p K pi)', 'scintillation counter', 'Cherenkov counter, aerogel', 'fast logic, time-of-flight', 'time resolution', 'magnetic detector, BELLE', 'KEK TRISTAN Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903045'],"['The working principle and performance of the BELLE particle identification device (PID), based on a hybrid system consisting of an array of high precision scintillator Time of Flight and silica Aerogel Counters, is discussed. The performances achieved in the beam tests are satisfactory and Monte Carlo tests of meeting physics objectives of BELLE are promising. Prior to the real experiment which is expected to commence in spring 1999, the BELLE PID is taking cosmic ray data for calibration and fine tuning.']",['1999-03-19']
1455,['eng'],"['Barberis, D']",['A partial wave analysis of the centrally produced $ \\pi^{+} \\pi^{-}$ system in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'pi, pair production', 'central region', 'mass spectrum, (pi+ pi-)', 'partial wave analysis', 'f0(975)', 'f0(1300)', 'f0(1500)', 'f0(1710)', 'f2(1270)', 'meson resonance, mass', 'meson resonance, width', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p pi+ pi-', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903043'],"['A partial wave analysis of the centrally produced pi+pi- channel has been performed in pp collisions using an incident beam momentum of 450 GeV/c. An unambiguous physical solution has been found. Evidence is found for the f0(980), f0(1300), f0(1500) and fJ(1710) with J = 0 in the the S-wave. The rho(770) is observed dominantly in the P0-wave and the f2(1270) is observed dominantly in the D0-wave. In addition, there is evidence for a broad enhancement in the D-wave below 1 GeV.']",['1999-03-19']
1456,['eng'],"['Barberis, D']",['A partial wave analysis of the centrally produced $K^{+}K^{-}$ and $K^{0}_{S}K^{0}_{S}$ systems in pp interactions at 450 GeV/c and new information on the spin of the $f_{J}(1710)$'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'K, pair production', 'central region', 'mass spectrum, (K+ K-)', 'mass spectrum, (2K0(S))', 'partial wave analysis', 'f0(1500)', 'f0(1710)', 'f2(1270)', 'a2(1320)', 'f2(1525)', 'f2(2150)', 'meson resonance, mass', 'meson resonance, width', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p K+ K-', 'p p --> 2p 2K0(S)', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903042'],"['A partial wave analysis of the centrally produced K+K- and K0K0 channels has been performed in pp collisions using an incident beam momentum of 450 GeV/c. An unambiguous physical solution has been found in each channel. The striking feature is the observation of peaks in the S-wave corresponding to the f0(1500) and fJ(1710) with J = 0. The D-wave shows evidence for the f2(1270)/a2(1320), the f2(1525) and the f2(2150) but there is no evidence for a statistically significant contribution in the D-wave in the 1.7 GeV mass region.']",['1999-03-19']
1457,['eng'],"['Abbott, B', 'Abolins, M', 'Abramov, V', 'Acharya, B S', 'Adam, I', 'Adams, D L', 'Adams, M', 'Ahn, S', 'Akimov, V E', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Baarmand, M M', 'Babintsev, V V', 'Babukhadia, L R', 'Baden, A', 'Baldin, B', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Baringer, P', 'Bartlett, J F', 'Belyaev, A', 'Beri, S B', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Biswas, N', 'Blazey, G C', 'Blessing, S', 'Bloom, P', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F', 'Boswell, C', 'Brandt, A', 'Breedon, R', 'Briskin, G M', 'Brock, R', 'Bross, A', 'Buchholz, D', 'Burtovoi, V S', 'Butler, J M', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chekulaev, S V', 'Chen, W', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cobau, W G', 'Cochran, J', 'Coney, L', 'Cooper, W E', 'Coppage, D', 'Cretsinger, C E', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Dyshkant, A', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Evdokimov, V N', 'Fahland, T', 'Fatyga, M K', 'Fehér, S', 'Fein, D K', 'Ferbel, T', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Forden, G E', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Gavrilov, V', 'Geld, T L', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gershtein, Yu', 'Gibbard, B', 'Gobbi, B', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, D R', 'Greenlee, H', 'Grinstein, S', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Guida, J A', 'Guida, J M', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, G', 'Gutíerrez, P', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hebert, C', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Hernández-Montoya, R', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hsieh, F', 'Hu Tong', 'Ito, A S', 'Jerger, S A', 'Jesik, R', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Jun, S Y', 'Jung, C K', 'Kahn, S', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kim, S K', 'Klima, B', 'Klopfenstein, C', 'Ko, W', 'Kohli, J M', 'Koltick, D S', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kuleshov, S', 'Kulik, Y', 'Kunori, S', 'Landry, F J', 'Landsberg, G L', 'Lauer, B M', 'Leflat, A', 'Li, J', 'Li, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Lucotte, A', 'Lueking, L H', 'Lyon, A L', 'Maciel, A K A', 'Madaras, R J', 'Madden, R', 'Magana-Mendoza, L', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Markeloff, R', 'Marshall, T', 'Martin, M I', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McKibben, T', 'McKinley, J', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miao, C', 'Miettinen, H', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mooney, P', 'Mostafa, M A', 'Da Motta, H', 'Murphy, C', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Narayanan, A', 'Neal, H A', 'Negret, J P', 'Némethy, P', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Oshima, N', 'Owen, D', 'Padley, P', 'Para, A', 'Parashar, N', 'Park, Y M', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pishchalnikov, Yu', 'Pope, B G', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramírez, O', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Sánchez-Hernández, A', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Scully, J R', 'Shabalina, E', 'Shaffer, C', 'Shankar, H C', 'Shivpuri, R K', 'Shpakov, D', 'Shupe, M', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sosebee, M', 'Sotnikova, N', 'Souza, M', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stichelbaut, F', 'Stoker, D', 'Stolin, V', 'Stoyanova, D A', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Sznajder, A', 'Tamburello, P D', 'Tarazi, J', 'Tartaglia, M', 'Thomas, T L T', 'Thompson, J', 'Trippe, T G', 'Tuts, P M', 'Vaniev, V', 'Varelas, N', 'Varnes, E W', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, G', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Wood, D R', 'Yamada, R', 'Yamin, P', 'Yasuda, T', 'Yepes, P', 'Yip, K', 'Yoshikawa, C', 'Youssef, S', 'Yu, J', 'Yu, Y', 'Zhang, B', 'Zhou, Z', 'Zhu, Z H', 'Zielinski, M', 'Zieminska, D', 'Zieminski, A', 'Zutshi, V', 'Zverev, E G', 'Zylberstejn, A']",['Search for bottom squarks in $p\\overline{p}$ collisions at $\\sqrt{s}=1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'squark, search for', 'squark, beauty', 'squark, pair production', 'squark, decay', 'neutralino, LSP', 'sparticle, mass', 'channel cross section, mass', 'upper limit', 'transverse energy, missing-energy', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2squark anything', 'squark --> neutralino beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903041'],['We report on a search for bottom squarks produced in pbarp collisions at sqrt(s) = 1.8 TeV using the D0 detector at Fermilab. Bottom squarks are assumed to be produced in pairs and to decay to the lightest supersymmetric particle (LSP) and a b quark with branching fraction of 100%. The LSP is assumed to be the lightest neutralino and stable. We set limits on the production cross section as a function of bottom squark mass and LSP mass.'],['1999-03-18']
1458,['eng'],"['Moinester, M A', 'Ocherashvili, A I', 'Steiner, V']",['Inelastic electron-pion scattering at FNAL (SELEX)'],['Particle Physics - Experimental Results'],"['talk, Bonn 1998/09/22', 'electron pi, inelastic scattering', 'electron, bound state', 'rho(770), radiative decay', 'rho(770), width', 'form factor, transition', 'pi, polarizability', 'photon, emission', 'anomaly, chiral', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi electron --> pi electron photon', 'pi electron --> pi pi0 electron', '590 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903039'],"[""In this report we describe the analysis status of electron-pion inelastic scattering $\\pi e \\to \\pi' e' \\gamma$ and $\\pi e \\to \\pi' e' \\pi^0$ reaction data, measured in inverse pion-electron scattering at 590 GeV/c at FNAL. The data give information on reactions that were never previously measured: (1) radiative width from a measurement of the transition form factor near zero momentum transfer, (2) $ \\pi e \\to e' \\pi' \\pi^0$ scattering near threshold for a determination of the chiral anomaly transition form factor and the $\\gamma field is Compton scattered on the pion, for a determination of the never previously measured generalized pion polarizabilities.""]",['1999-03-18']
1459,['eng'],"['Gounder, K']",['Recent Electroweak Results from the Tevatron'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'gauge boson, pair production', 'W, mass', 'W, width', 'transverse momentum, spectra', 'W, leptonic decay', 'coupling, (3gauge boson)', 'Z0, hadronic decay', 'channel cross section, branching ratio', 'coupling, (W lepton)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'W --> tau neutrino/tau', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903038'],"['Recent electroweak results from the CDF and D0 Collaborations at the Fermilab Tevatron Collider are presented. After a brief description of the \\D0 measurements of W/Z production cross sections, W width, W mass and W \\to \\tau search for anomalous gauge couplings by \\D0 in 1992-96 data is presented along with a detailed description of the WW/WZ \\to \\mu\\nu jj channel.']",['1999-03-18']
1460,['eng'],"['Harris, F A']",['Recent Charmonium Results from BES'],['Particle Physics - Experimental Results'],"['review, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), hadronic decay', 'psi(3685), branching ratio', 'J/psi(3100), leptonic decay', 'chi mesons, charm', 'chi mesons, hadronic decay', 'chi mesons, branching ratio', 'chi mesons, mass', 'eta/c(2980), mass', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> psi(3685)', 'psi(3685) --> J/psi(3100) pi+ pi-', 'psi(3685) --> (n)hadron', 'chi mesons --> (n)hadron', '3.68 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903036'],"['Recent results obtained from the BES psi(2S) data are summarized, including the measurement of the branching ratio of the J/psi to leptons, B(J/psi -> l^+ l^-) = 5.87 +/- 0.04 +/- 0.09, many psi(2S) and chi_c branching ratios, information on the rho-pi puzzle, and measurements of the mass of the chi_c0, m(chi_c0) = 3414.1 +/- 0.6 +/- 0.8 MeV, and the eta_c, m(eta_c) = 2975.8 +/- 3.9 +/- 1.2 MeV.']",['1999-03-18']
1461,['eng'],"['Richardson, J']",['The ATLAS Pixel Project'],['Detectors and Experimental Techniques'],"['talk, Los Angeles 1999/01/05', 'p p, colliding beam detector', 'semiconductor detector, pixel', 'electronics, readout', 'performance', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903035'],"['The ATLAS experiment, at the Large Hadron Collider, will incorporate discrete, high-resolution tracking sub-systems in the form of segmented silicon detectors with 40MHz radiation-hard readout electronics. In the region closest to the pp interaction point, the thin silicon tiles will be segmented into a pixel geometry providing two-dimensional space-point information. The current status of the ATLAS pixel project will be presented with an emphasis on the performance of the front-end electronics and prototype sensors.']",['1999-03-17']
1462,['eng'],"['Smy, M B']",['Solar Neutrinos with Super-Kamiokande'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'neutrino, solar', 'neutrino, flux', 'flux, time variation', 'neutrino, oscillation', 'neutrino, energy spectrum', 'neutrino electron, elastic scattering', 'electron, energy spectrum', 'MSW effect', 'Cherenkov counter, water', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903034'],['The discrepancy of the measured solar neutrino flux compared to the predictions of the standard solar model may be explained by the neutrino flavor oscillation hypothesis. A more direct and less model-dependent test of this hypothesis is a measurement of the distortion of the shape of the solar neutrino energy spectrum. Super-Kamiokande studies the energy spectrum of recoil electrons from solar neutrino scattering in water above 5.5 MeV.'],['1999-03-17']
1463,['eng'],"['Gottschalk, E E']",['Triggering BTeV'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'anti-p p, colliding beam detector', 'B0 anti-B0, interference', 'B, decay', 'violation, CP', 'forward spectrometer, proposed', 'trigger', 'semiconductor detector, vertex', 'Batavia TEVATRON Coll']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903033', 'http://www-lib.fnal.gov/archive/1999/conf/Conf-99-071-E.html']","['BTeV is a collider experiment at Fermilab designed for precision studies of CP violation and mixing. Unlike most collider experiments, the BTeV detector has a forward geometry that is optimized for the measurement of B and charm decays in a high-rate environment. While the rate of B production gives BTeV an advantage of almost four orders of magnitude over e+e- B factories, the BTeV Level 1 trigger must be able to accept data at a rate of 100 Gigabytes per second, reconstruct tracks and vertices, trigger on B events with high efficiency, and reject minimum bias events by a factor of 100:1. An overview of the Level 1 trigger will be presented.']",['1999-03-17']
1464,['eng'],"['Junk, T R']",['Recent Heavy-Flavor Measurements from OPAL'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Z0, branching ratio', 'quark, charm', 'quark, beauty', 'quark, pair production', 'Lambda/b0, semileptonic decay', 'Lambda/b0, branching ratio', 'Lambda/b0, polarization', 'D*(2010), excited state', 'postulated particle, D*(2629)', 'D*(2010), hadronic decay', 'momentum spectrum', 'transverse momentum, spectra', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903032'],"[""A selection of recent heavy-flavor results from OPAL using the LEP1 data sample are presented. The average polarization of b baryons in hadronic Z^0 decay has been measured to be -0.56^{+0.20}_{-0.13} (stat.) +- 0.09(syst.) using semileptonic decays of Lambda_b baryons. A search has been conducted for the radially excited D*' and has produced a 95% CL upper limit on its production of f(Z^0 -> D*'+-(2629))xBr(D*'+- -> D*+- pi+ pi-) < 2.1x10^{-3}. Finally, the measurement of the product branching ratio $f(b -> Lambda_b)xBr(Lambda_b -> Lambda X)= (2.67 +- 0.38 (stat) ^{+0.67}_{-0.60}(syst.))% has been made. This measurement, along with an earlier measurement of the product branching ratio f(b -> Lambda_b)xBr(Lambda_b -> Lambda l X), has been used to compute an updated R_{Lambda l} = Br(Lambda_b -> Lambda l X)/Br(Lambda_b -> \\Lambda X)= (8.0 +- 1.2 (stat.) +- 0.9 (syst.))%, consistent with the expected low semileptonic branching fraction of the Lambda_b inferred from its short lifetime compared to the other b hadrons.""]",['1999-03-17']
1465,['eng'],"['Alavi-Harati, A']",['Branching Ratio and Form Factor Measurements of $\\Xi^0$ $\\beta$ Decay'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'neutral particle, secondary beam', 'Xi0, semileptonic decay', 'Xi0, cascade decay', 'Xi0, branching ratio', 'form factor, vector', 'form factor, axial-vector', 'form factor, ratio', 'Sigma+, hadronic decay', 'mass spectrum, (p pi+)', 'experimental results', 'Batavia TEVATRON PS', 'Xi0 --> Sigma+ electron antineutrino/e', 'Xi0 --> Sigma+ muon+ antineutrino/mu', 'Sigma+ --> p pi0', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903031'],"['We present a branching ratio measurement for the beta decay of neutral Cascade hyperon to a positive Sigma, electron and neutrino. Data were collected during 1997 with the KTeV detector at Fermilab. We used the principal decay mode, Cascade to a Lambda and a neutral pion, as the flux normalization mode. The status of the measurement of the ratio of the axial-vector to vector coupling (g_1/f_1) for this decay will also be discussed. Furthermore, we present the preliminary branching ratio measurement for the muonic channel of Cascade beta decay.']",['1999-03-17']
1466,['eng'],"['Viren, B M']",['Current Status of Nucleon Decay Searches with Super-Kamiokande'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'p, semileptonic decay', 'p, lifetime', 'lower limit', 'background', 'deep underground detector, KAMIOKANDE', 'experimental results', 'p --> pi0 positron', 'p --> pi0 muon+', 'p --> eta lepton+', 'n --> eta antineutrino', 'p --> K+ antineutrino', 'p --> K0 muon+']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903029'],"['Evidence for Nucleon Decay has yet to be observed. Current results from the observation of a 45 kton-year exposure of Super-Kamiokande and lifetime limits for nucleons to decay via lepton + pion, lepton + eta and lepton + kaon modes are presented.']",['1999-03-16']
1467,['eng'],"['Margoni, M']","['New DELPHI Results from Semileptonic b, c Decays']",['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'quark, cascade decay', 'quark, charm', 'Kobayashi-Maskawa angle', 'charge correlation', 'lepton, transverse momentum', 'lepton, charge', 'B0, semileptonic decay', 'quark, branching ratio', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'B0 --> D*(2010) lepton- neutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903028'],"['The inclusive direct and cascade semileptonic branching ratios of the b quark were measured from a fit to the lepton momentum spectrum in the B-hadron rest frame, exploiting the charge correlation between the lepton and the heavy meson. The value of the Vcb element in the CKM quark mixing matrix was computed from the differential decay width of the process B0--> D+-* l- nu, measured as a function of the product W of the B and D* 4-velocities, using an inclusive method of D* reconstruction. A measurement of the ratio Vub/Vcb has been obtained by using the reconstructed secondary hadronic mass in semileptonic decays of B hadrons. The charm semileptonic branching ratio was measured using a double tag method based on the detection of exclusively reconstructed D mesons accompanied by a lepton in the opposite hemisphere.']",['1999-03-16']
1468,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Experimental properties of gluon and quark jets from a point source'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, multiple production', 'quark, jet', 'gluon, jet', 'jet, particle identification', 'charged particle, multiplicity', 'rapidity spectrum', 'energy spectrum', 'transverse momentum, spectra', 'color, recombination', 'quantum chromodynamics, perturbation theory', 'fragmentation function', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903027'],"['Gluon jets are identified in hadronic Z0 decays as all the particles in a hemisphere opposite to a hemisphere containing two tagged quark jets. Gluon jets defined in this manner are equivalent to gluon jets produced from a color singlet point source and thus correspond to the definition employed for most theoretical calculations. In a separate stage of the analysis, we select quark jets in a manner to correspond to calculations, as the particles in hemispheres of flavor tagged light quark (uds) events. We present the distributions of rapidity, scaled energy, the logarithm of the momentum, and transverse momentum with respect to the jet axes, for charged particles in these gluon and quark jets. We also examine the charged particle multiplicity distributions of the jets in restricted intervals of rapidity. For soft particles at large transverse momentum, we observe the charged particle multiplicity ratio of gluon to quark jets to be 2.29 +- 0.09 +- 0.15 in agreement with the prediction that this ratio should approximately equal the ratio of QCD color factors, CA/CF = 2.25. The intervals used to define soft particles and large transverse momentum for this result, p<4 GeV/c and 0.8<p_t<3.0 GeV/c, are motivated by the predictions of the Herwig Monte Carlo multihadronic event generator. Additionally, our gluon jet data allow a sensitive test of the phenomenon of non-leading QCD terms known as color reconnection. We test the model of color reconnection implemented in the Ariadne Monte Carlo multihadronic event generator and find it to be disfavored by our data.']",['1999-03-16']
1469,['eng'],"['Diwan, M V']",['Observation of the decay $K^{+} \\to \\pi^{+} \\nu \\overline{\\nu}$'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'K+, rare decay', 'K+, semileptonic decay', 'K+, branching ratio', 'neutrino, pair production', 'neutral current, flavor changing', 'pi+, momentum', 'path length, energy dependence', 'background', 'experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903026'],['We have observed 1 event consistent with the signature expected of the rare decay of a positive kaon to a positive pion and a neutrino anti-neutrino pair. In the examined momentum region of 211 to 230 MeV/c in the center of mass of the kaon we estimated the backgrounds to be about $0.08 \\pm 0.03$ events. From this observation we estimate the branching ratio to be $4.2^{+9.7}_{-3.5} analysis techniques. I will also discuss the expected improvements in the near future from the analysis of new data sets.'],['1999-03-16']
1470,['eng'],"['Belz, J E']",['Study of the Decays $K^{0}_{L} \\to \\pi^{+} \\pi^{-} \\gamma$ and $K^{0}_{L} \\to \\pi^{+} \\pi^{-} e^{+} e^{-}$ at KTeV'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'K0(L), radiative decay', 'K0(L), rare decay', 'decay, form factor', 'mass spectrum, (pi+ pi- photon)', 'mass spectrum, (pi+ pi- positron electron)', 'bremsstrahlung', 'cross section, ratio', 'angular distribution', 'time reversal, violation', 'magnetic detector, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi+ pi- photon', 'K0(L) --> pi+ pi- positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903025'],"['We present new results on the related rare KL decay modes KL -> pi+ pi- gamma and KL -> pi+ pi- e+ e-. KTeV has performed the first direct measurement of the form factor for the ""direct emission"" component of KL -> pi+ pi- gamma decays, a quantity with ramifications for particular chiral models. In addition, the form factor and direct emission/inner bremsstrahlung branching ratio - also presented here - are important input parameters for the understanding of the planar-angle distribution of KL -> pi+ pi- e+ e- decays. Preliminary results indicating the presence of a T-violating asymmetry in the KL -> pi+ pi- e+ e- angular distribution are presented.']",['1999-03-16']
1471,['eng'],"['Höcker, A']",['The Status of MSSM Higgs Boson Searches at LEP'],['Particle Physics - Experimental Results'],"['review, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'supersymmetry', 'Higgs particle, charged particle', 'Higgs particle, neutral particle', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, pair production', 'Higgs particle, hadronic decay', 'Higgs particle, leptonic decay', 'quark, beauty', 'tau', 'Higgs particle, mass', 'experimental results', 'CERN LEP Stor', 'electron positron --> Higgs particle Z0', 'electron positron --> 2Higgs particle', 'Higgs particle --> 2beauty', 'Higgs particle --> tau+ tau-', 'Higgs particle --> tau neutrino/tau', 'Higgs particle --> charm strangeness', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903024'],"['The most recently available results from searches conducted by the four LEP experiments at 189 GeV center-of-mass energy for Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) are presented. No evidence for a signal has been observed, and the null result is used by the experiments, both individually and collectively, to exclude regions of the MSSM parameter space and to set lower limits on Higgs boson masses at 95% confidence level in constrained MSSM scenarios.']",['1999-03-16']
1472,['eng'],"['Zhu, R']",['Precision Crystal Calorimetry in High Energy Physics'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'calorimeter, crystal', 'scintillation counter, crystal', 'cesium, iodine', 'lead, tungsten', 'bismuth-germanate', 'barium, fluorine', 'energy resolution', 'radiation, damage']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903023'],"['Crystal Calorimetry is widely used in high energy physics because of its precision. Recent development in crystal technology identified two key issues to reach and maintain crystal precision: light response uniformity and calibration in situ. Crystal radiation damage is understood. While the damage in alkali halides is found to be caused by the oxygen/hydroxyl contamination, it is the structure defects, such as oxygen vacancies, cause damage in oxides.']",['1999-03-16']
1473,['eng'],"['Bennett, S C', 'Wieman, C E']",['Measurement of the $6S \\to 7S$ transition polarizablility in atomic cesium and an improved test of the standard model'],['Particle Physics - Experimental Results'],"['cesium, atom', 'energy levels, transition', 'hyperfine structure', 'polarizability', 'electroweak interaction, validity test', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903022'],['The ratio of the off-diagonal hyperfine amplitude to the tensor transition polarizability (Mhf/beta) for the 6S-7S transition in cesium has been measured. The value of beta=27.024(43)(expt)(67)(theory)a_0^3 is then obtained using an accurate semi-empirical value of Mhf. This is combined with a previous measurement of parity nonconservation in atomic cesium and previous atomic structure calculations to determine the value of the weak charge. The uncertainties in the atomic structure calculations are updated (and reduced) in light of new experimental tests. The result Q_W=-72.06(28)(expt) (34)(theory) differs from the prediction of the standard model of elementary particle physics by 2.5 sigma.'],['1999-03-16']
1474,['eng'],"['Giacomelli, Giorgio']",['Recent OPAL measurements in non-perturbative QCD'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'hadron, multiple production', 'quantum chromodynamics, nonperturbative', 'correlation, two-particle', 'boson, statistics', 'intermittency', 'correlation, ((n)particle)', 'rho(770)', 'omega(783)', 'helicity, density matrix', 'spin, alignment', 'glueball, tensor', 'f4(2220), search for', 'mass spectrum, (2K)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903021'],"['Using multihadronic Z0 decays recorded in 1991-1995 by the OPAL detector in e+e- collisions at LEP1, experimental analyses were made of the following subjects: (a) Bose-Einstein correlations; (b) Intermittency and correlations; (c) rho and omega spin alignments; (d) A search for the tensor glueball candidate fj(2200).']",['1999-03-16']
1475,['eng'],"['Gary, J W']",['Recent QCD Results from LEP-1 and LEP-2'],['Particle Physics - Experimental Results'],"['review, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'quark, jet', 'gluon, jet', 'hadron, multiple production', 'quantum chromodynamics, perturbation theory', 'effect, nonperturbative', 'event shape analysis', 'charged particle, multiplicity', 'strong interaction, coupling constant', 'dependence, flavor', 'energy dependence', 'correction, hadronization', 'rapidity spectrum', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '91-189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903020'],"['A summary is given of some recent QCD results from LEP. For LEP-2, the topics include event shape measurements, determinations of the strong coupling constant, and measurements of the charged particle multiplicity distribution at the recently completed run at 189 GeV. For LEP-1, the topics presented are a test of the flavor independence of the strong coupling constant and a study of gluon jets using a hemisphere definition to correspond to analytic calculations. For the combined LEP data samples, the topics include a test of power law corrections for hadronization effects and the running of the strong coupling strength.']",['1999-03-15']
1476,['eng'],"['Coxe, R L']",['A Search for CP(T) Violation in B Decays at OPAL'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B, decay', 'B, lifetime', 'anti-B, lifetime', 'lifetime, difference', 'violation, CP', 'violation, CPT', 'decay, asymmetry', 'time dependence', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903018'],['A search for CP(T) violation is performed and the fractional difference between the $b$ and $\\bar b$ hadron lifetimes is measured using reconstructed secondary vertices in inclusive B hadron decays culled from 3.1 million $Z^0 collider at CERN at $\\sqrt{s} \\approx 91$ GeV from 1991-1995.'],['1999-03-15']
1477,['eng'],"['Moinester, M A', 'Steiner, V', 'Prakhov, S N']",['Hadron-Photon Interactions in COMPASS'],['Detectors and Experimental Techniques'],"['talk, Bormio 1999/01/25', 'pi- nucleus, nuclear reaction', 'photon pi, interaction', 'Primakoff effect', 'pi, polarizability', 'meson, hybrid', 'meson, photoproduction', 'anomaly, chiral', 'anomaly, axial', 'pi, pair production', 'magnetic spectrometer', 'calorimeter', 'proposed experiment, CERN SPS', 'pi- nucleus --> nucleus pi- photon', 'pi- photon --> meson', 'pi- photon --> pi- pi0', '50-280 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903017'],"['The COMPASS experiment at CERN SPS will use hadron beams (pion, kaon and proton) and muons at 50-280 GeV/c and virtual photon targets to investigate, via Primakoff effect, important hadron properties: polarizability, chiral anomaly, radiative transitions and hybrid meson production. We present simulation studies to optimize the beam, detector setup and trigger for measuring with high statistics above topics.']",['1999-03-12']
1478,['eng'],"['Konaka, A']",['$K_{L} \\to \\pi^{0} \\nu \\overline{\\nu}$ at the AGS $(E926)^{*}$'],['Detectors and Experimental Techniques'],"['talk, Tokyo 1998/12/18', 'K0(L), secondary beam', 'K0(L), rare decay', 'neutrino, pair production', 'pi0, radiative decay', 'scintillation counter', 'calorimeter, sandwich', 'lead', 'background', 'numerical calculations', 'proposed experiment, Brookhaven PS', 'K0(L) --> pi0 neutrino antineutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903016'],"['A proposed experiment to measure K_L -> pi^0 nu nubar at the AGS (E926) is described. It adopts a unique but general strategy of rare decay measurements with two independent rejection criteria, which allows reliable measurements of background levels. The method employs hermetic veto and full kinematic reconstruction using kaon time of flight and kinematic reconstruction of pi^0. Backgrounds are suppressed to a level well below an anticipated signal in the range 3 x 10^{-11}.']",['1999-03-12']
1479,['eng'],"['Greening, T C']",['Search for the Standard Model Higgs Boson at LEP'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'fusion, W W', 'fusion, Z0 Z0', 'Higgs particle, decay modes', 'Higgs particle, mass', 'lower limit', 'experimental results', 'CERN LEP Stor', '189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903013'],"['Preliminary results from the four LEP experiments using data collected at 189 GeV have shown no evidence for the Standard Model Higgs boson. The preliminary 95% confidence level lower limits on the SM Higgs boson mass from ALEPH, DELPHI, OPAL, and L3 are 90.4 GeV, 94.1 GeV, 95.5 GeV, and 95.2 GeV, respectively. When LEP finishes in the year 2000, each experiment expects to collect 200 pb-1 of data at 200 GeV. These data will allow the discovery of the SM Higgs boson with a mass lower than about 105 GeV. Assuming that no new evidence for the SM Higgs boson is found, the mass exclusion limit would be approximately 110 GeV.']",['1999-03-12']
1480,['eng'],[],['Measurements of Lifetimes and a Limit on the Lifetime Difference in the Neutral D-Meson System'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'D0, hadroproduction', 'D0, hadronic decay', 'D0, lifetime', 'D0 anti-D0, interference', 'lifetime, difference', 'mass spectrum, (K- pi+)', 'mass spectrum, (K+ K-)', 'invariance, CP', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> K+ K-', 'D0 --> K- pi+', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903012'],"['Using the large hadroproduced charm sample collected in experiment E791 at Fermilab, we report the first directly measured constraint on the decay-width difference Delta Gamma for the mass eigenstates of the D0-D0bar system. We obtain our result from lifetime measurements of the decays D0 --> K-pi+ and D0 --> K-K+, under the assumption of CP invariance, which implies that the CP eigenstates and the mass eigenstates are the same. The lifetime of D0 --> K-K+ (the CP-even final state is \\tau_KK = 0.410 +/- 0.011 +/- 0.006 ps, and the lifetime of D0 --> K-pi+ (an equal mixture of CP-odd and CP-even final states is tau_Kpi = 0.413 +/- 0.003 +/- 0.004 ps. The decay-width difference is Delta Gamma = 2(Gamma_KK - Gamma_Kpi) = 0.04 +/- 0.14 +/- 0.05 ps^-1. We relate these measurements to measurements of mixing in the neutral D-meson system.']",['1999-03-11']
1481,['eng'],"['Abe, F']",['Measurement of $B^{0} - \\overline{B}^{0}$ flavor oscillations using jet-charge and lepton flavor tagging in $p\\overline{p}$ collisions at $\\sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, oscillation', 'particle identification, beauty', 'B0, mass difference', 'B0, decay modes', 'jet, charge', 'lepton, charge', 'decay, time', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903011'],"['We present a measurement of the mass difference Delta m_d for the B0 meson and the statistical power of the b flavor tagging methods used. The measurement uses 90 (1/pb) of data from p p-bar collisions at sqrt[s] = 1.8 TeV collected with the CDF detector. An inclusive lepton trigger is used to collect a large sample of B hadron semileptonic decays. The mass difference Delta m_d is determined from the proper time dependence of the fraction of B hadrons that undergo flavor oscillations. The flavor at decay is inferred from the charge of the lepton from semileptonic B decay. The initial flavor is inferred by determining the flavor of the other B hadron produced in the collision, either from its semileptonic decay (soft-lepton tag) or from its jet charge. The measurement yields Delta m_d = 0.500 +/- 0.052 +/- 0.043 hbar/ps, where the first uncertainty is statistical and the second uncertainty is systematic. The statistical powers (epsilon D^2) of the soft-lepton and jet-charge flavor taggers are (0.91 +/- 0.10 +/- 0.11) % and (0.78 +/- 0.12 +/- 0.08) %, respectively.']",['1999-03-11']
1482,['eng'],"['Castera, A', 'Dumarchez, J', 'Lachaud, C', 'Vannucci, François']",['A search for energy deposition by neutrinos in matter'],['Particle Physics - Experimental Results'],"['neutrino/mu, secondary beam', 'germanium, crystal', 'neutrino, energy loss', 'upper limit', 'experimental results', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903010'],['An exploratory search for an anomalous energy deposition by neutrinos in a germanium crystal was performed in the CERN high energy neutrino beam. No signal was found and a limit is set at a level of about 10^-12 of the normal dE/dx for a minimum ionizing particle.'],['1999-03-11']
1483,['eng'],"['Gratta, Giorgio', 'Wang, Y F']","['Towards Low-Threshold, Real-Time Solar Neutrino Detectors']",['Detectors and Experimental Techniques'],"['neutrino, solar', 'neutrino nucleus, nuclear reaction', 'gadolinium', 'ytterbium', 'scintillation counter, liquid', 'background']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9905010'],"['We discuss an alternative approach to the detection of solar neutrinos using a coarsely segmented detector based on inverse-beta decay onto $^{160}$Gd or $^{176}$Yb. While it is know that similar approaches, already discussed in the literature, can in principle provide low-threshold, real-time energy spectroscopy with intrinsic background rejection features, the concepts presented here make this scheme possible with lower background and current technology.']",['1999-05-07']
1484,['eng'],"['Biebel, O', 'Movilla-Fernández, P A', 'Bethke, Siegfried']",['C-Parameter and Jet Broadening at PETRA Energies'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'final state, (2jet)', 'event shape analysis', 'parametrization', 'hadron, multiple production', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'magnetic detector, JADE', 'experimental results', 'DESY PETRA Stor', '35, 44 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903009'],"['e^+e^- annihilation data recorded by the JADE detector at PETRA were used to measure the C-parameter for the first time at \\sqrt{s}= 35 and 44 GeV. The distributions were compared to a resummed QCD calculation. In addition, we applied extended resummed calculations to the total and wide jet broadening variables, B_T and B_W. We combined the results on \\alpha_s with those of our previous study of differential 2-jet rate, thrust, and heavy jet mass, obtaining \\alpha_s(35 GeV) = 0.1448 +0.0117 -0.0070 and \\alpha_s(44 GeV) = 0.1392 +0.0105 -0.0074. Moreover power corrections to the mean values of the observables mentioned above were investigated considering the Milan factor and the improved prediction for the jet broadening observables. Our study, which considered e^+e^- data of five event shape observables between \\sqrt{s}= 14 and 183 GeV, yielded']",['1999-03-24']
1485,['eng'],"['Adloff, C']",['Charmonium Production in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'psi mesons, electroproduction', 'psi mesons, photoproduction', 'differential cross section, momentum transfer', 'energy dependence', 'psi mesons, leptonic decay', 'J/psi(3100)', 'psi(3685)', 'channel cross section, ratio', 'angular distribution', 'cross section, slope', 'quantum chromodynamics, perturbation theory', 'factorization', 'color, singlet', 'color, octet', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903008'],"['The electroproduction of J/psi and psi(2S) mesons is studied in elastic, quasi-elastic and inclusive reactions for four momentum transfers 2 < Q^2 < 80 GeV^2 and photon-proton centre of mass energies 25 < W < 180 GeV. The data were taken with the H1 detector at the electron proton collider HERA in the years 1995 to 1997. The total virtual photon-proton cross section for elastic J/psi production is measured as a function of Q^2 and W. The dependence of the production rates on the square of the momentum transfer from the proton (t) is extracted. Decay angular distributions are analysed and the ratio of the longitudinal and transverse cross sections is derived. The ratio of the cross sections for quasi-elastic psi(2S) and J/psi meson production is measured as a function of Q^2. The results are discussed in terms of theoretical models based upon perturbative QCD. Differential cross sections for inclusive and inelastic production of J/psi mesons are determined and predictions within two theoretical frameworks are compared with the data, the non-relativistic QCD factorization approach including colour octet and colour singlet contributions, and the model of Soft Colour Interactions.']",['1999-03-24']
1486,['eng'],[],['Measurement of the branching ratio of $\\pi^{0} \\to e^{+} e^{-}$ using $K_{L} \\to 3 \\pi^{0}$ decays in flight'],['Particle Physics - Experimental Results'],"['K0(L), secondary beam', 'K0(L), hadronic decay', 'pi0, multiple production', 'pi0, leptonic decay', 'pi0, branching ratio', 'mass spectrum, (positron electron)', 'perturbation theory, chiral', 'form factor', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> 3pi0', 'pi0 --> positron electron', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903007'],"[""The branching ratio of the rare decay pi^0 -> e^+e^- has been measured in E799-II, a rare kaon decay experiment using the KTeV detector at Fermilab. The pi^0's were produced in fully-reconstructed K_L -> 3 pi^0 decays in flight. We observed 275 candidate pi^0 -> e^+e^- events, with an expected background of 21.4 +- 6.2 events which includes the contribution from Dalitz decays. We measured BR(pi^0 -> e^+e^-, x>0.95) = (6.09 +- 0.40 +- 0.24) times 10^{-8}, where the first error is statistical and the second systematic. This result is the first significant observation of the excess rate for this decay above the unitarity lower bound. It is in agreement with expectations from pi^0 gamma gamma form factor models and recent chiral perturbation theory calculations.""]",['1999-03-24']
1487,['eng'],"['Takeuchi, Y']",['Measurement of radon concentrations at Super-Kamiokande'],['Detectors and Experimental Techniques'],"['neutrino, solar', 'background', 'radioactivity', 'radon', 'dosimetry', 'deep underground detector, KAMIOKANDE']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903006'],"['Radioactivity from radon is a major background for observing solar neutrinos at Super-Kamiokande. In this paper, we describe the measurement of radon concentrations at Super-Kamiokande, the method of radon reduction, and the radon monitoring system. The measurement shows that the current low-energy event rate between 5.0 MeV and 6.5 MeV implies a radon concentration in the Super-Kamiokande water of less than 1.4 mBq/m$^3$.']",['1999-03-24']
1488,['eng'],[],['Measurement of the Deuteron Spin Structure Function $g_{1}^{d(x)}$ for $1(GeV/c)^{2} < Q^{2} < 40 (GeV/c)^{2}$'],['Particle Physics - Experimental Results'],"['electron deuteron, deep inelastic scattering', 'electron, polarized beam', 'deuteron, polarized target', 'deuteron, structure function', 'structure function, spin', 'structure function, moment', 'momentum transfer, dependence', 'x-dependence', 'magnetic spectrometer, experimental results', 'SLAC Linac', '48.3 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9904002'],"['New measurements are reported on the deuteron spin structure function g_1^d. These results were obtained from deep inelastic scattering of 48.3 GeV electrons on polarized deuterons in the kinematic range 0.01 < x < 0.9 and 1 < Q^2 < 40 (GeV/c)^2. These are the first high dose electron scattering data obtained using lithium deuteride (6Li2H) as the target material. Extrapolations of the data were performed to obtain moments of g_1^d, including Gamma_1^d, and the net quark polarization Delta Sigma.']",['1999-04-05']
1489,['eng'],"['Abe, K']",['First study of the structure of $e^{+}e^{-} \\to b \\overline{b} g$ events and limits on the anomalous chromomagnetic moment of the b-quark'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'gluon, associated production', 'gluon, energy spectrum', 'gluon, angular distribution', 'quantum chromodynamics, perturbation theory', 'quark, magnetic moment', 'magnetic moment, color', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty gluon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903004'],"['The structure of e+e- -> b bbar g events was studied using Z0 decays recorded in the SLD experiment at SLAC. Three-jet final states were selected and the CCD-based vertex detector was used to identify two of the jets as b or bbar. Distributions of the gluon energy and polar angle were measured over the full kinematic range for the first time, and compared with perturbative QCD predictions. The energy distribution is potentially sensitive to an anomalous b chromomagnetic moment kappa. We measured kappa to be consistent with zero and set the first limits on its value, -0.17 < kappa < 0.11 at 95% c.l.']",['1999-03-10']
1490,['eng'],"['Stängle, H', 'Abe, K']",['Preliminary Direct Measurement of the s-Quark Asymmetry'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, strangeness', 'quark, pair production', 'coupling, (Z0 strangeness)', 'parametrization', 'parity, violation', 'angular distribution, asymmetry', 'polarization, asymmetry', 'particle identification, strangeness', 'track data analysis, vertex', 'analyzing power', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903003'],"['We present a preliminary direct measurement of the parity violating coupling of the Z boson to strange quarks, A_s, derived from a sample of approximately 300,000 hadronic decays of Z bosons produced with a polarized electron beam and recorded by the SLD experiment at SLAC between 1993 and 1997. Events with primary strange quarks are tagged by the presence in each event hemisphere of a high-momentum charged K meson, neutral K meson or Lambda hyperon identified using the Cherenkov Ring Imaging Detector and/or a mass tag. The CCD vertex detector is used to suppress the background from heavy flavor events. The strangeness of the tagged particle is used to sign the event thrust axis in the direction of the initial strange quark. The coupling A_s is obtained directly from a measurement of the left-right-forward-backward production asymmetry in polar angle of the tagged strange quark. To reduce the model dependence of the measurement, the background from primary up and down events is measured from the data, as is the analyzing power of the method for primary strange events. We measure A_s = 0.82+-0.10(stat.)+-0.08(syst.) (preliminary).']",['1999-03-10']
1491,['eng'],"['Paulini, M']","['B Lifetimes, Mixing and CP Violation at CDF']",['Particle Physics - Experimental Results'],"['review, experimental results', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'quark, hadronization', 'beautiful particle, lifetime', 'B', 'B/s0', 'Lambda/b0', 'B/c', 'B0 anti-B0, oscillation', 'time dependence', 'B0, mass difference', 'B0, hadronic decay', 'violation, CP', 'particle identification, flavor', 'magnetic detector, CDF', 'Batavia TEVATRON Coll', 'bibliography', 'B0 --> J/psi(3100) K0(S)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903002'],"['We review the status of bottom quark physics at the CDF experiment. The measurements reported are based on about 110 pb-1 of data collected at the Fermilab Tevatron pp= Collider operating at sqrt{s} = 1.8 TeV. In particular, we review results on B hadron lifetimes, measurements of the time dependence of B0 B0= oscillations, and a search for CP violation in B0 --> J/Psi K0s decays. Prospects for future B physics at CDF in the next run of the Tevatron Collider starting in the year 2000 are also given.']",['1999-03-10']
1492,['eng'],"['Asratyan, A E', 'Balats, M Ya', 'Böhnlein, D J', 'Childres, S', 'Davidenko, G', 'Dolgolenko, A', 'Dzyubenko, G B', 'Kaftanov, V S', 'Kubantsev, M A', 'Reay, N W', 'Musser, J', 'Rosenfeld, C', 'Stanton, N R', 'Thun, R', 'Tzanakos, G S', 'Verebryusov, V S', 'Vishniakov, V V']",['Detecting the (Quasi-)Two-Body Decays of $\\tau$ Leptons in Short-Baseline Neutrino Oscillation Experiments'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'neutrino/tau', 'neutrino/mu', 'tau, decay modes', 'nuclear emulsion', 'neutrino nucleus, nuclear reaction', 'calorimeter, electromagnetic', 'calorimeter, lead-glass', 'CERN Lab', 'Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0002027'],"['Novel detector schemes are proposed for the short-baseline neutrinoexperiments of next generation, aimed at exploring the large-$\\Delta m^2$domain of \\omutau oscillations in the appearance mode. These schemes emphasizegood spectrometry for charged particles and for electromagnetic showers andefficient reconstruction of \\ypi_gg decays. The basic elements are a sequenceof relatively thin emulsion targets, immersed in magnetic field andinterspersed with electronic trackers, and a fine-grained electromagneticcalorimeter built of lead glass. These elements act as an integral whole inreconstructing the electromagnetic showers. This conceptual scheme shows goodperformance in identifying the $\\tau$ (quasi-)two-body decays by theircharacteristic kinematics and in selecting the electronic decays of the $\\tau$.']",['2000-02-10']
1493,['eng'],"['Bonivento, W']",['Spin Physics at $e^{+}e^{-}$ Colliders'],['Particle Physics - Experimental Results'],"['talk, Prague 1998/08/30', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'fermion, pair production', 'polarized beam', 'tau, polarization', 'polarization, longitudinal', 'tau, decay modes', 'spin, correlation', 'Lambda, polarization', 'Lambda/b0, polarization', 'vector meson, electroproduction', 'spin, alignment', 'weak interaction, magnetic moment', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903001'],"['A large number of measurements with polarized beams and/or spin analysis of final state particles has been performed at the e^+e^- colliders LEP and SLC, providing important information on the dynamics of high energy interactions. In this paper three subjects, for which the role of spin studies was particularly relevant, will be covered: the measurements of the electroweak couplings, the study of fragmentation dynamics and the search for physics beyond the Standard Model.']",['1999-03-03']
1494,['eng'],"['Kudryavtsev, V A', 'Lehner, M J', 'Peak, C D', 'Lawson, T B', 'Lightfoot, P K', 'McMillan, J E', 'Roberts, J W', 'Spooner, N J C', 'Tovey, D R', 'Ward, C K', 'Smith, P F', 'Smith, N J T']","['Characteristics of $\\alpha$, $\\gamma$ and Nuclear Recoil Pulses from NaI(Tl) at 10-100 keV Relevant to Dark Matter Searches']",['Particle Physics - Experimental Results'],"['scintillation counter, crystal', 'sodium, iodine', 'nucleus, recoil', 'helium, interaction', 'photon, interaction', 'radiation, energy spectrum', 'astrophysics, missing-mass', 'search for, missing-mass', 'background']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902032'],"['Measurements of the shapes of scintillation pulses produced by nuclear recoils, alpha particles and photons in NaI(Tl) crystals at visible energies of 10-100 keV have been performed in order to investigate possible sources of background in NaI(Tl) dark matter experiments and, in particular, the possible origin of the anomalous fast time constant events observed in the UK Dark Matter Collaboration experiments at Boulby mine. Pulses initiated by X-rays (via photoelectric effect close to the surface of the crystal) were found not to differ from those produced by high-energy photons (via Compton electrons inside the crystal) within experimental errors. However, pulses induced by alpha particles (degraded from an external MeV source) were found to be ~10% faster than those of nuclear recoils, but insufficiently fast to account for the anomalous events.']",['1999-03-01']
1495,['eng'],"['Ong, S']",['Two-photon reactions with KLOE detector at DA$\\phi$NE'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'pi0, photoproduction', 'eta, photoproduction', 'pi, pair production', 'magnetic detector, KLOE', 'numerical calculations', 'proposed experiment, Frascati Stor', '10.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902030'],"['We reexamine the feasibility of two-photon reactions at DA$\\Phi$NE with the KLOE detector excluding the small angle tagging system. Event-rate predictions of interesting channels : $\\gamma \\gamma \\to \\pi^0, \\eta $ and $\\gamma \\gamma']",['1999-02-25']
1496,['eng'],"['Alavi-Harati, A']",['Measurement of the Decay $K_{L} \\to \\pi^{0}\\gamma \\gamma$'],['Particle Physics - Experimental Results'],"['K0(L), secondary beam', 'K0(L), radiative decay', 'K0(L), branching ratio', 'coupling constant, vector', 'perturbation theory, chiral', 'magnetic detector, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi0 2photon', '800 GeV/c (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902029'],"['We report on a new measurement of the decay KL -> pi0 gamma gamma by the KTeV experiment at Fermilab. We determine the KL -> pi0 gamma gamma branching ratio to be (1.68 +/- 0.07 +/- 0.08)x10**-6. Our data shows the first evidence for a low-mass gamma gamma signal as predicted by recent O(p**6) chiral perturbation calculations that include vector meson exchange contributions. From our data, we extract a value for the effective vector coupling aV = -0.72 +/- 0.05 +/- 0.06.']",['1999-02-23']
1497,['eng'],"['Muheim, F']",['B and D Spectroscopy at LEP'],['Particle Physics - Experimental Results'],"['review, Batavia 1998/10/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron spectroscopy', 'HQET model', 'charmed meson, mass spectrum', 'beautiful meson, mass spectrum', 'beautiful meson, width', 'B*2(5732), decay constant', 'postulated particle, B*1(5675)', 'B/c, hadronic decay', 'B, decay modes', 'D*2(2460), hadronic decay', 'experimental results', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902026'],"['Results from the four LEP experiments ALEPH, DELPHI, L3, and OPAL on the spectroscopy of B and charmed mesons are presented. The predictions of Heavy Quark Effective Theory (HQET) for the masses and the widths of excited L=1 B mesons are supported by a new measurement from L3. A few B_c candidate eve nts have masses consistent with the recent CDF observation and the predictions. New results on Ddstar production and B -> Ddstar l nu are also presented. The evidence for a Dstarpr meson reported recently by DELPHI is not supported by OPAL and CLEO.']",['1999-02-18']
1498,['eng'],"['Scapparone, E']",['NOE'],['Detectors and Experimental Techniques'],"['talk, Santander 1998/09/14', 'neutrino, oscillation', 'neutrino/mu, beam', 'neutrino nucleon, interaction', 'neutral current', 'charged current', 'cross section, ratio', 'neutrino, cosmic radiation', 'particle identification, (tau neutrino/tau)', 'neural network', 'transition radiation detector', 'calorimeter', 'deep underground detector, Gran Sasso', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902025'],['The project of a large underground experiment (NOE) devoted to long baseline neutrino oscillation measurement is presented'],['1999-02-17']
1499,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurements of the QED Structure of the Photon'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'muon, pair production', 'photon, structure function', 'quantum electrodynamics, structure function', 'differential cross section, x-dependence', 'angular correlation', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> muon+ muon- positron electron', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902024'],"['The structure of both quasi-real and highly virtual photons is investigated using the reaction e+e- -> e+e-mu+mu-, proceeding via the exchange of two photons. The results are based on the complete OPAL dataset taken at e+e- centre-of-mass energies close to the mass of the Z boson. The QED structure function F_2^gamma and the differential cross-section dsigdx for quasi-real photons are obtained as functions of the fractional momentum x from the muon momentum which is carried by the struck muon in the quasi-real photon for values of Q**2 ranging from 1.5 to 400 GeV**2. The differential cross-section dsigdx for highly virtual photons is measured for 1.5< Q**2 < 30 GeV**2 and 1.5< P**2 < 20 GeV**2, where Q**2 and P**2 are the negative values of the four-momentum squared of the two photons such that Q**2 > P**2. Based on azimuthal correlations the QED structure functions F_A^gamma and F_B^gamma for quasi-real photons are determined for an average Q**2 of 5.4 GeV**2.']",['1999-02-17']
1500,['eng'],"['Mountain, R J', 'Artuso, M', 'Ayad, R', 'Azfar, F', 'Efimov, A', 'Kopp, S E', 'Majumder, G', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Anderson, S', 'Smith, A', 'Kubota, Y', 'Lipeles, E', 'Coan, T E', 'Staeck, J', 'Fadeev, V', 'Volobuev, I']",['The CLEO-III Ring Imaging Cherenkov Detector'],['Detectors and Experimental Techniques'],"['talk, Ein Gedi 1998/11/15', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'Cherenkov counter, crystal', 'lithium, fluorine', 'drift chamber, wire', 'organic compounds, gas', 'electronics, readout', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902023'],"['The CLEO-III Detector upgrade for charged particle identification is discussed. The RICH design uses solid LiF crystal radiators coupled with multi-wire chamber photon detectors, using TEA as the photosensor, and low-noise Viking readout electronics. Results from our beam test at Fermilab are presented.']",['1999-03-11']
1501,['eng'],"['Asner, D M']",['Hadronic Structure in the Decay $\\tau^{-} \\to \\nu_{\\tau} \\pi^{-} \\pi^{0} \\pi^{0}$ and the Sign of the Tau Neutrino Helicity'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'amplitude analysis', 'pi, multiple production', 'mass spectrum, (pi- 2pi0)', 'neutrino/tau, helicity', 'Dalitz plot', 'a1(1260), mass', 'a1(1260), width', 'sigma meson', 'f0(1370)', 'f2(1270)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> pi- 2pi0 neutrino/tau', 'tau- --> a1(1260) neutrino/tau', 'a1(1260) --> pi- 2pi0', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902022'],"[""Based on a sample corresponding to 4.3 million produced tau-pair events, we have studied hadronic dynamics in the decay tau- --> nu_tau pi- pi0 pi0 in data recorded by the CLEO II detector operating at the CESR e+e- collider. The decay is dominated by the process tau --> nu_tau a_1(1260), with the a_1 meson decaying to three pions predominantly via the lowest dimensional (mainly S-wave) a_1 --> rho pi Born amplitude. From fits to the Dalitz plot and angular observables, we find significant additional contributions from amplitudes for a_1 decay to sigma pi, f_0(1370) pi and f_2(1270) pi, as well as higher dimensional a_1 --> rho pi and rho' pi amplitudes. The squared sigma pi amplitude accounts for ~15% of the total tau- --> nu_tau pi- pi0 pi0 rate in the models considered. We have searched for additional contributions from tau --> nu_tau pi'(1300). We place 90% confidence level upper limits on the branching fraction for this channel of between 1.0*10^{-4} and 1.9*10^{-4}, depending on the pi' decay mode. The pi- pi0 pi0 mass spectrum is parametrized by a Breit-Wigner form with a mass-dependent width which is specified according to the results of the Dalitz plot fits plus a coupling to an a_1 --> K* K amplitude. From a chi^2 fit, we extract the pole mass and width of the a_1, as well as the magnitude of the K* K coupling. We have also investigated the impact of a possible contribution from the a_1'(1700) meson on this spectrum. Finally, exploiting the parity-violating angular asymmetry in a_1 --> 3pi decay, we determine the signed value of the tau neutrino helicity to be h_{\\nu_\\tau} = -1.02 +- 0.13(stat.) +- 0.03(syst.+model), confirming the left-handedness of the tau neutrino.""]",['1999-03-11']
1502,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Frey, A', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kobayashi, T', 'Kobel, M', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Lu, J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rosati, S', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Intermittency and correlations in hadronic $Z^0$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'multiplicity, moment', 'correlation, ((n)particle)', 'intermittency', 'numerical calculations, Monte Carlo', 'quantum chromodynamics, validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902021'],"['A multidimensional study of local multiplicity fluctuations and multiparticle correlations of hadrons produced in Z decays is performed. The study is based on the data sample of more than 4 million events recorded with the OPAL detector at LEP. The fluctuations and correlations are analysed in terms of the normalized scaled factorial moments and cumulants up to the fifth order. The moments are observed to have intermittency-like behaviour, which is found to be more pronounced with increasing dimension. The large data sample allows for the first time a study of the factorial cumulants in e+e- annihilation. The analysis of the cumulants shows the existence of genuine multiparticle correlations with a strong intermittency rise up to higher orders. These correlations are found to be stronger in higher dimensions. The decomposition of the factorial moments into lower-order correlations that the dynamical fluctuations have important contributions from genuine many-particle correlations. The Monte Carlo models JETSET 7.4 and HERWIG 5.9 are found to reproduce the trend of the measured moments and cumulants but they underestimate the magnitudes. The results are found to be consistent with QCD jet formation dynamics, although additional contributions from other mechanisms in the hadronization process cannot be excluded.']",['1999-03-08']
1503,['eng'],"['Glenzinski, D A']",['Measurement of the W Mass from LEP2'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, mass', 'W, leptonic decay', 'W, hadronic decay', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', '161, 172, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902020'],"['In 1997 each LEP experiment collected approximately $55 {pb}^{-1}$ of data at a center-of-mass energy of 183 GeV. These data yield a sample of candidate $e^+e^- \\to W^+W^-$ events from which the mass of the W boson, M_W, is measured. The preliminary LEP combined result, including data taken at $\\roots = 161$ and 172 GeV and assuming the Standard Model relation between the W decay width and mass, is $M_W = 80.38 \\pm 0.07 (exp) \\pm 0.03 (CR/BE) \\pm 0.02 (E_{bm})$ GeV, where the uncertainties correspond to experimental, colour-reconnection/Bose-Einstein, and LEP beam energy respectively.']",['1999-03-11']
1504,['eng'],"['Adloff, C']",['Elastic Electroproduction of $\\rho$ Mesons at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, exclusive reaction', 'mass spectrum, two-pion', 'rho(770), electroproduction', 'rho(770), hadronic decay', 'momentum transfer, dependence', 'energy dependence', 'spin, density matrix', 'helicity, scattering amplitude', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'angular distribution', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'tables', 'positron p --> p rho(770) positron', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902019'],"['The elastic electroproduction of rho mesons is studied at HERA with the H1 detector for a photon virtuality in the range 1 < Q^2 < 60 GeV^2 and for a hadronic centre of mass energy in the range 30 < W < 140 GeV. The shape of the pipi mass distribution in the rho resonance region is measured as a function of Q^2. The full set of rho spin density matrix elements is determined, and evidence is found for a helicity flip amplitude at the level of 8 +- 3 % of the non-flip amplitudes. Measurements are presented of the dependence of the cross section on Q^2, W and t (the four-momentum transfer squared to the proton). They suggest that, especially at large Q^2, the gamma^*p cross section develops a stronger W dependence than that expected from the behaviour of elastic and total hadron-hadron cross sections.']",['1999-03-11']
1505,['eng'],"['Battistoni, G', 'Scapparone, E']",['Hints of $\\mu+N \\to \\mu+N + \\mu^{+}\\mu^{-}$ process observation with the MACRO experiment'],['Particle Physics - Experimental Results'],"['talk, Assergi 1998/07/12', 'muon, cosmic radiation', 'muon nucleon, exclusive reaction', 'muon, pair production', 'correlation, (muon+ muon-)', 'effect, coherence', 'numerical calculations, Monte Carlo', 'deep underground detector, MACRO', 'experimental results', 'muon nucleon --> nucleon 3muon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902018'],['We present the analysis of the distribution of the distance of muon pairs detected deep underground by the MACRO experiment. A detailed analysis of the low separation region pointed out an excess of experimental data with respect to the Monte Carlo expectation. The effect is discussed taking into account the mu + N ----> mu + N + mu- + mu+.'],['1999-02-15']
1506,['eng'],"['Adeva, B', 'Gómez, F', 'Pazos, A', 'Pfau, R', 'Pló, M', 'Rodríguez, J M', 'Vázquez, P', 'Labbé, J C']",['The Micro Wire Detector'],['Detectors and Experimental Techniques'],"['proportional chamber, gas', 'proportional chamber, wire', 'argon, organic compounds', 'position sensitive', 'charge, yield']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902017'],"['We present the performance of a new proportional gas detector. Its geometry consists of a cathode plane with 70x70 micron apertures, crossed by 25 micron anode strips to which it is attached by 50 micron kapton spacers. In the region where the avalanche takes place, the anode strips are suspended in the gas mixture like in a standard wire chamber. This detector exhibits high rate capability and large gains, introducing very little material.']",['1999-02-15']
1507,['eng'],"['Scapparone, E']",['Study of the Photonuclear interaction of muons in rock with the MACRO experiment'],['Particle Physics - Experimental Results'],"['talk, Assergi 1998/07/12', 'muon, cosmic radiation', 'muon nucleus, interaction', 'exchange, one-photon', 'hadron, photoproduction', 'cross section, energy dependence', 'background', 'charged particle, multiplicity', 'numerical calculations, Monte Carlo', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902016'],['We present first results about the measurement of the charged hadrons production by atmopsheric muons in the rock above MACRO. A comparison between the measure rate with the Monte Carlo expectation is presented'],['1999-02-15']
1508,['eng'],"['Bailly, P', 'Chauveau, J', 'Genat, J F', 'Huppert, J F', 'Lebbolo, H', 'Roos, L', 'Zhang, B']",['A 16-channel digital TDC chip'],['Detectors and Experimental Techniques'],"['Cherenkov counter, ring imaging', 'optics, reflection', 'integrated circuit', 'electronics, readout', 'signal processing', 'measurement, time', 'performance', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902015'],"['A 16-channel digital TDC chip has been built for the DIRC Cherenkov counter of the BaBar experiment at the SLAC B-factory (Stanford, USA). The binning is 0.5 ns, the conversion time 32 ns and the full-scale 32 mus. The data driven architecture integrates channel buffering and selective readout of data falling within a programmable time window. The time measuring scale is constantly locked to the phase of the (external) clock. The linearity is better than 80 ps rms. The dead time loss is less than 0.1% for incoherent random input at a rate of 100 khz on each channel. At such a rate the power dissipation is less than 100 mw. The die size is 36 mm2.']",['1999-02-11']
1509,['eng'],"['Baudis, L', 'Dietz, A', 'Heusser, G', 'Klapdor-Kleingrothaus, H V', 'Krivosheina, I V', 'Kolb, S', 'Majorovits, B', 'Melnikov, V F', 'Päs, H', 'Schwamm, F', 'Strecker, H', 'Alexeev, V I', 'Balysh, A Y', 'Bakalyarov, A', 'Belyaev, S T', 'Lebedev, V I', 'Zhukov, S V']",['Limits on the Majorana neutrino mass in the 0.1 eV range'],['Particle Physics - Experimental Results'],"['neutrino, Majorana', 'neutrino, mass', 'upper limit', 'double-beta decay, (0neutrino)', 'germanium, lifetime', 'lower limit', 'semiconductor detector, experimental results', 'deep underground detector, Gran Sasso']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902014'],"['The Heidelberg-Moscow experiment gives the most stringent limit on the Majorana neutrino mass. After 24 kg yr of data with pulse shape measurements, we set a lower limit on the half-life of the neutrinoless double beta decay in 76Ge of T_1/2 > 5.7 * 10^{25} yr at 90% C.L., thus excluding an effective Majorana neutrino mass greater than 0.2 eV. This allows to set strong constraints on degenerate neutrino mass models.']",['1999-02-11']
1510,['eng'],"['Abbott, B']",['Search for Squarks and Gluinos in Events Containing Jets and a Large Imbalance in Transverse Energy'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'jet, multiple production', 'transverse energy, missing-energy', 'sparticle, search for', 'squark, mass', 'gluino, mass', 'lower limit', 'supergravity', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902013'],"['Using data corresponding to an integrated luminosity of 79 pb-1, D0 has searched for events containing multiple jets and large missing transverse energy in pbar-p collisions at sqrt(s)=1.8 TeV at the Fermilab Tevatron collider. Observing no significant excess beyond what is expected from the standard model, we set limits on the masses of squarks and gluinos and on the model parameters m_0 and m_1/2, in the framework of the minimal low-energy supergravity models of supersymmetry. For tan(beta) = 2 and A_0 = 0, with mu < 0, we exclude all models with m_squark < 250 GeV/c^2. For models with equal squark and gluino masses, we exclude m < 260 GeV/c^2.']",['1999-02-11']
1511,['eng'],"['Yellin, S J']",['A Comparison of the LSND and KARMEN antineutrino Oscillation Experiments'],['Particle Physics - Experimental Results'],"['talk, Monterey 1998/11/15', 'neutrino, oscillation', 'antineutrino/mu, secondary beam', 'antineutrino/e, search for', 'experimental methods', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902012'],['The LSND and KARMEN neutrino oscillation experiments are compared in order to clarify the significance of the apparent disagreement between their results.'],['1999-02-11']
1512,['eng'],"['Bonvicini, G']",['Measurement of Charm Meson Lifetimes'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed meson, electroproduction', 'D0', 'D+', 'D/s+', 'charmed meson, hadronic decay', 'charmed meson, lifetime', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> charmed meson anything', 'D0 --> K- (n)pi', 'D+ --> K- 2pi+', 'D/s+ --> Phi(1020) pi+', 'Phi(1020) --> K+ K-', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902011'],"['We report measurements of the $D^0, D^+$, and $D^+_s$ meson lifetimes using 3.7 fb^{-1} of e^+e^- annihilation data collected near the $\\Upsilon(4S)$ resonance with the CLEO detector. The lifetimes of the $D^0, D^+$, and $D^+_s$ mesons are measured to be $408.5 \\pm 4.1 ^{+3.5}_{-3.4} fs, 1033.6 \\pm 22.1 ^{+9.9}_{-12.7} fs$, and $486.3 \\pm 15.0 ^{+4.9}_{-5.1} fs$, respectively. The precisions of the charm meson lifetimes reported here are comparable to those of the best previous measurements, and the systematic errors are very different.']",['1999-02-10']
1513,['eng'],"['Nachtman, J M', 'Saltzberg, D', 'Worcester, M']",['Study of a Like-Sign Dilepton Search for Chargino-Neutralino Production at CDF'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1999/01/05', 'anti-p p, colliding beams', 'sparticle, pair production', 'chargino', 'neutralino', 'sparticle, decay', 'final state, (3lepton)', 'transverse energy, missing-energy', 'search for, dilepton', 'charge, dilepton', 'background', 'channel cross section, branching ratio', 'particle identification, efficiency', 'magnetic detector, CDF', 'Batavia TEVATRON Coll', 'numerical calculations, Monte Carlo', 'anti-p p --> chargino neutralino anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902010'],"['We propose a like-sign dilepton search for chargino-neutralino production in p-pbar collisions at sqrt(s) = 1.8 TeV, which complements the previously published trilepton search by the CDF detector using Fermilab Run I data. Monte Carlo predictions for the signal and background efficiencies indicate a significant increase in sensitivity to chargino-neutralino production compared to the traditional trilepton analysis alone.']",['1999-02-10']
1514,['eng'],"['Junk, T R']",['Confidence Level Computation for Combining Searches with Small Statistics'],['Detectors and Experimental Techniques'],"['new particle, search for', 'statistical analysis', 'data analysis method', 'electron positron, annihilation', 'Higgs particle, electroproduction', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902006'],"['This article describes an efficient procedure for computing approximate confidence levels for searches for new particles where the expected signal and background levels are small enough to require the use of Poisson statistics. The results of many independent searches for the same particle may be combined easily, regardless of the discriminating variables which may be measured for the candidate events. The effects of systematic uncertainty in the signal and background models are incorporated in the confidence levels. The procedure described allows efficient computation of expected confidence levels.']",['1999-02-08']
1515,['eng'],"['Stocchi, A']",['$B^{0} - \\overline{B}^{0}$ oscillations and measurements of $|V_{ub}|/|V_{cb}|$ at LEP'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, oscillation', 'B0, mass difference', 'B/s0, mass difference', 'Kobayashi-Maskawa angle, parametrization', 'particle identification, flavor', 'B0, semileptonic decay', 'lepton, charge', 'correlation, (D/s lepton)', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902004'],['In this paper a review of the LEP analyses on $B^0-\\bar{B}^0$ oscillations and on the measurement of $|V_{ub}|/|V_{cb}|$ is presented . These measurements are of fundamental importance in constraining the $\\rho$ and $\\eta$ parameters of the CKM matrix. A review of the current status of the $V_{CKM}$ matrix determination is also given.'],['1999-02-04']
1516,['eng'],"['Chung, S U']",['Evidence for Exotic $J^{PC}=1^{\\mp}$ Meson Production in the Reaction $\\pi^{-}p \\to \\eta \\pi^{-}p$ at 18 GeV/c'],['Particle Physics - Experimental Results'],"['pi- p, exclusive reaction', 'eta, hadroproduction', 'mass spectrum, (eta pi-)', 'eta, hadronic decay', 'eta, radiative decay', 'angular distribution, asymmetry', 'mass, dependence', 'partial wave analysis', 'amplitude analysis', 'a2(1320), interference', 'meson resonance, exotic', 'meson resonance, quantum number', 'mass, width', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'bibliography', 'pi- p --> p eta pi-', 'eta --> pi+ pi- pi0', 'eta --> 2photon', '18 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902003'],['Details of the analysis of the eta pi- system studied in the reaction pi^{-} p --> eta pi^{-} p at 18 GeV/c are given. Separate analyses for the 2 gamma and pi+ pi- pi0 decay modes of the eta are presented. An amplitude analysis of the data indicates the presence of interference between the a(2)(1320)- and a J^{PC}=1^{-+} wave between 1.2 and 1.6 GeV/c^2. The phase difference between these waves shows phase motion not attributable solely to the a(2)(1320)-. The data can be fitted by interference between the a(2)(1320)- and an exotic 1^{-+} resonance with M = 1370 +-16 +50 -30} MeV/c^2 and Gamma = 385 +- 40 +65 -105 MeV/c^2. Our results are compared with those of other experiments.'],['1999-02-03']
1517,['eng'],[],['Measurement of the Associated $\\gamma + \\mu^{\\pm}$ Production Cross Section in $p\\overline{p}$ Collisions at $\\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'photon, direct production', 'muon, associated production', 'quark gluon, Compton scattering', 'quark, charm', 'p, charm', 'showers, parton', 'quantum chromodynamics, perturbation theory', 'angular correlation, (muon photon)', 'muon, transverse momentum', 'quark, transverse momentum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> muon photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902001'],"['We present the first measurement of associated direct photon + muon production in hadronic collisions, from a sample of 1.8 TeV $p \\bar p$ collisions recorded with the Collider Detector at Fermilab. Quantum chromodynamics (QCD) predicts that these events are primarily from the Compton scattering process $cg \\to c\\gamma$, with the final state charm quark producing a muon. Hence this measurement is sensitive to the charm quark content of the proton. The measured cross section of $29\\pm 9 pb^{-1}$ is compared to a leading-order QCD parton shower model as well as a next-to-leading-order QCD calculation.']",['1999-02-02']
1518,['eng'],"['Brook, N H']",['Momentum Spectra in the Current Region of the Breit Frame in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['talk, Durham 1998/09/20', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'charged particle, multiple production', 'kinematics, Breit frame', 'momentum spectrum, moment', 'momentum transfer, dependence', 'x-dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901041'],['The production of charged particles has been measured in deep inelastic scattering (DIS) with the ZEUS detector. The evolution of the moments of the scaled momenta distributions in $Q^2$ and $x$ has been investigated in the current fragmentation region of the Breit frame. The results in the current region are compared to $e^+e^-$ data and QCD analytical calculations. The results are consistent with the universality of single-particle spectra in DIS and $e^+e^-$ annihilation at high $Q^2.$ The results at low $Q^2$ disagree with analytical calculations based on the modified leading log approximation (MLLA) and local parton hadron duality (LPHD).'],['1999-02-01']
1519,['eng'],"['Abbott, B']",['Measurement of W and Z boson production cross sections in pp collisions at square root s=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'W, width', 'channel cross section, branching ratio', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901040'],"['DO has measured the inclusive production cross section of W and Z bosons in a sample of 13 pb$^{-1}$ of data collected at the Fermilab Tevatron. The cross sections, multiplied by their leptonic branching fractions, for production in pbar-p collisions at sqrt{s}=1.8 TeV are sigma_W*B(W->e nu) = 2.36+-0.02+-0.08+-0.13 nb, sigma_W*B(W->mu nu) = 2.09+-0.06+-0.22+-0.11 nb, sigma_Z*B(Z->e+ e-) = 0.218+-0.008+-0.008+-0.012 nb, and sigma_Z*B(Z->mu+ mu-) = 0.178+-0.022+-0.021+-0.009 nb, where the first uncertainty is statistical and the second systematic; the third reflects the uncertainty in the integrated luminosity. For the combined electron and muon analyses, we find sigma_W*B(W->l mu)/sigma_Z*B(Z->l+ l-) = 10.90+-0.52. Assuming standard model couplings, we use this result to determine the width of the W boson, and obtain Gamma(W) = 2.044+-0.097 GeV.']",['1999-02-01']
1520,['eng'],"['Miller, D J']",['Precision Studies at a Future Linear Collider'],['Detectors and Experimental Techniques'],"['talk, Barcelona 1998/09/08', 'electron positron, colliding beams', 'electron positron, annihilation', 'electroweak interaction, validity test', 'channel cross section, energy dependence', 'quark, electroproduction', 'quark, truth', 'Higgs particle, electroproduction', 'coupling, Yukawa', 'Higgs particle, mass', 'supersymmetry', 'sparticle, electroproduction', 'jet, pair production', 'energy spectrum, (2jet)', 'quantum chromodynamics', 'photon photon, exclusive reaction', 'photon electron, exclusive reaction', 'backscatter, laser', 'luminosity', 'counters and detectors, proposed', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901039'],"['A future linear collider will complement the programme of the Large Hadron Collider, especially for precision physics. The RADCOR community has an important part to play in refining the predictions for rates and processes in Electroweak, Higgs, SUSY, top and QCD physics, for e^+ e^-, e^- e^-, $\\gamma']",['1999-01-28']
1521,['eng'],"['Angelis, Aris L S', 'Bartke, J', 'Bogolyubsky, M Yu', 'Filippov, S N', 'Gladysz-Dziadus, E', 'Kharlov, Yu V', 'Kurepin, A B', 'Maevskaya, A I', 'Mavromanolakis, G', 'Panagiotou, A D', 'Sadovsky, S A', 'Stefanski, P', 'Wlodarczyk, Z']",['CASTOR'],['Detectors and Experimental Techniques'],"['talk, Delphi 1998/09/06', 'nucleus nucleus, nuclear reaction', 'search for, centauro', 'matter, strangeness', 'calorimeter, proposed', 'tungsten', 'Cherenkov counter', 'silicon, glass', 'magnetic detector, CASTOR', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901038'],"['The physics motivation for a very forward detector for the ALICE heavy ion experiment at the CERN LHC is discussed. A phenomenological model describing the formation and decay of a Centauro fireball in nucleus-nucleus collisions is presented. The CASTOR detector which is aimed to measure the hadronic and photonic content of an interaction and to identify deeply penetrating objects in the very forward, baryon-rich phase space 5.6 < eta < 7.2 in an event-by-event mode is described. Results of simulations of the expected response of the calorimeter, and in particular to the passage of strangelets, are presented.']",['1999-01-28']
1522,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Searches for R-Parity Violating Decays of Gauginos at 183 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'supersymmetry', 'sparticle, pair production', 'chargino', 'neutralino', 'coupling, Yukawa', 'gaugino, decay', 'R parity, violation', 'LSP, decay modes', 'event shape analysis', 'channel cross section, mass', 'upper limit', 'sparticle, mass', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901037'],"['Searches for pair-produced charginos and neutralinos with R-parity violating decays have been performed using a data sample corresponding to an integrated luminosity of 56 pb-1 collected with the OPAL detector at LEP at a centre-of-mass energy of 183 GeV. An important consequence of R-parity violation is that the lightest supersymmetric particle becomes unstable. The searches have been performed under the assumptions that the lightest supersymmetric particle promptly decays and that only one R-parity violating coupling is dominant for each of the decay modes considered. Such processes would yield multiple leptons, leptons plus jets, or multiple jets with or without significant missing energy in the final state. No excess of such events above Standard Model backgrounds has been observed. Limits are presented on the production cross-sections of gauginos in R-parity violating scenarios. Limits are also presented in the framework of the Minimal Supersymmetric Standard Model.']",['1999-01-28']
1523,['eng'],"['Adachi, K']",['Measurement of the jet width in $\\gamma\\gamma$ collisions and in $e^{+}e^{-}$ annihilation process at TRISTAN'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'exchange, two-photon', 'photon photon, interaction', 'photon, resolved', 'jet, photoproduction', 'jet, width', 'transverse energy, dependence', 'scaling', 'transverse energy, energy flow', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', 'approx. 58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901036'],"['The shape of jets produced in (quasi-) real photon-photon collisions as well as in e^+e^- annihilation process has been studied with a cone jet finding algorithm, using the data taken with the TOPAZ detector at the TRISTAN e^+e^- collider at an average center-of-mass energy of 58 GeV. The results are presented in terms of the jet width as a function of the jet transverse energy(E^{jet}_T) as well as a scaled transverse jet energy, x_T(=2E^{jet}_T/root(s)). The jet width narrows as E^{jet}_T increases; however, at the same value of E^{jet}_T the jet width in gamma-gamma collisions at TRISTAN is significantly narrower than that in gamma p collisions at HERA. By comparing our results with the data in other reactions, it has been shown that the jet width in gamma-gamma, gamma p, p\\bar{p} collisions as well as the e^+e^- annihilation process has an approximate scaling behavior as a function of x_T.']",['1999-01-27']
1524,['eng'],"['Boucrot, J']",['Oscillations of neutral B mesons systems'],['Particle Physics - Experimental Results'],"['review, Genoa 1998/06/30', 'B0 anti-B0, oscillation', 'B/s0 anti-B/s0, oscillation', 'B0, mass difference', 'B/s0, mass difference', 'lower limit', 'unitarity', 'B0, particle identification', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901035'],"['The oscillation phenomenon in the neutral B mesons systems is now well established. The motivations and principles of the measurements are given; then the most recent results from the LEP experiments, the CDF collaboration at Fermilab and the SLD collaboration at SLAC are reviewed. The present world average of the $\\bd$ meson oscillation frequency is $\\dmd = 0.471 \\pm 0.016 \\ps$ and the lower limit on the $\\bs$ oscillation frequency is']",['1999-01-27']
1525,['eng'],"['Amendolia, S R', 'Barbuto, E', 'Bozza, C', ""D'Apolito, C"", 'Bartolomeo, A D', 'Funaro, M', 'Grella, G', 'Iovane, G', 'Pelosi, P', 'Romano, G']",['Status of Salerno Laboratory'],['Detectors and Experimental Techniques'],"['talk, Nagoya 1998/06/12', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'muon, flux', 'nuclear emulsion']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901034'],"['A report on the analysis work in the Salerno Emulsion Laboratory is presented. It is related to the search for nu_mu->nu_tau oscillations in CHORUS experiment, the calibrations in the WANF (West Area Neutrino Facility) at Cern and tests and preparation for new experiments.']",['1999-01-26']
1526,['eng'],"['Naroska, B']",['Heavy Flavour Physics at HERA'],['Particle Physics - Experimental Results'],"['talk, Batavia 1998/10/10', 'positron p, colliding beams', 'positron p, inclusive reaction', 'positron p, inelastic scattering', 'quark, charm', 'quark, beauty', 'quark, pair production', 'J/psi(3100), photoproduction', 'D*(2010), photoproduction', 'p, structure function', 'structure function, charm', 'gluon, momentum spectrum', 'cross section, energy dependence', 'transverse momentum, dependence', 'rapidity dependence', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901033'],"['New results with increased statistics are presented for heavy flavour production at Q2<150 Gev2 and in the photoproduction limit Q2-->0. Cross sections for Dstar production, F2charm, the gluon density in the proton, and inelastic J/psi production are discussed and compared to theoretical calculations. A first measurement of the b anti-b cross section is reported.']",['1999-01-26']
1527,['eng'],"['De Trocóniz, J F']",['Tests of the Electroweak Symmetry Breaking Sector at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Illa da Toxa 1998/06/01', 'anti-p p, inclusive reaction', 'electroweak interaction, symmetry breaking', 'new particle, search for', 'resonance, hadroproduction', 'intermediate boson, associated production', 'Higgs particle, hadronic decay', 'Higgs particle, mass', 'quark, beauty', 'quark, pair production', 'W, leptonic decay', 'intermediate boson, hadronic decay', 'fermion, technicolor', 'technipion', 'technirho', 'leptoquark, pair production', 'tau, pair production', 'jet, multiplicity', 'channel cross section, branching ratio', 'upper limit', 'proposed experiment, Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902009'],['The phenomenology of the electroweak symmetry breaking sector is expected to involve resonances decaying preferentially into heavy fermions. Three recent CDF analyses are reviewed and used to constrain Higgs and Technicolor models.'],['1999-02-09']
1528,['eng'],"['Müller, D']",['Physics Results from SLD Using the CRID'],['Particle Physics - Experimental Results'],"['talk, Ein Gedi 1998/11/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'hadron, multiple production', 'angular distribution, asymmetry', 'leading particle', 'correlation', 'B0 anti-B0, interference', 'quark, jet', 'quark, hadronization', 'particle identification, flavor', 'Cherenkov counter, ring imaging', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901032'],"['We review recent Z^0 physics results from SLD that use the Cherenkov Ring Imaging Detector for charged particle identification. The performance of the detector and likelihood method are described briefly. Several hadronization measurements are presented, including identified hadron production in events of different primary flavors, leading hadron production, and new correlation studies sensitive to details of both leading and nonleading hadron production. Identified K^+- have been used in conjunction with precision vertexing to study charmless and doubly charmed B-hadron decays. This combination has also been used to tag b, b-bar, c and c-bar jets, yielding precise measurements of B^0-B^0bar mixing and of the asymmetric couplings A_b and A_c. Identified K^+- and Lambda^0 have been used to tag s and s-bar jets, yielding a measurement of A_s. The clean identified particle samples provided efficiently by the CRID allow the purities of these tags to be measured from the data, an essential ingredient for precision physics.']",['1999-01-25']
1529,['eng'],"['Amendolia, S R', 'Barbuto, E', 'Bozza, C', ""D'Apolito, C"", 'Bartolomeo, A D', 'Funaro, M', 'Grella, G', 'Iovane, G', 'Pelosi, P', 'Romano, G']",['SySa'],['Detectors and Experimental Techniques'],"['talk, Nagoya 1998/06/12', 'neutrino, oscillation', 'track data analysis', 'nuclear emulsion', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901031'],"['SySal (SYstem of SALerno) is the automatic scanning system developed in the emulsion laboratory of Salerno to take part in the emulsion scanning phase of the CHORUS experiment at CERN. In the following chapters we will present features, results and further developments of this automatic multi-tracking system.']",['1999-01-25']
1530,['eng'],"['King, B J']",['Estimates of Vertex Tagging Efficiencies at a Muon Collider Higgs Factory'],['Detectors and Experimental Techniques'],"['talk, Batavia 1997/11/06', 'muon+ muon-, colliding beams', 'Higgs particle, electroproduction', 'Higgs particle, hadronic decay', 'Higgs particle, leptonic decay', 'Higgs particle, branching ratio', 'particle identification, (beauty charm tau)', 'jet, particle identification', 'efficiency', 'muon+ muon- --> Higgs particle anything', 'Higgs particle --> 2beauty', 'Higgs particle --> 2charm', 'Higgs particle --> tau+ tau-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907034'],"['Tagging efficiencies and purities are estimated for the decay modes H -> b-bbar, H -> tau-taubar and H -> c-cbar of Higgs bosons produced at an s-channel muon collider Higgs factory.']",['1999-10-22']
1531,['eng'],"['King, B J']",['Neutrino Physics at a Muon Collider'],['Detectors and Experimental Techniques'],"['talk, Batavia 1997/11/06', 'muon+ muon-, colliding beams', 'muon, leptonic decay', 'neutrino, secondary beam', 'neutrino nucleon, interaction', 'charged current', 'neutral current', 'quantum chromodynamics', 'nucleon, structure function', 'Kobayashi-Maskawa angle', 'Weinberg angle', 'neutrino, oscillation', 'heavy lepton, search for', 'production, charm', 'neutrino, counters and detectors', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9907033'],"['An overview is given of the neutrino physics potential of future muon storage rings that use muon collider technology to produce, accelerate and store large currents of muons.']",['1999-10-22']
1532,['eng'],"['Bloch-Devaux, B']",['Z lineshape and forward-backward asymmetries'],['Particle Physics - Experimental Results'],"['review, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, leptonic decay', 'Z0, width', 'Z0, mass', 'angular distribution, asymmetry', 'cross section, hadronic', 'neutrino, flavor', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901029'],"['Preliminary but close to final results on the Z lineshape and Forward-Backward asymmetries from the four LEP experiments are presented. Combined values extracted from ALEPH. DELPHI, L3 and OPAL data recorded at energies around the Z pole are discussed.']",['1999-01-29']
1533,['eng'],"['Ambrosio, M', 'Antolini, R', 'Aramo, C', 'Auriemma, G', 'Baldini, A', 'Barbarino, G C', 'Barish, B C', 'Battistoni, G', 'Bellotti, R', 'Bemporad, C', 'Bernardini, E', 'Bernardini, P', 'Bilokon, H', 'Bisi, V', 'Bloise, C', 'Bower, C', 'Bussino, S', 'Cafagna, F', 'Calicchio, M', 'Campana, D', 'Carboni, M', 'Castellano, M G', 'Cecchini, S', 'Cei, F', 'Chiarella, V', 'Choudhary, B C', 'Coutu, S', 'De Cataldo, G', 'Dekhissi, H', 'De Marzo, C', 'De Mitri, I', 'Derkaoui, J E', 'De Vincenzi, M', 'Di Credico, A', 'Erriquez, O', 'Favuzzi, C', 'Forti, C', 'Fusco, P', 'Giacomelli, Giorgio', 'Giannini, G', 'Giglietto, N', 'Giorgini, M', 'Grassi, M', 'Gray, L', 'Grillo, A', 'Guarino, F', 'Gustavino, C', 'Habig, A', 'Hanson, K', 'Heinz, R', 'Huang, Y', 'Iarocci, Enzo', 'Katsavounidis, E', 'Katsavounidis, I', 'Kearns, E T', 'Kim, H', 'Kyriazopoulou, S', 'Lamanna, E', 'Lane, C', 'Lari, T', 'Levin, D S', 'Lipari, P', 'Longley, N P', 'Longo, M J', 'Loparco, F', 'Maaroufi, F', 'Mancarella, G', 'Mandrioli, G', 'Manzoor, S', 'Margiotta-Neri, A', 'Marini, A', 'Martello, D', 'Marzari-Chiesa, A', 'Mazziotta, M N', 'Mazzotta, C', 'Michael, D G', 'Mikheyev, S P', 'Miller, L', 'Monacelli, P', 'Montaruli, T', 'Monteno, M', 'Mufson, S L', 'Musser, J', 'Nicolo, D', 'Orth, C', 'Osteria, G', 'Ouchrif, M', 'Palamara, O', 'Patera, V', 'Patrizii, L', 'Pazzi, R', 'Peck, C W', 'Petrera, S', 'Pistilli, P', 'Popa, V', 'Rainó, A', 'Rastelli, A', 'Reynoldson, J', 'Ronga, F', 'Rubizzo, U', 'Satriano, C', 'Satta, L', 'Scapparone, E', 'Scholberg, K', 'Sciubba, A', 'Serra-Lugaresi, P', 'Severi, M', 'Sioli, M', 'Sitta, M', 'Spinelli, P', 'Spinetti, M', 'Spurio, M', 'Steinberg, R', 'Stone, J L', 'Sulak, Lawrence R', 'Surdo, A', 'Tarle, G', 'Togo, V', 'Ugolotti, D', 'Vakili, M', 'Walter, C W', 'Webb, R']",['High statistics measurement of the underground muon pair separation at Gran Sasso'],['Astrophysics and Astronomy'],"['muon, cosmic radiation', 'cosmic radiation, secondary radiation', 'muon, angular distribution', 'correlation, dimuon', 'coherence, decoherence', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901027'],"['We present a measurement of the underground decoherence function using multi-muon events observed in the MACRO detector at Gran Sasso at an average depth of 3800 hg/cm/sup 2/. Muon pair separations up to 70 m have been measured, corresponding to parent mesons with P/sub perpendicular to /<or=1-2 GeV/c. Improved selection criteria are used to reduce detector effects mainly in the low distance separation region of muon pairs. Special care is given to a new unfolding procedure designed to minimize systematic errors in the numerical algorithm. The accuracy of the measurement is such that the possible contribution of rare processes, such as mu /sup +or-/+N to mu /sup +or-/+N+ mu /sup +/+ mu /sup -/, can be experimentally studied. The measured decoherence function is compared with the predictions of the hadronic interaction model of the HEMAS Monte Carlo code. Good agreement is obtained. We interpret this agreement to indicate that no anomalous P/sub perpendicular to / components in soft hadron- nucleus and nucleus-nucleus collisions are required by the MACRO experimental data. Preliminary comparisons with other Monte Carlo codes point out that the uncertainties associated with the hadronic interaction model may be as large as 20, depending on the energy. MACRO data can be used as a benchmark for future work on the discrimination of shower models in the primary energy region around and below the knee of the spectrum. (36 refs).']",['1999-11-24']
1534,['eng'],"['Newman, P']",['Diffractive Phenomena at HERA'],['Particle Physics - Experimental Results'],"['talk, Stara Lesna 1998/09/07', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'photon p, exclusive reaction', 'vector meson, photoproduction', 'baryon, leading particle', 'diffraction', 'exchange, pomeron', 'color, singlet', 'exchange, two-gluon', 'exchange, Regge', 'rapidity, gap', 'photon, resolved', 'photon, dissociation', 'jet, pair production', 'energy dependence', 'momentum transfer, dependence', 'momentum spectrum, parton', 'helicity', 'structure function, pomeron', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901026'],"['Highlights selected from recent measurements of colour-singlet exchange processes at HERA are summarised. Particular emphasis is placed on energy and momentum transfer dependences and the decomposition of the data into an expansion in Regge trajectories. The latest results in vector meson helicity analysis, partonic descriptions of hard diffraction and diffractive dijet production are also covered.']",['1999-01-19']
1535,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the W Mass and Width in $e^{+}e^{-}$ Collisions at 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, mass', 'W, width', 'W, hadronic decay', 'W, leptonic decay', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', 'W --> quark antiquark', 'W --> lepton neutrino', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901025'],"['Using a data sample of 57 pb-1 recorded at a centre-of-mass energy of 183 GeV with the Opal detector at LEP, 282 W+W- -> qqqq and 300 W+W- -> qqlnu candidate events are used to obtain a measurement of the mass of the W boson, W_W = 80.39 +- 0.13(stat.) +- 0.05(syst.) GeV assuming the Standard Model relation between M_W and Gam_W. A second fit provides a direct measure of the width of the W boson and gives Gam_W = 1.96 +- 0.34(stat.) +- 0.20(syst.) GeV. These results are combined with previous OPAL results to obtain M_W = 80.38 +- 0.12(stat.) +- 0.05(syst.) GeV and Gam_W = 1.84 +- 0.32(stat.) +- 0.20(syst.) GeV.']",['1999-01-19']
1536,['eng'],"['Allison, W W M']",['The Atmospheric Neutrino Flavor Ratio from a 3.9 Fiducial Kiloton-Year Exposure of Soudan 2'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'ratio, (neutrino/mu neutrino/e)', 'neutrino nucleus, interaction', 'iron', 'calorimeter, sandwich', 'statistical analysis', 'particle identification, flavor', 'deep underground detector, Soudan', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901024'],"['We report a measurement of the atmospheric neutrino flavor ratio, R, using a sample of quasi-elastic neutrino interactions occurring in an iron medium. The flavor ratio (tracks/showers) of atmospheric neutrinos in a 3.9 fiducial kiloton-year exposure of Soudan 2 is 0.64 +- 0.11 (stat.) +- 0.06 (syst.) of that expected. Important aspects of our main analysis have been checked by carrying out two independent, alternative analyses; one is based upon automated scanning, the other uses a multivariate approach for background subtraction. Similar results are found by all three approaches.']",['1999-01-18']
1537,['eng'],"['Abbott, B']",['Measurement of the Top Quark Pair Production Cross Section in the All-jets Decay Channel'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, ((n)jet)', 'neural network', 'mass, truth', 'channel cross section', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', 'W --> quark antiquark', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901023'],"['We present a measurement of tbar-t production using multijet final states in pbar-p collisions at a center-of-mass energy of 1.8 TeV, with an integrated luminosity of 110.3 pb(-1). The analysis has been optimized using neural networks to achieve the smallest expected fractional uncertainty on the tbar-t production cross section, and yields a cross section of 7.1 +/- 2.8(stat.) +/- 1.5(syst.) pb, assuming a top quark mass of 172.1 GeV/c^(2). Combining this result with previous D0 measurements, where one or both of the W bosons decay leptonically, gives a tbar-t production cross section of 5.9 +/- 1.2(stat) +/- 1.1(syst) pb.']",['1999-01-18']
1538,['eng'],"['Bai, J Z']",['Charmonium decays to axial-vector plus pseudoscalar mesons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), hadronic decay', 'psi(3685), branching ratio', 'upper limit', 'b1(1235)', 'K1(1400)', 'K1(1270)', 'magnetic detector, BES', 'experimental results', 'Beijing Stor', 'psi(3685) --> axial-vector meson pseudoscalar meson', 'psi(3685) --> b1(1235) pi', 'psi(3685) --> K1(1400) K', 'psi(3685) --> K1(1270) K', '3.685 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901022'],['A sample of 3.79 million psi(2S) decays observed in the BES detector is used to study the decays of charmonium to axialvector plus pseudoscalar mesons. The branching fraction for psi(2S) to b1pi agrees with expectations. A contrasting behavior between the psi(2S) and the J/psi decays to K1K cannot be accommodated by an adjustment of the singlet-triplet axialvector mixing angle.'],['1999-01-18']
1539,['eng'],"['Klapdor-Kleingrothaus, H V']",['Double $\\beta$ and Dark Matter Search'],['Particle Physics - Experimental Results'],"['review, Trento 1998/04/20', 'double-beta decay, (2neutrino)', 'double-beta decay, (0neutrino)', 'nucleus, lifetime', 'new particle, search for', 'new interaction, search for', 'electroweak interaction, validity test', 'neutrino/e, mass', 'supersymmetry', 'symmetry, left-right', 'R parity, violation', 'sneutrino, mass', 'neutrino, sterile', 'leptoquark', 'model, composite', 'relativity theory', 'equivalence principle', 'neutrino, oscillation', 'astrophysics, missing-mass', 'WIMP', 'neutrino, Majorana', 'semiconductor detector, germanium', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901021'],"['Nuclear double beta decay provides an extraordinarily broad potential to search for beyond Standard Model physics, probing already now the TeV scale, on which new physics should manifest itself. These possibilities are reviewed here. First, the results of present generation experiments are presented. The most sensitive one of them - the Heidelberg-Moscow experiment in the Gran Sasso - probes the electron mass now in the sub eV region and will reach a limit of of the Heidelberg Double Beta Group in the last two years, results are obtained also for SUSY models (R-parity breaking, sneutrino mass), leptoquarks (leptoquark-Higgs coupling), compositeness, right-handed W boson mass, test of special relativity and equivalence principle in the neutrino sector and others. One of the enriched $^{76}$Ge detectors also yields the most stringent limits for cold dark matter (WIMPs) to date by using raw data. A new Heidelberg experimental proposal (GENIUS) is described which would allow to increase the sensitivity for Majorana neutrino masses from the present level of at best 0.1 eV down to 0.01 or even 0.001 eV. It would further, already in a first step using only 100 kg of natural Ge detectors, cover almost the full MSSM parameter space for prediction of neutralinos as cold dark matter.']",['1999-01-15']
1540,['eng'],"['Achasov, M N', 'Baru, S E', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Pakhtusova, E V', 'Polunin, A A', 'Pyata, E E', 'Salnikov, A A', 'Shary, V V', 'Serednyakov, S I', 'Shatunov, Yu M', 'Sidorov, V A', 'Skrinsky, A N', 'Silagadze, Z K', 'Velikzhanin, Yu S']",['Observation of the decay $\\phi \\to \\omega \\pi^0$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'omega(783)', 'pi0', 'four-pi-detector, experimental results', 'Novosibirsk Stor2', 'Phi(1020) --> omega(783) pi0', '1.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901020'],['The reaction e^+e^- ---> OMEGA+PI0 ---> PI+PI- 2PI0 has been studied with SND detector at VEPP-2M e^+e^- collider in the vicinity of the PHI(1020) meson resonance. The observed interference pattern in the energy dependence of the cross section is consistent with existence of the decay PHI ---> OMEGA+PI0 with a branching ratio of B(PHI ---> OMEGA+PI0)=(4.8+1.9-1.7+-0.8)x10^{-5}. The real and imaginary parts of the decay amplitude were measured. The PHI ---> OMEGA+PI0 decay was observed for the first time.'],['1999-01-15']
1541,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Colour reconnection studies in $e^{+}e^{-} \\to W^{+}W^{-}$ at $\\sqrt{s}$=183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'final-state interaction, color', 'W, leptonic decay', 'momentum spectrum', 'charged particle, multiplicity', 'fragmentation function', 'rapidity spectrum', 'W, mass', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', '182.7 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901019'],"['The predicted effects of final state interactions such as colour reconnection are investigated by measuring properties of hadronic decays of W bosons, recorded at a centre-of-mass energy of sqrt(s)=182.7 GeV in the OPAL detector at LEP. Dependence on the modelling of hadronic W decays is avoided by comparing W+W- -> qqqq events with the non-leptonic component of W+W- -> qqlnu events. The scaled momentum distribution, its mean value, x_p, and that of the charged particle multiplicity, n_ch, are measured and found to be consistent in the two channels. The measured differences are: Diff(x_p) = +0.7 +- 0.8 +- 0.6 and Diff(n_ch) = (-0.09 +- 0.09 +-0.05)*10**-2. In addition, measurements of rapidity and thrust are performed for W+W- -> qqqq events. The data are described well by standard QCD models and disfavour one model of colour reconnection within the ARIADNE program. The current implementation of the ELLIS-GEIGER model of colour reconnection is excluded. At the current level of statistical precision no evidence for colour reconnection effects was found in the observables studied. The predicted effect of colour reconnection on OPAL measurements of M_W is also quantified in the context of models studied.']",['1999-01-15']
1542,['eng'],"['Pauss, Felicitas', 'Dittmar, Michael']",['Experimental Challenges at the LHC'],['Particle Physics - Experimental Results'],"['lectures, St. Croix 1998/06/18', 'p p, interaction', 'new particle, search for', 'new interaction, search for', 'Higgs particle, decay modes', 'supersymmetry', 'supergravity', 'cross section, energy dependence', 'luminosity', 'muon, counters and detectors', 'calorimeter, hadronic', 'calorimeter, electromagnetic', 'semiconductor detector, vertex', 'data acquisition', 'trigger', 'magnetic detector, ATLAS', 'magnetic detector, CMS', 'numerical calculations, CERN LHC Coll', 'bibliography', '14000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901018'],['The Large Hadron Collider (LHC) at CERN will provide proton-proton collisions at a centre-of-mass energy of 14 TeV with a design luminosity of 10**34/cm**2/s. The exploitation of the rich physics potential offered by the LHC will be illustrated using the expected performance of the two general--purpose detectors ATLAS and CMS. The detector design requirements necessary to extract the physics under the challenging experimental conditions at the LHC are discussed. This is followed by an analysis of search methods for the Higgs sector and the detection of supersymmetric particles.'],['1999-01-15']
1543,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the $B^{+}$ and $B^{0}$ lifetimes and search for CP(T) violation using reconstructed secondary vertices'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'beautiful particle, semileptonic decay', 'B+, lifetime', 'B0, lifetime', 'lifetime, ratio', 'track data analysis, vertex', 'final state, (lepton)', 'violation, CP', 'violation, CPT', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901017'],"['The lifetimes of the B+ and B0 mesons, and their ratio, have been measured in the OPAL experiment using 2.4 million hadronic Z0 decays recorded at LEP. Z0 -> b bbar decays were tagged using displaced secondary vertices and high momentum electrons and muons. The lifetimes were then measured using well-reconstructed charged and neutral secondary vertices selected in this tagged data sample. The results are tau(B+) = 1.643 +- 0.037 +- 0.025 ps tau(B0) = 1.523 +- 0.057 +- 0.053 ps ratio tau(B+)/tau(B0) = 1.079 +- 0.064 +- 0.041 where in each case the first error is statistical and the second systematic. A larger data sample of 3.1 million hadronic Z0 decays has been used to search for CP and CPT violating effects by comparison of inclusive b and bbar hadron decays. No evidence for such effects is seen. The CP violation parameter Re(epsilon_B) is measured to be Re(epsilon_B) = 0.001 +- 0.014 +- 0.003 and the fractional difference between b and bbar hadron lifetimes is measured to be -0.001 +- 0.012 +- 0.008']",['1999-01-14']
1544,['eng'],"['Giunti, C']",['Treatment of the background error in the statistical analysis of Poisson processes'],['Detectors and Experimental Techniques'],"['statistical analysis', 'background, error']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901015'],"['The formalism that allows to take into account the error sigma_b of the expected mean background b in the statistical analysis of a Poisson process with the frequentistic method is presented. It is shown that the error sigma_b cannot be neglected if it is not much smaller than sqrt(b). The resulting confidence belt is larger that the one for sigma_b=0, leading to larger confidence intervals for the mean mu of signal events.']",['1999-01-13']
1545,['eng'],"['Russ, J']",['Radiative Width of the $a_{2}$ Meson'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'pi- nucleus, coherent interaction', 'carbon', 'copper', 'lead', 'pi, multiple production', 'Primakoff effect', 'a2(1320), radiative decay', 'a2(1320), width', 'mass spectrum, (pi+ 2pi-)', 'transverse momentum, spectra', 'experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> nucleus pi+ 2pi-', '600 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901014'],"['We present data on coherent production of the pi-pi-pi+ system by 600 GeV pion beam for the C, Cu and Pb targets. The Primakoff formalism was used for extracting the radiatve width of the a2 meson. We obtain a preliminary value']",['1999-01-12']
1546,['eng'],"['Ocariz, J']",['The NA48 Liquid Krypton Calorimeter Description and Performances'],['Particle Physics - Experimental Results'],"['K0, decay modes', 'violation, CP', 'calorimeter, performance', 'krypton, liquid', 'electronics, readout', 'time resolution', 'spatial resolution', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901013'],"[""The NA48 experiment at CERN aims at making a precision study of direct CP violation in the neutral kaons, by measuring $Re(\\epsilon'/\\epsilon)$ with an accuracy better than 0.02%. To achieve this goal, the experiment requires a neutral detector with fast response, high efficiency in a high-rate environment space precision, and an excellent energy resolution (1%) in the $5 \\to 100$ GeV range. To achieve these performances, a quasi-homogeneous Liquid Krypton calorimeter has been chosen, designed with a projective tower geometry, high transversal segmentation, and fast digital readout. The calorimeter was operative during the '97 data taking period, its performances were thoroughly studied, and found to be in agreement with design requirements. A detector description and performances analysis are here presented.""]",['1999-01-12']
1547,['eng'],"['Ianni, A', 'Montanino, D', 'Scioscia, G']",['Test of non-standard neutrino properties with the BOREXINO source experiments'],['Particle Physics - Experimental Results'],"['neutrino/e, particle source', 'antineutrino/e, particle source', 'radioactivity', 'neutrino, oscillation', 'neutrino, form factor', 'coupling, vector', 'coupling, axial-vector', 'deep underground detector, Gran Sasso', 'calibration', 'efficiency', 'proposed experiment', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901012'],"['We calculate the event rates induced by high-intensity radioactive sources of nu_e (51Cr) and of anti-nu_e (90Sr), to be located near the BOREXINO detector. Calculations are performed both in the standard case and assuming non-standard properties of neutrinos, including flavor oscillations, neutrino electromagnetic interactions, and deviations from the standard vector and axial couplings in the nu_e-e interaction. It is shown that, in some cases, the current limits on non-standard neutrino properties can be significantly improved.']",['1999-01-12']
1548,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for Baryon and Lepton Number Violating $Z^0$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, decay', 'baryon number, violation', 'lepton number, violation', 'Z0, width', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'Z0 --> p electron', 'Z0 --> p muon-', 'approx. 91 Gev-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901011'],"['Using data collected with the OPAL detector at LEP, we have searched for the processes e+e- -> Z0 -> p e-, p mu- and the charge conjugate final-states. These would violate the conservation of the baryon-number B, lepton-number L and the fermion-number n = (B+L). No evidence for such decays has been found, and the 95% confidence level upper limits on the partial widths Z0 -> p e and Z0 -> p mu are found to be 4.6 and 4.4 keV respectively.']",['1999-01-12']
1549,['eng'],"['Adloff, C']",['Measurement of Internal Jet Structure in Dijet Production in Deep-Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, pair production', 'event shape analysis', 'multiplicity', 'transverse energy, dependence', 'rapidity dependence', 'quantum chromodynamics', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901010'],"['Internal jet structure in dijet production in deep-inelastic scattering is measured with the H1 detector at HERA. Jets with transverse energies ET,Breit > 5 GeV are selected in the Breit frame employing k_perp and cone jet algorithms. In the kinematic region of squared momentum transfers 10 < Q2 <~ 120 GeV2 and x-Bjorken values 2.10^-4 <~ xBj <~ 8.10^-3, jet shapes and subjet multiplicities are measured as a function of a resolution parameter. Distributions of both observables are corrected for detector effects and presented as functions of the transverse jet energy and jet pseudo-rapidity. Dependences of the jet shape and the average number of subjets on the transverse energy and the pseudo-rapidity of the jet are observed. With increasing transverse jet energies and decreasing pseudo-rapidities, i.e.towards the photon hemisphere, the jets are more collimated. QCD models give a fair description of the data.']",['1999-01-12']
1550,['eng'],"['Dittmar, Michael']",['Searching for the Higgs and other Exotic Objects'],['Particle Physics - Experimental Results'],"['lectures, Marseille 1998/09/07', 'electron positron, interaction', 'hadron hadron, interaction', 'new particle, search for', 'Higgs particle, mass', 'electroweak interaction', 'supersymmetry', 'Higgs particle, decay modes', 'channel cross section, branching ratio', 'transverse momentum, spectra', ""W', leptonic decay"", ""Z', leptonic decay"", 'mass spectrum, dilepton', 'sparticle, mass', 'sparticle, pair production', 'sparticle, decay modes', 'channel cross section, mass', 'numerical calculations', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901009'],['Methods and ideas to search for new phenomena at existing and future collider facilities like LEPII and the LHC are analysed. Emphasis is put on the experimental aspects of discovery strategies for the Higgs Boson of the Standard Model. This is followed by a critical analysis of search methods for the extended Higgs sector and the direct detection of Supersymmetric Particles within the Minimal Supersymmetric Standard Model. We also discuss methods and the potential mass reach of the LHC experiments to discover new Bosons and Fermions.'],['1999-01-12']
1551,['eng'],"['Rodríguez, J L']",['Hadronic Decays of Beauty and Charm from CLEO'],['Particle Physics - Experimental Results'],"['talk, Batavia 1998/10/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, branching ratio', 'charmed meson, excited state', 'D*(2010)', 'rho(770)', 'D0, branching ratio', 'charmed meson, hadronic decay', 'angular distribution', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> 2D*(2010)', 'B --> D*(2010) rho(770)', 'B- --> charmed meson pi-', 'D0 --> K+ pi-', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901008'],"[""A selection of recent results on hadronic charm and beauty decays from the CLEO experiment are presented. We report preliminary evidence for the existence of final state interactions in B decays and the first observation of the decay B0 -> D*+D*- with a branching fraction of (6.2^{+4.0}_{-2.9}+/- 1.0)x10^{-4}. We also present preliminary results on the first observation of the broad, J^P=1^+, charmed meson resonance with a mass of 2.461^{+0.41}_{-0.34}+/-0.010+/-0.032 GeV and a width of 290^{+101}_{-79}+/-26+/-36 MeV and branching fraction measurements of the B- -> D_J^0pi- decays. Finally, we report on search for the radial excitation of a spin 1 charmed meson, the D*'+, and on an improved measurement of the ratio of (D0 -> K+pi-)/(D0 -> K-pi^+) decay rates.""]",['1999-01-12']
1552,['eng'],"['Eigen, G']",['Review of b-flavored Hadron Spectroscopy'],['Particle Physics - Experimental Results'],"['talk, Santa Barbara 1997/07/07', 'beautiful particle, hadron spectroscopy', 'pseudoscalar meson, mass spectrum', 'vector meson, mass spectrum', 'hyperfine structure', 'mass difference', 'beautiful particle, hadroproduction', 'beautiful particle, electroproduction', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901007'],['The current status of b-flavored hadron spectroscopy is reviewed.'],['1999-01-11']
1553,['eng'],"['Eigen, G']",['Measurements of $B \\to X_{s} \\gamma$ and Study of $B \\to X_{s} l^{+} l^{-}$'],['Particle Physics - Experimental Results'],"['talk, Barcelona 1998/09/08', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'Z0, electroproduction', 'B, pair production', 'quark, beauty', 'quark, pair production', 'B, semileptonic decay', 'neutral current, flavor changing', 'B, branching ratio', 'upper limit', 'supersymmetry', 'supergravity', 'experimental results', 'magnetic detector, CLEO', 'magnetic detector, ALEPH', 'CERN LEP Stor', 'Cornell CESR Stor', 'beauty --> strangeness photon', 'beauty --> strangeness positron electron', 'approx. 10.6, 91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901005'],['The updated CLEO measurement of the electromagnetic penguin process $B \\to X_s \\gamma$ is presented and compared to the ALEPH result. Implications on new physics are discussed and the status of recent searches for $B \\to X_s l^+ l^-$ modes is given.'],['1999-01-08']
1554,['eng'],"['Dittmar, Michael']",['SUSY discovery strategies at the LHC'],['Particle Physics - Experimental Results'],"['lectures, Zuoz 1998/08/16', 'p p, inclusive reaction', 'supersymmetry, search for', 'electroweak interaction, validity test', 'supergravity', 'sparticle, hadroproduction', 'sparticle, pair production', 'sparticle, mass', 'sparticle, decay modes', 'background', 'channel cross section, mass', 'electron, pair production', 'Drell-Yan process', 'mass spectrum, dilepton', 'final state, (3lepton)', 'angular distribution', 'lepton, multiple production', 'chargino', 'neutralino', 'transverse energy, missing-energy', 'squark', 'gluino', 'transverse momentum, asymmetry', 'Higgs particle', 'numerical calculations, CERN LHC Coll', '14000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901004'],"[""Current ideas for SUPERSYMMETRY searches at the LHC are reviewed. We analyse the discovery prospects for various supersymmetric particles and describe recent ideas on the possibilities of detailed SUSY studies at the LHC. We also combine today's experimental knowledge with some speculations about what might be known by the year 2005 to provide a realistic picture for the LHC start.""]",['1999-01-08']
1555,['eng'],"['Blondel, Alain', 'Böge, M', 'Bravin, E', 'Bright-Thomas, P G', 'Camporesi, T', 'Dehning, B', 'Heemskerk, M', 'Hildreth, M D', 'Koratzinos, M', 'Lançon, E', 'Mugnai, G', 'Müller, A', 'Peschardt, E', 'Placidi, M', 'Qi, N', 'Quast, G', 'Renton, P B', 'Sonnemann, F', 'Torrence, E', 'Weber, A', 'Wells, P S', 'Wenninger, J', 'Wilkinson, G R']",['Evaluation of the LEP Centre-of-Mass Energy Above the W-Pair Production Threshold'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'threshold', 'beam, energy', 'CERN LEP Stor', '161, 172, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901002'],"['Knowledge of the centre-of-mass energy at LEP2 is of primary importance to set the absolute energy scale for the measurement of the W-boson mass. The beam energy above 80 GeV is derived from continuous measurements of the magnetic bending field by 16 NMR probes situated in a number of the LEP dipoles. The relationship between the fields measured by the probes and the beam energy is calibrated against precise measurements of the average beam energy between 41 and 55 GeV made using the resonant depolarisation technique. The linearity of the relationship is tested by comparing the fields measured by the probes with the total bending field measured by a flux loop. This test results in the largest contribution to the systematic uncertainty. Several further corrections are applied to derive the the centre-of-mass energies at each interaction point. In addition the centre-of-mass energy spread is evaluated. The beam energy has been determined with a precision of 25 MeV for the data taken in 1997, corresponding to a relative precision of 2.7x10^{-4}. This is small in comparison to the present uncertainty on the W mass measurement at LEP. However, the ultimate statistical precision on the W mass with the full LEP2 data sample should be around 25 MeV, and a smaller uncertainty on the beam energy is desirable. Prospects for improvements are outlined.']",['1999-01-08']
1556,['eng'],"['Stone, S']",['Physics Results from RICH Detectors'],['Particle Physics - Experimental Results'],"['review, Ein Gedi 1998/11/15', 'neutrino, solar', 'neutrino, oscillation', 'neutrino, cosmic radiation', 'cosmic radiation, particle source', 'ratio, (neutrino/mu neutrino/e)', 'gravitation', 'neutrino, mass difference', 'neutrino, mixing angle', 'quantum chromodynamics', 'charmed particle, hadroproduction', 'mass spectrum', 'Kobayashi-Maskawa angle', 'K0(L), decay', 'violation, CP', 'B, semileptonic decay', 'W, hadronic decay', 'W, branching ratio', 'Cherenkov counter, ring imaging', 'Cherenkov counter, water', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9901001'],"['RICH detectors have become extraordinarily useful. Results include measurement of solar neutrino rates, evidence for neutrino oscillations, measurement of TeV gamma-rays from gravitational sources, properties of QCD, charm production and decay, and measurement of the CKM matrix elements Vcs, Vcb and Vub. A new value |Vub/Vcb|=0.087+/-0.012 is determined.']",['1999-01-05']
1557,['eng'],"['Gagunashvili, N D']",['Stable Algorithm for Extraction of Asymmetries from the Data on Polarized Lepton-Nucleon Scattering'],['Particle Physics - Experimental Results'],"['lepton nucleon, deep inelastic scattering', 'lepton, polarized beam', 'nucleon, polarized target', 'polarization, asymmetry', 'data analysis method, proposed', 'statistical analysis']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812032'],['A new algorithm for extraction of asymmetries from polarized lepton-nucleon scattering data is proposed. The algorithm is stable to set-up acceptance and/or luminosity monitor acceptance variations. A statistical test for checking the data quality is proposed.'],['1998-12-28']
1558,['eng'],"['Russ, J']",['First Charm Hadroproduction Results from SELEX'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'hadron nucleus, inclusive reaction', 'pi', 'Sigma-', 'p', 'carbon', 'copper', 'D, hadroproduction', 'Lambda/c+, hadroproduction', 'particle identification, charm', 'track data analysis, vertex', 'resolution', 'mass spectrum', 'charmed particle, yield', 'yield, (particle antiparticle)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '600 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812031'],"['The SELEX experiment (E781) at Fermilab is a 3-stage magnetic spectrometer for the high statistics study of charm hadroproduction out to large x_F using 600 GeV Sigma^-, p and pi beams. The main features of the spectrometer are: high precision silicon vertex system, broad-coverage particle identification with TRD and RICH, 3-stage lead glass photon detector. Preliminary results on differences in hadroproduction characteristics of charm mesons and Lambda_c^+ for x_F>0.3 are reported. For baryon beams there is a striking asymmetry in the production of baryons compared to antibaryons. Leading particle effects for all incident hadrons are discussed.']",['1998-12-25']
1559,['eng'],"['Doyle, T', 'Erdmann, M']","['Structure Functions, Diffraction and Low-$Q^2$ Physics Including Two-Photon Physics']",['Particle Physics - Experimental Results'],"['review, Vancouver 1998/07/23', 'electron positron, colliding beams', 'positron p, colliding beams', 'anti-p p, colliding beams', 'photon photon, interaction', 'diffraction', 'momentum transfer, low', 'photon, structure function', 'p, structure function', 'quark, momentum spectrum', 'gluon, momentum spectrum', 'cross section, energy dependence', 'color, singlet', 'baryon, electroproduction', 'vector meson, electroproduction', 'jet, pair production', 'experimental results', 'CERN LEP Stor', 'DESY HERA Stor', 'Batavia TEVATRON Coll', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812030'],"['Recent measurements of the structure of the proton, photon and of diffractive exchange are reviewed (invited plenary talks at the XXIX International Conference on High Energy Physics, Vancouver, B.C. Canada (1998)).']",['1998-12-24']
1560,['eng'],"['Doyle, A T']",['Structure Functions'],['Particle Physics - Experimental Results'],"['review, Vancouver 1998/07/23', 'lepton nucleon, interaction', 'nucleon, structure function', 'deuteron, structure function', 'Altarelli-Parisi equation', 'Lipatov equation', 'momentum spectrum, parton', 'strong interaction, coupling constant', 'structure function, spin', 'structure function, charm', 'structure function, longitudinal', 'x-dependence', 'momentum transfer, dependence', 'sum rule', 'neutral current', 'charged current', 'cross section', 'scaling, violation', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812029'],"['The latest structure function results, as presented at the ICHEP98 conference, are reviewed. A brief introduction to the formalism and the status of global analyses of parton distributions is given. The review focuses on three experimental areas: fixed-target results and their constraints on the parton densities at high $x$; spin structure and spin parton densities as well as the status of the associated sum rules; HERA results on the dynamics of $F_2$ at low $(x,Q^2)$, charm and $F_L$ as well as the measurement and interpretation of the high-$Q^2$ neutral and charged current cross-sections.']",['1998-12-24']
1561,['eng'],"['Baier, V N', 'Katkov, V M']",['Transition radiation as a source of quasi-monochromatic X-rays'],['Detectors and Experimental Techniques'],"['charged particle, relativistic', 'radiation, transition', 'energy spectrum', 'lithium, sandwich', 'silicon, sandwich', 'organic compounds, sandwich', 'angular dependence', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812028'],['Transition radiation (TR) from ultrarelativistic particles is considered. It is shown that performing collimation of the TR from the periodic N-foil stack (parameters of which are selected in a appropriate manner) one obtains the spectrum of the TR which has a form of a peak position of which $\\omega_1$ depends on the plasma frequency and the thickness of the radiator foils. The height and width of the peak depend on the collimation angle $\\vartheta_c$. The height of the peak for given $\\vartheta_c$ is proportional to N. Selecting parameters one can have the source of X-rays of desired frequency with rather good monochromaticity.'],['1998-12-23']
1562,['eng'],"['Gu, Y F', 'Li, X H']",['On recent data of branching ratios for $\\psi(2S) \\to J/\\psi\\pi\\pi$ and $\\psi(2S) \\to J/\\psi\\eta$'],['Particle Physics - Experimental Results'],"['review, experimental results', 'psi(3685), hadronic decay', 'J/psi(3100)', 'psi(3685), radiative decay', 'chi/c1(3510)', 'chi/c2(3555)', 'psi(3685), branching ratio', 'chi mesons, charm', 'chi mesons, radiative decay', 'data analysis method, proposed', 'psi(3685) --> J/psi(3100) 2pi', 'psi(3685) --> J/psi(3100) eta']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812027'],"['Recent data on branching ratios for $\\psi(2S)$ decays to $J/\\psi\\pi^+\\pi^-$, $J/\\psi\\pi^0\\pi^0$ and $J/\\psi\\eta$ are reviewed. An alternative treatment of data is proposed to get rid of the logical inconsistency which occurs in original computational procedure.']",['1998-12-23']
1563,['eng'],"['Bethke, Siegfried']",['Jet Physics at LEP and World Summary of $\\alpha_{s}$'],['Particle Physics - Experimental Results'],"['review, Barcelona 1998/09/08', 'electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'hadron, multiple production', 'quantum chromodynamics, validity test', 'strong interaction, coupling constant', 'coupling constant, error', 'event shape analysis', 'energy dependence', 'charged particle, multiplicity', 'experimental results', 'CERN LEP Stor', 'DESY PETRA Stor', '((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812026'],"['Recent results on jet physics and tests of QCD from hadronic final states in $e^+e^-$ annihilation at PETRA and at LEP are reviewed, with special emphasis on hadronic event shapes, charged particle production rates, properties of quark and gluon jets and determinations of $\\alpha_s$. The data in the entire energy range from PETRA to LEP-2 are in broad agreement with the QCD predictions. The world summary of measurements of $\\alpha_s$ is updated and a detailed discussion of various methods to determine the overall error of uncertainties.']",['1998-12-22']
1564,['eng'],"['Sapozhnikov, M G']",['Experimental results on strangeness production'],['Particle Physics - Experimental Results'],"['talk, Villasimius 1998/09/08', 'anti-p p, annihilation', 'at rest', 'meson, hadroproduction', 'Phi(1020)', 'f2(1525)', 'omega(783)', 'production, strangeness', 'nucleon, strangeness', 'nucleon, wave function', 'polarization', 'Iizuka-Okubo-Zweig rule, violation', 'mass spectrum, (K+ K-)', 'mass spectrum, (K pi0)', 'channel cross section, branching ratio', 'experimental results', 'CERN LEAR', 'anti-p p --> K+ K- pi0', 'anti-p p --> K pi0', 'anti-p p --> Phi(1020) eta', '0 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812025'],"[""New experimental results on the production of $\\phi$ and $f_2'(1525)$ mesons in the annihilation of stopped antiprotons are discussed. The explanation of these facts in the framework of the polarized strangeness model is considered.""]",['1998-12-22']
1565,['eng'],"['Abramowicz, H', 'Caldwell, A']",['HERA Collider Physics'],['Particle Physics - Experimental Results'],"['review', 'electron p, colliding beams', 'positron p, colliding beams', 'electron p, interaction', 'exchange, one-photon', 'photon p, interaction', 'hadron, electroproduction', 'quark, heavy', 'vector meson, photoproduction', 'jet', 'cross section', 'p, structure function', 'small-x', 'gluon, momentum spectrum', 'diffraction', 'model, quark parton', 'Regge poles', 'pomeron', 'new particle, search for', 'new interaction, search for', 'leptoquark', 'leptogluon', 'sparticle', 'supersymmetry', 'fermion, excited state', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903037'],"['HERA, the first electron-proton collider, has been delivering luminosity since 1992. It is the natural extension of an impressive series of fixed-target lepton-nucleon scattering experiments. The increase of a factor ten in center-of-mass energy over that available for fixed-target experiments has allowed the discovery of several important results, such as the large number of slow partons in the proton, and the sizeable diffractive cross section at large $Q^2$. Recent data point to a possible deviation from Standard Model expectations at very high $Q^2$, highlighting the physics potential of HERA for new effects. The HERA program is currently in a transition period. The first six years of data taking have primarily elucidated the structure of the proton, allowed detailed QCD studies and had a strong impact on the understanding of QCD dynamics. The coming years will bring the era of electroweak studies and high $Q^2$ measurements. This is therefore an appropriate juncture at which to review HERA results.']",['1999-03-18']
1566,['eng'],"['Adloff, C']",['Measurement of Dijet Cross-Sections at Low $Q^{2}$ and the Extraction of an Effective Parton Density for the Virtual Photon'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'jet, pair production', 'jet, photoproduction', 'differential cross section, momentum transfer', 'transverse energy, dependence', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'photon, structure function', 'momentum spectrum, parton', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812024'],"[""The triple-differential dijet cross-section, d^3 sigma_{ep}/dQ2 dE_t2 dxgjets, is measured with the H1 detector at HERA as a function of the photon virtuality Q^2, the fraction of the photon's momentum carried by the parton entering the hard scattering, xgjets, and the square of the mean transverse energy, E_t2, of the two highest E_t jets. Jets are found using a longitudinal boost-invariant k_T clustering algorithm in the gamma* p center of mass frame. The measurements cover the ranges 1.6 < Q^2 < 80 GeV$^2 in virtuality and 0.1 < y < 0.7 in inelasticity y. The results are well described by leading order QCD models which include the effects of a resolved component to the virtual photon. Models which treat the photon as point-like fail to describe the data. An effective leading order parton density for the virtual photon is extracted as a function of the photon virtuality, the probing scale and the parton momentum fraction. The x_gamma and probing scale dependences of the parton density show characteristic features of photon structure, and a suppression of this structure with increasing Q^2 is seen.""]",['1998-12-21']
1567,['eng'],"['Adloff, C']",['Measurement of $D^{*}$ Meson Cross Sections at HERA and Determination of the Gluon Density in the Proton using NLO QCD'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'D*(2010), electroproduction', 'D*(2010), photoproduction', 'D*(2010), hadronic decay', 'quantum chromodynamics, perturbation theory', 'differential cross section, transverse momentum', 'rapidity dependence', 'momentum transfer, dependence', 'p, structure function', 'gluon, momentum spectrum', 'scaling, violation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> D*(2010) anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812023'],"['With the H1 detector at the ep collider HERA, D* meson production cross sections have been measured in deep inelastic scattering with four-momentum transfers Q^2>2 GeV2 and in photoproduction at energies around W(gamma p)~ 88 GeV and 194 GeV. Next-to-Leading Order QCD calculations are found to describe the differential cross sections within theoretical and experimental uncertainties. Using these calculations, the NLO gluon momentum distribution in the proton, x_g g(x_g), has been extracted in the momentum fraction range 7.5x10^{-4}< x_g <4x10^{-2} at average scales mu^2 =25 to 50 GeV2. The gluon momentum fraction x_g has been obtained from the measured kinematics of the scattered electron and the D* meson in the final state. The results compare well with the gluon distribution obtained from the analysis of scaling violations of the proton structure function F_2.']",['1998-12-21']
1568,['eng'],"['Barberis, D']",['A study of the centrally produced baryon-antibaryon systems in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, interaction', 'p, pair production', 'Lambda, pair production', 'pi, pair production', 'pi0, hadroproduction', 'pomeron, exchange', 'mass spectrum', 'f4(2220), search for', 'channel cross section, slope', 'transverse momentum, dependence', 'magnetic spectrometer, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 3p anti-p', 'p p --> 3p anti-p pi+ pi-', 'p p --> 3p anti-p pi0', 'p p --> Lambda Antilambda 2p', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812022'],"['A study of the centrally produced ppbar, ppbarpi, ppbarpipi and lambda lambda channels has been performed in pp collisions using an incident beam momentum of 450 GeV/c. No significant new structures are observed in the mass spectra, however, important new information on the production dynamics is obtained. A systematic study of the production properties of these systems has been performed and it is found that these systems are not produced dominantly by double Pomeron exchange.']",['1998-12-18']
1569,['eng'],"['Hahn, S']",['The Strong Coupling'],['Particle Physics - Experimental Results'],"['review, Stara Lesna 1998/09/07', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'event shape analysis', 'moment, higher-order', 'strong interaction, coupling constant', 'energy dependence', 'quantum chromodynamics, perturbation theory', 'Z0', 'electroweak interaction', 'tau, semileptonic decay', 'spectral representation', 'neutrino nucleon, deep inelastic scattering', 'sum rule, Gross-Llewellyn-Smith', 'scaling, violation', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=open-98-037', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812021']","['Measurements of \\alpha_s from event shapes in e^+ e^- annihilationare discussed including recent deteminations using experimentallyoptimized scales, studies of theoretically motivated scale settingprescriptions, and recently observed problems with predictions inNext to Leading Logarithmic Approximation. Other recent precisionmeasurements of \\alpha_s are briefly discussed. The relevance ofpower terms for the energy evolution of event shape means and distributions is demonstrated. Finally, a summary on the currentresults on \\alpha_s(M_Z) and its running is given.']",['1999-01-04']
1570,['eng'],"['Ambrosio, M']",['Limits on dark matter WIMPs using upward-going muons in the MACRO detector'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'WIMP, search for', 'WIMP, annihilation', 'neutrino nucleus, interaction', 'charged current', 'muon, flux', 'upper limit', 'angular distribution', 'supersymmetry', 'neutralino, annihilation', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812020'],"['We perform an indirect search for Weakly Interacting Massive Particles (WIMPs) using the MACRO detector to look for neutrino-induced upward-going muons resulting from the annihilation of WIMPs trapped in the Sun and Earth. The search is conducted in various angular cones centered on the Sun and Earth to accommodate a range of WIMP masses. No significant excess over the background from atmospheric neutrinos is seen and limits are placed on the upward-going muon fluxes from Sun and Earth. These limits are used to constrain neutralino particle parameters from supersymmetric theory, including those suggested by recent results from DAMA/NaI.']",['1998-12-17']
1571,['eng'],"['Eschrich, I']",['Hyperon Physics Results from SELEX'],['Particle Physics - Experimental Results'],"['talk, Batavia 1998/10/10', 'electron hadron, elastic scattering', 'hadron p, inclusive reaction', 'pi-', 'Sigma-, form factor', 'form factor, electric', 'hyperon, hadroproduction', 'total cross section', 'Sigma(1385), radiative decay', 'Sigma(1385), width', 'mass spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '600 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812019'],"['In parallel to charm hadroproduction the experiment SELEX (E781) at Fermilab is pursuing a rich hyperon physics program. SELEX employs a 600 GeV/c beam consisting of 50% \\Sigma^- and \\pi^- each. The three-stage magnetic spectrometer covering 0.1 <= x_F <= 1.0 features a high-precision silicon vertex system, broad-coverage particle identification using TRD and RICH, and a three-stage lead glass photon calorimeter. First results for the \\Sigma^- charge radius, total (\\Sigma^-)-nucleon cross sections, and a new upper limit for the radiative width of the \\Sigma^-*(1385) are presented.']",['1998-12-17']
1572,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Darling, C L', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['A Measurement of the Product Branching Ratio $f(b \\to \\Lambda_{b}).BR (\\Lambda_{b} \\to \\Lambda X)$ in $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, fragmentation', 'Lambda/b0, decay modes', 'Lambda, hadronic decay', 'Lambda, momentum spectrum', 'transverse momentum, spectra', 'branching ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'Lambda/b0 --> Lambda anything', 'Lambda --> p pi', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812018'],"['The product branching ratio, f(b->Lambda_b).BR(Lambda_b->Lambda X), where Lambda_b denotes any weakly-decaying b-baryon, has been measured using the OPAL detector at LEP. Lambda_b are selected by the presence of energetic Lambda particles in bottom events tagged by the presence of displaced secondary vertices. A fit to the momenta of the Lambda particles separates signal from B meson and fragmentation backgrounds. The measured product branching ratio is f(b->Lambda_b).BR(Lambda_b->Lambda X) = (2.67+-0.38(stat)+0.67-0.60(sy s))% Combined with a previous OPAL measurement, one obtains f(b->Lambda_b).BR(Lambda_b->Lambda X) = (3.50+-0.32(stat)+-0.35(sys ))%.']",['1998-12-16']
1573,['eng'],"['Biryukov, V M']",['Simulation of crystal extraction experiments'],['Particle Physics - Experimental Results'],"['talk, Batavia 1997/09/22']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0110074'],['We discuss the simulation methods and results for the crystal extraction experiments performed recently at the high energy accelerators. Possible future applications of the crystal channeling technique are considered.'],['2001-10-30']
1574,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['A measurement of the $\\tau^{-} \\to e^{-} \\overline{\\nu}_{e}\\nu_{\\tau}$ branching ratio'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, leptonic decay', 'tau, pair production', 'tau-, leptonic decay', 'tau-, branching ratio', 'tau, lifetime', 'lepton, universality', 'electron, energy spectrum', 'strong interaction, coupling constant', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau- --> electron neutrino/tau antineutrino/e']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812017'],"['The branching ratio for the decay tau->e nue nutau has been measured using Z0 decay data collected by the OPAL experiment at LEP. In total 33073 tau->e nue nutau candidates were identified from a sample of 186197 selected tau decays, giving a branching ratio of 17.81 +- 0.09(stat) +_ 0.06(sys)%. This result is combined with other measurements to test e-mu and mu-tau universality in charged-current weak interactions. Additionally, the strong coupling constant alpha_s has been extracted and evolved to the Z0 mass scale, giving alpha_s = 0.1204 +- 0.0011(exp) +- 0.0019(theory).']",['1998-12-15']
1575,['eng'],"['Bai, J Z']",['Study of the hadronic decays of $\\chi_{c}$ states'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'chi mesons, charm', 'psi(3685), electroproduction', 'psi(3685), radiative decay', 'chi mesons, hadronic decay', 'chi mesons, branching ratio', 'chi/c1(3510)', 'chi/c2(3555)', 'chi/c0(3415), mass', 'eta/c(2980), mass', 'magnetic detector, BES', 'experimental results', 'Beijing Stor', 'electron positron --> psi(3685)', 'psi(3685) --> chi mesons photon', 'chi/c1(3510) --> K0(S) K+ pi-', 'chi mesons --> 2K0(S)', 'chi mesons --> 2Phi(1020)', 'chi mesons --> 2pi+ 2pi-', 'chi mesons --> K+ K- pi+ pi-', 'chi mesons --> p anti-p pi+ pi-', 'chi mesons --> 3pi+ 3pi-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812016'],"['Hadronic decays of the P-wave spin-triplet charmonium states \\chi_cJ (J=0,1,2) are studied using a sample of \\psi(2S) decays collected by the BES detector operating at the BEPC storage ring. Branching fractions for the decays going to K_s^0 K_s^0, \\chi_c0 going to \\phi \\phi, \\chi_c2 going to \\phi \\phi and \\chi_cJ going to K^+ K^- K^+ K^- are measured for the first time, and those for \\chi_cJ going to \\pi^+ \\pi^- \\pi^+ \\pi^-, $ \\chi_cJ going to \\pi^+ \\pi^- K^+ K^-, \\chi_cJ going to \\pi^+ \\pi^- p \\bar{p} and \\chi_cJ going to 3(\\pi^+ masses of the \\chi_c0 and \\eta_c to be M_{\\chi_{c0}}=3414.1 \\pm 0.6(stat) \\pm 0.8 (sys) MeV and M_{\\eta_c}=2975.8 \\pm 3.9(stat) \\pm 1.2 (sys) MeV.']",['1998-12-15']
1576,['eng'],"['Schmitz, N']",['News on Neutrino Oscillations and Neutrino Masses'],['Particle Physics - Experimental Results'],"['review, Delphi 1998/09/06', 'neutrino, oscillation', 'neutrino, mass', 'neutrino, cosmic radiation', 'neutrino nucleon, interaction', 'charged current', 'neutrino electron, elastic scattering', 'neutrino, mass difference', 'neutrino, mixing angle', 'neutrino, solar', 'neutrino, beam', 'deep underground detector, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9902027'],"['Recent results on neutrino oscillations and neutrino masses are presented. The most exciting news are the Super-Kamiokande measurements of atmospheric neutrinos, which show evidence for the neutrinos being massive. Various possible schemes for the neutrino masses are discussed.']",['1999-02-23']
1577,['eng'],"['Iovane, G']",['The OPERA Experiment'],['Detectors and Experimental Techniques'],"['talk, Heidelberg 1998/07/20', 'neutrino, oscillation', 'neutrino, mass', 'neutrino/mu', 'neutrino/tau', 'neutrino, beam', 'neutrino nucleon, interaction', 'charged current', 'tau-, decay modes', 'iron', 'nuclear emulsion, sandwich', 'proposed experiment', 'deep underground detector, Gran Sasso', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812015'],"['OPERA(Oscillation Project with Emulsion-tRacking Apparatus) is a new detector concept, iron(lead)-emulsion for a long-baseline neutrino oscillation experiment. This experiment would perform an appearance search for nu_mu-nu_tau oscillation in the parameter region indicated by the atmospheric neutrino anomaly. OPERA can run at the Gran Sasso Laboratory in the proposed NGS (Neutrino to Gran Sasso) Beam from CERN.']",['1998-12-14']
1578,['eng'],[],['Measurement of the flux and zenith-angle distribution of upward through-going muons by Super-Kamiokande'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'muon, flux', 'muon, energy', 'angular distribution', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812014'],"['A total of 614 upward through-going muons of minimum energy 1.6 GeV are observed by Super-Kamiokande during 537 detector live days. The measured muon flux is 1.74+/-0.07(stat.)+/-0.02(sys.)x10^{-13}cm^{-2}s^{-1}sr^{-1} compared to an expected flux of 1.97+/-0.44(theo.)x10^{-13}cm^{-2}s^{-1}sr^{-1}. The absolute measured flux is in agreement with the prediction within the errors. However, the zenith angle dependence of the observed upward through-going muon flux does not agree with no-oscillation predictions. The observed distortion in shape is consistent with the \\nu_\\mu <-> \\nu_\\tau oscillation hypothesis with confidence level.']",['1998-12-14']
1579,['eng'],"['Aitala, E M', 'Amato, S']",['Measurement of the form-factor ratios for $D_{s}^{+} \\to \\phi l^{+} \\nu_{l}$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'platinum', 'carbon', 'D/s+, hadroproduction', 'D/s+, semileptonic decay', 'Phi(1020)', 'form factor, ratio', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D/s+ --> Phi(1020) positron neutrino/e', 'D/s+ --> Phi(1020) muon+ neutrino/mu', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812013'],"['We have measured the form factor ratios r_V = V(0)/A_1(0) and r_2 = A_2(0)/A_1(0) for the decay D_s^+ -> phi ell^+ nu_ell, phi -> K^+ K^-, using data from charm hadroproduction experiment E791 at Fermilab. Results are based on 144 signal and 22 background events in the electron channel and 127 signal and 34 background events in the muon channel. We combine the measurements from both lepton channels to obtain r_V = 2.27 +- 0.35 +- 0.22 and r_2 = 1.57 +- 0.25 +- 0.19.']",['1998-12-11']
1580,['eng'],"['Grindhammer, G']",['Photon Structure'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon p, interaction', 'photon gluon, fusion', 'photon, resolved', 'vector dominance', 'jet, pair production', 'quantum chromodynamics, perturbation theory', 'gluon, momentum spectrum', 'differential cross section, x-dependence', 'differential cross section, momentum transfer', 'transverse momentum, dependence', 'rapidity dependence', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'photon p --> 2jet anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812012'],"['Large pT processes at HERA, initiated by almost real and by virtual photons, provide information on the structure of the photon. We report on the latest measurements of dijets and large pT particle production with the H1 detector. This includes a leading order determination of an effective virtual photon parton density, of the gluon density of the photon, and comparisons with models.']",['1998-12-11']
1581,['eng'],"['Abbott, B']",['Measurement of the High-Mass Drell-Yan Cross Section and Limits on Quark-Electron Compositeness Scales'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electron, pair production', 'Drell-Yan process', 'electroweak interaction, validity test', 'quark, composite', 'electron, composite', 'lower limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> positron electron anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812010'],['We present a measurement of the Drell-Yan cross section at high dielectron invariant mass using 120/pb of data collected in pbar-p collisions at sqrt(s) = 1.8 TeV by the D0 collaboration during 1992-96. No deviation from standard model expectations is observed. We use the data to set limits on the energy scale of quark-electron compositeness with common constituents. The 95% confidence level lower limits on the compositeness scale vary between 3.3 TeV and 6.1 TeV depending on the assumed form of the effective contact interaction.'],['1998-12-08']
1582,['eng'],['Zou Bing Song'],['Search for glueballs from three-body annihilation of pp in flight'],['Particle Physics - Experimental Results'],"['talk, Villasimius 1998/09/08', 'anti-p p, annihilation', 'glueball, search for', 'glueball, scalar', 'glueball, tensor', 'meson, multiple production', 'final state, (3pseudoscalar meson)', 'pi0', 'eta', 'eta(958)', 'final state, (omega(783) 2pi0)', 'Dalitz plot', 'mass spectrum', 'partial wave', 'four-pi-detector, experimental results', 'CERN LEAR']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812007'],"['Lattice QCD and other theoretical models predict that the 0(-+), 2(++) and 2(-+) glueballs have masses in the range of 2.0 to 2.4 GeV. For resonances in such an energy range, three-body decay modes are expected to be large. The strategy for looking for these glueballs and the newest results from studying Crystal Barrel data on the three-body annihilation of proton-antiproton in flight are presented.']",['1998-12-07']
1583,['eng'],"['Abe, F', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amadon, A', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Aota, S', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bagdasarov, S L', 'Bailey, M W', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Baumann, T', 'Bedeschi, F', 'Behrends, S', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bettelli, S', 'Bevensee, B E', 'Bhatti, A A', 'Biery, K', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Bloom, K', 'Blusk, S R', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Breccia, L', 'Bromberg, C', 'Bruner, N L', 'Brunetti, R', 'Buckley-Geer, E', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chang, P S', 'Chang, P T', 'Chao, H Y', 'Chapman, J', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chiou, C N', 'Chlebana, F S', 'Christofek, L S', 'Cropp, R', 'Chu, M L', 'Cihangir, S', 'Clark, A G', 'Cobal, M', 'Cocca, E', 'Contreras, M', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Costanzo, D', 'Couyoumtzelis, C', 'Cronin-Hennessy, D', 'Culbertson, R J', 'Dagenhart, D', 'Daniels, T', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Ely, R P', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Feng, Z', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Frisch, H', 'Fukui, Y', 'Gadomski, S', 'Galeotti, S', 'Gallinaro, M', 'Ganel, O', 'García, M', 'Sciveres', 'Garfinkel, A F', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giokaris, N D', 'Giromini, P', 'Giusti, G', 'Gold, M', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Grassmann, H', 'Green, C', 'Groer, L S', 'Grosso-Pilcher, C', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hamilton, R', 'Handa, T', 'Handler, R', 'Hao, W', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hauser, J', 'Hayashi, E', 'Heinrich, J', 'Heiss, A', 'Hinrichsen, B', 'Hoffman, K D', 'Hohlmann, M', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Huang, Z', 'Huffman, B T', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incagli, M', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Joshi, U', 'Kajfasz, E', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kennedy, R D', 'Kephart, R D', 'Kestenbaum, D S', 'Khazins, D M', 'Kikuchi, T', 'Kim, B J', 'Kim, H S', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Knoblauch, D', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korytov, A V', 'Kovacs, E', 'Kowald, W', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kuns, E W', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Lanzoni, M', 'Latino, G', 'LeCompte, T J', 'Leone, S', 'Lewis, J D', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Long, O', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lys, J', 'Maeshima, K', 'Maksimovic, P', 'Mangano, Michelangelo L', 'Mariotti, M', 'Marriner, J P', 'Martignon, G', 'Martin, A', 'Matthews, J A J', 'Mazzanti, P', 'McFarland, K', 'McIntyre, P', 'Mélèse, P', 'Menguzzato, M', 'Menzione, A', 'Meschi, E', 'Metzler, S', 'Miao, C', 'Miao, T', 'Michail, G', 'Miller, R', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Miyashita, S', 'Moggi, N', 'Moore, E', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nakada, H', 'Nakaya, T', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okabe, M', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Parashar, N', 'Parri, A', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Perazzo, A', 'Pescara, L', 'Peters, M D', 'Phillips, T J', 'Piacentino, G', 'Pillai, M', 'Pitts, K T', 'Plunkett, R K', 'Pompos, A', 'Pondrom, L', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Reher, D', 'Reischl, M', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Robinson, A', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Saab, T', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shaw, N M', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Ströhmer, R', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, J', 'Suzuki, T', 'Takahashi, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tanaka, M', 'Tannenbaum, B', 'Tartarelli, F', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Teramoto, Y', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thomas, T L', 'Thurman-Keup, R M', 'Keup, R M', 'Timko, M', 'Tipton, P', 'Titov, A', 'Tkaczyk, S M', 'Toback, D', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Truitt, S', 'Tseng, J', 'Turini, N', 'Uchida, T', 'Ukegawa, F', 'Valls, J', 'van den Brink, S C', 'Vejcik, S', 'Velev, G V', 'Volobuev, I', 'Vidal, R', 'Vilar, R', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Warburton, A', 'Watanabe, T', 'Watts, T', 'Webb, R', 'Wei, C', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Wilkinson, R P', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolinski, D', 'Wolinski, J', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yasuoka, K', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Search for R-parity Violating Supersymmetry using Like-Sign Dielectrons in $p\\overline{p}$ Collisions at $\\sqrt{s} = 1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'supersymmetry, search for', 'sparticle, pair production', 'squark', 'gluino', 'final state, ((n)jet 2electron)', 'final state, ((n)jet 2positron)', 'sparticle, decay', 'R parity, violation', 'channel cross section, branching ratio', 'upper limit', 'sparticle, mass', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9908063'],"[""We present a search for like-sign dielectron plus multijet events using 107 pb-1 of data in \\ppbar collisions at $\\sqrt{s} = 1.8$ TeV collected in 1992-95 by the CDF experiment. Finding no events that pass our selection, we set experimental signature: gluino-gluino or squark-antisquark production with R-parity violating decays of the charm squark or lightest neutralino via a non-zero lambda'_121 coupling. We compare our results to NLO calculations for gluino and squark production cross sections and set lower limits on M(gluino), M(stop1), and M(squark).""]",['1999-08-30']
1584,['eng'],"['Baird, K G']",['Measurements of $A_{LR}$ and $A_{lepton}$ from SLD'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, leptonic decay', 'electron, pair production', 'muon, pair production', 'tau, pair production', 'angular distribution, asymmetry', 'polarization, asymmetry', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812008'],"['This paper presents measurements of the leptonic asymmetries in Z0 decays measured with the SLD detector. Using a data sample of approximately 500,000 Z0 bosons, we report preliminary values for A_e, A_mu and A_tau using both hadronic and leptonic decays.']",['1998-12-07']
1585,['eng'],"['Arneodo, F', 'Cavanna, F', 'De Mitri, I', 'Mazza, D', 'Parlati, S', 'Petrera, S', 'Piano Mortari, G', 'Verdecchia, M', 'Benetti, P', 'Borio di Tigliole, A', 'Calligarich, E', 'Cesana, E', 'Dolfini, R', 'Mauri, F', 'Montanari, C', 'Rappoldi, A', 'Raselli, G L', 'Terrani, M', 'Torre, P', 'Vignoli, C', 'Bettini, A', 'Carpanese, C', 'Centro, S', 'Pepato, A', 'Pietropaolo, Francesco', 'Ventura, S', 'Bonesini, M', 'Boschetti, B', 'Calvi, M', 'Curioni, A', 'Cavalli, D', 'Ferrari, A', 'Ferrari, P', 'Negri, P', 'Paganoni, M', 'Pullia, A', 'Sala, P R', 'Ragazzi, S', 'Redaelli, N G', 'Tabarelli de Fatis, T', 'Terranova, F', 'Tonazzo, A', 'Casagrande, Federico', 'Cennini, P', 'Puccini, A', 'Rubbia, André', 'Rubbia, Carlo', 'Revol, Jean-Pierre', 'Cline, D', 'Matthey, C', 'Otwinowski, Stanislas', 'Park, J', 'Wang, H', 'Woo, J', 'Givoletti, J', 'Lamarina, A', 'Periale, R', 'Picchi, P', 'Mannocchi, G', 'Periale, L', 'Suzuki, S', 'Sergiampietri, F']",['The ICARUS 50 1 LAr TPC in the CERN $\\nu$ beam'],['Detectors and Experimental Techniques'],"['talk, Erice 1997/11/01', 'drift chamber, time projection', 'liquid argon', 'neutrino, beam', 'neutrino nucleon, interaction', 'neutrino/mu', 'charged current', 'electronics, readout', 'data acquisition', 'performance', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812006'],"['The 50 litre liquid Argon TPC is a detector built and successfully operated at CERN for R&D purposes within the ICARUS programme. In the year 1997 it has been exposed at the CERN neutrino beam for the entire SPS neutrino run period as proposed and approved at the SPSLC of January 1997. The detector, complemented with scintillators acting as veto, trigger counters and pre-shower counters, was installed in front of the NOMAD detector. The year 1997 was scheduled to be the last for the operation of the West Area Neutrino Facility. It was important to take this last opportunity for a parasitic exposure, which did not interfere with running experiments, of an already existing and operating liquid Argon TPC. As we had expected, the collected data brought important information for a better understanding of the performance of liquid Argon TPCs which should be useful for the entire ICARUS program. (9 refs).']",['2000-04-25']
1586,['eng'],"['Bulekov, O V', 'Galanina, N D', 'Demidov, V S', 'Endalov, A L', 'Kiselevich, I E', 'Martemyanov, A N', 'Mikhailichenko, V I', 'Okorokov, V A', 'Ponosov, A K', 'Sergeev, F M', 'Khaldeeva, N A']",['The $\\Lambda K$ system production in the hadron interactions'],['Particle Physics - Experimental Results'],"['pi+ p, exclusive reaction', 'n nucleus, inclusive reaction', 'copper', 'carbon', 'Lambda, hadroproduction', 'K, associated production', 'transverse momentum, low', 'mass spectrum, (Lambda K)', 'differential cross section, x-dependence', 'dependence, mass number', 'baryon resonance, effect', 'magnetic spectrometer', 'bubble chamber(hydrogen)', 'experimental results', 'Moscow ITEF PS', 'n nucleus --> Lambda K0 anything0', 'pi+ p --> Lambda K+ pi+', 'pi+ p --> Lambda K+ pi+ pi0', 'pi+ p --> Lambda K 2pi+', '4-10 GeV (n), 4.23 GeV/c (pi+)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812005'],"[""The A-dependence is observed in $x_F$-distributions for the $\\Lambda K^0$ system produced with the small transverse momentum in the neutron-nucleus interactions. For the $\\Lambda$ hyperons similar dependence isn't seen. The result is interpreted as an effect from intermediate excitative nucleon state, which decays into strange particles. Such interpretation is confirmed experimental data on $\\Lambda K$ pair production in the pion-nucleon interactions.""]",['1998-12-04']
1587,['eng'],"['Thompson, J C']",['Measurements of $\\alpha_{s}$ from hadronic event shapes in $e^{+}e^{-}$ annihilation'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'event shape analysis', 'strong interaction, coupling constant', 'energy dependence', 'Z0', 'quantum chromodynamics, perturbation theory', 'correction, nonperturbative', 'data analysis method', 'experimental results', '((4)) ((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812004'],['New studies of hadronic event shape observables in e+ e- collisions between 13 and 183 GeV CM energy have enabled the running of alpha_s to be confirmed and the validity of non-perturbative power-law corrections to be investigated. A more precise value of alpha_s(M_Z) with reduced theoretical errors has been reported from fitting 18 oriented event shape distributions measured in one experiment at the Z.'],['1998-12-03']
1588,['eng'],"['Barate, R']",['$B/\\overline{B}$ flavour tagging and doubly charmed B decays in ALEPH'],['Particle Physics - Experimental Results'],"['review, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'particle identification, flavor', 'B, decay modes', 'B, excited state', 'mass spectrum, (B pi)', 'mass, B*2(5732)', 'charmed meson, pair production', 'D', 'D*(2010)', 'D/s', 'K, associated production', 'B, branching ratio', 'B/s, hadronic decay', 'B/s, width', 'anti-B/s, width', 'final state, (2Phi(1020))', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812003'],['This contribution concerns three contributed papers that share the common feature of analysing fully- (or almost fully-) reconstructed B decays coming from a sample of four million hadronic Z decays collected with the ALEPH detector at LEP...'],['1998-12-03']
1589,['eng'],"['Fanourakis, G K', 'Fassouliotis, D', 'Leisos, A', 'Mastroyiannopoulos, N', 'Tzamarias, S']",['Extended Modified Observable Technique for a Multi-Parametric Trilinear Gauge Coupling Estimation at LEP II'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'W, pair production', 'W, leptonic decay', 'W, hadronic decay', 'coupling, (3gauge boson)', 'cross section, parametrization', 'final state, (2jet lepton neutrino)', 'statistical analysis', 'counters and detectors, effect', 'numerical calculations, Monte Carlo', 'electron positron --> W+ W-', 'W --> lepton neutrino', 'W --> quark antiquark', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812002'],"['This paper describes the extension of the Modified Observables technique in estimating simultaneously more than one Trilinear Gauge Couplings. The optimal properties, unbiasedness and consistent error estimation of this method are demonstrated by Monte Carlo experimentation using $\\ell \\nu jj $ four-fermion final state topologies. Emphasis is given in the determination of the expected sensitivities in estimating the $\\lambda_{\\gamma} - \\Delta g_{1}^{z}$ and GeV LEPII run.']",['1998-12-02']
1590,['eng'],"['Fanourakis, G K', 'Fassouliotis, D', 'Leisos, A', 'Mastroyiannopoulos, N', 'Tzamarias, S']",['Multidimensional Binning Techniques for a Two Parameter Trilinear Gauge Coupling Estimation at LEP II'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'coupling, (3gauge boson)', 'statistical analysis', 'data analysis method, cluster', 'higher-dimensional', 'cross section, parametrization', 'numerical calculations, Monte Carlo', 'electron positron --> W+ W-', 'W --> lepton neutrino', 'W --> quark antiquark', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9812001'],"[""This paper describes two generalization schemes of the Optimal Variables technique in estimating simultaneously two Trilinear Gauge Couplings. The first is an iterative procedure to perform a 2-dimensional fit using the linear terms of the expansion of the probability density function with respect to the corresponding couplings, whilst the second is a clustering method of probability distribution representation in five dimensions. The pair production of W's at 183 GeV center of mass energy, where one W decays leptonically and the other hadronically, was used to demonstrate the optimal properties of the proposed estimation techniques.""]",['1998-12-02']
1591,['eng'],"['Stugu, B']",['Summary on tau Leptonic Branching Ratios and Universality'],['Particle Physics - Experimental Results'],"['talk, Santander 1998/09/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, leptonic decay', 'tau, branching ratio', 'charged current, coupling', 'lepton, universality', 'lepton, momentum spectrum', 'Michel parameter', 'magnetic detector, CLEO', 'Cornell CESR Stor', 'magnetic detector, DELPHI', 'CERN LEP Stor', 'tau- --> electron neutrino/tau antineutrino/e', 'tau- --> muon- neutrino/tau antineutrino/e', '((3)) ((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811048'],"['The large samples of tau decays available from CLEO and the four LEP experiment have resulted in new, precise measurements of the leptonic branching ratios of the $\\tau$. The experimental techniques to obtain these results are reviewed with special emphasis on the DELPHI measurement. World averages are found to be Be = (17.81 +/- 0.06) % and Bmu = (17.36 +/- 0.06) %. These results are consistent with universality in the charged current couplings to a precision of about 0.25 %. The branching ratio measurements can also be used to constrain the ""low energy parameter"" eta. It is shown that the sensitivity to eta depends on details of the momentum acceptance for muon identification in the different experiments. Assuming universality in the couplings, the estimate eta = 0.012 +/- 0.024 is obtained.']",['1998-12-01']
1592,['eng'],"['Perret, P']",['b Physics'],['Particle Physics - Experimental Results'],"['review, San Juan 1998/04/08', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Z0, branching ratio', 'quark, beauty', 'quark, pair production', 'quark, decay modes', 'yield, charm', 'B0 anti-B0, oscillation', 'B/s0 anti-B/s0, oscillation', 'B0, mass difference', 'Kobayashi-Maskawa angle', 'gluon, fragmentation', 'angular distribution, asymmetry', 'beautiful particle, lifetime', 'beautiful particle, branching ratio', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811047'],"['A summary of the most recent and important measurements in b physics is presented. The production of beauty particles in Z decays, b quark couplings, lifetimes, B0-B0bar oscillations, semileptonic b decays and studies of the number of charm quarks produced in b decays are reviewed. Extraction of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements |V_{td}|, |V_{cb}|, |V_{ub}| and implication for |V_{ts}| are discussed.']",['1998-12-01']
1593,['eng'],"['Ganis, G']",['Search for SUSY with R-parity violation at LEP'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'R parity, violation', 'supersymmetry, symmetry breaking', 'sparticle, pair production', 'sparticle, decay modes', 'gaugino', 'slepton', 'sneutrino', 'squark', 'neutralino, electroproduction', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '91-189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811046'],['Searches for supersymmetry at LEP allowing for R-parity violation are reviewed. The results are compared with the R-parity conserving scenarios.'],['1998-11-30']
1594,['eng'],"['Baudis, L', 'Hellmig, J', 'Heusser, G', 'Klapdor-Kleingrothaus, H V', 'Kolb, S', 'Majorovits, B', 'Päs, H', 'Ramachers, Y', 'Strecker, H', 'Alexeev, V I', 'Bakalyarov, A', 'Balysh, A Y', 'Belyaev, S T', 'Lebedev, V I', 'Zhukov, S V']",['New limits on dark-matter WIMPs from the Heidelberg-Moscow experiment'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'search for, WIMP', 'scattering, nucleon WIMP', 'cross section, upper limit', 'mass, dependence', 'semiconductor detector, germanium', 'deep underground detector, Gran Sasso', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811045'],['New results after 0.69 kg yr of measurement with an enriched 76Ge detector of the Heidelberg--Moscow experiment with an active mass of 2.758 kg are presented. An energy threshold of 9 keV and a background level of 0.042 counts/(kg d keV) in the energy region between 15 keV and 40 keV was reached.The derived limits on the WIMP--nucleon cross section are the most stringent limits on spin--independent interactions obtained to date by using essentially raw data without background subtraction.'],['1998-11-30']
1595,['eng'],"['Weinstein, A J']",['Tau 98 Conference Summary'],['Particle Physics - Experimental Results'],"['conference, review', 'Santander 1998/09/14', 'electron positron, annihilation', 'anti-p p, interaction', 'Z0, electroproduction', 'W, pair production', 'intermediate boson, leptonic decay', 'tau, pair production', 'tau, decay modes', 'angular distribution, asymmetry', 'lepton, universality', 'tau, lifetime', 'tau, branching ratio', 'Michel parameter', 'electroweak interaction, validity test', 'supersymmetry', 'violation, flavor', 'violation, CP', 'weak interaction, moment', 'spectral representation', 'perturbation theory, chiral', 'muon, magnetic moment', 'CVC model', 'neutrino/tau, mass', 'neutrino, oscillation', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811044'],"['I very briefly review the highlights of the fifth workshop on the physics of the tau lepton and its neutrino. There has been much progress in many sub-fields, which I touch upon in this review: the couplings of the tau to the $Z^0$ and $W^\\pm$; the leptonic branching fractions, lifetime, and tests of universality; the Lorentz structure of tau decays; searches for neutrinoless decays; limits on weak and electromagnetic dipole moments and CP violation; inclusive semi-hadronic decays, spectral functions, sum rules, QCD, and applications; substructure in tau decays to three pseudoscalars; tau decays to kaons; limits on the mass of the tau neutrino; tau neutrinos from solar, atmospheric, and AGN sources; accelerator searches for neutrino oscillations; and prospects for the future.']",['1998-11-26']
1596,['eng'],"['Weinstein, A J']",['CLEO Results on $\\tau$ Michel Parameters'],['Particle Physics - Experimental Results'],"['talk, Santander 1998/09/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, leptonic decay', 'tau, semileptonic decay', 'Michel parameter', 'lepton, momentum spectrum', 'spin, dependence', 'spin, correlation', 'four-fermion interaction, coupling', 'Higgs particle, mass', 'W, right-handed', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> lepton- neutrino/tau antineutrino', 'tau- --> pi- pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811043'],"['We present measurements of the tau Michel Parameters made by the CLEO experiment. Three different analyses are performed: a spin-independent lepton spectrum analysis and a second spin-dependent analysis using $\\ell^\\pm$ \\vs\\ four-fermion couplings, the mass of the charged Higgs in the MSSM, and a right-handed $W$ in left-right models. Many of these measurements are more precise than the PDG world averages.']",['1998-11-26']
1597,['eng'],"['Bartelt, J']",['Measurement of the $B\\to D\\ell\\nu$ Branching Fractions and Form Factor'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'correlation, (D lepton)', 'recoil, energy', 'B, width', 'B-, branching ratio', 'anti-B0, branching ratio', 'form factor, decay', 'Kobayashi-Maskawa angle', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B- --> D0 lepton- antineutrino', 'anti-B0 --> D+ lepton- antineutrino', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811042'],"['Using a sample of 3.3 million B-meson decays collected with the CLEO detector at the Cornell Electron Storage Ring, we have studied $B^- \\to D^0 \\ell\\nu$ and muon. We distinguish $B \\to D \\ell\\nu$ from other B semileptonic decays by examining the net momentum and energy of the particles recoiling against the D-lepton pairs. We find the decay rate $\\Gamma(B \\to D\\ell\\nu)$ = (14.1 +- 1.0 +- 1.2) ns-1 and derive branching fractions for $B^- \\to D^0 \\ell\\nu$ and 0.19)% respectively, where the uncertainties are statistical and systematic. We also investigate the $B \\to D \\ell\\nu$ form factor and the implication of the result for $|V_{cb}|$.']",['1998-11-26']
1598,['eng'],"['Pepé-Altarelli, M']",['W physics at LEP'],['Particle Physics - Experimental Results'],"['talk, Frascati 1998/06/17', 'electron positron, colliding beams', 'W, electroproduction', 'W, pair production', 'channel cross section, energy dependence', 'coupling, (3gauge boson)', 'W, mass', 'W, hadronic decay', 'W, leptonic decay', 'charged particle, multiplicity', 'Kobayashi-Maskawa angle', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161, 172, 183, 189 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811041'],['A summary of the W-boson properties measured by the four LEP collaborations is presented here. These properties are updated to take into account the most recent results presented at the ICHEP98 conference.'],['1998-11-26']
1599,['eng'],"['Baudis, L', 'Heusser, G', 'Majorovits, B', 'Ramachers, Y', 'Strecker, H', 'Klapdor-Kleingrothaus, H V']",['Background and Technical Studies for GENIUS as a Dark Matter Experiment'],['Detectors and Experimental Techniques'],"['astrophysics, missing-mass', 'WIMP', 'astrophysics, galaxy', 'semiconductor detector, germanium', 'nitrogen, liquid', 'background', 'radioactivity', 'sparticle', 'deep underground detector, Gran Sasso', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811040'],"['The GENIUS project is a proposal for a new dark matter detector, with an increased sensitivity of three orders of magnitude relative to existing direct dark matter detection experiments. We performed a technical study and calculated the main background sources for the relevant energy region in a detailed detector geometry. The achieved overall background level and detector performance confirm the outstanding potential of GENIUS as a powerful tool for the direct search of WIMPs in our Galaxy.']",['1998-11-25']
1600,['eng'],"['Tanaka, R']",['Single W Production at LEP2'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, electroproduction', 'W, magnetic moment', 'W, decay modes', 'W, width', 'neutrino, pair production', 'coupling, (2W photon)', 'channel cross section', 'supersymmetry', 'experimental results', 'CERN LEP Stor', 'electron positron --> W neutrino electron', 'W --> neutrino antineutrino photon', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811039'],"['Single W and single gamma productions which are sensitive to the trilinear gauge coupling WWgamma have been studied at LEP. It is shown that single W production has particular sensitivity to the ""anomalous"" magnetic moment Kgamma of the W boson, complementary to WW production at LEP and Wgamma production at hadron colliders. The invisible decay of W boson has been searched and the limit on the invisible decay width of 27 MeV at 95% C.L. has been obtained.']",['1998-11-25']
1601,['eng'],"['Ambrose, D A']",['New Limit on Muon and Electron Lepton Number Violation from $K^{0}_{L} \\to \\mu^{\\pm} e^{\\mp}$ Decay'],['Particle Physics - Experimental Results'],"['K0(L), leptonic decay', 'violation, flavor', 'K0(L), branching ratio', 'upper limit', 'experimental results', 'Brookhaven PS', 'K0(L) --> muon+ electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811038'],"['The most sensitive experiment to date to search for the muon and electron lepton number violating decay $K^0_L \\to \\mu^\\pm e^\\mp$ has detected no events consistent with this process. Based on this result, the 90% confidence level upper limit on the branching fraction is $B(K^0_L \\to \\mu^\\pm e^\\mp) < 4.7\\times10^{-12}$.']",['1998-11-24']
1602,['eng'],"['Wasserbaech, S R']",['Review of $\\tau$ lifetime measurements'],['Particle Physics - Experimental Results'],"['review, Santander 1998/09/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'decay, path length', 'track data analysis, impact parameter', 'track data analysis, vertex', 'tau, lifetime', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811037'],"['The measurements of the mean lifetime of the tau lepton are reviewed. The conditions for measuring the lifetime at various e+e- colliders are compared and the analysis methods are briefly described. The new developments since the previous Workshop on Tau Lepton Physics are listed. The world average is tau_tau = 290.5 +- 1.0 fs. The LEP experiments dominate this average and have analyzed nearly all of their data. In anticipation of the next era of precision measurements at CLEO and the b factories, the important sources of systematic errors and the treatment of systematic biases are discussed.']",['1998-11-24']
1603,['eng'],"['Drucker, R B']",['Search for Neutral Heavy Leptons in the NuTeV Experiment at Fermilab'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'p nucleus, inclusive reaction', 'beryllium, oxygen', 'heavy lepton, search for', 'heavy lepton, neutral particle', 'coupling, (heavy lepton neutrino)', 'mass, dependence', 'calorimeter, experimental results', 'Batavia TEVATRON PS', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811036'],"['Preliminary results from a search for neutral heavy leptons in the NuTeV experiment at Fermilab. The upgraded NuTeV neutrino detector for the 1996-1997 run included an instrumented decay region for the NHL search which, combined with the NuTeV calorimeter, allows detection in several decay modes (mu-mu-nu, mu-e-nu, mu-pi, e-pi, and e-e-nu). We see no evidence for neutral heavy leptons in our current search in the mass range from 0.3 GeV to 2.0 GeV decaying into final states containing a muon.']",['1998-11-24']
1604,['eng'],"['Partridge, R']",['Heavy Quark Production and Decay'],['Particle Physics - Experimental Results'],"['review, Vancouver 1998/07/23', 'anti-p p, colliding beams', 'electron positron, colliding beams', 'positron p, colliding beams', 'quark, truth', 'quark, pair production', 'quark, decay modes', 'W, polarization', 'quark, beauty', 'quark, radiative decay', 'quark, fragmentation', 'quarkonium, charm', 'quarkonium, hadroproduction', 'chi mesons, charm', 'chi mesons, radiative decay', 'electroweak interaction, validity test', 'transverse momentum, dependence', 'rapidity dependence', 'color, singlet', 'color, octet', 'J/psi(3100), leptonic decay', 'mass spectrum, dilepton', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811035'],"['This paper summarizes a variety of recent results on heavy quark production and decay. Considerable progress has been made by CDF and D0 in measuring top quark production and decay properties. The top quark mass been measured with an uncertainty that is less than 3%, a relative precision that is better than has been achieved for other quarks. Measurements of the top production and decay properties are consistent with the Standard Model predictions, but are generally limited in precision by the small number of top quark events in the present data samples. ALEPH and CLEO have measured the branching ratio for the flavor changing neutral current decay b->s gamma and find good agreement with the Standard Model. Measurements of b-quark production cross sections in ppbar collisions by CDF and D0 and in ep collisions by H1 continue to show discrepancies between theory and experiment. CDF and DELPHI have measured the b-quark fragmentation fractions with better accuracy than previous measurements. Finally, measurements of charmonium production by D0, E771, and L3 are consistent with predictions of the color octet model.']",['1998-11-24']
1605,['eng'],"['De Angelis, A']",['Two topics in multiparticle dyamics at LEP'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, colliding beams', 'electron positron, annihilation', 'quark, beauty', 'quark, pair production', 'quark, fragmentation', 'hadron, multiple production', 'charged particle, multiplicity', 'dependence, flavor', 'showers, parton', 'gluon, emission', 'quantum chromodynamics, perturbation theory', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811034'],"['This talk deals with two topics in multiparticle dynamics investigated by means of the DELPHI detector at LEP. Related to the first topic, we have used the data collected at 183 GeV to measure the average charged particle multiplicity in $e^+e^- \\to b\\bar{b}$ events. The result is remarkably in agreement with QCD predictions, while it is more than two standard deviations larger than calculations assuming that the multiplicity accompanying the decay of a heavy quark is independent of the mass of the quark itself. The second topic deals with a recent theoretical model by Andersson et al., in which soft gluons order themselves in the form of a helix at the end of the QCD cascades. In our data at the Z peak, we have found no evidence for such an effect.']",['1998-11-20']
1606,['eng'],"['Artuso, M']",['Progress towards CLEO III'],['Detectors and Experimental Techniques'],"['talk, Vancouver 1998/07/23', 'semiconductor detector, vertex', 'Cherenkov counter, ring imaging', 'lithium, fluorine', 'proportional chamber, wire', 'organic compounds, gas', 'Cherenkov counter, angular resolution', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811031'],"['We describe the two major components of CLEO III: the Silicon Vertex Detector and the Ring Imaging Cherenkov Detector (RICH). The Silicon Vertex Detector is a four layer barrel-style device which spans the radial distance from 2.5 cm to 10.1 cm and covers 93% of the solid angle. It is being constructed using double-sided silicon sensors read out by front end electronics devices especially designed for this application. The RICH system consists of LiF radiators and multiwire proportional chambers containing a mixture of CH4 and TEA gases. The radiators are both flat and ""sawtooth."" Results from a test beam run of final CLEO III RICH modules will be presented, as well as test beam data on sensors to be employed in the Silicon Vertex Tracker.']",['1998-11-19']
1607,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Bose-Einstein Correlations in $e^{+} e^{-} \\to W^{+}W^{-}$ at 172 and 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'hadron, multiple production', 'correlation, two-pion', 'boson, statistics', 'model, production', 'chaos, parametrization', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '172, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811030'],"['Bose-Einstein correlations between like-charge pions are studied in hadronic final states produced by e+e- annihilations at center-of-mass energies of 172 and 183 GeV. Three event samples are studied, each dominated by one of the processes W+W- to qqlnu, W+W- to qqqq, or (Z/g)* to qq. After demonstrating the existence of Bose-Einstein correlations in W decays, an attempt is made to determine Bose-Einstein correlations for pions originating from the same W boson and from different W bosons, as well as for pions from (Z/g)* to qq events. The following results are obtained for the individual chaoticity parameters lambda assuming a common source radius R: lambda_same = 0.63 +- 0.19 +- 0.14, lambda_diff = 0.22 +- 0.53 +- 0.14, lambda_Z = 0.47 +- 0.11 +- 0.08, R = 0.92 +- 0.09 +- 0.09. In each case, the first error is statistical and the second is systematic. At the current level of statistical precision it is not established whether Bose-Einstein correlations, between pions from different W bosons exist or not.']",['1998-11-19']
1608,['eng'],"['Artuso, M']",['First Observation of the Decay $B^{0}\\to D^{*+}D^{*-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B0, hadronic decay', 'D*(2010), pair production', 'D*(2010), hadronic decay', 'B0, branching ratio', 'violation, CP', 'time dependence', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> 2D*(2010)', 'D*(2010) --> D pi', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811027'],"['We have observed four fully reconstructed B0 -> D*+D*- candidates in 5.8 million Upsilon(4S) -> BBbar decays recorded with the CLEO detector. The background is estimated to be 0.31 +- 0.10 events. The probability that the background could produce four or more signal candidates with the observed distribution among D*+ and D*- decay modes is 1.1 X 10^{-4}. The measured decay rate, Br(B0 -> D*+D*-) = [6.2 +4.0-2.9 (stat) +- 1.0(syst)] X 10^{-4}, is large enough for this decay mode to be of interest for the measurement of a time-dependent CP asymmetry.']",['1998-11-19']
1609,['eng'],"['Heltsley, B K']",['Experimental Summary on Hadronic Decays'],['Particle Physics - Experimental Results'],"['conference, review', 'talk, Santander 1998/09/14', 'tau, semileptonic decay', 'tau, decay modes', 'tau, branching ratio', 'CVC model, validity test', 'final state, (0strangeness)', 'strange meson, production', 'spectral representation', 'experimental results', 'tau- --> (n)hadron neutrino/tau']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811026'],"['Selected results on hadronic decays of the tau lepton from the TAU98 Workshop are reviewed. A comprehensive picture emerges for strange particle branching fractions, and exploration of resonant substructure of both strange and non-strange decays is seen to have matured substantially.']",['1998-11-19']
1610,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for Higgs Bosons in $e^{+} e^{-}$ Collisions at 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, pair production', 'Higgs particle, decay modes', 'Higgs particle, multiplet', 'particle identification, beauty', 'doublet, 2', 'supersymmetry', 'Higgs particle, mass', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811025'],"['The data collected by the OPAL experiment at sqrts=183 GeV were used to search for Higgs bosons which are predicted by the Standard Model and various extensions, such as general models with two Higgs field doublets and the Minimal Supersymmetric Standard Model (MSSM). The data correspond to an integrated luminosity of approximately 54pb-1. None of the searches for neutral and charged Higgs bosons have revealed an excess of events beyond the expected background. This negative outcome, in combination with similar results from searches at lower energies, leads to new limits for the Higgs boson masses and other model parameters. In particular, the 95% confidence level lower limit for the mass of the Standard Model Higgs boson is 88.3 GeV. Charged Higgs bosons can be excluded for masses up to 59.5 GeV. In the MSSM, mh > 70.5 GeV and mA > 72.0 GeV are obtained for tan{beta}>1, no and maximal scalar top mixing and soft SUSY-breaking masses of 1 TeV. The range 0.8 < tanb < 1.9 is excluded for minimal scalar top mixing and m{top} < 175 GeV. More general scans of the MSSM parameter space are also considered.']",['1998-11-19']
1611,['eng'],"['Nisius, R']",['Two Photon Physics at a Future Linear Collider'],['Particle Physics - Experimental Results'],"['talk, Lund 1998/09/10', 'electron positron, linear collider', 'linear collider, proposed', 'photon electron, Compton scattering', 'laser, backscatter', 'photon photon, interaction', 'total cross section', 'jet, photoproduction', 'differential cross section', 'photon, structure function', 'quark, charm', 'quark, pair production', 'model, pomeron', 'Lipatov equation', 'W, pair production', 'Higgs particle, photoproduction', 'numerical calculations', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811024'],"['Some general considerations on a future linear collider and selected topics of two photon physics measurements which can be performed at such a collider are presented. This review discusses the total photon-photon cross section, jet cross sections, structure functions, charm production, the BFKL Pomeron, $W$ pair production, and Higgs production.']",['1998-11-13']
1612,['eng'],"['Surrow, B']",['The structure of the photon and its interactions'],['Particle Physics - Experimental Results'],"['talk, Lund 1998/09/10', 'electron positron, colliding beams', 'photon electron, interaction', 'photon photon, interaction', 'photon, resolved', 'photon, structure function', 'jet, pair production', 'hadron, multiple production', 'energy flow, hadronic', 'rapidity dependence', 'muon, pair production', 'angular correlation, dilepton', 'event shape analysis', 'angular distribution', 'channel cross section, energy dependence', 'chi/c2(3555)', 'quantum chromodynamics, perturbation theory', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811023'],['The OPAL experiment at LEP has performed a variety of measurements of photon-photon and electron-photon scattering at the electron-positron collider LEP to gain a deeper insight into the structure of the photon and its interactions. This review presents a summary of these results.'],['1998-11-12']
1613,['eng'],"['Baudis, L', 'Heusser, G', 'Majorovits, B', 'Ramachers, Y', 'Strecker, H', 'Klapdor-Kleingrothaus, H V']",['The GENIUS Project'],['Detectors and Experimental Techniques'],"['talk, Buxton 1998/09/07', 'astrophysics, missing-mass', 'sparticle, search for', 'WIMP', 'solid-state counter', 'germanium, crystal', 'deep underground detector, Gran Sasso']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811022'],['The potential of GENIUS as a dark matter detector is discussed. A study was performed to demonstrate the good behaviour of the proposed detector design of naked HPGe-crystals in liquid nitrogen. The expected background components were simulated and are discussed in some detail.With the obtained background GENIUS could cover a large part of the favoured MSSM parameter-space.'],['1998-11-12']
1614,['eng'],"['Kozlov, Yu Z', 'Khalturtsev, S V', 'Machulin, I N', 'Martemyanov, A N', 'Martemyanov, B V', 'Sabelnikov, A A', 'Sukhotin, S V', 'Tarasenkov, V G', 'Turbin, E V', 'Vyrodov, V N']",['Modern Status of Neutrino Experiments at the Underground Neutrino Laboratory of Kurchatov Institute Near Krasnoyarsk Nuclear Reactor'],['Particle Physics - Experimental Results'],"['antineutrino deuteron, interaction', 'charged current', 'neutral current', 'fission, particle source', 'channel cross section, ratio', 'neutrino, mass difference', 'neutrino, mixing angle', 'upper limit', 'deep underground detector, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811020'],"[""The investigation of antineutrino-deuteron interaction at Krasnoyarsk reactor are discussed. The characteristics of the installation ''Deuteron'', present results and perspectives of Krasnoyarsk neutrino laboratory are presented.""]",['1998-11-12']
1615,['eng'],"['Anikina, M K', 'Chkhaidze, L V', 'Djobava, T', 'Garsevanishvili, V R', 'Kharkhelauri, L L']",['The Light Front Analysis of $\\pi^{-}$ Mesons Produced in the Relativistic Nucleus-Nucleus Collisions'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'pi-, hadroproduction', 'nuclear reaction, temperature', 'dependence, mass number', 'kinematics, light front', 'phase space', 'spectra, x-dependence', 'transverse momentum, spectra', 'angular distribution', 'streamer chamber, experimental results', 'Dubna PS', 'nucleus nucleus --> pi- anything', '4.5 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811019'],"['The light front analysis of pi^{-} mesons in A_{P} (He, C, Mg, O) + A_{T} (Li,C, Ne, Mg,Cu,Pb) collisions is carried out. The phase space of secondary pions is naturally divided into two parts in one of which the thermal equilibration assumption seems to be in a good agreement with data. Corresponding temperatures are extracted and compared to the results of other experiments. The dependence of the average temperature T on (A_{P}*A_{T})^{1/2} is studied.']",['1998-11-12']
1616,['eng'],"['Braccini, S']",['The $K^{0}_{s}K^{0}_{s}$ Final State in Two-Photon Collisions and Some Implications for Glueball Searches'],['Particle Physics - Experimental Results'],"['talk, Villasimius 1998/09/08', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'K0(S), hadronic decay', 'glueball, search for', 'mass spectrum, (2K0(S))', 'angular distribution', 'f2(1525)', 'f0(1500)', 'f4(2220)', 'width, branching ratio', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2K0(S) positron electron', 'K0(S) --> pi+ pi-', '91-183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811017'],"[""The K0sK0s final state in two-photon collisions is studied with the L3 detector at LEP using data at centre of mass energies from 91 GeV to 183 GeV. The K0sK0s mass spectrum is dominated by the formation of the f_2'(1525) tensor meson whose two-photon partial width is measured. Clear evidence for destructive f_2-a_2 interference is observed. No signal is present in the region around 2.2 GeV. An upper limit for the two-photon partial width times the K0sK0s branching ratio of the \\xi(2230) glueball candidate is then derived. An enhancement is observed around 1750 MeV. It may be due to the formation of a radial recurrence of the f_2'(1525) or to the s\\bar{s} member of the 0++ meson nonet.""]",['1998-11-11']
1617,['eng'],"['Aitala, E M']",['Measurement of the $D_{s}$ Lifetime'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D/s, hadroproduction', 'D/s, hadronic decay', 'mass spectrum, (Phi(1020) pi)', 'D/s, lifetime', 'D0, lifetime', 'lifetime, ratio', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON Coll', 'pi nucleus --> D/s anything', 'D/s --> Phi(1020) pi', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811016'],"['We report the results of a precise measurement of the Ds meson lifetime based on 1662 +/- 56 fully reconstructed Ds -> phi pi decays, from the charm hadroproduction experiment E791 at Fermilab. Using an unbinned maximum likelihood fit, we measure the Ds lifetime to be 0.518 +/- 0.014 +/- 0.007 ps. The ratio of the measured Ds lifetime to the world average D0 lifetime is 1.25 +/- 0.04. This result differs from unity by six standard deviations, indicating significantly different lifetimes for the Ds and the D0.']",['1998-11-11']
1618,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'Dervan, P J', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Graham, K', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Harel, A', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hobson, P R', 'Hoch, M', 'Höcker, A', 'Hoffman, K', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kim, D H', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Landsman, H Yu', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Spagnolo, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomas, J', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Vachon, B', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['$W^{+}W^{-}$ production and triple gauge boson couplings at LEP energies up to 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'angular distribution', 'W, branching ratio', 'lepton, universality', 'coupling, (3gauge boson)', 'W, polarization', 'polarization, longitudinal', 'spin, density matrix', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W-', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811028'],"['A study of W-pair production in e+e- annihilations at Lep2 is presented, based on 877 W+W- candidates corresponding to an integrated luminosity of 57 pb-1 at sqrt(s) = 183 GeV. Assuming that the angular distributions of the W-pair production and decay, as well as their branching fractions, are described by the Standard Model, the W-pair production cross-section is measured to be 15.43 +- 0.61 (stat.) +- 0.26 (syst.) pb. Assuming lepton universality and combining with our results from lower centre-of-mass energies, the W branching fraction to hadrons is determined to be 67.9 +- 1.2 (stat.) +- 0.5 (syst.)%. The number of W-pair candidates and the angular distributions for each final state (qqlnu,qqqq,lnulnu) are used to determine the triple gauge boson couplings. After combining these values with our results from lower centre-of-mass energies we obtain D(kappa_g)=0.11+0.52-0.37, D(g^z_1)=0.01+0.13-0.12 and lambda=-0.10+0.13-0.12, where the errors include both statistical and systematic uncertainties and each coupling is determined setting the other two couplings to the Standard Model value. The fraction of W bosons produced with a longitudinal polarisation is measured to be 0.242+-0.091(stat.)+-0.023(syst.). All these measurements are consistent with the Standard Model expectations.']",['1998-11-19']
1619,['eng'],"['Bourdarios, C']","[""Study of $D^{**}$ and $D^{*'}$ Production in B and C Jets, with the DELPHI Detector""]",['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, charm', 'quark, beauty', 'quark, pair production', 'B, semileptonic decay', 'charmed meson, hadron spectroscopy', 'charmed meson, hadronic decay', 'D*2(2460), multiplicity', 'D1(2420), multiplicity', 'mass spectrum, (D*(2010) pi+ pi-)', 'mass enhancement, (2637)', 'angular distribution', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811014'],"[""Using D$^{*+}$ mesons exclusively reconstructed in the DELPHI detector at LEP, orbital and radial excitations of non strange charmed mesons are studied. The multiplicities of the two narrow $D^0_1$ and $D^{*0}_2$ orbital excitations are measured in $Z^0 \\to c \\bar c$ and $Z^0 \\to b \\bar b$ decays. Preliminary results are obtained on the production of broad D$^{**}$ states, using B meson semi-leptonic decays. A narrow signal of 66 $\\pm$ 14 events is observed in the $(D^{*+} \\pi^+ \\pi^-)$ final state, interpreted as the first evidence of the predicted $D^{*'}$ radial excitation.""]",['1998-11-10']
1620,['eng'],"['Adloff, C']",['Measurement of Leading Proton and Neutron Production in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'p, leading particle', 'n, leading particle', 'model, production', 'cross section, parametrization', 'factorization, validity test', 'Regge poles', 'pi, exchange', 'exchange, pomeron', 'exchange, Regge', 'pi, structure function', 'small-x', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811013'],"[""Deep--inelastic scattering events with a leading baryon have been detected by the H1 experiment at HERA using a forward proton spectrometer and a forward neutron calorimeter. Semi--inclusive cross sections have been measured in the kinematic region 2 <= Q^2 <= 50 GeV^2, 6.10^-5 <= x <= 6.10^-3 and baryon p_T <= MeV, for events with a final state proton with energy 580 <= E' <= 740 GeV, or a neutron with energy E' >= 160 GeV. The measurements are used to test production models and factorization hypotheses. A Regge model of leading baryon production which consists of pion, pomeron and secondary reggeon exchanges gives an acceptable description of both semi-inclusive cross sections in the region 0.7 <= E'/E_p <= 0.9, where E_p is the proton beam energy. The leading neutron data are used to estimate for the first time the structure function of the pion at small Bjorken--x.""]",['1998-11-10']
1621,['eng'],"['Adams, T']",['Neutrino Trident Production from NuTeV'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'neutrino nucleus, interaction', 'antineutrino nucleus, interaction', 'neutrino/mu', 'muon, pair production', 'electroweak interaction, interference', 'energy, hadronic', 'background', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'neutrino/mu nucleus --> nucleus muon+ muon- neutrino/mu']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811012'],['A preliminary analysis of zero hadronic energy dimuon production in the NuTeV experiment is presented (nu_mu (anti-nu_mu) + N -> nu_mu(anti-nu_mu) + mu^+ + mu^- + N). The data show a signal in excess of background which is attributed to neutrino trident production. This excess is consistent with the Standard Model prediction including electroweak interference. Other sources of low-hadronic energy dimuon events are also considered.'],['1998-11-10']
1622,['eng'],"['Ackerstaff, K']",['Observation of a Coherence Length Effect in Exclusive $\\rho^{0}$ Electroproduction'],['Particle Physics - Experimental Results'],"['positron p, exclusive reaction', 'positron nucleus, incoherent interaction', 'deuteron', 'helium, nuclide', 'nitrogen', 'photon, resolved', 'quark antiquark, initial-state interaction', 'rho(770)0, electroproduction', 'rho(770)0, hadronic decay', 'mass spectrum, two-pion', 'momentum transfer, spectra', 'channel cross section, ratio', 'dependence, mass number', 'transparency', 'coherence, length', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'positron nucleon --> nucleon rho(770)0 positron', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811011'],"['Exclusive incoherent electroproduction of the rho^0(770) meson from 1H, 2H, 3He, and 14N targets has been studied by the HERMES experiment at squared four-momentum transfer Q**2>0.4 GeV**2 and positron energy loss nu from 9 to 20 GeV. The ratio of the 14N to 1H cross sections per nucleon, known as the nuclear transparency, was found to decrease with increasing coherence length of quark-antiquark fluctuations of the virtual photon. The data provide clear evidence of the interaction of the quark- antiquark fluctuations with the nuclear medium.']",['1998-11-09']
1623,['eng'],"['Kobel, M']",['Single and Pair Production of Neutral Electroweak Gauge Bosons at LEP'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'photon, electroproduction', 'Z0, electroproduction', 'gauge boson, pair production', 'photon, off-shell', 'photon electron, Compton scattering', 'electron, excited state', 'coupling, (2Z0 photon)', 'coupling, (3Z0)', 'channel cross section, energy dependence', 'Z0, leptonic decay', 'Z0, hadronic decay', 'magnetic detector, DELPHI', 'magnetic detector, L3', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811010'],"[""Recent LEP results on single and pair production of neutral electroweak gauge bosons are reviewed. QED and Electroweak gamma-e Compton scattering at LEP covers gamma-e center-of-mass energies sqrt{shat} in the range from about 20 GeV to 170 GeV, and leads to single production of on-shell gamma, off-shell gamma*, and Z bosons, also known as ``Zee'' process. The latter two final states have been observed for the first time by the OPAL collaboration, while the measurement of the scattered on-shell gamma's by L3 represents the highest energies at which QED Compton scattering has been studied so far. These processes can be used to set limits on excited electrons. Pair production of gamma* and/or Z at the e+e- center-of-mass energy sqrt{s}=183 GeV has been studied by the DELPHI, L3, and OPAL collaborations. The combination of these experiments yields the first significant measurement of Z pair production. With more statistics at higher energies, interesting limits on anomalous gammaZZ and ZZZ couplings can be derived from this process.""]",['1998-11-06']
1624,['eng'],"['Conrad, J M']",['Recent Results on Neutrino Oscillations'],['Particle Physics - Experimental Results'],"['conference, review', 'talk, Vancouver 1998/07/23', 'neutrino, oscillation', 'neutrino, solar', 'neutrino, cosmic radiation', 'neutrino, beam', 'neutrino/e, flux', 'neutrino/mu, flux', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811009'],"[""This article reviews the many new results from neutrino oscillation searches which were presented at ICHEP '98. Exciting indications of neutrino oscillations have been seen in the solar neutrino deficit, atmospheric neutrino deficit and LSND excess. These indications and reported limits on oscillations are considered. Attempts to develop a theory which addresses all of the neutrino oscillation data are discussed. Some of the remaining questions and the future experiments which will help answer these questions are described.""]",['1998-11-06']
1625,['eng'],"['LoSecco, J M']",['Bounds on $\\nu_{\\mu}$ Oscillations from Atmospheric Neutrinos'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'neutrino, cosmic radiation', 'neutrino/mu, interaction', 'angular distribution', 'neutrino, mass difference', 'neutrino, mixing angle', 'upper limit', 'numerical calculations', 'interpretation of experiments, IMB']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811008'],['A reanalysis of identified muon neutrino interactions from IMB 3 yields bounds on $\\sin^{2}(2 \\theta)$ and $\\Delta m^{2}$. The limit $\\sin^{2}(2'],['1998-11-06']
1626,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amato, S', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Beillière, P', 'Belokopytov, Yu A', 'Belous, K S', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Bertini, D', 'Bertrand, D', 'Besançon, M', 'Bianchi, F', 'Bigi, M', 'Bilenky, S M', 'Bizouard, M A', 'Bloch, D', 'Blom, H M', 'Bonesini, M', 'Bonivento, W', 'Boonekamp, M', 'Booth, P S L', 'Borgland, A W', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bourdarios, C', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Branchini, P', 'Brenke, T', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buran, T', 'Burgsmüller, T', 'Buschmann, P', 'Cabrera, S', 'Caccia, M', 'Calvi, M', 'Camacho-Rozas, A J', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chabaud, V', 'Chapkin, M M', 'Charpentier, P', 'Chaussard, L', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Chliapnikov, P V', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Collins, P', 'Colomer, M', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Cowell, J H', 'Crawley, H B', 'Crennell, D J', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', 'Damgaard, G', 'Davenport, M', 'Da Silva, W', 'Deghorain, A', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Brabandere, S', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Dolbeau, J', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Duperrin, A', 'Durand, J D', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ekspong, Gösta', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Erzen, B', 'Espirito-Santo, M C', 'Falk, E', 'Fanourakis, G K', 'Fassouliotis, D', 'Fayot, J', 'Feindt, Michael', 'Fenyuk, A', 'Ferrari, P', 'Ferrer, A', 'Ferrer-Ribas, E', 'Fichet, S', 'Firestone, A', 'Fischer, P A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J A', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'García, J', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Górski, M', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Green, C', 'Grimm, H J', 'Gris, P', 'Grzelak, K', 'Günther, M', 'Guy, J', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Harris, F J', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hessing, T L', 'Heuser, J M', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Holthuizen, D', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Huet, K', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Janik, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kersevan, B P', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kjaer, N J', 'Klapp, O', 'Klein, H', 'Kluit, P M', 'Kokkinias, P', 'Koratzinos, M', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kreuter, C', 'Kriznic, E', 'Krstic, J', 'Krumshtein, Z', 'Kubinec, P', 'Kucewicz, W', 'Kurvinen, K L', 'Lamsa, J W', 'Lane, D W', 'Langefeld, P', 'Lapin, V', 'Laugier, J P', 'Lauhakangas, R', 'Leder, Gerhard', 'Ledroit, F', 'Lefébure, V', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lemonne, J', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Lörstad, B', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Malmgren, T G M', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Martínez-Vidal, F', 'Marti i Garcia, S', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Masik, J', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Meroni, C', 'Meyer, W T', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Møller, R', 'Mönig, K', 'Monge, M R', 'Moreau, X', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mulet-Marquis, C', 'Muresan, R', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Naraghi, F', 'Navarria, Francesco Luigi', 'Navas, S', 'Nawrocki, K', 'Negri, P', 'Neufeld, N', 'Neumeister, N', 'Nicolaidou, R', 'Nielsen, B S', 'Nikolenko, M', 'Nomokonov, V P', 'Normand, Ainsley', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Orazi, G', 'Österberg, K', 'Ouraou, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Papageorgiou, K', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passon, O', 'Pegoraro, M', 'Peralta, L', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Rakoczy, D', 'Rames, J', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Røhne, O M', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Schneider, H', 'Schwemling, P', 'Schwickerath, U', 'Schyns, M A E', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Sekulin, R L', 'Shellard, R C', 'Sheridan, A', 'Siebel, M', 'Silvestre, R', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Skaali, T B', 'Smadja, G', 'Smirnov, N', 'Smirnova, O G', 'Smith, G R', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Sponholz, P', 'Squarcia, S', 'Stampfer, D', 'Stanescu, C', 'Stanic, S', 'Stapnes, Steinar', 'Stevenson, K', 'Stocchi, A', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Tegenfeldt, F', 'Terranova, F', 'Thomas, J', 'Tilquin, A', 'Timmermans, J', 'Tkatchev, L G', 'Todorova, S', 'Toet, D Z', 'Tomaradze, A G', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tranströmer, G', 'Treille, D', 'Tristram, G', 'Troncon, C', 'Tsirou, A L', 'Turluer, M L', 'Tyapkin, I A', 'Tzamarias, S', 'Überschär, B', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'Van der Velde, C', 'van Apeldoorn, G W', 'van Dam, P', 'Van Doninck, W K', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Vulpen, I B', 'Vassilopoulos, N', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Vollmer, C F', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Walck, C', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zaitsev, A', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zucchelli, G C', 'Zumerle, G']",['A search for heavy stable and long-lived squarks and sleptons in $e^+ e^-$ collisions at energies from 130 to 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'squark, truth', 'squark, beauty', 'slepton', 'squark, hadronization', 'channel cross section, mass', 'ionization, energy loss', 'radiation, Cherenkov', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', '130-183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811007'],"['A search for stable and long-lived heavy charged particles used the data taken by the DELPHI experiment at energies from 130 to 183 GeV. The Cherenkov light detected in the Ring Imaging Cherenkov Detector and the ionization loss measured in the Time Projection Chamber identify heavy particles from masses of 2 to nearly 89 GeV/c$^2$. Upper limits are given on the production cross-section and masses of sleptons, free squarks with a charge of $q = \\pm 2/3e$ and hadronizing squarks.']",['1998-11-06']
1627,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amato, S', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Beillière, P', 'Belokopytov, Yu A', 'Belous, K S', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Bertini, D', 'Bertrand, D', 'Besançon, M', 'Bianchi, F', 'Bigi, M', 'Bilenky, S M', 'Bizouard, M A', 'Bloch, D', 'Blom, H M', 'Bonesini, M', 'Bonivento, W', 'Boonekamp, M', 'Booth, P S L', 'Borgland, A W', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bourdarios, C', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Branchini, P', 'Brenke, T', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buran, T', 'Burgsmüller, T', 'Buschmann, P', 'Cabrera, S', 'Caccia, M', 'Calvi, M', 'Camacho-Rozas, A J', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Chabaud, V', 'Chapkin, M M', 'Charpentier, P', 'Chaussard, L', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Chliapnikov, P V', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Collins, P', 'Colomer, M', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Cowell, J H', 'Crawley, H B', 'Crennell, D J', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', 'Damgaard, G', 'Davenport, M', 'Da Silva, W', 'Deghorain, A', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Brabandere, S', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Dolbeau, J', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Duperrin, A', 'Durand, J D', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ekspong, Gösta', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Erzen, B', 'Espirito-Santo, M C', 'Falk, E', 'Fanourakis, G K', 'Fassouliotis, D', 'Fayot, J', 'Feindt, Michael', 'Fenyuk, A', 'Ferrari, P', 'Ferrer, A', 'Ferrer-Ribas, E', 'Fichet, S', 'Firestone, A', 'Fischer, P A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J A', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'García, J', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Górski, M', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Green, C', 'Grimm, H J', 'Gris, P', 'Grzelak, K', 'Günther, M', 'Guy, J', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Harris, F J', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hessing, T L', 'Heuser, J M', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Holthuizen, D', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Huet, K', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Janik, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Kersevan, B P', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kjaer, N J', 'Klapp, O', 'Klein, H', 'Kluit, P M', 'Kokkinias, P', 'Koratzinos, M', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kreuter, C', 'Kriznic, E', 'Krstic, J', 'Krumshtein, Z', 'Kubinec, P', 'Kucewicz, W', 'Kurvinen, K L', 'Lamsa, J W', 'Lane, D W', 'Langefeld, P', 'Lapin, V', 'Laugier, J P', 'Lauhakangas, R', 'Ledroit, F', 'Lefébure, V', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Lörstad, B', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Malmgren, T G M', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Martínez-Vidal, F', 'Marti i Garcia, S', 'Masik, J', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Masik, J', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Meroni, C', 'Meyer, W T', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Møller, R', 'Mönig, K', 'Monge, M R', 'Moreau, X', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mulet-Marquis, C', 'Muresan, R', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Naraghi, F', 'Navarria, Francesco Luigi', 'Navas, S', 'Nawrocki, K', 'Negri, P', 'Neufeld, N', 'Neumeister, N', 'Nicolaidou, R', 'Nielsen, B S', 'Nikolenko, M', 'Nomokonov, V P', 'Normand, Ainsley', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Orazi, G', 'Österberg, K', 'Ouraou, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Papageorgiou, K', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Pegoraro, M', 'Peralta, L', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Piana, G', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Rakoczy, D', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Røhne, O M', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Schneider, H', 'Schwemling, P', 'Schwickerath, U', 'Schyns, M A E', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Sekulin, R L', 'Shellard, R C', 'Sheridan, A', 'Siebel, M', 'Silvestre, R', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Skaali, T B', 'Smadja, G', 'Smirnov, N', 'Smirnova, O G', 'Smith, G R', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Sponholz, P', 'Squarcia, S', 'Stampfer, D', 'Stanescu, C', 'Stanic, S', 'Stapnes, Steinar', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Tegenfeldt, F', 'Terranova, F', 'Thomas, J', 'Tilquin, A', 'Timmermans, J', 'Tkatchev, L G', 'Todorova, S', 'Toet, D Z', 'Tomaradze, A G', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tranströmer, G', 'Treille, D', 'Tristram, G', 'Troncon, C', 'Tsirou, A L', 'Turluer, M L', 'Tyapkin, I A', 'Tzamarias, S', 'Überschär, B', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'van Apeldoorn, G W', 'van Dam, P', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Vulpen, I B', 'Vassilopoulos, N', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Vollmer, C F', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Walck, C', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zaitsev, A', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zucchelli, G C', 'Zumerle, G']",['Search for lightest neutralino and stau pair production in light gravitino scenarios with stau NLSP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'gravitino, LSP', 'neutralino, pair production', 'slepton, tau', 'slepton, pair production', 'sparticle, decay', 'sparticle, mass', 'lower limit', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2neutralino', 'electron positron --> 2slepton', 'neutralino --> tau slepton', 'slepton --> tau gravitino', '161, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811006'],"['Promptly decaying lightest neutralinos and long-lived staus are searched for in the context of light gravitino scenarios. It is assumed that the stau is the next to lightest supersymmetric particle (NLSP) and that the lightest neutralino is the next to NLSP (NNLSP). Data collected with the Delphi detector at centre-of-mass energies from 161 to 183~\\GeV\\ are analysed. No evidence of the production of these particles is found. Hence, lower mass limits for both kinds of particles are set at 95\\% C.L.. The mass of gaugino-like neutralinos is found to be greater than 71.5 GeV/$c^2$. In the search for long-lived stau, masses less than 70.0 to 77.5~\\GeVcc\\ are excluded for gravitino masses from 10 to 150~\\eVcc . Combining this search with the searches for stable heavy leptons and Minimal Supersymmetric Standard Model staus a lower limit of 68.5~\\GeVcc\\ may be set for the stau mass']",['1998-11-06']
1628,['eng'],"['Abreu, P', 'Adam, W', 'Adye, T', 'Adzic, P', 'Alderweireld, T', 'Alekseev, G D', 'Alemany, R', 'Allmendinger, T', 'Allport, P P', 'Almehed, S', 'Amaldi, Ugo', 'Amato, S', 'Anassontzis, E G', 'Andersson, P', 'Andreazza, A', 'Andringa, S', 'Antilogus, P', 'Apel, W D', 'Arnoud, Y', 'Åsman, B', 'Augustin, J E', 'Augustinus, A', 'Baillon, Paul', 'Bambade, P', 'Barão, F', 'Barbiellini, Guido', 'Barbier, R', 'Bardin, Dmitri Yuri', 'Barker, G', 'Baroncelli, A', 'Battaglia, M', 'Baubillier, M', 'Becks, K H', 'Begalli, M', 'Beillière, P', 'Belokopytov, Yu A', 'Benvenuti, Alberto C', 'Bérat, C', 'Berggren, M', 'Bertini, D', 'Bertrand, D', 'Besançon, M', 'Bianchi, F', 'Bigi, M', 'Bilenky, S M', 'Bizouard, M A', 'Bloch, D', 'Blom, H M', 'Bonesini, M', 'Bonivento, W', 'Boonekamp, M', 'Booth, P S L', 'Borgland, A W', 'Borisov, G', 'Bosio, C', 'Botner, O', 'Boudinov, E', 'Bouquet, B', 'Bourdarios, C', 'Bowcock, T J V', 'Boyko, I', 'Bozovic, I', 'Bozzo, M', 'Branchini, P', 'Brenke, T', 'Brenner, R A', 'Brückman, P', 'Brunet, J M', 'Bugge, L', 'Buran, T', 'Burgsmüller, T', 'Buschmann, P', 'Cabrera, S', 'Caccia, M', 'Calvi, M', 'Camacho-Rozas, A J', 'Camporesi, T', 'Canale, V', 'Carena, F', 'Carroll, L', 'Caso, Carlo', 'Castillo-Gimenez, M V', 'Cattai, A', 'Cavallo, F R', 'Cerruti, C', 'Chabaud, V', 'Chapkin, M M', 'Charpentier, P', 'Chaussard, L', 'Checchia, P', 'Chelkov, G A', 'Chierici, R', 'Chliapnikov, P V', 'Chochula, P', 'Chorowicz, V', 'Chudoba, J', 'Collins, P', 'Colomer, M', 'Contri, R', 'Cortina, E', 'Cosme, G', 'Cossutti, F', 'Cowell, J H', 'Crawley, H B', 'Crennell, D J', 'Crosetti, G', 'Cuevas-Maestro, J', 'Czellar, S', 'Damgaard, G', 'Davenport, M', 'Da Silva, W', 'Deghorain, A', 'Della Ricca, G', 'Delpierre, P A', 'Demaria, N', 'De Angelis, A', 'de Boer, W', 'De Brabandere, S', 'De Clercq, C', 'De Lotto, B', 'De Min, A', 'De Paula, L S', 'Dijkstra, H', 'Di Ciaccio, Lucia', 'Di Diodato, A', 'Dolbeau, J', 'Doroba, K', 'Dracos, M', 'Drees, J', 'Dris, M', 'Duperrin, A', 'Durand, J D', 'Eigen, G', 'Ekelöf, Tord Johan Carl', 'Ekspong, Gösta', 'Ellert, M', 'Elsing, M', 'Engel, J P', 'Erzen, B', 'Espirito-Santo, M C', 'Falk, E', 'Fanourakis, G K', 'Fassouliotis, D', 'Fayot, J', 'Feindt, Michael', 'Fenyuk, A', 'Ferrari, P', 'Ferrer, A', 'Ferrer-Ribas, E', 'Fichet, S', 'Firestone, A', 'Fischer, P A', 'Flagmeyer, U', 'Föth, H', 'Fokitis, E', 'Fontanelli, F', 'Franek, B J', 'Frodesen, A G', 'Frühwirth, Rudolf', 'Fulda-Quenzer, F', 'Fuster, J A', 'Galloni, A', 'Gamba, D', 'Gamblin, S', 'Gandelman, M', 'García, C', 'García, J', 'Gaspar, Clara', 'Gaspar, M', 'Gasparini, U', 'Gavillet, P', 'Gazis, E N', 'Gelé, D', 'Gerber, J P', 'Gerdyukov, L N', 'Ghodbane, N', 'Gil, I', 'Glege, F', 'Gokieli, R', 'Golob, B', 'Gómez-Ceballos, G', 'Gonçalves, P', 'González-Caballero, I', 'Gopal, Gian P', 'Gorn, L', 'Górski, M', 'Guz, Yu', 'Gracco, Valerio', 'Grahl, J', 'Graziani, E', 'Green, C', 'Grimm, H J', 'Gris, P', 'Grzelak, K', 'Günther, M', 'Guy, J', 'Hahn, F', 'Hahn, S', 'Haider, S', 'Hallgren, A', 'Hamacher, K', 'Harris, F J', 'Hedberg, V', 'Heising, S', 'Hernández, J J', 'Herquet, P', 'Herr, H', 'Hessing, T L', 'Heuser, J M', 'Higón, E', 'Holmgren, S O', 'Holt, P J', 'Holthuizen, D', 'Hoorelbeke, S', 'Houlden, M', 'Hrubec, Josef', 'Huet, K', 'Hultqvist, K', 'Jackson, J N', 'Jacobsson, R', 'Jalocha, P', 'Janik, R', 'Jarlskog, C', 'Jarlskog, Göran', 'Jarry, P', 'Jean-Marie, B', 'Johansson, E K', 'Jönsson, P E', 'Joram, Christian.', 'Juillot, P', 'Kapusta, F', 'Karafasoulis, K', 'Katsanevas, S', 'Katsoufis, E C', 'Keränen, R', 'Khomenko, B A', 'Khovanskii, N N', 'Kiiskinen, A P', 'King, B J', 'Kjaer, N J', 'Klapp, O', 'Klein, H', 'Kluit, P M', 'Kokkinias, P', 'Koratzinos, M', 'Kostyukhin, V', 'Kourkoumelis, C', 'Kuznetsov, O', 'Krammer, Manfred', 'Kreuter, C', 'Kriznic, E', 'Krstic, J', 'Krumshtein, Z', 'Kubinec, P', 'Kucewicz, W', 'Kurvinen, K L', 'Lamsa, J W', 'Lane, D W', 'Langefeld, P', 'Lapin, V', 'Laugier, J P', 'Lauhakangas, R', 'Leder, Gerhard', 'Ledroit, F', 'Lefébure, V', 'Leinonen, L', 'Leisos, A', 'Leitner, R', 'Lenzen, Georg', 'Lepeltier, V', 'Lesiak, T', 'Lethuillier, M', 'Libby, J', 'Liko, D', 'Lipniacka, A', 'Lippi, I', 'Lörstad, B', 'Loken, J G', 'Lopes, J H', 'López, J M', 'López-Fernandez, R', 'Loukas, D', 'Lutz, P', 'Lyons, L', 'MacNaughton, J N', 'Mahon, J R', 'Maio, A', 'Malek, A', 'Malmgren, T G M', 'Malychev, V', 'Mandl, F', 'Marco, J', 'Marco, R P', 'Maréchal, B', 'Margoni, M', 'Marin, J C', 'Mariotti, C', 'Markou, A', 'Martínez-Rivero, C', 'Martínez-Vidal, F', 'Marti i Garcia, S', 'Mastroyiannopoulos, N', 'Matorras, F', 'Matteuzzi, C', 'Matthiae, G', 'Masik, J', 'Mazzucato, F', 'Mazzucato, M', 'McCubbin, M L', 'McKay, R', 'McNulty, R', 'McPherson, G', 'Meroni, C', 'Meyer, W T', 'Migliore, E', 'Mirabito, L', 'Mitaroff, Winfried A', 'Mjörnmark, U', 'Moa, T', 'Møller, R', 'Mönig, K', 'Monge, M R', 'Moreau, X', 'Morettini, P', 'Morton, G A', 'Müller, U', 'Münich, K', 'Mulders, M', 'Mulet-Marquis, C', 'Muresan, R', 'Murray, W J', 'Muryn, B', 'Myatt, Gerald', 'Myklebust, T', 'Naraghi, F', 'Navarria, Francesco Luigi', 'Navas, S', 'Nawrocki, K', 'Negri, P', 'Neufeld, N', 'Neumeister, N', 'Nicolaidou, R', 'Nielsen, B S', 'Nikolaenko, V', 'Nikolenko, M', 'Nomokonov, V P', 'Normand, Ainsley', 'Nygren, A', 'Obraztsov, V F', 'Olshevskii, A G', 'Onofre, A', 'Orava, Risto', 'Orazi, G', 'Österberg, K', 'Ouraou, A', 'Paganoni, M', 'Paiano, S', 'Pain, R', 'Paiva, R', 'Palacios, J', 'Palka, H', 'Papadopoulou, T D', 'Papageorgiou, K', 'Pape, L', 'Parkes, C', 'Parodi, F', 'Parzefall, U', 'Passeri, A', 'Passon, O', 'Pegoraro, M', 'Peralta, L', 'Pernicka, Manfred', 'Perrotta, A', 'Petridou, C', 'Petrolini, A', 'Phillips, H T', 'Piana, G', 'Pierre, F', 'Pimenta, M', 'Piotto, E', 'Podobnik, T', 'Pol, M E', 'Polok, G', 'Poropat, P', 'Pozdnyakov, V', 'Privitera, P', 'Pukhaeva, N', 'Pullia, A', 'Radojicic, D', 'Ragazzi, S', 'Rahmani, H', 'Rakoczy, D', 'Rames, J', 'Ratoff, P N', 'Read, A L', 'Rebecchi, P', 'Redaelli, N G', 'Regler, Meinhard', 'Reid, D', 'Reinhardt, R', 'Renton, P B', 'Resvanis, L K', 'Richard, F', 'Rídky, J', 'Rinaudo, G', 'Røhne, O M', 'Romero, A', 'Ronchese, P', 'Rosenberg, E I', 'Rosinsky, P', 'Roudeau, Patrick', 'Rovelli, T', 'Ruhlmann-Kleider, V', 'Ruiz, A', 'Saarikko, H', 'Sacquin, Yu', 'Sadovskii, A', 'Sajot, G', 'Salt, J', 'Sampsonidis, D', 'Sannino, M', 'Schneider, H', 'Schwemling, P', 'Schwickerath, U', 'Schyns, M A E', 'Scuri, F', 'Seager, P', 'Sedykh, Yu', 'Segar, A M', 'Sekulin, R L', 'Shellard, R C', 'Sheridan, A', 'Siebel, M', 'Silvestre, R', 'Simard, L C', 'Simonetto, F', 'Sissakian, A N', 'Skaali, T B', 'Smadja, G', 'Smirnov, N', 'Smirnova, O G', 'Smith, G R', 'Sopczak, André', 'Sosnowski, R', 'Spassoff, Tz', 'Spiriti, E', 'Sponholz, P', 'Squarcia, S', 'Stanescu, C', 'Stanic, S', 'Stapnes, Steinar', 'Stevenson, K', 'Stocchi, A', 'Strauss, J', 'Strub, R', 'Stugu, B', 'Szczekowski, M', 'Szeptycka, M', 'Tabarelli de Fatis, T', 'Tegenfeldt, F', 'Terranova, F', 'Thomas, J', 'Tilquin, A', 'Timmermans, J', 'Tkatchev, L G', 'Todorov, T', 'Todorova, S', 'Toet, D Z', 'Tomaradze, A G', 'Tomé, B', 'Tonazzo, A', 'Tortora, L', 'Tranströmer, G', 'Treille, D', 'Tristram, G', 'Troncon, C', 'Tsirou, A L', 'Turluer, M L', 'Tyapkin, I A', 'Tzamarias, S', 'Überschär, B', 'Ullaland, O', 'Uvarov, V', 'Valenti, G', 'Vallazza, E', 'van Apeldoorn, G W', 'van Dam, P', 'Van Eldik, J', 'Van Lysebetten, A', 'Van Vulpen, I B', 'Vassilopoulos, N', 'Vegni, G', 'Ventura, L', 'Venus, W A', 'Verbeure, F', 'Verlato, M', 'Vertogradov, L S', 'Verzi, V', 'Vilanova, D', 'Vitale, L', 'Vlasov, E', 'Vodopyanov, A S', 'Vollmer, C F', 'Voulgaris, G', 'Vrba, V', 'Wahlen, H', 'Walck, C', 'Weiser, C', 'Wicke, D', 'Wickens, J H', 'Wilkinson, G R', 'Winter, M', 'Witek, M', 'Wolf, G', 'Yi, J', 'Yushchenko, O P', 'Zaitsev, A', 'Zalewska, Agnieszka', 'Zalewski, Piotr', 'Zavrtanik, D', 'Zevgolatakos, E', 'Zimin, N I', 'Zucchelli, G C', 'Zumerle, G']",['Search for composite and exotic fermions at LEP 2'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'fermion, heavy', 'fermion, decay modes', 'heavy lepton, pair production', 'lepton, excited state', 'quark, excited state', 'fermion, composite', 'fermion, mass', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'bibliography', '161, 172, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811005'],"['A search for unstable heavy fermions with the DELPHI detector at LEP is reported. Sequential and non-canonical leptons, as well as excited leptons and quarks, are considered. The data analysed correspond to an integrated luminosity of about 48~pb$^{-1}$ at an $e^+e^-$ centre-of-mass energy of 183~GeV and about 20~pb$^{-1}$ equally shared between the centre-of-mass energies of 172~GeV and 161~GeV. The search for pair-produced new leptons establishes 95\\% confidence level mass limits in the region between 70~GeV/$c^2$ and 90~GeV/$c^2$, depending on the channel. The search for singly produced excited leptons and quarks establishes upper limits on the ratio of the coupling of the excited fermion']",['1998-11-06']
1629,['eng'],"['Butterworth, J M']","['Charm ""in"" the Photon']",['Particle Physics - Experimental Results'],"['talk, Lund 1998/09/10', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'quark, pair production', 'quark, charm', 'charmed particle, photoproduction', 'jet, photoproduction', 'fusion, photon gluon', 'photon, resolved', 'quark, massless', 'quark, massive', 'D*(2010), particle identification', 'rapidity spectrum', 'jet, energy flow', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811004'],['Some recent ZEUS results on the photoproduction of open charm and possible implications for photon structure are discussed.'],['1998-11-05']
1630,['eng'],"['Eschrich, I']",['Measurement of the $\\Sigma^{-}$ Charge Radius at SELEX'],['Particle Physics - Experimental Results'],"['talk, Bonn 1998/09/22', 'electron hadron, elastic scattering', 'electron, bound state', 'hadron, secondary beam', 'Sigma-, form factor', 'pi-, form factor', 'form factor, electric', 'momentum transfer, dependence', 'angular distribution', 'momentum spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '600 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811003'],"['The charge radii of Sigma^- and pi^- have been determined by direct elastic scttering on shell electrons. The measurement was performed in the framework of the SELEX (E781) charm hadroproduction experiment at Fermilab which employs a 600 GeV/c high-intensity Sigma^-/pi^- beam and a 3-stage magnetic spectrometer covering 0.1 <= x_F <= 1.0. Scattering angles and momenta of both hadron and electron were measured with high precision using silicon microstrip detectors, thus allowing for a segmented solid target. Two TRDs provided full particle identification. A preliminary result for the Sigma^- charge radius for a four-momentum transfer squared of 0.03 GeV^2/c^2 <= Q^2 <= 0.16 GeV^2/c^2 will be reported. In a parallel analysis the pi^- charge radius has been determined for 0.03 GeV^2/c^2 <= Q^2 <= 0.2 GeV^2/c^2, and is found to be consistent with previous experiments.']",['1998-11-03']
1631,['eng'],"['Duboscq, J E']",['Limits on the Mass of the $\\nu_\\tau$ Neutrino from CLEO'],['Particle Physics - Experimental Results'],"['talk, Santander 1998/09/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, semileptonic decay', 'neutrino/tau, mass', 'upper limit', 'mass spectrum, (5pi)', 'spectral representation', 'statistical analysis', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> tau+ tau-', 'tau --> 5pi neutrino/tau', 'tau --> 3pi pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811002'],"['A limit on the mass of the tau neutrino is derived from 4.5x10^6 tau pairs produced at a center of mass energy of 10.6 GeV. The measurement technique involves a two-dimensional extended likelihood analysis, including the dependence of the end-point population on the tau neutrino mass, and allows for the first time an explicit background contribution. We use the decays of the tau to five charged pions and a neutrino and to 3 charged pions, 2 neutral pions and a neutrino to obtain an upper limit of 30 MeV, as well as a preliminary limit of 31 MeV from the decay of a tau to 3 charged hadrons, a neutral pi and a neutrino.']",['1998-11-03']
1632,['eng'],"['Engelfried, J', 'Filimonov, I M', 'Kilmer, J', 'Kozhevnikov, A P', 'Kubarovskii, V P', 'Molchanov, V V', 'Nemitkin, A V', 'Ramberg, E', 'Rud, V I', 'Stutte, L']",['The SELEX Phototube RICH Detector'],['Particle Physics - Experimental Results'],"['charmed baryon, decay modes', 'particle identification, (p K pi)', 'Cherenkov counter, ring imaging', 'neon', 'optics, reflection', 'optics, dispersion', 'efficiency', 'spatial resolution', 'photoelectron, amplifier', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9811001'],"['In this article, construction, operation, and performance of the RICH detector of Fermilab experiment 781 (SELEX) are described. The detector utilizes a matrix of 2848 phototubes for the photocathode to detect Cherenkov photons generated in a 10m Neon radiator. For the central region an N0 of 104/cm, corresponding to 13.6 hits on a beta=1 ring, was obtained. The ring radius resolution measured is 1.6%.']",['1998-11-03']
1633,['eng'],"['Braun, G', 'Fischer, H', 'Franz, J', 'Grünemaier, A', 'Heinsius, F H', 'Königsmann, Kay C', 'Schierloh, M', 'Schmidt, T', 'Schmitt, H', 'Urban, H J']",['TDC Chip and Readout Driver Developments for COMPASS and LHC-Experiments'],['Particle Physics - Experimental Results'],"['talk, Rome 1998/09/21', 'integrated circuit', 'electronics, readout', 'signal processing', 'control system, time', 'trigger', 'CERN SPS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810048'],"['A new TDC-chip is under development for the COMPASS experiment at CERN. The ASIC, which exploits the 0.6 micrometer CMOS sea-of-gate technology, will allow high resolution time measurements with digitization of 75 ps, and an unprecedented degree of flexibility accompanied by high rate capability and low power consumption. Preliminary specifications of this new TDC chip are presented. Furthermore a FPGA based readout-driver and buffer-module as an interface between the front-end of the COMPASS detector systems and an optical S-LINK is in development. The same module serves also as remote fan-out for the COMPASS trigger distribution and time synchronization system. This readout-driver monitors the trigger and data flow to and from front-ends. In addition, a specific data buffer structure and sophisticated data flow control is used to pursue local pre-event building. At start-up the module controls all necessary front-end initializations.']",['1998-11-02']
1634,['eng'],"['Graugès, E']",['Determination of the LEP center-of-mass energy from $Z\\gamma$ events'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'photon, radiation', 'radiation, initial-state interaction', 'Z0, associated production', 'numerical calculations, Monte Carlo', 'energy, measurement', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'electron positron --> Z0 photon', '182.5 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810047', 'http://alephwww.cern.ch/ALPUB/oldconf/vancouver.html']","['Radiative returns to the Z resonance (Zgamma events) provide a method to determine the centre-of-mass energy of the high energy e+e- colliders and already at LEP2. The method is applied for the data collected with the ALEPH detector in 1997 at 181-184 GeV, using e+e- -> gammaZ -> hadrons events.']",['1998-11-02']
1635,['eng'],"['Richard, F']",['Search for Higgs Bosons in $e^{+}e^{-}$ Colliders'],['Particle Physics - Experimental Results'],"['talk, Zuoz 1998/08/16', 'electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, neutral particle', 'Higgs particle, mass', 'supersymmetry', 'Higgs particle, multiplet', 'astrophysics', 'Higgs particle, associated production', 'Z0, associated production', 'Higgs particle, decay modes', 'particle identification, beauty', 'p p, interaction', 'muon+ muon-, interaction', 'experimental results', 'CERN LEP Stor', 'proposed experiment', '((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810045'],['Table of contents 1. Introduction 2. Theory 3. Searches at LEP2 4. Results 5. Futur colliders 6. Final remarks'],['1998-10-29']
1636,['eng'],"['Sinclair, L E']",['Jets and Prompt Photons in Photoproduction at ZEUS'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'positron p, colliding beams', 'jet, photoproduction', 'photon, direct production', 'photon, resolved', 'momentum spectrum, parton', 'transverse energy, spectra', 'differential cross section, rapidity dependence', 'mass spectrum, (2jet)', 'mass spectrum, (3jet)', 'angular distribution', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810044'],"[""In the ZEUS experiment at HERA, photoproduction processes have been studied for photon-proton centre-of-mass energies in the range 100 < W_gamma p < 300 GeV and jet transverse energies extending to E_T^jet ~ 70 GeV. The data contribute to our understanding of QCD dynamics, and also provide new constraints on the photon's parton density.""]",['1998-10-28']
1637,['eng'],"['Coan, T E']",['Search for exclusive rare baryonic decays of $B$ mesons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, rare decay', 'B, hadronic decay', 'B0, branching ratio', 'B+, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> Lambda Antilambda', 'B+ --> Antilambda p', 'B0 --> p anti-p', 'B0 --> Antilambda p pi-', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810043'],"['We report the results of a search for the rare baryonic decay modes B -> Lambda Lambdabar, B -> Lambdabar p, B -> Lambdabar p pi, and B -> p pbar using 5.8M BBbar pairs collected with the CLEO detector. We see no statistically significant signals in any of these modes and set 90% confidence level upper limits on their branching fractions, B(B -> Lambda Lambdabar) < 3.9 \\times 10^{-6}, B(B -> Lambdabar p) < 2.6 \\times 10^{-6}, B(B -> Lambdabar p pi) < 1.3 \\times 10^{-5}, and B(B -> p pbar) < 7.0 \\times 10^{-6}.']",['1998-10-28']
1638,['eng'],"['Tournefier, E']",['Extraction of $\\alpha_s$ and constraint on the Higgs mass from Electroweak fits at the Z resonance'],['Particle Physics - Experimental Results'],"['talk, Suzdal 1998/05/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Z0, leptonic decay', 'Z0, width', 'strong interaction, coupling constant', 'radiative correction', 'cross section, hadronic', 'Z0, branching ratio', 'Higgs particle, mass', 'Weinberg angle', 'electron, polarized beam', 'polarization, asymmetry', 'experimental results', 'CERN LEP Stor', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810042'],['The determination of the Z lineshape parameters at LEP1 is presented and the value of $\\alsmz$ is derived from these measurements. The constraint on the Higgs mass obtained from a global fit to LEP1 and SLC data is also given.'],['1998-10-28']
1639,['eng'],"['Wing, M']",['Photon Structure and the Hadronic Final State in Photoproduction Processes at ZEUS'],['Particle Physics - Experimental Results'],"['talk, Stara Lesna 1998/09/07', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'jet, multiple production', 'hadron, multiple production', 'transverse energy, high', 'mass spectrum, (2jet)', 'angular distribution', 'rapidity spectrum', 'differential cross section', 'photon, resolved', 'production, charm', 'D*(2010)', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810041'],"['Advances in knowledge of the structure of the photon and tests of perturbative QCD have been made using the increased luminosity with the ZEUS detector at HERA. Events with a low photon virtuality and two high transverse energy jets have been studied. Measurements of inclusive dijet and multijet production are herein compared to Next-to-Leading-Order calculations. In order to analyse the structure of the photon, dijet production of quasi-real and virtual photons and dijet production containing $D^{*\\pm}$ mesons were measured.']",['1998-10-28']
1640,['eng'],"['Anderson, B', 'Anjomshoaa, A', 'Dervan, P J', 'Lauber, J A', 'Thomas, J']",['Ultra Bright LED Light Injection Calibration System for MINOS'],['Detectors and Experimental Techniques'],"['neutrino, oscillation', 'calorimeter', 'iron', 'scintillation counter, plastics', 'calibration', 'photoproduction, amplifier', 'deep underground detector, Soudan']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810040'],"['We describe here a proposal for a light injection calibration system for the MINOS detectors based on ultra bright blue LEDs as the light source. We have shown that these LEDs are bright enough to span over two orders of magnitude in light intensity, commensurate with that expected in a single scintillator strip in the MINOS neutrino detectors.']",['1998-10-27']
1641,['eng'],"['Taylor, L', 'Williams, D O']",['On the use of Satellite Television in High Energy Physics'],['Detectors and Experimental Techniques'],"['talk, Chicago 1998/08/31', 'communications, satellite', 'experimental results, proposed', 'costs']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810039'],['This paper assesses the feasibility of exploiting commercial satellite television technologies to broadcast video signals and data from major High Energy Physics facilities to collaborating institutes throughout the world.'],['1998-10-27']
1642,['eng'],"['Bussey, Peter J']",['Physics with two photons at HERA'],['Particle Physics - Experimental Results'],"['talk, Lund 1998/09/10', 'positron p, interaction', 'positron p, deep inelastic scattering', 'photon, direct production', 'photon, radiation', 'approximation, Bethe-Heitler', 'bremsstrahlung', 'Compton scattering', 'channel cross section, rapidity dependence', 'photon, resolved', 'numerical calculations, Monte Carlo', 'interpretation of experiments, DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810038'],['A survey is presented of the various processes measurable at HERA in which two photons are involved. Their current experimental status and future prospects are discussed.'],['1998-10-26']
1643,['eng'],"['Markou, A']",['On the observability of free quarks near their production thresholds'],['Detectors and Experimental Techniques'],"['electron positron, annihilation', 'quark, pair production', 'threshold, hadronization', 'quark, search for', 'charge, fractional', 'channel cross section, energy dependence', 'angular distribution', 'photon nucleus, interaction', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810037'],"['It is proposed to search for free quarks near their production thresholds. If the current-quark masses for u, d quarks are smaller than the pion mass, $u\\bar{u}$ and $d\\bar{d}$ pairs produced below the pion pair threshold, would not have sufficient energy to hadronize and could be observable. In the case of large u,d quark masses and also for the heavy quarks, production near threshold may show hadronization probability $<1$, and lead to free quarks. Searches for fractional charges in stable matter could be more promising, through irradiation of samples at energies near the quark pair production thresholds.']",['1998-10-26']
1644,['eng'],"['Jessop, C P']",['Observation of Two Narrow States Decaying into $\\Xi_{c}^{+}\\gamma$ and $\\Xi_{c}^{0}\\gamma$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'charmed baryon, electroproduction', 'charmed baryon, radiative decay', 'Xi/c+, excited state', 'Xi/c0, excited state', 'Xi/c+, hadronic decay', 'Xi/c0, hadronic decay', 'charmed baryon, mass difference', 'fragmentation function', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> charmed baryon anything', 'charmed baryon --> Xi/c+ photon', 'charmed baryon --> Xi/c0 photon', 'Xi/c+ --> Xi 2pi', 'Xi/c0 --> Xi 2pi', 'Xi/c0 --> Xi- pi+', 'Xi/c0 --> Omega- K+', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810036'],"['We report the first observation of two narrow charmed strange baryons decaying to $\\Xi_c^+\\gamma$ and $\\Xi_c^0\\gamma$, respectively, using data from the CLEO II detector at CESR. We interpret the observed signals as the of the well-established antisymmetric $\\Xi_c^+(c[su])$ and $\\Xi_c^0(c[sd])$. The mass differences $M(\\Xi_c^{+\\prime})-M(\\Xi_c^+)$ and $M(\\Xi_c^{0\\prime})-M(\\Xi_c^0)$ are measured to be $107.8\\pm 1.7\\pm 2.5$ and $107.0\\pm 1.4\\pm 2.5 MeV/c^2$, respectively.']",['1998-10-22']
1645,['eng'],[],['Measurement of Three-jet Distributions in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'mass spectrum, (3jet)', 'angular distribution, (3jet)', 'showers, parton', 'quantum chromodynamics, perturbation theory', 'radiation, initial-state interaction', 'color, coherence', 'channel cross section', 'transverse energy, energy flow', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> 3jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810046'],['The cross section for the photoproduction of events containing three jets with a three-jet invariant mass of M_3J > 50 GeV has been measured with the ZEUS detector at HERA. The three-jet angular distributions are inconsistent with a uniform population of the available phase space but are well described by parton shower models and O(alpha alpha_s^2) pQCD calculations. Comparisons with the parton shower model indicate a strong contribution from initial state radiation as well as a sensitivity to the effects of colour coherence.'],['1998-10-29']
1646,['eng'],"['Nodulman, L']",['Experimental Tests of the Standard Model'],['Particle Physics - Experimental Results'],"['review, St. Croix 1998/06/18', 'electroweak interaction, validity test', 'muon, magnetic moment', 'muon, leptonic decay', 'neutrino nucleon, interaction', 'neutral current', 'charged current', 'Weinberg angle', 'electron positron, annihilation', 'hadron hadron, interaction', 'intermediate boson, electroproduction', 'Z0, mass', 'Z0, width', 'polarization, asymmetry', 'intermediate boson, hadroproduction', 'W, mass', 'quark, truth', 'quark, pair production', 'mass, truth', 'Higgs particle, search for', 'experimental methods', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810035'],['Four lectures on experimental test of the standard model presented at the Advanced Summer Institute on Techniques and Concepts of High Energy Physics.'],['1998-10-20']
1647,['eng'],"['Kalelkar, M S']",['Identified Hadron Production and Light Quark Fragmentation in $Z_0$ Decays'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1998/07/02', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'hadron, pair production', 'pi', 'K', 'K*(892)', 'Phi(1020)', 'p', 'Lambda', 'differential cross section, momentum dependence', 'dependence, flavor', 'model, fragmentation', 'asymmetry, strangeness', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810034'],"['We have measured the differential cross sections for the production of corresponding antiparticles in separate samples of flavor-tagged $Z^{0}\\to$ light-flavor ($u\\bar{u}$, $d\\bar{d}$, or $s\\bar{s}$), $Z^{0}\\to c\\bar{c}$ and $Z^{0}\\to b\\bar{b}$ events. Clear flavor dependences are observed, and the results are compared with the predictions of three fragmentation models. We have also performed a direct measurement of $A_{s}$, the parity-violating coupling of the $Z^{0}$ to strange quarks, by measuring the left-right-forward-backward production asymmetry in polar angle of the tagged $s$ quark. Our preliminary result is $A_{s}$ = $0.82\\pm 0.10(stat.)\\pm 0.07(syst.)$.']",['1998-10-20']
1648,['eng'],"['Bodek, Arie']",['Performance of a Prototype CMS Hadron Barrel Calorimeter in a Test Beam'],['Detectors and Experimental Techniques'],"['talk, Toronto 1998/11/08', 'calorimeter, hadronic', 'copper', 'scintillation counter, fibre', 'optics, transformation', 'calorimeter, electromagnetic', 'lead, tungsten', 'scintillation counter, crystal', 'energy resolution', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810033'],"['We report on the performance of a prototype CMS Hadron Barrel Calorimeter (HCAL) module in a test beam. The prototype sampling calorimeter used copper absorber plates and scintillator tiles with wavelength shifting fibers for readout. Placing a lead tungstate crystal electromagnetic calorimeter in front of HCAL affects the linearity and energy resolution of the combined system to hadrons. The data are used to optimize the choice of total absorber depth, sampling frequency, and longitudinal readout segmentation.']",['1998-10-19']
1649,['eng'],"['Amelin, D V', 'Berdnikov, E B', 'Bityukov, S I', 'Borisov, G', 'Dzhelyadin, R I', 'Dorofeev, V A', 'Ekimov, A V', 'Guz, Yu', 'Konoplyannikov, A K', 'Karyukhin, A N', 'Kachaev, I A', 'Khokhlov, Yu A', 'Likhoded, S A', 'Matveev, V D', 'Ostankov, A P', 'Ryabchikov, D I', 'Solovyanov, O', 'Solodkov, A A', 'Starchenko, E A', 'Vishnevski, N K', 'Vlasov, E V', 'Zaitsev, A M', 'Sekhniaidze, G G', 'Tskhadadze, E G']",['Study of $\\eta \\pi^{-}$ production by pions in the Coulomb field'],['Particle Physics - Experimental Results'],"['pi- nucleus, inelastic scattering', 'beryllium', 'potential, Coulomb', 'eta, production', 'mass spectrum, (eta pi-)', 'eta, radiative decay', 'channel cross section', 'magnetic spectrometer, experimental results', 'Serpukhov PS', 'pi- beryllium --> beryllium eta pi-', 'eta --> pi+ pi- photon', '37 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810032'],['The production of eta pi - system at low mass by the pi- beam in the Coulomb field of Be nuclei was studied. The cross section of the reaction pi- Be --> eta pi- Be was compared to the experimental data on the decay eta --> pi+ pi- gamma and to the theoretical predictions.'],['1998-10-15']
1650,['eng'],"['Abe, F']",['Search for a Technicolor $\\omega_{T}$ Particle in Events with a Photon and a $b$-quark Jet at CDF'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'quark, beauty', 'quark, pair production', 'photon, direct production', 'new particle, search for', 'omega(783), technicolor', 'postulated particle, radiative decay', 'technipion, hadronic decay', 'mass, technicolor', 'production, upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'omega(783) --> technipion photon', 'technipion --> 2beauty', 'anti-p p --> 2beauty photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810031'],"['If the Technicolor omega_T particle exists, a likely decay mode is omega_T -> gamma pi_T, followed by pi_T -> bb-bar, yielding the signature gamma bb-bar. We have searched 85 pb^-1 of data collected by the CDF experiment at the Fermilab Tevatron for events with a photon and two jets, where one of the jets must contain a secondary vertex implying the presence of a b quark. We find no excess of events above standard model expectations. We express the result of an exclusion region in the M_omega_T - M_pi_T mass plane.']",['1998-10-15']
1651,['eng'],"['Abe, F']",['Measurement of the Top Quark Mass with the Collider Detector at Fermilab'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'mass, truth', 'quark, decay', 'final state, dilepton', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810029'],"['We present a new measurement of the top quark mass in $t\\bar t$ events in which both $W$ bosons from top quarks decay into lepton ($e \\nu,\\mu \\nu$). We use events collected by the CDF experiment from $p\\bar p$ collisions at this result with previous CDF measurements in other decay channels to obtain a mass value of 176.0 \\pm 6.5 GeV/c^2.']",['1998-10-13']
1652,['eng'],"['Daoudi, M']",['Charmless and Double-Charm B Decays at SLD'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'B+, hadronic decay', 'final state, (0charm)', 'final state, (2charm)', 'B+, branching ratio', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'B+ --> rho(770)0 pi+', 'B+ --> rho(770)0 K+', 'B+ --> K*(892) meson', 'B+ --> D anti-D anything', '91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810027'],"['We present new results from the study of B decays at SLD: a measurement of the inclusive double-charm branching fraction in B-hadron decays and a search for the rare exclusive charmless decays B+ --> Rho0 Pi+(K+) and B+ --> K*0 Pi+(K+). Using a novel technique which consists of counting charged kaons produced at the secondary (B) vertex and the tertiary (D) vertex, we measure BR(B-->DDbarX) = 0.188 +- 0.025(stat) +- 0.059(syst). Another technique, based on the comparison of the charge of the D vertex to the flavor of the B hadron at production, yields a consistent result. In the search for rare exclusive B+ decays, no candidates were found and competitive branching ratio upper limits are derived.']",['1998-10-13']
1653,['eng'],"['Richichi, S']",['Study of 3-prong Hadronic $\\tau$ Decays with Charged Kaons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, semileptonic decay', 'tau, branching ratio', 'final state, (3charged particle)', 'final state, (3charged particle pi0)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810026'],"['Using a sample of 4.7/fb integrated luminosity accumulated with the CLEO-II detector at the Cornell Electron Storage Ring (CESR), we have measured the branching fractions of the tau lepton into $K^- h^+ \\pi^- \\nu_\\tau$ and $K^- K^+ \\pi^- \\nu_\\tau$ relative to $h^- h^+ h^- \\nu_\\tau; K^- h^+ \\pi^- (1.52+-0.14+-0.29)*$10^{-2}$, (2.54+-0.44+-0.39)*$10^{-2}$ and $<0.0154$ at 95% C.L., respectively. Coupled with additional experimental information, we use our results to extract information on the structure of three-prong tau decays to charged kaons.']",['1998-10-13']
1654,['eng'],"['Scherberger, G', 'Paschhoff, V', 'Waldmann, V', 'Landgraf, U', 'Herten, G', 'Mohr, W']",['High Rate Performance of Drift Tubes'],['Detectors and Experimental Techniques'],"['drift chamber, gas', 'drift chamber, drift tube', 'argon, organic compounds', 'gas, admixture', 'effect, space charge', 'charge, yield', 'spatial resolution', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810025'],"['This article describes calculations and measurements of space charge effects due to high rate irradiation in high resolution drift tubes. Two main items are studied: the reduction of the gas gain and changes of the drift time. Whereas the gain reduction is similar for all gases and unavoidable, the drift time changes depend on the kind of gas that is used. The loss in resolution due to high particle rate can be minimized with a suitable gas. This behaviour is calculable, allowing predictions for new gas mixtures.']",['1998-10-13']
1655,['eng'],"['Lang, K', 'Ting, J', 'Vassilakopoulos, V I']",['A Technique of Direct Tension Measurement of a Strung Fine Wire'],['Detectors and Experimental Techniques'],"['drift chamber, wire', 'forces, wire', 'measurement, wire', 'oscillation, wire', 'electronics']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810023'],['We present a new technique of direct measurement of wire tensions in wire chambers. A specially designed circuit plucks the wire using the Lorentz force and measures the frequency of damped transverse oscillations of the wire. The technique avoids the usual time-consuming necessity of tuning circuit parameter to a resonance. It allows a fast and convenient determination of tensions and is straightforward to implement.'],['1998-10-12']
1656,['eng'],"['Zuber, K']",['Long baseline neutrino oscillations'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1998/07/06', 'neutrino, oscillation', 'neutrino, beam', 'fission, particle source', 'antineutrino p, interaction', 'charged current', 'deep underground detector', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810022'],['The motivation for possible future long baseline neutrino experiments is discussed. The proposed experiments as well as their physics potential is reviewed.'],['1998-10-12']
1657,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']","['Search for Anomalous Photonic Events with Missing Energy in $e^{+} e^{-}$ Collisions at $\\sqrt{s}$ = 130, 136 and 183 GeV']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'photon, electroproduction', 'transverse energy, missing-energy', 'photon, pair production', 'neutrino, pair production', 'channel cross section, branching ratio', 'upper limit', 'new particle, search for', 'neutrino, excited state', 'neutralino', 'gravitino', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> neutrino antineutrino photon', 'electron positron --> 2photon missing-energy', '130, 136, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810021'],"['Photonic events with large missing energy have been observed in e+e- collisions at centre-of-mass energies of 130, 136 and 183 GeV collected in 1997 using the OPAL detector at LEP. Results are presented for event topologies with a single photon and missing transverse energy or with an acoplanar photon pair. Cross-section measurements are performed within the kinematic acceptance of each selection. These results are compared with the expectations from the Standard Model process e+e- to nunubar + photon(s). No evidence is observed for new physics contributions to these final states. Using the data at Ecm = 183 GeV, upper limits on sigma(e+e- to X.Y)*BR(X to Y gamma) and sigma(e+e- to X.X)*BR(X to Y gamma)**2 are derived for the case of stable and invisible Y. These limits apply to single and pair production of excited neutrinos (X = nu*, Y = nu), to neutralino production (X = Chi_2^0, Y = Chi_1^0) and to supersymmetric models in which X = chi_1^0 and Y is a light gravitino.']",['1998-10-12']
1658,['eng'],"['Adloff, C']",['Charged Particle Cross Sections in Photoproduction and Extraction of the Gluon Density in the Photon'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'charged particle, photoproduction', 'transverse momentum, high', 'differential cross section, transverse momentum', 'differential cross section, rapidity dependence', 'quantum chromodynamics, perturbation theory', 'photon, resolved', 'gluon, momentum spectrum', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810020'],"['Photoproduction data collected with the H1 detector at HERA in 1994 are used to study the cross-sections for inclusive charged particle production and the structure of the photon. The differential cross-sections dsigma/dpT2, for |eta| < 1 in the HERA laboratory frame, and dsigma/deta for pT > 2 GeV/c and pT > 3 GeV/c have been measured. Model calculations of these cross-sections, based on perturbative QCD, indicate that the results are sensitive to the parton densities of the photon as well as to higher order effects, which are phenomenologically treated by multiple interactions. This sensitivity is exploited to determine the leading order x_gamma distribution of partons in the photon using a new method based on high pT charged particles. The gluon content of the photon is extracted and found to rise with decreasing x_gamma.']",['1998-10-09']
1659,['eng'],"['Telnov, V I']","['$\\gamma-\\gamma$, $\\gamma$-electron colliders']",['Particle Physics - Experimental Results'],"['talk, Dubna 1998/09/07', 'electron positron, linear collider', 'linear collider, proposed', 'photon electron, colliding beams', 'photon photon, colliding beams', 'radiation, laser', 'Compton scattering', 'luminosity, spectra', 'proposed experiment', 'Higgs particle, photoproduction', 'cross section', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810019'],"['It is very likely that in 3-4 years the construction of one or two linear colliders with c.m.s energy up to 0.5--1.5 TeV will be started. Besides e^+e^- collisions, linear colliders give a unique possibility to study gamma-gamma and gamma-electron interactions at energies and luminosities comparable to those in e^+e^- collisions. High energy photons for gamma-gamma and gamma-electron collisions can be obtained using laser backscattering. These types of collisions considerably increase the physics potential of linear colliders for relatively a small incremental cost. This report briefly reviews the physics goals and possible parameters of gamma-gamma colliders.']",['1998-10-09']
1660,['eng'],"['Takeuchi, Y', 'Hemmi, Y', 'Kurashige, H', 'Matono, Y', 'Murakami, K', 'Nomura, T', 'Sakamoto, H', 'Sasao, N', 'Suehiro, M', 'Fukushima, Y', 'Ikegami, Y', 'Nakamura, T T', 'Taniguchi, T', 'Asai, M']",['Observation of the decay mode $K_{L} \\to \\pi^{+}\\pi^{-}e^{+}e^{-}$'],['Particle Physics - Experimental Results'],"['K0(L), secondary beam', 'K0(L), semileptonic decay', 'K0(L), branching ratio', 'violation, CP', 'magnetic spectrometer, experimental results', 'KEK PS', 'K0(L) --> pi+ pi- positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810018'],['We report on results of an experimental search for the K_L -> pi^+ pi^- e^+ e^- decay mode. We found 13.5 +- 4.0 events and determined its branching ratio to be (4.4 +- 1.3(stat) +- 0.5(syst))*10^{-7}. The result agrees well with the theoretical prediction.'],['1998-10-09']
1661,['eng'],"['Montaruli, T']",['Atmospheric and Astrophysics Neutrinos with MACRO'],['Particle Physics - Experimental Results'],"['talk, Heidelberg 1998/07/20', 'neutrino, cosmic radiation', 'neutrino, astrophysics', 'neutrino nucleon, interaction', 'charged current', 'muon, angular distribution', 'muon, flux', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, mixing angle', 'astrophysics, missing-mass', 'WIMP, annihilation', 'supersymmetry', 'neutralino, flux', 'upper limit', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810017'],"['MACRO can detect three topologies of neutrino induced events, corresponding to different parent neutrino energies. The most numerous sample is made of upward throughgoing muons induced by atmospheric neutrinos of average energy 100 GeV. We have observed less events than expected events and the observed zenith distribution does not fit the expected one in the no-oscillation hypothesis, giving a maximum probability of 0.1 percent. Considering the neutrino (numu-nutau) oscillation hypothesis the best probability (17 percent) is obtained for maximum mixing and difference of square masses of a few times 10-3 eV2. The other detected samples are due to internally produced events and upward-going stopping muons, corresponding to an average neutrino energy of around 4 GeV. The results concerning these lower energy sample show a deficit and a shape of the angular distributions in agreement with that predicted by the oscillation model suggested by the higher energy sample. No evidence of a neutrino signal due to dark matter particles in the direction of the core of the Earth and of the Sun has been found among the background due to atmospheric neutrinos and limits have been set. The neutralino hypothesis is investigated and limits on its mass are given.']",['1998-10-08']
1662,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the Semileptonic Branching Ratio of Charm Hadrons Produced in $Z^{0} \\to c\\bar{c}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Z0, branching ratio', 'quark, charm', 'quark, pair production', 'quark, semileptonic decay', 'quark, branching ratio', 'correlation, (D*(2010) lepton)', 'electron, momentum spectrum', 'muon, momentum spectrum', 'transverse momentum, spectra', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810016'],"['The inclusive charm hadron semileptonic branching fractions B(c to e) and B(c to mu) in Z to ccbar events have been determined using 4.4 million hadronic Z decays collected with the OPAL detector at LEP. A charm-enriched sample is obtained by selecting events with reconstructed D*+- mesons. Using leptons found in the hemisphere opposite that of the D*+- mesons, the semileptonic branching fractions of charm hadrons are measured to be B(c to e) = 0.103 +-0.009 +0.009 -0.008 and B(c to mu) = 0.090 +-0.007 +0.007 -0.006 where the first errors are in each case statistical and the others systematic. Combining these measurements, an inclusive semileptonic branching fraction of charm hadrons of B(c to l) = 0.095 +-0.006 +0.007 -0.006 is obtained.']",['1998-10-08']
1663,['eng'],"['Grosso-Pilcher, C']",['Combined Limits on First Generation Leptoquarks from the CDF and D0 Experiments'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'leptoquark, search for', 'leptoquark, scalar', 'leptoquark, decay', 'leptoquark, mass', 'lower limit', 'statistical analysis', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810015'],"['We have combined recently published leptoquark results from the CDF and D0 Collaborations which yielded 95% CL lower limits on the first generation scalar leptoquark mass of 213 GeV and 225 GeV, respectively, under assumption of 100% branching fraction of the leptoquark decay into the eq channel. The combined limit from the two experiments is 242 GeV. This is the most stringent limit on the first generation scalar leptoquark mass to date.']",['1998-10-07']
1664,['eng'],"['Montaruli, T', 'Bellotti, R', 'Cafagna, F', 'Circella, M', 'De Marzo, C', 'Lipari, P']",['A simulation code to assist designing space missions of the Airwatch type'],['Detectors and Experimental Techniques'],"['talk, San Diego 1997/07/27', 'cosmic radiation', 'counters and detectors, satellite', 'showers, air', 'photon, counters and detectors', 'optics, reflection', 'semiconductor detector, pixel', '> 3*10**6 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810014'],"['The design of an Airwatch type space mission can greatly benefit from a flexible simulation code for establishing the values of the main parameters of the experiment. We present here a code written for this purpose. The cosmic ray primary spectrum at very high energies, the atmosphere modelling, the fluorescence yield, the photon propagation and the detector response are taken into account in order to optimize the fundamental design parameters of the experiment, namely orbit height, field of view, mirror radius, number of pixels of the focal plane, threshold of photo-detection. The optimization criterion will be to maximize counting rates versus mission cost, which imposes limits both on weight and power consumption. Preliminary results on signals with changing energy and zenith angle of incident particles are shown.']",['1998-10-07']
1665,['eng'],[],['Study of the reaction $\\pi^{-} Be \\to \\omega \\pi^{-} \\pi^{0} Be$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inelastic scattering', 'beryllium', 'omega(783), hadroproduction', 'pi0, hadroproduction', 'meson resonance, hadroproduction', 'meson resonance, hadronic decay', 'mass spectrum, (omega(783) pi-)', 'partial wave analysis', 'a2(1320), branching ratio', 'pi2(1670), branching ratio', 'a4(2040), mass', 'a4(2040), width', 'magnetic spectrometer, experimental results', 'Serpukhov PS', 'pi- beryllium --> beryllium omega(783) pi- pi0', '37 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810013'],"['The results of patial wave analysis of the omega pi- pi0 system, produced in the reaction pi- Be --> pi+ 2pi- 2pi0 Be at beam momentum of 37 GeV are presented. An indication of the resonant type structure with mass near 1.74 GeV and JpMetha=0-0+ in the omega rho- system was found. The decay branching ratio of a2(1320)- to omega pi- pi0 was measured. A wave with JpMetha=2+1+ shows a broad bump at M near 1.7 GeV. The decays pi2(1670)- --> omega rho- and a4(2040)- --> omega rho- were observed for the first time. The bump in the b1(1235)pi wave with exotic quantum numbers Jpc=1-+ at M near 1.7 GeV was observed.']",['1998-10-07']
1666,['eng'],"['Cei, F']",['Search for Rare Particles with the MACRO Detector'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'new particle, search for', 'WIMP, annihilation', 'new particle', 'charge, fractional', 'magnetic monopole, flux', 'ionization, low', 'nuclear matter, strangeness', 'muon, flux', 'flux, upper limit', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810012'],"['We report on the search for Rare Particles (Magnetic Monopoles, Nuclearites, Weakly Interacting Massive Particles and Lightly Ionizing Particles) with the MACRO detector. For magnetic monopoles (the main goal of the experiment) our limit is about 0.4 times the Parker bound for monopole velocities between 10^{-4} and 10^{-1}.']",['1998-10-07']
1667,['eng'],"['Söldner-Rembold, S']",['Final States in Photon-Photon and Photon-Proton Interactions'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'photon photon, interaction', 'photon p, interaction', 'hadron, multiple production', 'cross section, energy dependence', 'cross section, factorization', 'jet, photoproduction', 'exchange, pomeron', 'exchange, Regge', 'photon, resolved', 'angular distribution, (2jet)', 'transverse energy, dependence', 'transverse energy, energy flow', 'differential cross section, rapidity dependence', 'differential cross section, transverse momentum', 'baryon antibaryon, asymmetry', 'experimental results', 'magnetic detector, OPAL', 'magnetic detector, L3', 'CERN LEP Stor', 'magnetic detector, H1', 'DESY HERA Stor', '((5)) ((6))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810011'],['The total hadronic photon-photon cross-section measured by L3 and OPAL and the apparent discrepancy between the results are discussed. OPAL measurements of jet and charged hadron production in photon-photon scattering and preliminary H1 results on neutral pion production in photon-proton scattering are also presented. The mechanism of baryon number transfer in photon-proton interactions at HERA has been studied for the first time by H1.'],['1998-10-07']
1668,['eng'],"['Müller, D']",['QCD Tests Using $b\\bar{b}g$ Events and a New Measurement of the B-Hadron Energy Distribution'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1998/07/02', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'gluon, energy spectrum', 'coupling, (2beauty gluon)', 'angular distribution, asymmetry', 'quantum chromodynamics, validity test', 'parity, violation', 'time reversal, invariance', 'invariance, CP', 'B, energy spectrum', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 2beauty gluon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810010'],"['We present new studies of 3-jet final states from hadronic $Z^0$ decays recorded by the SLD experiment, in which jets are identified as quark, antiquark or gluon. Our gluon energy spectrum, measured over the full kinematic range, is consistent with the predictions of QCD, and we derive a limit on an anomalous chromomagnetic $bbg$ coupling. We measure the parity violation in $Z^0$ decays into $b\\bar{b}g$ to be consistent with the predictions of electroweak theory and QCD, and perform new tests of T- and CP-conservation at the $bbg$ vertex. We also present a new technique for reconstructing the energy of a $B$ hadron using the set of charged tracks attached to a secondary vertex. The $B$ hadron energy spectrum is measured over the full kinematic range, allowing improved tests of predictions for the shape of the spectrum. The average scaled energy is measured to be $ = 0.719 \\pm 0.005 (stat.)$ (Preliminary).']",['1998-10-07']
1669,['eng'],"['Ronga, F']",['Atmospheric neutrino-induced muons in the MACRO detector'],['Particle Physics - Experimental Results'],"['talk, Takayama 1998/06/04', 'neutrino, cosmic radiation', 'neutrino nucleon, interaction', 'charged current', 'muon, flux', 'angular distribution', 'neutrino, oscillation', 'neutrino, energy', 'neutrino/mu', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810008'],"['A measurement of the flux of neutrino-induced muons using the MACRO detector is presented. Different event topologies, corresponding to different neutrino parent energies can be detected. The upward throughgoing muon sample is the larger event sample. The observed upward-throughgoing muons are 26% fewer than expected and the zenith angle distribution does not fit with the expected one. Assuming neutrino oscillations, both measurements suggest maximum mixing and Dm2 of a few times 10-3 eV2. The other samples are due to the internally produced events and to upward-going stopping muons. These data show a regular deficit of observed events in each angular bin, as expected assuming neutrino oscillations with maximum mixing, in agreement with the analysis of the upward-throughgoing muon sample.']",['1998-10-05']
1670,['eng'],"['Ambrose, D A', 'Arroyo, C G', 'Bachman, M', 'De Cecco, P', 'Connor, D', 'Eckhause, M', 'Ecklund, K M', 'Graessle, S C', 'Hancock, A D', 'Hartman, K', 'Hebert, M', 'Hoff, C H', 'Hoffmann, G W', 'Irwin, G M', 'Kane, J R', 'Kanematsu, N', 'Kuang Yu Ping', 'Lang, K', 'Lee, R', 'Martin, R D', 'McDonough, J', 'Milder, A J', 'Molzon, W R', 'Pommot-Maia, M C', 'Riley, P J', 'Ritchie, J L', 'Rubin, P D', 'Vassilakopoulos, V I', 'Ware, C B', 'Welsh, R E', 'Wojcicki, S G', 'Wolin, E', 'Worm, S D']",['First Observation of the Rare Decay Mode $K_{L}^{0} \\to e^{+}e^{-}$'],['Particle Physics - Experimental Results'],"['K0, secondary beam', 'K0(L), leptonic decay', 'K0(L), rare decay', 'K0(L), branching ratio', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'K0(L) --> positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810007'],"['In an experiment designed to search for and study very rare two-body decay modes of the K-long, we have observed four examples of the decay K-long -> e+ e-, where the expected background is 0.17+-0.10 events. This observation translates into a branching fraction of 8.7^{+5.7}_{-4.1} X 10^{-12}, consistent with recent theoretical predictions. This result represents by far the smallest branching fraction yet measured in particle physics.']",['1998-10-15']
1671,['eng'],"['Diehl, H T']",['Vector Boson Pair Production and Trilinear Gauge Boson Couplings'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'photon, hadroproduction', 'coupling, (3gauge boson)', 'gauge boson, pair production', 'intermediate boson, leptonic decay', 'Z0, hadronic decay', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810006'],"[""Direct measurements of vector boson pair production processes and trilinear gauge boson couplings have been conducted by the CDF and DO Collaborations. Preliminary results from searches for anomalous WW/WZ->muon-neutrino-jet-jet and WZ->e-e-e-neutrino production are presented. 95% CL anomalous coupling limits from previously published DO results are -0.20 < lambda < 0.20 (Delta kappa=0) and -0.30 < Delta kappa < 0.43 (lambda=0) for Lambda=2000 GeV where the WWgamma couplings are assumed to equal the WWZ couplings. Combined DO + LEP experiment anomalous coupling limits are presented for the first time. 95% CL limits are -0.16<lambda(gamma)< 0.10 (Delta kappa=0) and -0.15 < Delta kappa(gamma) < 0.41 (lambda=0) under the assumption that the couplings are related by the ``HISZ'' constraints. 95% CL anomalous ZZg and Zgg coupling limits from DO are |h(30)^Z|<0.36 (h(40)^Z=0) and |h(40)^Z|<0.05 (h(30)^Z=0) for Lambda=750 GeV. CDF reports the first observation of a ZZ event. Prospects for Run II are discussed.""]",['1998-10-15']
1672,['eng'],"['Hildreth, M D']",['Evaluation of the LEP Centre-of-Mass Energy Above the W-Pair Production Threshold'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, storage ring', 'energy, upgrade', 'energy, beam monitoring', 'bending magnet', 'magnetic field, measurement', 'electron, polarized beam', 'polarization, depolarization', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810005'],"['Knowledge of the beam energy at LEP2 is of primary importance to set the absolute energy scale for the measurement of the W-boson mass. The beam energy above 80 GeV is derived from continuous measurements of the magnetic bending field by 16 NMR probes situated in a number of the LEP dipoles. The relationship between the fields measured by the probes and the beam energy is calibrated against precise measurements of the average beam energy between 41 and 55 GeV made using the resonant depolarisation technique. The linearity of the relationship is tested by comparing the fields measured by the probes with the total bending field measured by a flux loop. Several further corrections are applied to derive the the centre-of-mass energies at each interaction point. The beam energy has been determined with a precision of 25 MeV for the data taken in 1997, corresponding to a relative precision of 2.7x 10^{-4}. Prospects for improvements are outlined.']",['1998-10-15']
1673,['eng'],"['Avakian, H']",['Performance of the Electromagnetic Calorimeter of the HERMES Experiment'],['Detectors and Experimental Techniques'],"['calorimeter, electromagnetic', 'calorimeter, lead-glass', 'performance', 'calibration', 'energy resolution', 'stability', 'radiation, damage', 'magnetic spectrometer, HERMES', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810004'],"['The performance of the electromagnetic calorimeter of the HERMES experiment is described. The calorimeter consists of 840 radiation resistant F101 lead-glass counters. The response to positrons up to 27.5 GeV, the comparison between the measured energy and the momentum reconstructed from tracking, long-term stability, hadron rejection and neutral meson invariant mass reconstruction are shown.']",['1998-10-15']
1674,['eng'],"['Barberis, D']",['A measurement of the branching fractions of the $f_{1}(1285)$ and $f_{1}(1420)$ produced central p p interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, interaction', 'meson resonance, hadroproduction', 'meson resonance, hadronic decay', 'meson resonance, radiative decay', 'f1(1285), branching ratio', 'f1(1420), branching ratio', 'exchange, pomeron', 'spectra, momentum transfer', 'angular distribution, (2p)', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> f1(1285) 2p', 'p p --> f1(1420) 2p', 'meson resonance --> eta pi+ pi-', 'meson resonance --> rho(770)0 photon', 'meson resonance --> Phi(1020) photon', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810003'],['A study of the f1(1285) and f1(1420) produced in central pp interactions has been performed. For the first time in a single experiment the branching fractions of both mesons in all major decay modes have been determined. Both the f1(1285) and f1(1420) are consistent with being produced by double Pomeron exchange.'],['1998-10-15']
1675,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for Chargino and Neutralino Production at $\\sqrt{s}$ = 181-184 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'sparticle, pair production', 'chargino', 'neutralino', 'sparticle, decay modes', 'sparticle, mass', 'lower limit', 'astrophysics, missing-mass', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '181-184 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809031'],"['A search for charginos and neutralinos, predicted by supersymmetric theories, has been performed using a data sample of 57 pb-1 at centre-of-mass energies of 181-184 GeV taken with the OPAL detector at LEP. No evidence for chargino or neutralino production has been found. Upper limits on chargino and neutralino pair production cross-sections are obtained as a function of the chargino mass, the lightest neutralino mass, and the second lightest neutralino mass. For large chargino masses the limits have been improved with respect to the previous analyses at lower centre-of-mass energies. Exclusion regions at 95% confidence level of parameters of the Constrained Minimal Supersymmetric Standard Model are determined for the case of a large universal scalar mass, m_0, implying heavy scalar fermions, and for the case of a small m_0 resulting in light scalar fermions and giving the worst-case limits. Within this framework and for the lightest chargino-neutralino mass difference greater than 5 GeV the 95% C.L. lower limits on the lightest chargino mass for m_0 = 500 GeV are 90.0 and 90.2 GeV for tan(beta) = 1.5 and 35 respectively. These limits for all m_0 (the worst-case) are 69.1 and 65.2 GeV for tan(beta) = 1.5 and 35 respectively. Exclusion regions are also presented for neutralino masses, including an absolute lower limit at 95% C.L. for the mass of the lightest neutralino of 30.1 GeV for m_0 = 500 GeV (24.2 GeV for all m_0), with implications for experimental searches for the lightest neutralino as a dark matter candidate.']",['1998-10-01']
1676,['eng'],"['Willocq, S']","['$B^{+}, B^{0}_{d}$ and b-baryon Lifetimes']",['Particle Physics - Experimental Results'],"['review, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'anti-p p, colliding beams', 'anti-p p, interaction', 'beautiful particle, electroproduction', 'beautiful particle, hadroproduction', 'beautiful particle, hadronic decay', 'beautiful particle, semileptonic decay', 'B+, lifetime', 'B0, lifetime', 'Lambda/b0, lifetime', 'experimental results', 'SLAC SLC Linac', 'CERN LEP Stor', 'Batavia TEVATRON Coll', '((4)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809030'],"['We review recent B+, B0d and b-baryon lifetime measurements performed by the LEP, SLD and CDF collaborations. Lifetime ratios of tau(B+) / tau(B0d) = 1.070 +/- 0.027 and tau(b baryon) / tau(B0d) = 0.77 +/- 0.04 are obtained using all existing measurements. The ratio between charged and neutral B meson lifetimes is in good agreement with theory but the ratio between b-baryon and B meson lifetimes remains somewhat lower than expected.']",['1998-09-30']
1677,['eng'],"['Aitala, E M']",['Correlations between D and $\\overline{D}$ mesons produced in 500 GeV/c $\\pi^{-}$-nucleon interactions'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'charmed meson, pair production', 'charmed meson, hadroproduction', 'charmed meson, hadronic decay', 'correlation, (D anti-D)', 'D0', 'D+', 'transverse momentum, spectra', 'longitudinal momentum, spectra', 'quantum chromodynamics, perturbation theory', 'mass, charm', 'momentum spectrum, parton', 'renormalization, dependence', 'showers, parton', 'numerical calculations, Monte Carlo', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809029'],['We have fully reconstructed 791 D meson pairs to study correlations between the transverse and longitudinal momenta of the two D mesons and the relative production rates for different types of D meson pairs. The experimental distributions are compared to a next-to-leading-order QCD calculation and to predictions of the Pythia/Jetset Monte Carlo event generator.'],['1998-09-29']
1678,['eng'],"['Adloff, C']",['Forward Jet and Particle Production at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'pi, electroproduction', 'jet, electroproduction', 'small-angle', 'small-x', 'channel cross section, x-dependence', 'angular correlation, (jet lepton)', 'transverse energy, energy flow', 'quantum chromodynamics', 'ladder approximation', 'Lipatov equation', 'Altarelli-Parisi equation', 'photon, resolved', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809028'],"['Single particles and jets in deeply inelastic scattering at low x are measured with the H1 detector in the region away from the current jet and towards the proton remnant, known as the forward region. Hadronic final state measurements in this region are expected to be particularly sensitive to QCD evolution effects. Jet cross-sections are presented as a function of Bjorken-x for forward jets produced with a polar angle to the proton direction, theta, in the range 7 < theta < 20 degrees. Azimuthal correlations are studied between the forward jet and the scattered lepton. Charged and neutral single particle production in the forward region are measured as a function of Bjorken-x, in the range 5 < theta < 25 degrees, for particle transverse momenta larger than 1 GeV. QCD based Monte Carlo predictions and analytical calculations based on BFKL, CCFM and DGLAP evolution are compared to the data. Predictions based on the DGLAP approach fail to describe the data, except for those which allow for a resolved photon contribution.']",['1998-09-25']
1679,['eng'],"['Botje, M', 'Wolf, G']",['Enhancing Squark/Leptoquark Production by Increasing the HERA Beam Energies'],['Detectors and Experimental Techniques'],"['positron p, interaction', 'new particle, search for', 'R parity, violation', 'squark, electroproduction', 'squark, mass', 'leptoquark, electroproduction', 'leptoquark, mass', 'channel cross section, energy dependence', 'beam, energy', 'background', 'numerical calculations', '27.5-35.0 GeV (positron), 820-1000 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809027'],"['The cross section for production of R-parity violating squarks ($\\tilde{q}$) or leptoquarks ($LQ$) with masses above 200 GeV by positron-proton scattering at HERA can be substantially increased by a moderate increase of the beam energies. If, for example, the positron energy is raised from 27.5 to 32.5 GeV and the proton energy from 820 to 1000 GeV, the $\\tilde{q}/LQ$ production cross section for masses of 200 -- 230 GeV increases by a factor of about 2--6 and the search range for $\\tilde{q}/LQ$ is extended by about 40 GeV to masses of 270 -- 280 GeV. In this report event yields are presented for beam energies in the range E_e = 27.5--35 GeV and E_p = 820--1100 GeV. Also presented is the rate of background events expected from Standard Model neutral and charged current $e^{\\pm}p$ scattering.']",['1998-09-25']
1680,['eng'],"['Aitala, E M']",['Measurement of the form-factor ratios for $D^{+} \\to \\overline{K^{*0}}\\ell^{+}_{\\nu\\ell}$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D+, hadroproduction', 'D+, semileptonic decay', 'K*(892), hadronic decay', 'form factor, vector', 'form factor, axial-vector', 'form factor, ratio', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> K*(892) lepton+ neutrino', 'K*(892) --> K- pi+', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809026'],"['The form factor ratios rv=V(0)/A1(0), r2=A2(0)/A1(0) and r3=A3(0)/A1(0) in the decay D+ --> K* l nu, K* -->K-pi+ have been measured using data from charm hadroproduction experiment E791 at Fermilab. From 3034 (595) signal (background) events in the muon channel, we obtain rv=1.84+-0.11+-0.09, r2=0.75+-0.08+-0.09 and, as a first measurement of r3, we find 0.04+-0.33 +-0.29. The values of the form factor ratios rv and r2 measured for the muon channel are combined with the values of rv and r2 that we have measured in the electron channel. The combined E791 results for the muon and electron channels are rv=1.87+-0.08+-0.07 and r2=0.73+-0.06+-0.08.']",['1998-09-25']
1681,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['A Measurement of $R_{b}$ using a Double Tagging Method'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'Z0, branching ratio', 'quark, semileptonic decay', 'particle identification, beauty', 'particle identification, (muon electron)', 'track data analysis, vertex', 'neural network', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810002'],"['The fraction of Z to bbbar events in hadronic Z decays has been measured by the OPAL experiment using the data collected at LEP between 1992 and 1995. The Z to bbbar decays were tagged using displaced secondary vertices, and high momentum electrons and muons. Systematic uncertainties were reduced by measuring the b-tagging efficiency using a double tagging technique. Efficiency correlations between opposite hemispheres of an event are small, and are well understood through comparisons between real and simulated data samples. A value of Rb = 0.2178 +- 0.0011 +- 0.0013 was obtained, where the first error is statistical and the second systematic. The uncertainty on Rc, the fraction of Z to ccbar events in hadronic Z decays, is not included in the errors. The dependence on Rc is Delta(Rb)/Rb = -0.056*Delta(Rc)/Rc where Delta(Rc) is the deviation of Rc from the value 0.172 predicted by the Standard Model. The result for Rb agrees with the value of 0.2155 +- 0.0003 predicted by the Standard Model.']",['1998-10-15']
1682,['eng'],"['Halzen, Francis']",['The AMANDA Neutrino Telescope'],['Detectors and Experimental Techniques'],"['talk, Takayama 1998/06/04', 'neutrino, counters and detectors', 'Cherenkov counter, water', 'solids, water', 'photoelectron, amplifier', 'calibration', 'optics, laser', 'muon, tracks', 'angular resolution', 'deep underground detector, AMANDA', 'performance', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809025'],"[""With an effective telescope area of order $10^4$ m$^2$ for TeV neutrinos, a threshold near $\\sim$50 GeV and a pointing accuracy of 2.5 degrees per muon track, the AMANDA detector represents the first of a new generation of high energy neutrino telescopes, reaching a scale envisaged over 25 years ago. We describe early results on the calibration of natural deep ice as a particle detector as well as on AMANDA's performance as a neutrino telescope.""]",['1998-09-24']
1683,['eng'],"['Andreev, V P', 'Belousov, A S', 'Fomenko, A M', 'Gorbov, L A', 'Greenshaw, T J', 'Malinovskii, E I', 'Maxfield, S J', 'Semenov, A Yu', 'Shevyakov, I', 'Smirnov, P A', 'Soloviev, I V', 'Winter, G G']",['Tagging High Energy Photons in the H1 Detector at HERA'],['Detectors and Experimental Techniques'],"['photon p, interaction', 'calorimeter', 'lead', 'scintillation counter, fibre', 'radiation, damage', 'calibration', 'acceptance', 'magnetic detector, H1', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809024'],"['Measures taken to extend the acceptance of the H1 detector at HERA for photoproduction events are described. These will enable the measurement of electrons scattered in events in the high y range 0.85 < y < 0.95 in the 1998 and 1999 HERA run period. The improvement is achieved by the installation of an electromagnetic calorimeter, the ET8, in the HERA tunnel close to the electron beam line 8 m downstream of the H1 interaction point in the electron direction. The ET8 will allow the study of tagged gamma p interactions at centre-of-mass energies significantly higher than those previously attainable. The calorimeter design and expected performance are discussed, as are results obtained using a prototype placed as close as possible to the position of the ET8 during the 1996 and 1997 HERA running.']",['1998-09-23']
1684,['eng'],"['Naples, D', 'Romosan, A']",['A High Statistics Search for $\\nu_{e}(\\overline{\\nu{e}}) \\to \\nu_{\\tau}(\\overline{\\nu_{\\tau}})$ Oscillations'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'neutrino/e, energy spectrum', 'neutrino/tau', 'neutrino, beam', 'neutrino, mass difference', 'neutrino, mixing angle', 'neutrino nucleon, interaction', 'charged current', 'neutrino/e, flux', 'calorimeter, experimental results', 'Batavia TEVATRON Coll', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809023'],['We present a new limit on nu_e to nu_tau oscillations by searching for electron neutrino dissappearance in the high-energy wide-band CCFR neutrino beam. The beam is composed primarily of muon neutrinos but this analysis uses the 2.3% electron neutrino component of the beam. Electron neutrino energies range from 30 to 600 GeV and flight lengths vary from 0.9 to 1.4 km. This limit improves the sensitivity os existing limits and obtains a lowest 90% confidence upper limit in sin**2(2alpha) of 9.9 x 10**(-2) at delta-m**2 of 125 eV**2.'],['1998-09-22']
1685,['eng'],"['Abe, F']",['Search for New Particles Decaying to $b\\overline{b}$ in $p\\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'rho(770), technicolor', 'topcolor', 'postulated particle, topgluon', 'color, octet', 'symmetry breaking, SU(3) x SU(3)', 'postulated particle, hadronic decay', 'quark, beauty', 'quark, pair production', 'mass spectrum, (2beauty)', 'channel cross section, branching ratio', 'upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809022'],"['We have used 87 pb^-1 of data collected with the Collider Detector at Fermilab to search for new particles decaying to b bbar. We present model-independent upper limits on the cross section for narrow resonances which excludes the color-octet technirho in the mass interval 350 < M < 440 GeV/c^2. In addition, we exclude topgluons, predicted in models of topcolor-assisted technicolor, of width Gamma = 0.3 M in the mass range 280 < M < 670 GeV/c^2, of width Gamma = 0.5 M in the mass range 340 < M < 640 GeV/c^2, and of width Gamma = 0.7 M in the mass range 375 < M < 560 GeV/c^2.']",['1998-09-22']
1686,['eng'],"['Mankel, R', 'Spiridonov, A A']",['The Concurrent Track Evolution Algorithm'],['Detectors and Experimental Techniques'],"['track data analysis', 'magnetic field, slope', 'efficiency', 'programming', 'numerical calculations', 'magnetic detector, HERA-B', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809021'],"['The Concurrent Track Evolution method, which was introduced in a previous paper (DESY 97-054), has been further explored by applying it to the propagation of track candidates into an inhomogeneous magnetic field volume equipped with tracking detectors, as is typical for forward B spectrometers like HERA-B or LHCb. Compared to the field-free case, the method was extended to three-dimensional propagation, with special measures necessary to achieve fast transport in the presence of a fast-varying magnetic field. The performance of the method is tested on HERA-B Monte Carlo events with full detector simulation and a realistic spectrometer geometry.']",['1998-09-22']
1687,['eng'],"['Moscoso, L']",['Neutrino telescopes under the ocean'],['Detectors and Experimental Techniques'],"['talk, Takayama 1998/06/04', 'deep underground detector, ANTARES', 'deep underground detector, proposed', 'Cherenkov counter, water', 'optics, absorption', 'photoelectron, amplifier', 'neutrino/mu, cosmic radiation', 'muon, neutrinoproduction']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809020'],['Neutrino telescopes offer an alternative way to explore the Universe. Several projects are in operation or under construction. A detector under the ocean is very promising because of the very accurate angular resolution that it provides. The ANTARES project is intended to demonstrate the feasibilty of such a detector.'],['1998-09-21']
1688,['eng'],"['Hamacher, K']",['Properties of Gluon and Quark Jets'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'quark, jet', 'gluon, jet', 'fragmentation function, slope', 'dependence, scaling', 'hadron, multiple production', 'multiplicity, ratio', 'color', 'Altarelli-Parisi equation', 'effect, nonperturbative', 'electron positron, annihilation', 'jet, multiple production', 'final state, (3jet)', 'mass spectrum, (2jet)', 'numerical calculations', 'interpretation of experiments, CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809018'],['Recent developments and results on the comparison of gluon to quark jets are discussed. A most important topic is the introduction of explicit energy scales of the jets. The scaling violation of the fragmentation function and the increase of the multiplicity with scale is shown to be directly proportional to the corresponding gluon or quark colour factor. The ratio of the hadron multiplicity in gluon to quark jets is understood to be smaller than the colour factor ratio due to differences in the fragmentation of the leading quark or gluon. Novel algorithms to reconstruct the colour portraits or the colour flow of an event are presented.'],['1998-09-18']
1689,['eng'],"['Bernardini, P', 'Barbarino, G C', 'Guarino, F']","['NOE, a Neutrino Oscillation Experiment at Gran Sasso Laboratory']",['Detectors and Experimental Techniques'],"['talk, Amsterdam 1998/09/07', 'neutrino, oscillation', 'neutrino, beam', 'neutrino, counters and detectors', 'calorimeter', 'transition radiation detector', 'plastics', 'proportional chamber, gas', 'argon, organic compounds', 'xenon', 'neutrino nucleon, interaction', 'charged current', 'tau, particle identification', 'neural network', 'deep underground detector, Gran Sasso']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809017'],['The project of a large underground experiment (NOE) devoted to long baseline neutrino oscillation measurement is presented. The apparatus is composed by calorimetric modules interleaved with TRD modules and has been optimized to be sensitive in the region of sin2 2theta and Dm2 suggested by the atmospheric neutrino oscillation signal.'],['1998-09-18']
1690,['eng'],"['Abbott, B']",['Probing Hard Color-Singlet Exchange in $p\\overline p$ Collisions at $\\sqrt {s}=630 GeV$ and $800 GeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, pair production', 'rapidity, gap', 'color, singlet', 'exchange, singlet', 'transverse energy, dependence', 'energy dependence', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809016'],"['We present results on dijet production via hard color-singlet exchange in proton-antiproton collisions at root-s = 630 GeV and 1800 GeV using the DZero detector. The fraction of dijet events produced via color-singlet exchange is measured as a function of jet transverse energy, separation in pseudorapidity between the two highest transverse energy jets, and proton-antiproton center-of-mass energy. The results are consistent with a color-singlet fraction that increases with an increasing fraction of quark-initiated processes and inconsistent with two-gluon models for the hard color-singlet.']",['1998-09-17']
1691,['eng'],"['Ackerstaff, K']",['Determination of the Deep Inelastic Contribution to the Generalised Gerasimov-Drell-Hearn Integral for the Proton and Neutron'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron nucleus, deep inelastic scattering', 'positron, polarized beam', 'helium, nuclide', 'polarized target, internal', 'exchange, one-photon', 'photon nucleon, absorption', 'cross section, difference', 'sum rule, Drell-Hearn-Gerasimov', 'energy dependence', 'momentum transfer, dependence', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809015'],['The virtual photon absorption cross section differences [sigma_1/2-sigma_3/2] for the proton and neutron have been determined from measurements of polarised cross section asymmetries in deep inelastic scattering of 27.5 GeV longitudinally polarised positrons from polarised 1H and 3He internal gas targets. The data were collected in the region above the nucleon resonances in the kinematic range nu < 23.5 GeV and 0.8 GeV**2 < Q**2 < 12 GeV**2. For the proton the contribution to the generalised Gerasimov-Drell-Hearn integral was found to be substantial and must be included for an accurate determination of the full integral. Furthermore the data are consistent with a QCD next-to-leading order fit based on previous deep inelastic scattering data. Therefore higher twist effects do not appear significant.'],['1998-09-17']
1692,['eng'],"['Baurov, Yu A', 'Konradov, A A', 'Kushniruk, V F', 'Sobolev, Yu G']",['Global Anisotropy of Space and experimental investigation of changes in $\\beta$-decay count rate of radioactive elements'],['Particle Physics - Experimental Results'],"['nucleus, semileptonic decay', 'cesium', 'cobalt', 'strontium', 'radioactivity', 'time dependence', 'space, anisotropy', 'astrophysics, model', 'fundamental constant, vector', 'potential, vector', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809014'],"['The results of experimental investigations of changes in beta-decay count rate of radioactive elements, are presented, and an explanation of those on the base of a new physical conception of forming the observed three-dimensional space from a finite set of one-dimensional discrete vectorial objects (byuons), containing the cosmological vectorial potential, a new fundamental vectorial constant, is given. In the theory, the vector direction corresponds with that of the axis of Universe rotation being discussed in literature.']",['1998-09-17']
1693,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Baru, S E', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Ganyushin, D I', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Koop, I A', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Lysenko, A P', 'Mamutkin, A A', 'Nesterenko, I N', 'Otboev, A V', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Polunin, A A', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V', 'Valishev, A A', 'Varganov, A V', 'Vasilev, A', 'Velikzhanin, Yu S']",['Experiments at VEPP-2M with SND detector'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron positron, inelastic scattering', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'final state, ((n)neutral particle)', 'K0(S), hadronic decay', 'photon, electroproduction', 'photon, pair production', 'pi, multiple production', 'K0, pair production', 'f2(1270), width', 'mass spectrum', 'angular distribution', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'tables', 'bibliography', '0.984-1.060 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809013'],['Short overview of experiments with SND detector at VEPP-2M e^+e^- collider in the energy range 2E = 400 - 1400 MeV and preliminary results of data analysis are presented.'],['1998-09-17']
1694,['eng'],"['Bishai, M']",['First Observation of the Decay $\\tau^{-}\\to K^{*-}\\eta\\nu_{\\tau}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'K*(892), hadronic decay', 'eta, radiative decay', 'tau-, branching ratio', 'mass spectrum, (K0(S) pi-)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> tau+ tau-', 'tau- --> K*(892) eta neutrino/tau', 'K*(892) --> K0(S) pi-', 'K*(892) --> K- pi0', 'eta --> 2photon', '10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809012'],"['Using data recorded by the CLEO-II detector at CESR, we report the first measurement of the branching fraction for the decay of $\\tau^-$ into $K^{*-}\\eta \\nu_{\\tau}$. The measured branching fraction is (2.9 +- 0.8 +- 0.4) $10^{-4}$. We also measure the inclusive branching fractions without requiring the $K^*$ resonance: $\\tau^-$ into $K_S \\pi^- \\eta \\nu_{\\tau}$, $\\tau^-$ into $K^- \\pi^0 \\eta \\nu_{\\tau}$. The measured branching fractions are (1.10 +- 0.35 +- 0.11) $10^{-4}$, (1.77 +- 0.56 +- 0.71) $10^{-4}$ respectively.']",['1998-09-16']
1695,['eng'],"['Bhat, P', 'Prosper, H B', 'Snyder, S']",['Top Quark Physics at the Tevatron'],['Particle Physics - Experimental Results'],"['review, experimental results', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, hadroproduction', 'mass, truth', 'channel cross section', 'quark, decay modes', 'final state, dilepton', 'final state, ((n)jet lepton)', 'final state, ((n)jet)', 'Kobayashi-Maskawa angle', 'neutral current, flavor changing', 'Higgs particle, charged particle', 'W, helicity', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll', 'upgrade, proposed', 'proposed experiment', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809011'],"['The discovery of the top quark in 1995, by the CDF and D0 collaborations at the Fermilab Tevatron, marked the dawn of a new era in particle physics. Since then, enormous efforts have been made to study the properties of this remarkable particle, especially its mass and production cross section. In this article, we review the status of top quark physics as studied by the two collaborations using the p-pbar collider data at sqrt(s) = 1.8 TeV. The combined measurement of the top quark mass, m_t = 173.8 +- 5.0 GeV/c^2, makes it known to a fractional precision better than any other quark mass. The production cross sections are measured as sigma (t-tbar) = 7.6 -1.5 +1.8 pb by CDF and sigma (t-tbar) = 5.5 +- 1.8 pb by D0. Further investigations of t-tbar decays and future prospects are briefly discussed.']",['1998-09-15']
1696,['eng'],"['Achasov, M N', 'Aulchenko, V M', 'Baru, S E', 'Berdyugin, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P M', 'Korol, A A', 'Koshuba, S V', 'Lysenko, A P', 'Pakhtusova, E V', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V']",['Evidence of the $\\phi(1020)\\to\\eta\\pi^{0}\\gamma$ Decay'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), branching ratio', 'upper limit', 'eta, radiative decay', 'pi0, radiative decay', 'mass spectrum, (eta pi0)', 'photon, energy spectrum', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> eta pi0 photon', '0.98-1.04 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809010'],"['Signal of the rare radiative decay PHI--->ETA+PI0+GAMMA was observed in the SND experiment at VEPP-2M electron-positron collider.The result is based on the analysis of data, corresponding to a total integrated luminosity of 4 pb^{-1}, or 8x10^6 PHI mesons produced. The measured branching ratio of PHI--->ETA+PI0+GAMMA decay is equal to (0.83+-0.23)x10^{-4}.']",['1998-09-15']
1697,['eng'],"['Varelas, N']",['A Summary of Recent Color Coherence Results'],['Particle Physics - Experimental Results'],"['review, Frascati 1998/06/17', 'electron positron, annihilation', 'positron p, interaction', 'anti-p p, interaction', 'hadron, multiple production', 'color, coherence', 'quantum chromodynamics, perturbation theory', 'leading logarithm approximation', 'duality, parton hadron', 'expansion 1/N, color', 'jet, coherence', 'jet, multiple production', 'charged particle, momentum spectrum', 'charged particle, multiplicity', 'energy spectrum', 'W, associated production', 'model, fragmentation', 'Z0, hadronic decay', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809019'],"['Recent experimental results on color coherence phenomena from e+e-, ep, and ppbar collisions are presented. The data are compared to analytic perturbative QCD calculations based on the modified leading logarithm approximation and the local parton hadron duality hypothesis.']",['1998-09-18']
1698,['eng'],"['Abbott, B']",['Coloron Limits using the D0 Dijet Angular Distribution'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'angular distribution, (2jet)', 'symmetry, SU(3) x SU(3)', 'model, coloron', 'mass, coloron', 'lower limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809009'],['The D0 dijet angular distribution is used to place limits on flavor--universal colorons. Models with M_c / cot{theta} < 759 GeV/c^2 are excluded at the 95% confidence level.'],['1998-09-14']
1699,['eng'],"['Abreu, P', 'De Angelis, A', 'Della Ricca, G', 'Fassouliotis, D', 'Grefrath, A', 'Kjaer, N J', 'Henriques, R P', 'Mulders, M', 'Pimenta, M', 'Vitale, L']",['The Estimation of the Effective Centre of Mass Energy in $q\\overline{q} \\gamma$ Events from DELPHI'],['Detectors and Experimental Techniques'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, pair production', 'hadron, multiple production', 'photon, associated production', 'radiation, initial-state interaction', 'energy', 'energy resolution', 'jet, angular distribution', 'numerical calculations, Monte Carlo', 'magnetic detector, DELPHI', 'CERN LEP Stor', '((5))']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809008', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=open-98-026']","['The photon radiation in the initial state lowers the energy available for the e$^+$e$^-$ collisions; this effect is particularly important at LEP2 energies (above the mass of the Z boson). Being aligned to the beam direction, such initial state radiation is mostly undetected. This article describes the procedure used by the DELPHI experiment at LEP to estimate the effective centre-of-mass energy in hadronic events collected at energies above the Z peak. Typical resolutions ranging from 2 to 3 GeV on the effective center-of-mass energy are achieved, depending on the event topology.']",['1998-09-14']
1700,['eng'],"['Eitel, K', 'Zeitnitz, B']",['The Search for Neutrino Oscillations $\\overline{\\nu}_{\\mu} \\to \\overline{\\nu}_{e}$ with KARMEN'],['Particle Physics - Experimental Results'],"['talk, Takayama 1998/06/04', 'neutrino, oscillation', 'antineutrino/mu', 'antineutrino/e', 'neutrino, particle source', 'antineutrino p, interaction', 'charged current', 'p n, radiative capture', 'neutrino, mass difference', 'neutrino, mixing angle', 'correlation, (positron photon)', 'calorimeter, experimental results', 'Rutherford ISIS PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809007'],"[""The neutrino experiment KARMEN is situated at the beam stop neutrino source ISIS. It provides numu's, nue's and numubar's in equal intensities from the pi+ mu+ decay at rest (DAR). The oscillation channel numub->nueb is investigated in the appearance mode with a 56t liquid scintillation calorimeter at a mean distance of 17.7m from the nu source looking for p(nue,e+)n reactions. The cosmic induced background for this oscillation search could be reduced by a factor of 40 due to an additional veto counter installed in 1996. In the data collected through 1997 and 1998 no potential oscillation event was observed. Using a unified approach to small signals this leads to an upper limit for the mixing angle of sin**2(2t) < 1.3x10^{-3} (90%CL) at large Dm**2. The excluded area in (sin**2(2t),Dm**2) covers almost entirely the favored region defined by the LSND numub->nueb evidence.""]",['1998-09-10']
1701,['eng'],"['Battistoni, G']",['Study of Photo-Nuclear Interaction of muons in rock with the MACRO experiment'],['Particle Physics - Experimental Results'],"['talk, Vulcano 1998/05/25', 'muon, cosmic radiation', 'muon nucleus, interaction', 'exchange, one-photon', 'hadron, photoproduction', 'showers, hadronic', 'showers, electromagnetic', 'numerical calculations, Monte Carlo', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809006'],['We present first results about the measurement of the characteristics of charged hadrons production by atmospheric muons in the rock above MACRO. Selection criteria which allow to discriminate hadron cascades from e.m. showers generated by muons are described. A comparison between the measured rate with that expected from a Monte Carlo simulation which treats the process as dominated by photo-nuclear interaction is presented. These data can be used to validate such models aiming to the evaluation of hadron background from cosmic muons in different experimental environments.'],['1998-09-10']
1702,['eng'],"['Breitweg, J']",['ZEUS Results on the Measurement and Phenomenology of $F_2$ at Low x and Low $Q^2$'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'p, structure function', 'structure function, slope', 'momentum transfer, low', 'small-x', 'quantum chromodynamics, perturbation theory', 'nonperturbative', 'vector dominance', 'Regge poles', 'gluon, momentum spectrum', 'quark, momentum spectrum', 'quark, sea', 'cross section, energy dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'tables', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809005'],"['Measurements of the proton structure function $F_2$ for $0.6 < Q^2 < 17 {GeV}^2$ and $1.2 \\times 10^{-5} < x <1.9 \\times 10^{-3}$ from ZEUS 1995 shifted vertex data are presented. From ZEUS $F_2$ data the slopes $dF_2/d\\ln Q^2$ at fixed $x$ and $d\\ln F_2/d\\ln(1/x)$ for $x < 0.01$ at fixed $Q^2$ are derived. For the latter E665 data are also used. The transition region in $Q^2$ is explored using the simplest non-perturbative models and NLO QCD. The data at very low $Q^2$ $\\leq 0.65 {GeV}^2$ are described successfully by a combination of generalised vector meson dominance and Regge theory. From a NLO QCD fit to ZEUS data the gluon density in the proton is extracted in the range $3\\times 10^{-5} < x < 0.7$. Data from NMC and BCDMS constrain the fit at large $x$. Assuming the NLO QCD description to be valid down to $Q^2\\sim 1 {GeV}^2$, it is found that the $q\\bar{q}$ sea distribution is still rising at small $x$ and the lowest $Q^2$ values whereas the gluon distribution is strongly suppressed.']",['1998-09-08']
1703,['eng'],"['Buschbeck, Brigitte', 'Lipa, P', 'Eggers, H C']",['Multiplicity Dependence of Like-Sign and Opposite-Sign Correlations in $\\overline{p}p$ Reactions'],['Particle Physics - Experimental Results'],"['talk, Matrahaza 1998/06/14', 'anti-p p, interaction', 'hadron, multiple production', 'correlation function, two-particle', 'boson, statistics', 'charge', 'multiplicity, moment', 'multiplicity, dependence', 'numerical calculations', 'interpretation of experiments, UA1', '630 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809004'],['Discussions about Bose-Einstein correlations between decay products of coproduced W-bosons again raise the question about the behaviour of correlations if several strings are produced. This is studied by the multiplicity dependence of correlation functions of particle pairs with like-sign and opposite-sign charge in $\\bar{p}p$ reactions at $\\sqrt{s} = 630$ GeV.'],['1998-09-08']
1704,['eng'],"['Bernardini, P']",['Measurement of the Atmospheric Neutrino Induced Muon Flux with the MACRO detector'],['Particle Physics - Experimental Results'],"['talk, Vulcano 1998/05/25', 'neutrino, cosmic radiation', 'neutrino nucleon, interaction', 'charged current', 'muon, flux', 'angular distribution', 'neutrino, oscillation', 'neutrino, mass difference', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809003'],"['The flux of neutrino-induced muons has been measured with the MACRO detector. Different event topologies have been detected, due to neutrino interactions in the apparatus and in the rock below it. The upward-throughgoing muon sample is the larger one and is generated by neutrinos with an average energy of ~ 100 GeV. The observed upward-throughgoing muons are 26% fewer than expected and the zenith angle distribution does not fit with the expected one. Assuming neutrino oscillations, both measurements suggest maximum mixing and Dm2 of a few times 10-3 eV2. The other event categories due to interactions of low-energy neutrinos (average energy ~ 4 GeV) have been recently studied and the results of these new analyses are presented for the first time at this workshop. These data show a regular deficit of observed events in each angular bin, as expected assuming neutrino oscillations with maximum mixing, in agreement with the analysis of the upward-throughgoing muona sample.']",['1998-09-07']
1705,['eng'],"['Achasov, M N', 'Baru, S E', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Koshuba, S V', 'Nesterenko, I N', 'Pakhtusova, E V', 'Polunin, A A', 'Pyata, E E', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Velikzhanin, Yu S']",['Experimental study of the decay $\\phi(1020)\\to \\eta+\\gamma$ in multi-photon final state'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), branching ratio', 'four-pi-detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> eta photon', '1.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809002'],['In the SND experiment at VEPP-2M e^+e^- collider the phi(1020) ---> eta+gamma ---> 3pi^0+gamma decay was studied. The branching ratio B(phi--->eta+gamma) = (1.246 +- 0.025 +- 0.057)% was measured.'],['1998-09-15']
1706,['eng'],"['Abe, F']",['Measurement of the lepton charge asymmetry in W-boson decays produced in $p\\overline {p}$ collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'lepton, charge', 'charge, asymmetry', 'rapidity dependence', 'quark, momentum spectrum', 'quark, up', 'quark, down', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'W --> lepton neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9809001'],"['We describe a measurement of the charge asymmetry of leptons from W boson decays in the rapidity range 0<|y_l|<2.5 using W --> enu, munu events from 110+/-7 pb^{-1}of data collected by the CDF detector during 1992-95. The asymmetry data constrain the ratio of d and u quark momentum distributions in the proton over the x range of 0.006 to 0.34 at Q2 \\approx M_W^2. The asymmetry predictions that use parton distribution functions obtained from previously published CDF data in the central rapidity region (0.0<|y_l|<1.1) do not agree with the new data in the large rapidity region (|y_l|>1.1).']",['1998-09-02']
1707,['eng'],"['Belz, J E', 'Diwan, M V', 'Eckhause, M', 'Guss, C M', 'Hancock, A D', 'Heinson, A P', 'Highland, V L', 'Hoffmann, G W', 'Irwin, G M', 'Kane, J R', 'Kettell, S H', 'Kuang Yu Ping', 'Lang, K', 'McDonough, J', 'McFarlane, W K', 'Molzon, W R', 'Riley, P J', 'Ritchie, J L', 'Schwartz, A J', 'Ware, B', 'Welsh, R E', 'Winter, R G', 'Witkowski, M T', 'Wojcicki, S G', 'Worm, S D', 'Yamashita, A']",['A Compact Beam Stop for a Rare Kaon Decay Experiment'],['Detectors and Experimental Techniques'],"['K0(L), rare decay', 'K0, beam dump', 'n, shielding', 'n, flux', 'magnetic spectrometer, background', 'numerical calculations, Monte Carlo', 'Brookhaven PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808037'],"['We describe the development and testing of a novel beam stop for use in a rare kaon decay experiment at the Brookhaven AGS. The beam stop is located inside a dipole spectrometer magnet in close proximity to straw drift chambers and intercepts a high-intensity neutral hadron beam. The design process, involving both Monte Carlo simulations and beam tests of alternative beam-stop shielding arrangements, had the goal of minimizing the leakage of particles from the beam stop and the resulting hit rates in detectors, while preserving maximum acceptance for events of interest. The beam tests consisted of measurements of rates in drift chambers, scintilation counter hodoscopes, a gas threshold Cherenkov counter, and a lead glass array. Measurements were also made with a set of specialized detectors which were sensitive to low-energy neutrons, photons, and charged particles. Comparisons are made between these measurements and a detailed Monte Carlo simulation.']",['1998-09-01']
1708,['eng'],"['Abbott, B']",['Measurement of the top quark pair production cross section in $p\\overline{p}$ collisions using multijet final states'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, ((n)jet)', 'neural network', 'channel cross section', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808034'],"['We have studied tbar-t production using multijet final states in pbar-p collisions at a center-of-mass energy of 1.8 TeV, with an integrated luminosity of 110.3 pb(-1). Each of the top quarks with these final states decays exclusively to a bottom quark and a W boson, with the W bosons decaying into quark-antiquark pairs. The analysis has been optimized using neural networks to achieve the smallest expected fractional uncertainty on the tbar-t production cross section, and yields a cross section of 7.1 +/- 2.8(stat.) +/- 1.5(syst.) pb, assuming a top quark mass of 172.1 GeV/c^(2). Combining this result with previous D0 measurements, where one or both of the W bosons decay leptonically, gives a tbar t production cross section of 5.9 +/- 1.2(stat) =/- 1.1(syst) pb.']",['1998-09-01']
1709,['eng'],"['Lanou, R E']",['Future Solar Neutrino Projects'],['Detectors and Experimental Techniques'],"['talk, Takayama 1998/06/04', 'neutrino, solar', 'astrophysics', 'neutrino, energy spectrum', 'counters and detectors, proposed', 'neutrino electron, elastic scattering', 'electron, energy spectrum', 'helium, superfluid', 'calorimeter', 'drift chamber, time projection', 'scintillation counter, liquid', 'neutrino nucleus, nuclear reaction', 'ytterbium', 'lithium', 'gallium, arsenic', 'radioactivity, chemistry', 'cryogenics']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808033'],"['A review is presented of several projects under development which aim to be ""third generation"" solar neutrino detectors.']",['1998-08-31']
1710,['eng'],"['Smirnova, O G', 'Lörstad, B', 'Muresan, R']",['Tests of the JETSET Bose-Einstein correlation model in the $e^{+}e^-$ annihilation process'],['Particle Physics - Experimental Results'],"['talk, Matrahaza 1998/06/14', 'electron positron, annihilation', 'multiple production', 'correlation function, two-particle', 'boson, statistics', 'numerical calculations, Monte Carlo', 'interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808032'],"['Studies of implementation of the simulation of the Bose-Einstein correlation effects in the JETSET particle generator are performed. Analysis of dependance of the one-dimensional correlation function parameters on the presumed boson source size reveals appearance of the effective new length scale, which limits applicability of the simple momentum-shifting mechanism, employed by JETSET to simulate the Bose-Einstein correlation. Two- and three-dimensional correlation functions are analysed as well and compared to the DELPHI data.']",['1998-08-31']
1711,['eng'],"['Abbott, B']",['Measurement of the Top Quark Mass in the Dilepton Channel'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, dilepton', 'mass, truth', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808029'],"['We report a measurement of the top quark mass using six candidate events for the process pbarp->ttbar->l^+ nu l^- nubar b bbar + X, observed in the D0 experiment at the Fermilab ppbar collider. Using maximum likelihood fits to the dynamics of the decays, we measure a mass for the top quark of m(top) = 168.4 +- 12.3 (stat) +- 3.6 (syst) GeV/c^2. We combine this result with our previous measurement in the ttbar->l+jets channel to obtain m(top) = 172.1 +- 7.1 GeV/c^2 as the best value of the mass of the top quark measured by D0.']",['1998-08-28']
1712,['eng'],"['Abe, K', 'Akagi, T', 'Anthony, P L', 'Antonov, R D', 'Arnold, R G', 'Averett, T', 'Band, H R', 'Bauer, J M', 'Borel, H', 'Bosted, P E', 'Breton-Shafer, V', 'Chen, J P', 'Chupp, T E', 'Clendenin, J E', 'Comptour, C', 'Coulter, K P', 'Court, G', 'Crabb, D', 'Daoudi, J P', 'Day, D', 'Dietrich, F S', 'Dunne, J', 'Dutz, H', 'Erbacher, R D', 'Fellbaum, J', 'Fonvieille, H', 'Frlez, E', 'Garvey, D', 'Gearhart, B R', 'Gómez, J', 'Grenier, P', 'Griffioen, A', 'Høibraten, S', 'Hughes, E W', 'Hyde-Wright, C E', 'Johnson, J R', 'Kawall, D', 'Klein, A', 'Kuhn, S E', 'Kuriki, M', 'Lindgren, R', 'Liu, T J', 'Lombard-Nelsen, R M', 'Marroncle, J', 'Maruyama, T', 'Maruyama, X K', 'McCarthy, J', 'Meyer, W T', 'Meziani, Z E', 'Minehart, R C', 'Mitche, J', 'Morgenstern, J', 'Petratos, G G', 'Pitthan, R', 'Pocanic, D', 'Prescott, C', 'Prepost, R', 'Raines, P', 'Raue, B A', 'Reyna, D', 'Rijllart, A', 'Roblin, Y', 'Rochester, L S', 'Rock, S E', 'Rondon-Aramayo, O A', 'Sick, I', 'Smith, C', 'Smith, T B', 'Spengos, M', 'Staley, F', 'Steiner, P', 'Saint-Lorant, S J', 'Stuart, L M', 'Suekane, F', 'Szalata, Z M', 'Tang, H', 'Terrien, Y', 'Usher, T', 'Walz, D', 'Wesselmann, F', 'White, J L', 'Witte, K', 'Young, C C', 'Youngman, B', 'Yuta, H', 'Zapalac, G H', 'Zihlmann, B', 'Zimmermann, D M']",['Measurements of $R=\\sigma_{L}/\\sigma_{T}$ for 0.03<x<0.1 and Fit to World Data'],['Particle Physics - Experimental Results'],"['electron nucleus, elastic scattering', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'experimental results', 'SLAC Linac', '29.1 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808028'],"['Measurements were made at SLAC of the cross section for scattering 29 GeV electrons from carbon at a laboratory angle of 4.5 degrees, corresponding to 0.03<x<0.1 and 1.3<Q^2<2.7 GeV^2. Values of R=sigma_L/sigma_T were extracted in this kinematic range by comparing these data to cross sections measured at a higher beam energy by the NMC collaboration. The results are in reasonable agreement with pQCD calculations and with extrapolations of the R1990 parameterization of previous data. A new fit is made including these data and other recent results.']",['1998-08-27']
1713,['eng'],"['Frolov, V V']",['Electroproduction of the $\\Delta$ Resonance at High Momentum Transfer'],['Particle Physics - Experimental Results'],"['electron p, inelastic scattering', 'Delta(1232), electroproduction', 'Delta(1232), hadronic decay', 'pi0, angular distribution', 'form factor, transition', 'amplitude analysis, multipole', 'experimental results', 'Newport News CEBAF Linac', 'electron p --> p pi0 electron', '3.2, 4.0 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808024'],"[""We studied the electroproduction of the Delta(1232) resonance via the reaction p(e,e'p)\\pi0 at four-momentum transfers Qsq = 2.8 and 4.0 GeV^2. This is the highest Qsq for which exclusive resonance electroproduction has ever been observed. Decay angular distributions for Delta to p-pi0$ were measured over a wide range of barycentric energies covering the resonance. The $N-\\Delta$ transition form factor G*_M and ratios of resonant multipoles E{1+}/M{1+} and S{1+}/M{1+} were extracted from the decay angular distributions. These ratios remain small, indicating that perturbative QCD is not applicable for this reaction at these momentum transfers.""]",['1998-08-25']
1714,['eng'],"['Doyle, A T']",['Highlights and Open Questions from ZEUS'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'diffraction', 'jet, photoproduction', 'production, small-angle', 'production, charm', 'p, structure function', 'momentum transfer, dependence', 'event shape analysis', 'baryon, leading particle', 'upsilon mesons, photoproduction', 'neutral current', 'charged current', 'channel cross section', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808022'],"['The latest results from the ZEUS experiment, as presented at the DIS98 workshop, are reviewed. A brief introduction to the status of the experiment is given. The review focuses on three areas: multi-scale problems in QCD including results on jets, charm, the dynamics of $F_2$ at low $Q^2$, forward jets and fragmentation functions; diffractive structure including results on $\\Upsilon$ production, inclusive diffraction in DIS, event shapes and leading baryon production; and, the measurement and interpretation of the high-$Q^2$ neutral and charged current cross-sections.']",['1998-08-25']
1715,['eng'],"['Madaras, R J']",['W Boson Physics at the Fermilab Tevatron Collider'],['Particle Physics - Experimental Results'],"['talk, Frascati 1998/06/17', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, pair production', 'W, decay modes', 'W, width', 'W, mass', 'coupling, (3gauge boson)', 'channel cross section, branching ratio', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808021'],"['This talk at the XVIII International Conference on Physics in Collision, Frascati, Italy, June 17-19, 1998, presents CDF and D0 results on W and Z Boson Production Cross Sections, the W Boson Width, Rare W Boson Decays, Trilinear Gauge Boson Couplings, and the W Boson Mass.']",['1998-08-21']
1716,['eng'],[],['Exclusive Electroproduction of $\\rho^0$ and $J/\\psi$ Mesons at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, exclusive reaction', 'vector meson, electroproduction', 'vector meson, photoproduction', 'rho(770)0, hadronic decay', 'J/psi(3100), leptonic decay', 'mass spectrum, (pi+ pi-)', 'mass spectrum, (lepton+ lepton-)', 'channel cross section, energy dependence', 'momentum transfer, dependence', 'channel cross section, ratio', 'differential cross section, transverse momentum', 'differential cross section, slope', 'spin, density matrix', 'angular distribution', 'channel cross section, ratio', 'cross section, longitudinal', 'cross section, transverse', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'electron p --> p rho(770)0 electron', 'electron p --> J/psi(3100) p electron', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808020'],"['Exclusive production of $\\rho^0$ and $J/\\psi$ mesons in e^+ p collisions has been studied with the ZEUS detector in the kinematic range $0.25 < Q^2 < 50 GeV^2, 20 < W < 167 GeV$ for the $\\rho^0$ data and $2 < Q^2 < 40 GeV^2, 50 < W < 150 GeV$ for the $J/\\psi$ data. Cross sections for exclusive $\\rho^0$ and $J/\\psi$ production have been measured as a function of $Q^2, W$ and $t$. The spin-density matrix elements $r^{04}_{00}, r^1_{1-1}$ and $Re r^{5}_{10}$ have been determined for exclusive $\\rho^0$ production as well as $r^{04}_{00}$ and $r^{04}_{1-1}$ for exclusive $J/\\psi$ production. The results are discussed in the context of theoretical models invoking soft and hard phenomena.']",['1998-08-21']
1717,['eng'],"['Anikina, M K', 'Chkhaidze, L V', 'Djobava, T', 'Garsevanishvili, V R', 'Kharkhelauri, L L']",['Light-Front Analysis of $\\pi^{-}$ Mesons Produced in Mg - Mg Collisions at 4.3 A Gev/c'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'magnesium', 'pi-, hadroproduction', 'quark gluon, string model', 'nuclear reaction, temperature', 'kinematics, light front', 'transverse momentum, spectra', 'angular distribution', 'streamer chamber, experimental results', 'Dubna PS', '4.3 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808018'],['Light-front analysis of pi^{-} mesons in Mg-Mg collisions is carried out. The phase space of secondary pions is naturally divided into two parts in one of which the thermal equilibration assumption seems to be in a good agreement with data. Corresponding temperatures are extracted and compared to the results of other experiments. The experimental results have been compared with the predictions of the Quark Gluon String Model (QGSM) and satisfactory agreement between the experimental data and the model has been found.'],['1998-08-20']
1718,['eng'],"['Burrows, P N']",['Heavy quark mass effects and improved tests of the flavour independence of strong interactions'],['Particle Physics - Experimental Results'],"['review, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'strong interaction, coupling constant', 'quark, pair production', 'gluon', 'dependence, flavor', 'quantum chromodynamics, perturbation theory', 'mass, beauty', 'mass, effect', 'experimental results', 'SLAC SLC Linac', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808017'],['A review is given of latest results on tests of the flavour independence of strong interactions. Heavy quark mass effects are evident in the data and are now taken into account at next-to-leading order in QCD perturbation theory. The strong-coupling ratios alpha_s^b/alpha_s^uds and alpha_s^c/alpha_s^uds are found to be consistent with unity. Determinations of the b-quark mass m_b(M_Z) are discussed.'],['1998-08-20']
1719,['eng'],"['Kim, J H', 'Harris, D A']",['A measurement of $\\alpha_{s} Q^{2}$ from the Gross-Llewellyn Smith Sum Rule'],['Particle Physics - Experimental Results'],"['neutrino nucleon, interaction', 'nucleon, structure function', 'sum rule, Gross-Llewellyn Smith', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'momentum transfer, low', 'validity test', 'calorimeter, experimental results', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808015'],"['We extract a set of values for the Gross-Llewellyn Smith sum rule at different values of 4-momentum transfer squared ($Q^{2}$), by combining revised CCFR neutrino data with data from other neutrino deep-inelastic scattering experiments for $1 < Q^2 < 15 GeV^2/c^2$. A comparison with the order at the scale of the Z-boson mass of $0.114 \\pm^{.009}_{.012}$. This measurement provides a new and useful test of perturbative QCD at low $Q^2$, because of the low uncertainties in the higher order calculations.']",['1998-08-20']
1720,['eng'],"['Adloff, C']",['Diffractive dijet production at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, pair production', 'jet, photoproduction', 'diffraction, production', 'photon, dissociation', 'rapidity, gap', 'photon, resolved', 'quark, pair production', 'p, structure function', 'gluon, momentum spectrum', 'factorization, violation', 'transverse energy, energy flow', 'differential cross section, transverse momentum', 'exchange, pomeron', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808013'],"['Interactions of the type ep -> eXY are studied, where the component X of the hadronic final state contains two jets and is well separated in rapidity from a leading baryonic system Y. Analyses are performed of both resolved and direct photoproduction and of deep-inelastic scattering with photon virtualities in the range 7.5 < Q^2 < 80 GeV^2. Cross sections are presented where Y has mass M_Y < 1.6 GeV, the squared four-momentum transferred at the proton vertex satisfies |t| < 1 GeV^2 and the two jets each have transverse momentum p^jet_T > 5 GeV relative to the photon direction in the rest frame of X. Models based on a factorisable diffractive exchange with a gluon dominated structure, evolved to a scale set by the transverse momentum p^hat_T of the outgoing partons from the hard interaction, give good descriptions of the data. Exclusive qqbar production, as calculated in perturbative QCD using the squared proton gluon density, represents at most a small fraction of the measured cross section. The compatibility of the data with a breaking of diffractive factorisation due to spectator interactions in resolved photoproduction is investigated.']",['1998-08-18']
1721,['eng'],"['Abbott, B']",['Search for Squarks and Gluinos in Single-Photon Events with Jets and Large Missing Transverse Energy in $p \\overline {p}$ Collisions at $\\sqrt {S}=1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'jet, hadroproduction', 'jet, multiplicity', 'photon, associated production', 'squark, search for', 'gluino, search for', 'transverse energy, missing-energy', 'sparticle, mass', 'lower limit', 'sparticle, decay', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> (n)jet photon missing-energy anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808010'],"['We search for physics beyond the standard model using events with a photon, two or more hadronic jets, and an apparent imbalance in transverse energy, in $p\\bar{p}$ collisions at the Fermilab Tevatron at $\\sqrt{s}=1.8$ TeV. Such events are predicted for production of supersymmetric particles. No excess is observed beyond expected background. For the parameter space of the minimal supersymmetric standard model with branching fraction $B(\\tilde\\chi^0_2 \\to we obtain a 95% confidence level lower limit of 310 GeV for the masses of squarks and gluinos, where their masses are assumed equal.']",['1998-08-14']
1722,['eng'],"['Glenn, S']",['Gamma dipion transitions at energies near the gamma (4S)'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'upsilon mesons, electroproduction', 'Upsilon(10570), hadronic decay', 'Upsilon(10355), hadronic decay', 'Upsilon(10020), hadronic decay', 'pi, pair production', 'upsilon mesons, branching ratio', 'upper limit', 'channel cross section', 'mass spectrum, (pi+ pi- lepton+ lepton-)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Upsilon(10570)', 'electron positron --> Upsilon(10355) photon', 'electron positron --> Upsilon(10020) photon', 'Upsilon(10570) --> Upsilon(9460) pi+ pi-', 'Upsilon(10570) --> Upsilon(10020) pi+ pi-', 'Upsilon(10355) --> Upsilon(9460) pi+ pi-', 'Upsilon(10355) --> Upsilon(10020) pi+ pi-', 'Upsilon(10020) --> Upsilon(9460) pi+ pi-', '10.52-10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808008'],"['Using a data sample collected with the CLEO II detector at CESR, we have searched for dipion transitions between pairs of $\\Upsilon$ resonances at energies near the $\\Upsilon(4S)$. We obtain upper limits $B(\\Upsilon(4S)\\to the radiative processes $e^{+}e^{-} \\to \\Upsilon(3S)\\gamma$ and $e^{+}e^{-} \\to$']",['1998-08-12']
1723,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the longitudinal cross-section using the direction of the thrust axis in hadronic events at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'hadron, multiple production', 'gluon, emission', 'cross section, longitudinal', 'total cross section', 'thrust', 'angular distribution', 'cross section, ratio', 'quantum chromodynamics, validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808035'],"['In the process e+e- to hadrons, one of the effects of gluon emission is to modify the 1+cos(theta)**2 form of the angular distribution of the thrust axis, an effect which may be quantified by the longitudinal cross-section. Using the OPAL detector at LEP, we have determined the longitudinal to total cross-section ratio to be 0.0127+-0.0016+-0.0013 at the parton level, in good agreement with the expectation of QCD computed to Order(alpha_s**2) Comparisions at the hadron level with Monte Carlo models are presented. The dependence of the longitudinal cross-section on the value of thrust has also been studied, and provides a new test of QCD.']",['1998-09-01']
1724,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']","['Search for Acoplanar Lepton Pair Events in $e^{+}e^{-}$ Collisions at $\\sqrt{s}$ = 161, 172 and 183 GeV']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'transverse momentum, missing-energy', 'lepton, energy spectrum', 'W, pair production', 'W, leptonic decay', 'event shape analysis, planarity', 'new particle, search for', 'slepton, pair production', 'slepton, semileptonic decay', 'slepton, right-handed', 'slepton, mass', 'lower limit', 'channel cross section, branching ratio', 'supersymmetry', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161, 172, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808036'],"['A selection of di-lepton events with significant missing transverse momentum has been performed using a total data sample of 77.0 pb-1 at e+e- centre-of-mass energies of 161 GeV, 172 GeV and 183 GeV. The observed numbers of events: four at 161 GeV, nine at 172 GeV, and 78 at 183 GeV, are consistent with the numbers expected from Standard Model processes, which arise predominantly from W+W- production with each W decaying leptonically. This topology is an experimental signature also for the pair production of new particles that decay to a charged lepton accompanied by one or more invisible particles. Further event selection criteria are described that optimise the sensitivity to particular new physics channels. No evidence for new phenomena is apparent and model independent limits on the production cross-section times branching ratio squared for various new physics processes are presented. Assuming a 100% branching ratio for the decay of a right-handed charged slepton to a charged lepton and the lightest neutralino, we exclude at 95% CL: right-handed smuons with masses below 65 GeV for smuon - neutralino mass differences greater than 2 GeV and right-handed staus with masses below 64 GeV for stau - neutralino mass differences greater than 10 GeV. Right-handed selectrons are excluded at 95% CL for masses below 77 GeV for selectron - neutralino mass differences greater than 5 GeV within the framework of the Minimal Supersymmetric Standard Model assuming mu < -100 GeV and tan{beta} = 1.5.']",['1998-09-01']
1725,['eng'],"['Benayoun, M', 'Del Buono, L', 'Leruste, P J']",['Reconstruction and Particle Identification for a DIRC System'],['Particle Physics - Experimental Results'],"['review', 'particle identification', 'Cherenkov counter, ring imaging', 'optics, reflection', 'imaging', 'statistical analysis', 'photoelectron, amplifier']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808007'],"['We study the reconstruction and particle identification (PID) problem for Ring Imaging devices providing a good knowledge of the direction of the Cerenkov photons, as the DIRC system, on which we specialize. We advocate first the use of the stereographic projection as a tool allowing a suitable representation of the photon data, as it allows to represent the Cerenkov cone always as a circle. We set up an algorithm able to perform reliably a fit of circle arcs of small angular opening, by minimising a true Chi2 expression. The system we develop for PID relies on this algorithm and on a procedure able to remove background photons with a high efficiency. We thus show that, even when the background is large, it is possible to perform an efficient PID by means of a fit algorithm which finally provides all the circle parameters; these are connected with the charged track direction and its Cerenkov angle. It is shown that background effects can be dealt without spoiling significantly the reconstruction probability distributions.']",['1998-08-11']
1726,['eng'],"['Movilla-Fernández, P A']",['Event Shapes from JADE Data and Studies of Power Corrections'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1998/07/02', 'electron positron, annihilation', 'jet, electroproduction', 'event shape analysis', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'parametrization', 'numerical calculations, interpretation of experiments', '35-183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808005'],"['Studies of event shape observables at PETRA and LEP energies are presented. Previously published determinations of the strong coupling constant \\alpha_s at for the C parameter and improved calculations for the jet broadening variables B_T and B_W which recently became available. Furthermore, recently predicted power corrections to the differential distributions of these observables are investigated. In this study, e^+e^- data between \\sqrt{s} = 35 and 183 GeV are considered.']",['1998-08-07']
1727,['eng'],"['Strovink, M']","[""Rencontres de Moriond '98 - QCD and Hadronic Interactions""]",['Particle Physics - Experimental Results'],"['review, Les Arcs 1998/03/21', 'positron p, colliding beams', 'momentum transfer, high', 'search for, leptoquark', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'jet, associated production', 'jet, hadroproduction', 'channel cross section, ratio', 'W, transverse momentum', 'mass spectrum, transverse', 'transverse energy, missing-energy', 'transverse energy, high', 'experimental results', 'DESY HERA Stor', 'Batavia TEVATRON Coll', '((6)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808004'],"[""I discuss new experimental results reported at this conference that bear directly on three previously reported anomalies: the excess of high Q^2 events at HERA; the excess of W + 1 jet events, relative to W's without jets, in D0 data; and the excess of high E_T inclusive jets observed by CDF. The new results all point in the direction of reducing the experimental significance of these excesses.""]",['1998-08-07']
1728,['eng'],"['Abe, F']",['Measurement of the B$_{s}^{0}$ meson lifetime using semileptonic decays'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B/s0, hadroproduction', 'B/s0, semileptonic decay', 'B/s0, lifetime', 'decay, path length', 'D/s-, decay modes', 'Phi(1020)', 'K*(892)', 'mass spectrum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B/s0 --> D/s- lepton+ neutrino anything', 'D/s- --> Phi(1020) pi-', 'D/s- --> K*(892) K-', 'D/s- --> K0(S) K-', 'D/s- --> Phi(1020) muon- neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808003'],"['The lifetime of the Bs0 meson is measured using the semileptonic decay Bs0 --> Ds- l+ nu X. The data sample consists of about 110 pb^-1 of pp= collisions at sqrt{s} = 1.8 TeV collected by the CDF detector at Fermilab. Four different Ds- decay modes are reconstructed resulting in approximately 600 Ds-l+ signal events. The Bs0 meson lifetime is determined to be tau(Bs0) = (1.36 +- 0.09 +0.06-0.05) ps, where the first and second uncertainties are statistical and systematic, respectively. The Bs0 meson decay length distribution is examined for a lifetime difference Delta_Gamma/Gamma between the two mass eigenstates of the Bs0 meson. An upper limit of Delta_Gamma/Gamma < 0.83 is set at 95% confidence level.']",['1998-08-07']
1729,['eng'],"['De Angelis, A', 'Vitale, L']",['Estimating the Parameters of Bose-Einstein Correlations from the Two-Particle Correlation Function in Multihadronic Final States'],['Detectors and Experimental Techniques'],"['hadron, multiple production', 'correlation function, two-particle', 'parametrization', 'boson, statistics', 'W, pair production', 'W, hadronic decay', 'statistical analysis', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808002'],"['To estimate the strength of the Bose-Einstein correlations and the radius of the hadronization region in multiparticle production, the two-particle correlation functions $R$ for identical pairs is adjusted to a parametric function describing the enhancement at small momentum differences. This is usually done by means of a binned uncorrelated least squares fit. This article demonstrates that this procedure underestimates the statistical errors. A recipe is given to construct from the data the covariance matrix To estimate the strength of the Bose-Einstein correlations and the radius of the hadronization region in multiparticle production, the two-particle correlation functions $R$ for identical pairs is adjusted to a parametric function describing the enhancement at small momentum differences. This is usually done by means of a binned uncorrelated least squares fit. This article demonstrates that this procedure underestimates the statistical errors. A recipe is given to construct from the data the covariance matrix between the bins of the histogram of the two-particle correlation function.']",['1998-08-04']
1730,['eng'],"['Spurio, M']",['Low energy atmospheric muon neutrinos in MACRO'],['Particle Physics - Experimental Results'],"['talk, Alcala de Henares 1998/07/20', 'neutrino, cosmic radiation', 'neutrino/mu, flux', 'neutrino nucleon, interaction', 'charged current', 'muon-, angular distribution', 'neutrino, oscillation', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808001'],"['The flux of low energy neutrinos (<E_nu>~ 4 GeV) has been studied with the MACRO detector at Gran Sasso via the detection of muon neutrinos interactions inside the apparatus, and of upward-going stopping muons. Data collected in ~3 y with the full apparatus were analyzed. The results are compatible with a deficit of the flux of atmospheric muon neutrinos from below, and no reduction from above, with respect to Monte Carlo predictions. The deficit and the angular distributions are interpreted in terms of neutrino oscillations, and compared with the MACRO results on the upward throughgoing muons (<E_nu>~ 100 GeV).']",['1998-08-04']
1731,['eng'],"['Hayashi, N', 'Goto, Y', 'Saitô, N']",['RHIC Spin Physics'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'p p, interaction', 'p, polarized beam', 'p, structure function', 'structure function, spin', 'photon, direct production', 'gluon, polarization', 'W, hadroproduction', 'W, leptonic decay', 'antiquark, polarization', 'magnetic detector, PHENIX', 'proposed experiment, Brookhaven RHIC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807033'],['We describe the foreseen spin physics of the polarized proton-proton collider at RHIC. The study of the spin structure of the nucleon at RHIC is unique and complementary to the traditional polarized DIS experiments. The sensitivities of the gluon polarization measurement via prompt photon production and anti-quark polarization measurement using W production with the PHENIX detector system are reviewed.'],['1998-08-03']
1732,['eng'],"['Anastassov, A']",['First Observation of $\\Upsilon(1S)\\to \\gamma\\pi\\pi$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(9460), electroproduction', 'Upsilon(9460), radiative decay', 'mass spectrum, two-pion', 'helicity, angular distribution', 'f2(1270)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Upsilon(9460) --> pi+ pi- photon', 'Upsilon(9460) --> 2pi0 photon', '9.46 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807031'],"['We report on a study of exclusive radiative decays of the Upsilon(1S) resonance collected with the CLEO-II detector operating at CESR. We present the first observation of the radiative decays Upsilon(1S)->gamma pi+pi- and Upsilon(1S)->gamma pi0pi0. For the dipion mass regime m(pipi)>1.0 GeV, we obtain Br(Upsilon(1S)->gamma pi+pi-=(6.3+/-1.2+/-1.3) x 10^(-5), and Br(Upsilon(1S)->gamma pi0pi0=(1.7+/-0.6+/-0.3) x 10^(-5). The observed gamma pipi events are consistent with the hypothesis Upsilon(1S)->gamma f2(1270).']",['1998-07-31']
1733,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seiler, T', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['First measurement of $Z/\\gamma^{*}$ production in Compton scattering of quasi-real photons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'photon electron, Compton scattering', 'Z0, electroproduction', 'Z0, hadronic decay', 'hadron, multiple production', 'analytic properties', 'angular distribution', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> Z0 positron electron', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808030'],"['We report the first observation of Z/gamma* production in Compton scattering of quasi-real photons. This is a subprocess of the reaction e+e- to e+e-Z/gamma*, where one of the final state electrons is undetected. Approximately 55 pb-1 of data collected in the year 1997 at an e+e- centre-of-mass energy of 183 GeV with the OPAL detector at LEP have been analysed. The Z/gamma* from Compton scattering has been detected in the hadronic decay channel. Within well defined kinematic bounds, we measure the product of cross-section and Z/gamma* branching ratio to hadrons to be (0.9+-0.3+-0.1) pb for events with a hadronic mass larger than 60 GeV, dominated by (e)eZ production. In the hadronic mass region between 5 GeV and 60 GeV, dominated by (e)egamma* production, this product is found to be (4.1+-1.6+-0.6) pb. Our results agree with the predictions of two Monte Carlo event generators, grc4f and PYTHIA.']",['1998-08-28']
1734,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the average polarization of b baryons in hadronic $Z^0$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'Lambda/b0, polarization', 'Lambda/b0, semileptonic decay', 'charge correlation, (Lambda lepton)', 'lepton, energy spectrum', 'neutrino, energy spectrum', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'Lambda/b0 --> Lambda/c+ lepton- antineutrino anything', 'Lambda/c+ --> Lambda pi+ anything', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808006'],"['In the Standard Model, b quarks produced in e^+e^- annihilation at the Z^0 peak have a large average longitudinal polarization of -0.94. Some fraction of this polarization is expected to be transferred to b-flavored baryons during hadronization. The average longitudinal polarization of weakly decaying b baryons, <P_L^{\\Lambda_b}>, is measured in approximately 4.3 million hadronic Z^0 decays collected with the OPAL detector between 1990 and 1995 at LEP. Those b baryons that decay semileptonically and produce a \\Lambda baryon are identified through the correlation of the baryon number of the \\Lambda and the electric charge of the lepton. In this semileptonic decay, the ratio of the neutrino energy to the lepton energy is a sensitive polarization observable. The neutrino energy is estimated using missing energy measurements. From a fit to the distribution of this ratio, the value <P_L^{\\Lambda_b}> = -0.56^{+0.20}_{-0.13} +/- 0.09 is obtained, where the first error is statistical and the second systematic.']",['1998-08-11']
1735,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schmitz, R E', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['A Study of Parton Fragmentation in Hadronic $Z^{0}$ Decays Using $\\Lambda \\overline\\Lambda$ Correlations'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Lambda, pair production', 'final state, (2jet)', 'final state, (3jet)', 'correlation, (Lambda Antilambda)', 'rapidity, difference', 'angular distribution', 'model, fragmentation', 'string model', 'model, cluster', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> Lambda Antilambda anything', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808031'],"['The correlated production of Lambda and Lambdabar baryons has been studied using 4.3 million multihadronic Zo decays recorded with the OPAL detector at LEP. Di-lambda pairs were investigated in the full data sample and for the first time also in 2-jet and 3-jet events selected with the k_t algorithm. The distributions of rapidity differences from correlated Lambda-Lambdabar pairs exhibit short-range, local correlations and prove to be a sensitive tool to test models, particularly for 2-jet events. The JETSET model describes the data best but some extra parameter tuning is needed to improve agreement with the experimental results in the rates and the rapidity spectra simultaneously. The recently developed modification of JETSET, the MOdified Popcorn Scenarium (MOPS), and also HERWIG do not give satisfactory results. This study of di-lambda production in 2- and 3-jet events supports the short-range compensation of quantum numbers.']",['1998-08-31']
1736,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barillari, T', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bobinski, M', 'Bloodworth, Ian J', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Bürgin, R', 'Burgard, C', 'Burckhart, H J', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'de Roeck, A', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hillier, S J', 'Hill, J C', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Di-Jet Production in Photon-Photon Collisions at $\\sqrt{s}_{ee}$ = 161 and 172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'jet, pair production', 'photon, resolved', 'angular distribution', 'quantum chromodynamics, perturbation theory', 'event shape analysis', 'channel cross section, transverse energy', 'rapidity dependence', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2jet positron electron', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808027'],"[""Di-jet production is studied in collisions of quasi-real photons radiated by the LEP beams at e+e- centre-of-mass energies 161 and 172 GeV. The jets are reconstructed using a cone jet finding algorithm. The angular distributions of direct and double-resolved processes are measured and compared to the predictions of leading order and next-to-leading order perturbative QCD. The jet energy profiles are also studied. The inclusive two-jet cross-section is measured as a function of transverse energy and rapidity and compared to next-to-leading order perturbative QCD calculations. The inclusive two-jet cross-section as a function of rapidity is compared to the prediction of the leading order Monte Carlo generators PYTHIA and PHOJET. The Monte Carlo predictions are calculated with different parametrisations of the parton distributions of the photon. The influence of the `underlying event' has been studied to reduce the model dependence of the predicted jet cross-sections from the Monte Carlo generators.""]",['1998-08-27']
1737,['eng'],"['Gittelman, B']","[""An Update on CLEO's Study of B Meson Decays""]",['Particle Physics - Experimental Results'],"['review, Suzdal 1998/05/18', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, decay modes', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807030'],['This is a discussion of the main branching fractions of B Meson decays $(b\\to cW^{-})$. A summary of what has been measured and what remains unmeasured is presented.'],['1998-07-30']
1738,['eng'],"['Abbott, B']",['Small Angle $J/\\psi$ Production in $p \\overline{p}$ Collisions at $\\sqrt{s}$ =1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'J/psi(3100), hadroproduction', 'small-angle', 'J/psi(3100), leptonic decay', 'mass spectrum, dimuon', 'differential cross section, transverse momentum', 'rapidity dependence', 'model, production', 'decay, beauty', 'color, octet', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> J/psi(3100) anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807029'],['This paper presents the first measurement of the inclusive J/Psi production cross section in the forward pseudorapidity region 2.5<|eta|<3.7 in ppbar collisions at sqrt(s)=1.8TeV. The results are based on 9.8 pb-1 of data collected using the D0 detector at the Fermilab Tevatron Collider. The inclusive J/Psi cross section for transverse momenta between 1 and 16 GeV/c is compared with theoretical models of charmonium production.'],['1998-07-30']
1739,['eng'],"['Eisele, Franz']",['Nucleon Structure Functions'],['Particle Physics - Experimental Results'],"['review, Frascati 1998/06/17', 'nucleon, structure function', 'lepton nucleon, deep inelastic scattering', 'momentum spectrum, parton', 'parametrization', 'Drell-Yan process', 'lepton, pair production', 'photon, direct production', 'strong interaction, coupling constant', 'Altarelli-Parisi equation', 'quantum chromodynamics, perturbation theory', 'structure function, x-dependence', 'momentum transfer, dependence', 'small-x', 'structure function, charm', 'sum rule', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807028'],['New structure function measurements from fixed target experiments and especially HERA are reviewed. The extraction of parton distributions from these measurements is discussed with special emphasis on systematic problems. Finally the present uncertainty of our knowledge on parton distributions and on the strong coupling constant from DIS are dicussed.'],['1998-07-29']
1740,['eng'],[],['Calibration of Super-Kamiokande Using an Electron Linac'],['Detectors and Experimental Techniques'],"['neutrino, solar', 'Cherenkov counter, water', 'neutrino electron, elastic scattering', 'electron, recoil', 'calibration', 'electron, linear accelerator', 'deep underground detector, KAMIOKANDE']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807027'],"['In order to calibrate the Super-Kamiokande experiment for solar neutrino measurements, a linear accelerator (LINAC) for electrons was installed at the detector. LINAC data were taken at various positions in the detector volume, tracking the detector response in the variables relevant to solar neutrino analysis. In particular, the absolute energy scale is now known with less than 1 percent uncertainty.']",['1998-07-29']
1741,['eng'],"['Aggarwal, M M', 'Agnihotri, A', 'Ahammed, Z', 'Baba, P V K S', 'Badyal, S K', 'Bhalla, K B', 'Bhatia, V S', 'Chattopadhyay, S', 'Das, A C', 'Dutta-Majumdar, M R', 'Ganti, M S', 'Ghosh, T K', 'Sen-Gupta, S K', 'Gutbrod, H H', 'Kachroo, S', 'Kolb, B W', 'Kumar, V', 'Langbein, I', 'Mahapatra, D P', 'Mishra, G C', 'Mukhopadhyay, D S', 'Nandi, B K', 'Nayak, S K', 'Nayak, T K', 'Purschke, M L', 'Raniwala, S', 'Ramamurthy, V S', 'Rao, N K', 'Sambyal, S S', 'Sinha, B C', 'Trivedi, M D', 'Urbán, J', 'Viyogi, Y P']",['A Preshower Photon Multiplicity Detector for the WA98 Experiment'],['Detectors and Experimental Techniques'],"['nucleus nucleus, nuclear reaction', 'lead', 'photon, emission', 'photon, multiplicity', 'photon, counters and detectors', 'scintillation counter, plastics', 'scintillation counter, fibre', 'optics, transformation', 'semiconductor, optical', 'numerical calculations, Monte Carlo', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807026'],['A high granularity preshower detector has been fabricated and installed in the WA98 Experiment at the CERN SPS for measuring the spatial distribution of photons produced in the forward region in lead ion induced interactions. Photons are counted by detecting the preshower signal in plastic scintillator pads placed behind a 3 radiation length thick lead converter and applying a threshold on the scintillator signal to reject the minimum ionizing particles. Techniques to improve the imaging of the fibre and performance of the detector in the high multiplicity environment of lead-lead collisions are described. Using Monte-Carlo simulation methods and test beam data of pi- and e- at various energies the photon counting efficiency is estimated to be 68% for central and 73% for peripheral Pb+Pb collisions.'],['1998-07-29']
1742,['eng'],"['Geer, S', 'Marriner, J P', 'Ray, R', 'Streets, J', 'Wester, W C', 'Hu, M', 'Snow, G A', 'Armstrong, T A', 'Buchanan, C D', 'Corbin, B', 'Lindgren, M', 'Müller, T', 'Gustafson, R', 'Martens, M', 'Geer, S']",['Search for muonic decays of the antiproton at the Fermilab Antiproton Accumulator'],['Particle Physics - Experimental Results'],"['anti-p, semileptonic decay', 'anti-p, radiative decay', 'muon-, final state', 'anti-p, lifetime', 'lower limit', 'experimental results', 'anti-p, accumulator', 'Fermilab', 'anti-p --> meson muon-', 'anti-p --> muon- photon', 'anti-p --> muon- 2photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807025'],"['A search for antiproton decay has been made at the Fermilab Antiproton Accumulator. Limits are placed on six antiproton decay modes which contain a final-state muon. At the 90% C.L. we find that tau/B(mu gamma) > 5.0 x 10^4 yr, tau/B(mu pi0) > 4.8 x 10^4 yr, tau/B(mu eta) > 7.9 x 10^3 yr, tau/B(mu gamma gamma) > 2.3 x 10^4 yr, tau/B(mu K0S > 4.3 x 10^3 yr, and tau/B(mu K0L) > 6.5 x 10^3 yr.']",['1998-07-27']
1743,['eng'],"['Migliozzi, P']",['New results on the $\\nu_{\\mu} \\to \\nu_{\\tau}$ oscillation search with the CHORUS detector'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'neutrino, oscillation', 'neutrino/mu, beam', 'neutrino/tau', 'upper limit', 'neutrino nucleon, interaction', 'charged current', 'tau, search for', 'tau, decay modes', 'nuclear emulsion, experimental results', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807024'],"['The present results on the $\\numtonut$ oscillation search by the CHORUS experiment at CERN are summarised. A fraction of the neutrino interactions collected in 1994-1995-1996 by the CHORUS experiment has been analysed, searching for $\\nu_{\\tau}$ charged current interactions followed by the $\\tau$ lepton decay into a negative hadron or into a muon. A sample of 68,156 events with an identified final state muon and 7,206 events without an identified muon in the final state have been located in the emulsion target. Within the applied cuts, no $\\nu_{\\tau}$ candidate has been found. This result leads to a 90% C.L. limit $P(\\numtonut)< 6.0\\cdot 10^{-4}$ on the mixing probability.']",['1998-07-24']
1744,['eng'],"['Tasevsky, M']",['Jets as a Source of Information about Photon Structure'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'positron p, colliding beams', 'exchange, one-photon', 'jet, photoproduction', 'jet, pair production', 'photon, structure function', 'momentum spectrum, parton', 'differential cross section, transverse energy', 'momentum transfer, dependence', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> jet positron anything', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807023'],['A review of recent jet measurements of the photon structure from the H1 experiment at HERA. The scale and the virtuality dependence of the effective parton distribution function of the photon is discussed.'],['1998-07-24']
1745,['eng'],"['Ackerstaff, K']",['Production of $\\chi_{c2}$ Mesons in Photon-Photon Collisions at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'chi/c2(3555), photoproduction', 'chi/c2(3555), radiative decay', 'chi/c2(3555), width', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> chi/c2(3555) positron electron', 'chi/c2(3555) --> J/psi(3100) photon', 'J/psi(3100) --> lepton+ lepton-', '91, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808025'],"['We present an observation at LEP of the production of chi_c2 mesons in the collisions of two quasi-real photons using the OPAL detector. The chi_c2 mesons are reconstructed in the decay channel Chi_c2 to J/psi gamma to l+l- gamma (with l= e,mu) using all data taken at e+e- centre-of-mass energies of 91 and 183 GeV, corresponding to integrated luminosities of 167 and 55 pb-1 respectively. The two-photon width of the Chi_2 is determined to be 1.76 +- 0.47 +- 0.37 +- 0.15 keV where the first error is statistical, the second is systematic and the third comes from branching ratio uncertainties.']",['1998-08-25']
1746,['eng'],"['Ackerstaff, K']",['Search for scalar top and scalar bottom quarks at $\\sqrt {s} $ = 183 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'squark, truth', 'squark, beauty', 'squark, mass', 'lower limit', 'squark, decay', 'mass difference, (squark neutralino)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> squark anything', 'squark --> charm neutralino', 'squark --> beauty lepton sneutrino', 'squark --> beauty neutralino', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808026'],"['Searches for a scalar top quark and a scalar bottom quark have been performed using a total data sample of 56.8 pb-1 at a centre-of-mass energy of 183 GeV collected with the OPAL detector at LEP. No candidate events were observed. Combining this result with those obtained at lower centre-of-mass energies, the 95% C.L. lower limit on the scalar top quark mass is 85.0 GeV if the mixing angle between the supersymmetric partners of the left- and right-handed states of the top quark is zero. The lower limit is 81.3 GeV, even if the scalar top quark decouples from the Z boson. These limits were obtained assuming that the scalar top quark decays into a charm quark and the lightest neutralino, and that the mass difference between the scalar top quark and the lightest neutralino is larger than 10 GeV. Assuming a relatively light scalar neutrino, The complementary decay mode of the scalar top quark in which it decays into a bottom quark, a charged lepton and a scalar neutrino was also studied. From a similar analysis, a mass limit on the light scalar bottom quark was set at 82.7 GeV for a mass difference between the scalar bottom quark and the lightest neutralino larger than 7 GeV, and at 84.0 GeV for the mass difference larger 10 GeV and the lightest neutralino heavier than 30 GeV. These limits were obtained assuming that the scalar bottom quark decays into a bottom quark and the lightest neutralino, and that a mixing angle between the supersymmetric partners of the left- and right-handed states of the bottom quark is zero.']",['1998-08-26']
1747,['eng'],"['Abbiendi, G', 'Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bellerive, A', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Gaycken, G', 'Geich-Gimbel, C', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Harder, K', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kühl, T U', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mader, W F', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Surrow, B', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Tests of the Standard Model and constraints on new physics from measurements of fermion-pair production at 183 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, pair production', 'lepton, pair production', 'angular distribution, asymmetry', 'channel cross section', 'cross section, hadronic', 'coupling constant, electromagnetic interaction', 'energy dependence', 'new interaction, four-fermion interaction', 'model, composite', 'leptoquark, exchange', 'squark, exchange', 'sneutrino, exchange', 'sparticle, mass', 'supersymmetry', 'R parity, violation', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '130-136, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808023'],"['Cross-sections for hadronic, b-bbar and lepton pair final states in e+e- collisions at sqrt(s) = 183 GeV, measured with the OPAL detector at LEP, are presented and compared with the predictions of the Standard Model. Forward-backward asymmetries for the leptonic final states have also been measured. Cross-sections and asymmetries are also presented for data recorded in 1997 at sqrt(s) = 130 and 136 GeV. The results are used to measure the energy dependence of the electromagnetic coupling constant alpha_em, and to place limits on new physics as described by four-fermion contact interactions or by the exchange of a new heavy particle such as a leptoquark, or of a squark or sneutrino in supersymmetric theories with R-parity violation.']",['1998-08-25']
1748,['eng'],"['Barberis, D', 'Beusch, Werner', 'Binon, Freddy G', 'Blick, A M', 'Close, Francis Edwin', 'Danielsen, K M', 'Dolgopolov, A V', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Inyakin, A V', 'Ishida, T', 'Jacholkowski, A', 'Jacobsen, T', 'Jones, G T', 'Khaustov, G V', 'Kinashi, T', 'Kinson, J B', 'Kirk, A', 'Klempt, W', 'Kolosov, V N', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Maljukov, S', 'Martinengo, P', 'Minashvili, I A', 'Nakagawa, T', 'Norman, K L', 'Peigneux, J P', 'Polovnikov, S A', 'Polyakov, V A', 'Romanovsky, V I', 'Rotscheidt, Herbert', 'Rumyantsev, V', 'Rusakovitch, N', 'Samoylenko, V D', 'Semenov, A A', 'Sené, M', 'Sené, R', 'Shagin, P M', 'Shimizu, H M', 'Singovsky, A V', 'Sobol, A E', 'Soloviev, A S', 'Stassinaki, M', 'Stroot, J P', 'Sugonyaev, V P', 'Takamatsu, K', 'Tchlatchidze, G A', 'Tsuru, T', 'Venables, M', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the centrally produced $K^{*}(892)\\overline{K}^{*}$ and $\\phi\\omega$ systems in pp interaction at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'vector meson, pair production', 'K*(892)', 'Phi(1020)', 'omega(783)', 'vector meson, hadronic decay', 'channel cross section, mass', 'momentum transfer, dependence', 'exchange, (2pomeron)', 'transverse momentum, dependence', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p 2K*(892)', 'p p --> Phi(1020) 2p omega(783)', 'p p --> 2p K+ K- pi+ pi-', 'p p --> 2p K+ K- pi+ pi- pi0', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807021'],"['A study of the reactions pp -> pfps(K+K-pi+pi-) and pp -> pfps(K+K-pi+pi-pi0) shows evidence for the K*K* and phi omega channels respectively. The K*K* mass spectrum shows a broad distribution with a maximum near threshold and an angular analysis shows that it is compatible with having JP = 2+. The behaviour of the cross-section as a function of centre of mass energy, and the four momentum transfer dependence, are compatible with what would be expected if the K*K* system was produced via double Pomeron exchange. The dPT behaviour of the phi omega channel is similar to what has been observed for all the undisputed qqbar states. In contrast, the dPT behaviour of the K*K* final state is similar to what has been observed for the phi phi final state and for previously observed glueball candidates.']",['1998-07-22']
1749,['eng'],[],['Measurement of Elastic $\\Upsilon$ Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'photon p, exclusive reaction', 'upsilon mesons, photoproduction', 'upsilon mesons, leptonic decay', 'mass spectrum, (muon+ muon-)', 'channel cross section, branching ratio', 'energy dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> upsilon mesons photon', 'upsilon mesons --> muon+ muon-', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807020'],"['The photoproduction reaction gamma p -> mu+ mu- p has been studied in ep interactions using the ZEUS detector at HERA. The data sample corresponds to an integrated luminosity of 43.2 pb^{-1}. The Upsilon meson has been observed in photoproduction for the first time. The sum of the products of the elastic Upsilon(1S), Upsilon(2S), Upsilon(3S) photoproduction cross sections with their respective branching ratios is determined to be 13.3 +- 6.0(stat.)^{+2.7}_{-2.3}(syst.) pb at a mean photon-proton centre of mass energy of 120 GeV. The cross section is above the prediction of a perturbative QCD model.']",['1998-07-21']
1750,['eng'],"['Abbott, B']",['The Inclusive Jet Cross Section in $\\overline{p}p$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'channel cross section, transverse energy', 'quantum chromodynamics, perturbation theory', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> jet anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807018'],"['We have made a precise measurement of the central inclusive jet cross section at sqrt(s) = 1.8 TeV. The measurement is based on an integrated luminosity of 92 pb-1 collected at the Fermilab Tevatron pbar-p Collider with the D-Zero detector. The cross section, reported as a function of jet transverse energy (ET >= 60 GeV) in the pseudorapidity interval |eta| <= 0.5, is in good agreement with predictions from next-to-leading order quantum chromodynamics.']",['1998-07-20']
1751,['eng'],"['Miller, D J']",['Photon Structure and $\\gamma -\\gamma$ Physics'],['Particle Physics - Experimental Results'],"['talk, Frascati 1998/06/17', 'electron positron, colliding beams', 'photon electron, interaction', 'photon photon, interaction', 'hadron, multiple production', 'meson resonance, photoproduction', 'photon, structure function', 'quantum electrodynamics, validity test', 'quantum chromodynamics, validity test', 'momentum transfer, dependence', 'energy flow', 'small-x', 'gluon', 'transverse momentum, spectra', 'cross section, energy dependence', 'experimental results', 'CERN LEP Stor', 'Cornell CESR Stor', 'bibliography', '((3)) ((4)) ((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807017'],"['The LEP experiments are making real progress in understanding the structure of the photon, though the results do not yet give such clear demonstrations of QCD in action as the proton structure has done. Other new results are reported, including QED related effects and $\\gamma \\gamma \\to Resonances$, from LEP and from CLEO II.']",['1998-07-20']
1752,['eng'],"['Aulchenko, V M']",['First Observation of $\\phi(1020) \\to \\pi ^{0}+\\pi^{0}+\\gamma$ Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), branching ratio', 'f0(975), mass', 'quark, multiquark', 'mass spectrum, (2pi0)', 'mass spectrum, (pi0 photon)', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> 2pi0 photon', '1.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807016'],"['In the SND experiment at the VEPP-2M electron-positron collider the PHI(1020)--->PI0+PI0+GAMMA decay was studied. The branching ratio B(PHI--->PI0+PI0+GAMMA)=(1.14+-0.10+-0.12)x10^{-4} was measured. It was shown, that the F0(980)GAMMA mechanism dominates in this decay and the 4-quark model of F0(980) describes our data most consistently.']",['1998-07-20']
1753,['eng'],"['Airapetian, A']",['Measurement of the Proton Spin Structure Function $g_{1}^{p}$ with a Pure Hydrogen Target'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron p, polarized beam', 'hydrogen, polarized target', 'polarization, longitudinal', 'p, structure function', 'structure function, spin', 'x-dependence', 'cross section, asymmetry', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807015'],"['A measurement of the proton spin structure function g1p(x,Q^2) in deep-inelastic scattering is presented. The data were taken with the 27.6 GeV longitudinally polarised positron beam at HERA incident on a longitudinally polarised pure hydrogen gas target internal to the storage ring. The kinematic range is 0.021<x<0.85 and 0.8 GeV^2<Q^2<20 GeV^2. The integral Int_{0.021}^{0.85} g1p(x)dx evaluated at Q0^2 of 2.5 GeV^2 is 0.122+/-0.003(stat.)+/-0.010(syst.).']",['1998-07-17']
1754,['eng'],"['Abbott, B']",['The Dijet Mass Spectrum and a Search for Quark Compositeness in $\\overline{p}p$ Collisions at $\\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'mass spectrum, (2jet)', 'quark, composite', 'lower limit', 'rapidity, central region', 'quantum chromodynamics, perturbation theory', 'channel cross section, mass', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807014'],"['Using the DZero detector at the 1.8 TeV pbarp Fermilab Tevatron collider, we have measured the inclusive dijet mass spectrum in the central pseudorapidity region |eta_jet| < 1.0 for dijet masses greater than 200 Gev/c^2. We have also measured the ratio of spectra sigma(|eta_jet| < 0.5)/sigma(0.5 < |eta_jet| < 1.0). The order alpha_s^3 QCD predictions are in good agreement with the data and we rule out models of quark compositeness with a contact interaction scale < 2.4 TeV at the 95% confidence level.']",['1998-07-17']
1755,['eng'],"['Ackerstaff, K']",['The Flavor Asymmetry of the Light Quark Sea from Semi-inclusive Deep-inelastic Scattering'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'positron deuteron, deep inelastic scattering', 'pi, electroproduction', 'yield, (pi+ pi-)', 'quark, sea', 'asymmetry, flavor', 'x-dependence', 'momentum transfer, dependence', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', 'positron nucleon --> pi positron anything', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807013'],"['The flavor asymmetry of the light quark sea of the nucleon is determined in the kinematic range 0.02<x<0.3 and 1 GeV^2<Q^2<10 GeV^2, for the first time from semi-inclusive deep-inelastic scattering. The quantity (dbar(x)-ubar(x))/(u(x)-d(x)) is derived from a relationship between the yields of positive and negative pions from unpolarized hydrogen and deuterium targets. The flavor asymmetry dbar-ubar is found to be non-zero and x dependent, showing an excess of dbar over ubar quarks in the proton.']",['1998-07-16']
1756,['eng'],"['Chattopadhyaya, S', 'Ahammed, Z', 'Viyogi, Y P']",['Application of neural network for photon-hadron discrimination in a preshower detector in high energy heavy ion collisions'],['Detectors and Experimental Techniques'],"['scattering, heavy ion', 'lead', 'multiple production, small-angle', 'multiplicity, high', 'proportional chamber', 'particle identification, (hadron photon)', 'neural network, performance', 'preprocessing', 'numerical calculations, Monte Carlo', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807012'],"['Using a combination of a preshower detector and a charged particle veto, it is shown that the neural network method is able to provide satisfactory discrimination between photons and hadrons in the case of extremely high particle density produced in the forward region of heavy ion collisions at the LHC energy.']",['1998-07-16']
1757,['eng'],"['Abe, F']",['Search for second generation leptoquarks in the dimuon plus dijet channel of $p - \\bar{p}$ collisions at $\\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'leptoquark, search for', 'leptoquark, decay', 'final state, (2jet muon+ muon-)', 'channel cross section, upper limit', 'mass, leptoquark', 'lower limit', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2leptoquark anything', 'leptoquark --> quark muon', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810024'],"['We report on a search for second generation leptoquarks (Phi_2) using a data sample corresponding to an integrated luminosity of 110 pb^{-1} collected at the Collider Detector at Fermilab. We present upper limits on the production cross section as a function of Phi_2 mass, assuming that the leptoquarks are produced in pairs and decay into a muon and a quark with branching ratio beta. Using a Next-to-Leading order QCD calculation, we extract a lower mass limit of M_{\\Phi_2} > 202 (160) GeV$/c^{2} at 95% confidence level for scalar leptoquarks with beta=1(0.5).']",['1998-10-13']
1758,['eng'],"['Willmann, L', 'Schmidt, P V', 'Wirtz, H P', 'Abela, R', 'Baranov, V', 'Bagaturia, Yu S', 'Bertl, W', 'Engfer, R', 'Grossmann, A', 'Hughes, V W', 'Jungmann, K', 'Karpukhin, V V', 'Kisel, I V', 'Korenchenko, A S', 'Korenchenko, S M', 'Kravchuk, N', 'Kuchinskii, N A', 'Leuschner, A', 'Meyer, V', 'Merkel, J', 'Moiseenko, A', 'Mzhavia, D A', 'zu Putlitz, G', 'Reichart, W', 'Reinhard, I', 'Renker, D', 'Sakhelashvili, T M', 'Träger, K', 'Walter, H K']",['New Bounds from Searching for Muonium to Antimuonium Conversion'],['Particle Physics - Experimental Results'],"['muon+ nucleus, interaction', 'silicon, oxygen', 'muonium, production', 'muonium, transition', 'muonium, antiparticle', 'upper limit', 'violation, flavor', 'supersymmetry', 'R parity, violation', 'gauge boson, bilepton', 'mass, lower limit', 'symmetry, Z(8)', 'symmetry, left-right', 'muon-, leptonic decay', 'particle identification, (positron electron)', 'magnetic spectrometer, experimental results', 'PSI Cycl', '0.026 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807011'],"['A new upper limit for the probability of spontaneous muonium to antimuonium conversion was established at ${\\rm P_{M\\bar{M}}} \\leq 8.2 \\cdot 10^{-11}$ (90%C.L.) in 0.1~T magnetic field, which implies consequences for speculative extensions to the standard model. Coupling parameters in R-parity violating supersymmetry and the mass of a flavour diagonal bileptonic gauge boson can be significantly restricted. A Z$_8$ model with radiative mass generation through heavy lepton seed and the minimal version of 331-GUT models are ruled out.']",['1998-07-13']
1759,['eng'],[],['Measurement of the Diffractive Cross Section in Deep Inelastic Scattering using ZEUS 1994 Data'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon, diffraction', 'exchange, pomeron', 'p, diffraction', 'diffraction, structure function', 'cross section, energy dependence', 'cross section, mass', 'momentum transfer, dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807010'],"['The DIS diffractive cross section, $d\\sigma^{diff}_{\\gamma^* p \\to XN}/dM_X$, has been measured in the mass range $M_X < 15$ GeV for $\\gamma^*p$ c.m. energies $60 < W < 200$ GeV and photon virtualities $Q^2 = 7$ to 140 GeV$^2$. For fixed $Q^2$ and $M_X$, the diffractive cross section rises rapidly with $W$, $d\\sigma^{diff}_{\\gamma^*p \\to XN}(M_X,W,Q^2)/dM_X \\propto W^{a^{diff}}$ with $a^{diff} = 0.507 \\pm 0.034 (stat)^{+0.155}_{-0.046}(syst)$ corresponding to a $t$-averaged pomeron trajectory of $\\bar{\\alphapom} = 1.127 \\pm 0.009 (stat)^{+0.039}_{-0.012} (syst)$ which is larger than $\\bar{\\alphapom}$ observed in hadron-hadron scattering. The $W$ dependence of the diffractive cross section is found to be the same as that of the total cross section for scattering of virtual photons on protons. The data are consistent with the assumption that the diffractive structure function $F^{D(3)}_2$ factorizes according to $\\xpom F^{D(3)}_2 (\\xpom,\\beta,Q^2) = (x_0/ \\xpom)^n F^{D(2)}_2(\\beta,Q^2)$. They are also consistent with QCD based models which incorporate factorization breaking. The rise of $\\xpom F^{D(3)}_2$ with decreasing $\\xpom$ and the weak dependence of $F^{D(2)}_2$ on $Q^2$ suggest a substantial contribution from partonic interactions.']",['1998-07-13']
1760,['eng'],"['Ambrosio, M']",['Measurement of the energy spectrum of underground muons at Gran Sasso with a transition radiation detector'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'muon, energy spectrum', 'deep underground detector, Gran Sasso', 'transition radiation detector, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807009'],"['We have measured directly the residual energy of cosmic ray muons crossing the MACRO detector at the Gran Sasso Laboratory. For this measurement we have used a transition radiation detector consisting of three identical modules, each of about 12 m^2 area, operating in the energy region from 100 GeV to 1 TeV. The results presented here were obtained with the first module collecting data for more than two years. The average single muon energy is found to be 320 +/- 4 (stat.) +/- 11 (syst.) GeV in the rock depth range 3000-6500 hg/cm^2. The results are in agreement with calculations of the energy loss of muons in the rock above the detector.']",['1998-07-10']
1761,['eng'],[],['Measurement of inclusive $D^{*\\pm}$ and associated dijet cross sections in photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'D*(2010), photoproduction', 'D*(2010), hadronic decay', 'jet, pair production', 'photon, resolved', 'channel cross section', 'differential cross section, transverse momentum', 'differential cross section, rapidity dependence', 'quark, charm', 'massive', 'massless', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> D*(2010) anything', 'positron p --> 2jet anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807008'],"['Inclusive photoproduction of D*+- mesons has been measured for photon-proton centre-of-mass energies in the range 130 < W < 280 GeV and a photon virtuality Q^2 < 1 GeV^2. The data sample used corresponds to an integrated luminosity of 37 pb^-1. Total and differential cross sections as functions of the D* transverse momentum and pseudorapidity are presented in restricted kinematical regions and the data are compared with next-to-leading order (NLO) perturbative QCD calculations using the ""massive charm"" and ""massless charm"" schemes. The measured cross sections are generally above the NLO calculations, in particular in the forward (proton) direction. The large data sample also allows the study of dijet production associated with charm. A significant resolved as well as a direct photon component contribute to the cross section. Leading order QCD Monte Carlo calculations indicate that the resolved contribution arises from a significant charm component in the photon. A massive charm NLO parton level calculation yields lower cross sections compared to the measured results in a kinematic region where the resolved photon contribution is significant.']",['1998-07-09']
1762,['eng'],"['Movilla-Fernández, P A', 'Biebel, O', 'Bethke, Siegfried']",['Measurement of C-Parameter and Determinations of $\\alpha_{s}$ from C-Parameter and Jet Broadening at PETRA Energies'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'jet, electroproduction', 'emission, multigluon', 'quark, recoil', 'event shape analysis', 'C-parameter', 'magnetic detector, JADE', 'experimental results', 'DESY PETRA Stor', '35, 44 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807007'],"['e^+e^- annihilation data recorded by the JADE detector at PETRA were used to measure the C-parameter for the first time at sqrt{s}= 35 and 44 GeV. The distributions were compared to a resummed QCD calculation which recently became available for this observable. In addition, we applied extended resummed calculations to the heavy and wide jet broadening variables, B_T and B_W, which now include a proper treatment of the quark recoil against multi-gluon emission with single-logarithmic accuracy. We further investigated power corrections to the mean values of the observables mentioned above. In this study, we considered all available e^+e^- data between sqrt{s}= 35 and 172 GeV.']",['1998-07-09']
1763,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the Michel Parameters in Leptonic Tau Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, pair production', 'tau, leptonic decay', 'Michel parameter', 'universality, (muon electron)', 'tau, polarization', 'tau, branching ratio', 'tau, lifetime', 'model, weak interaction', 'validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808016'],"['The Michel parameters of the leptonic tau decays are measured using the OPAL detector at LEP. The Michel parameters are extracted from the energy spectra of the charged decay leptons and from their energy-energy correlations. A new method involving a global likelihood fit of Monte Carlo generated events with complete detector simulation and background treatment has been applied to the data recorded at center-of-mass energies close to sqrt(s) = M(Z) corresponding to an integrated luminosity of 155 pb-1 during the years 1990 to 1995. If e-mu universality is assumed and inferring the tau polarization from neutral current data, the measured Michel parameters are extracted. Limits on non-standard coupling constants and on the masses of new gauge bosons are obtained. The results are in agreement with the V-A prediction of the Standard Model.']",['1998-08-20']
1764,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the Strong Coupling Constant $\\alpha_s$ and the Vector and Axial-Vector Spectral Functions in Hadronic Tau Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, pair production', 'tau, semileptonic decay', 'current, vector', 'current, axial-vector', 'spectral representation', 'strong interaction, coupling constant', 'operator product expansion', 'operator, higher-dimensional', 'dimension, 6', 'dimension, 8', 'quantum chromodynamics, sum rule', 'perturbation theory', 'pi, polarizability', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', '88-94 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808019'],"['The spectral functions of the vector current and the axial-vector current have been measured in hadronic tau decays using the OPAL detector at LEP. Within the framework of the Operator Product Expansion a simultaneous determination of the strong coupling constant alpha_s, the non-perturbative operators of dimension 6 and 8 and of the gluon condensate has been performed. Different perturbative descriptions have been compared to the data. The Contour Improved Fixed Order Perturbation Theory gives alpha_s(mtau**2) = 0.348 +- 0.009 +- 0.019 at the tau-mass scale and alpha_s(mz**2) = 0.1219 +- 0.0010 +- 0.0017 at the Z-mass scale. The values obtained for alpha_s(mz**2) using Fixed Order Perturbation Theory or Renormalon Chain Resummation are 2.3% and 4.1% smaller, respectively. The running of the strong coupling between s_0 ~1.3 GeV**2 and s_0 = mtau**2 has been tested from direct fits to the integrated differential hadronic decay rate R_tau. A test of the saturation of QCD sum rules at the tau-mass scale has been performed.']",['1998-08-21']
1765,['eng'],"['Ambrosio, M']",['Observation of the Shadowing of Cosmic Rays by the Moon using a Deep Underground Detector'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'cosmic radiation, flux', 'shadowing, lunar', 'statistical analysis', 'angular resolution', 'experimental results', 'deep underground detector, MACRO']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807006'],"[""Using data collected by the MACRO experiment during the years 1989-1996, we show evidence for the shadow of the moon in the underground cosmic ray flux with a significance of 3.6 sigma. This detection of the shadowing effect is the first by an underground detector. A maximum-likelihood analysis is used to determine that the angular resolution of the apparatus is 0.9+/-0.3 degrees. These results demonstrate MACRO's capabilities as a muon telescope by confirming its absolute pointing ability and quantifying its angular resolution.""]",['1998-07-08']
1766,['eng'],"['Ambrosio, M', 'Antolini, R', 'Aramo, C', 'Auriemma, G', 'Baldini, A', 'Barbarino, G C', 'Barish, B C', 'Battistoni, G', 'Bellotti, R', 'Bemporad, C', 'Bernardini, P', 'Bilokon, H', 'Bisi, V', 'Bloise, C', 'Bower, C', 'Bussino, S', 'Cafagna, F', 'Calicchio, M', 'Campana, D', 'Carboni, M', 'Castellano, M G', 'Cecchini, S', 'Cei, F', 'Chiarella, V', 'Choudhury, B C', 'Coutu, S', 'De Benedictis, L', 'De Cataldo, G', 'Dekhissi, H', 'De Marzo, C', 'De Mitri, I', 'Derkaoui, J E', 'De Vincenzi, M', 'Di Credico, A', 'Erriquez, O', 'Fantini, R', 'Favuzzi, C', 'Forti, C', 'Fusco, P', 'Giacomelli, Giorgio', 'Giannini, G', 'Giglietto, N', 'Giorgini, M', 'Grassi, M', 'Gray, L', 'Grillo, A', 'Guarino, F', 'Guarnaccia, P', 'Gustavino, C', 'Habig, A', 'Hanson, K', 'Hawthorne, A', 'Heinz, R', 'Huang, Y', 'Iarocci, Enzo', 'Katsavounidis, E', 'Katsavounidis, E', 'Kearns, E T', 'Kim, H', 'Kyriazopoulou, S', 'Lamanna, E', 'Lane, C', 'Levin, D S', 'Lipari, P', 'Longley, N P', 'Longo, M J', 'Maaroufi, F', 'Mancarella, G', 'Mandrioli, G', 'Manzoor, S', 'Margiotta-Neri, A', 'Marini, A', 'Martello, D', 'Marzari-Chiesa, A', 'Mazziotta, M N', 'Mazzotta, C', 'Michael, D G', 'Mikheyev, S P', 'Miller, L', 'Monacelli, P', 'Montaruli, T', 'Monteno, M', 'Mufson, S L', 'Musser, J', 'Nicoló, D', 'Nolty, R', 'Okada, C', 'Orth, C', 'Osteria, G', 'Ouchrif, M', 'Palamara, O', 'Patera, V', 'Patrizii, L', 'Pazzi, R', 'Peck, C W', 'Petrera, S', 'Pistilli, P', 'Popa, V', 'Pugliese, V', 'Rainó, A', 'Reynoldson, J', 'Ronga, F', 'Rubizzo, U', 'Sanzgiri, A', 'Satriano, C', 'Satta, L', 'Scapparone, E', 'Scholberg, K', 'Sciubba, A', 'Serra-Lugaresi, P', 'Severi, M', 'Sioli, M', 'Sitta, M', 'Spinelli, P', 'Spinetti, M', 'Spurio, M', 'Steinberg, R', 'Stone, J L', 'Sulak, Lawrence R', 'Surdo, A', 'Tarlé, G', 'Togo, V', 'Ugolotti, D', 'Vakili, M', 'Walter, C W', 'Webb, R']",['Measurement of the atmospheric neutrino-induced upgoing muon flux using MACRO'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'neutrino nucleon, interaction', 'charged current', 'muon, flux', 'angular dependence', 'neutrino, oscillation', 'neutrino/mu', 'neutrino/tau', 'neutrino, mass difference', 'neutrino, mixing angle', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807005'],"['We present a measurement of the flux of neutrino-induced upgoing muons (<E_nu>~100 GeV) using the MACRO detector.The ratio of the number of observed to expected events integrated over all zenith angles is 0.74 +/- 0.036 (stat) +/- 0.046(systematic) +/- 0.13 (theoretical). The observed zenith distribution for -1.0 < cos(theta) < -0.1 does not fit well with the no oscillation expectation, giving a maximum probability for chi^2 of 0.1%. The acceptance of the detector has been extensively studied using downgoing muons, independent analyses and Monte-Carlo simulations. The other systematic uncertainties cannot be the source of the discrepancies between the data and expectations. We have investigated whether the observed number of events and the shape of the zenith distribution can be explained by a neutrino oscillation hypothesis. Fitting either the flux or zenith distribution independently yields mixing parameters of sin^2 (2theta)=1.0 and delta m^2 of a few times 10^-3 eV^2. However, the observed zenith distribution does not fit well with any expectations giving a maximum probability for chi^2 of 5% for the best oscillation hypothesis, and the combined probability for the shape and number of events is 17%. We conclude that these data favor a neutrino oscillation hypothesis, but with unexplained structure in the zenith distribution not easily explained by either the statistics or systematics of the experiment.']",['1998-12-03']
1767,['eng'],"['Fukuda, Y']",['Evidence for oscillation of atmospheric neutrinos'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'neutrino, oscillation', 'neutrino/e, flux', 'neutrino/mu, flux', 'neutrino/tau', 'flux, ratio', 'neutrino nucleon, interaction', 'charged current', 'yield, (muon electron)', 'neutrino, mass difference', 'neutrino, mixing angle', 'Cherenkov counter, water', 'experimental results', 'deep underground detector, KAMIOKANDE']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807003'],"['We present an analysis of atmospheric neutrino data from a 33.0 kiloton-year (535-day) exposure of the Super-Kamiokande detector. The data exhibit a zenith angle dependent deficit of muon neutrinos which is inconsistent with expectations based on calculations of the atmospheric neutrino flux. Experimental biases and uncertainties in the prediction of neutrino fluxes and cross sections are unable to explain our observation. The data are consistent, however, with two-flavor nu_mu <-> nu_tau oscillations with sin^2(2theta)>0.82 and 5x10^-4 < delta m^2 < 6x10^-3 eV^2 at 90% confidence level.']",['1998-07-06']
1768,['eng'],"['Singh, P P']",['Discovery of the $B_{c}$ Meson'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1998/03/01', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B/c, hadroproduction', 'B/c, semileptonic decay', 'B/c, mass', 'B/c, lifetime', 'channel cross section, branching ratio', 'mass spectrum, (J/psi(3100) lepton)', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B/c --> J/psi(3100) lepton neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807022'],['This paper reports on the discovery of the B_c meson.'],['1998-07-23']
1769,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for Higgs bosons and new particles decaying into two photons at $\\sqrt{s}$ = 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'Higgs particle, radiative decay', 'scalar particle, radiative decay', 'photon, pair production', 'Z0, associated production', 'Higgs particle, associated production', 'fermion, pair production', 'final state, (fermion antifermion 2photon)', 'mass spectrum, two-photon', 'channel cross section, branching ratio', 'upper limit', 'Higgs particle, mass', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '183 GeV-cms']","['http://www.cern.ch/Opal/pubs/paper/html/pr244.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808014']","['A search for the resonant production of high mass photon pairs associated with a leptonic or hadronic system has been performed using a data sample of 57.7 pb-1 collected at an average center-of-mass energy of 182.6 GeV with the OPAL detector at LEP. No evidence for contributions from non-Standard Model physics processes was observed. The observed candidates are used to place limits on BR (H to gamma gamma) assuming a Standard Model production rate for Higgs boson masses up to 92 GeV, and on the production cross section for a scalar resonance decaying into di-photons up to a mass of 170 GeV. Upper limits on the product of cross section and branching ratios, sigma(e+e- to XY) * BR(X to gamma gamma) * BR(Y to f fbar) as low as 70fb are obtained over the M(X) range 10 - 170 GeV for the case where 10 < M(Y) < 160 GeV and M(X)+M(Y) > 90 GeV, independent of the nature of Y provided it decays to a fermion pair and has negligible width. Higgs scalars which couple only to gauge bosons at Standard Model strength are ruled out up to a mass of 90.0 GeV at the 95% confidence level. Limits are also placed on non-minimal Higgs sectors having triplet representations.']",['1998-08-19']
1770,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Multi-photon production in $e^{+}e^{-}$ collisions at $\\sqrt{s}$= 183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'photon, multiple production', 'mass spectrum, two-photon', 'final state, (3photon)', 'resonance, search for', 'resonance, radiative decay', 'photon, angular distribution', 'quantum electrodynamics, Lambda parameter', 'electron, excited state', 'mass, lower limit', 'channel cross section, branching ratio', 'mass, dependence', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2photon', 'electron positron --> 3photon', '183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808012'],"['The process e+e- to gamma gamma (gamma) is studied using data recorded with the OPAL detector at LEP. The data sample corresponds to a total integrated luminosity of 56.2 pb-1 taken at a centre-of-mass energy of 183 GeV. The measured cross-section agrees well with the expectation from QED. A fit to the angular distribution is used to obtain improved limits at 95% CL on the QED cut-off parameters: Lambda+ > 233 GeV and Lambda- > 265 GeV as well as a mass limit for an excited electron, M(e*) > 227 GeV assuming equal e*egamma and eegamma couplings. No evidence for resonance production is found in the invariant mass spectrum of photon pairs. Limits are obtained for the cross-section times branching ratio for a resonance decaying into two photons.']",['1998-08-18']
1771,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wiesler, T', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Inclusive production of charged hadrons and $K_{s}^{0}$ mesons in photon-photon collisions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'charged particle, photoproduction', 'K0(S), photoproduction', 'hadron, multiple production', 'differential cross section, transverse momentum', 'differential cross section, rapidity dependence', 'quantum chromodynamics, perturbation theory', 'hard scattering', 'photon, resolved', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tables', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808009'],['The production of charged hadrons and K_s mesons in the collisions of quasi-real photons has been measured using the OPAL detector at LEP. The data were taken at e+e- centre-of-mass energies of 161 and 172 GeV. The differential cross-sections as a function of the transverse momentum and the pseudorapidity of the charged hadrons and K_s mesons have been compared to the leading order Monte Carlo simulations of PHOJET and PYTHIA and to perturbative next-to-leading order (NLO) QCD calculations. The distributions have been measured in the range 10-125 GeV of the hadronic invariant mass W. By comparing the transverse momentum distribution of charged hadrons measured in gamma-gamma interactions with gamma-proton and meson-proton data we find evidence for hard photon interactions in addition to the purely hadronic photon interactions.'],['1998-08-14']
1772,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Stumpf, L', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of Tau Branching Ratios to Five Charged Hadrons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, pair production', 'tau-, semileptonic decay', 'final state, (5charged particle)', 'tau-, branching ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau- --> 2hadron+ 3hadron- neutrino/tau', 'tau- --> 2hadron+ 3hadron- pi0 neutrino/tau', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9808011'],['The branching ratios of the decay of the tau lepton to five charged hadrons have been measured with the OPAL detector at LEP using data collected between 1991 and 1995 at e+e- centre-of-mass energies close to the Z resonance. The branching ratios are measured to be BR(tau- to 3h-2h+nutau) = 0.091+-0.014+-0.005% BR(tau- to 3h-2h+pi0nutau) = 0.027+-0.018+-0.007% where the first error is statistical and the second systematic.'],['1998-07-28']
1773,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurements of flavour dependent fragmentation functions in $Z^{0} \\to q\\overline{q}$ events'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, fragmentation function', 'dependence, flavor', 'particle identification, flavor', 'D*(2010), hadronic decay', 'track data analysis, vertex', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ep-98-089', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807004']","['Fragmentation functions for charged particles in Z -> qq(bar) events have been measured for bottom (b), charm (c) and light (uds) quarks as well as for all flavours together. The results are based on data recorded between 1990 and 1995 using the OPAL detector at LEP. Event samples with different flavour compositions were formed using reconstructed D* mesons and secondary vertices. The \\xi_p = ln(1/x_E) distributions and the position of their maxima \\xi_max are also presented separately for uds, c and b quark events. The fragmentation function for b quarks is significantly softer than for uds quarks.']",['1998-07-07']
1774,['eng'],"['Bai, J Z']",['Study of the P-wave charmonium state $\\chi_{cJ}$ in $\\psi(2S)$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), radiative decay', 'chi mesons, charm', 'chi mesons, hadronic decay', 'pi, pair production', 'K, pair production', 'p, pair production', 'mass spectrum', 'chi/c0(3415), width', 'chi/c0(3415), branching ratio', 'magnetic detector, BES', 'experimental results', 'Beijing Stor', 'psi(3685) --> chi/c0(3415) photon', 'electron positron --> pi+ pi- photon', 'electron positron --> K+ K- photon', 'electron positron --> p anti-p photon', '3.7 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807001'],"['The processes $\\psi(2S)\\to \\gamma \\pi^+ \\pi^-$, $\\gamma K^+ K^-$ and $\\gamma p \\bar{p}$ have been studied using a sample of $3.7 \\times 10^6$ produced measurement of the branching fraction $B(\\chi_{c0} \\to p \\bar{p}) = (16.3 \\pm 4.4 \\pm 5.4)\\times 10^{-5}$, where the first error is statistical and the second one systematic. Branching fractions of $\\chi_{c0,2} \\to \\pi^+ \\pi^-$ and $K^+ K^-$ are also reported.']",['1998-07-02']
1775,['eng'],"['Hatakeyama, S']",['Measurement of the flux and zenith-angle distribution of upward through-going muons in Kamiokande II+III'],['Particle Physics - Experimental Results'],"['muon, flux', 'angular dependence', 'neutrino/mu, cosmic radiation', 'neutrino nucleon, interaction', 'charged current', 'Cherenkov counter, water', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806038'],"['The flux of upward through-going muons of minimum (mean) threshold energy > 1.6 (3.0) GeV is measured, based on a total of 372 events observed by the Kamiokande II+III detector during 2456 detector live days. The observed muon flux was (1.94+-0.10(stat.)+0.07-0.06(sys.))*10^-13 /cm^2/s/sr, which is compared to an expected value of (2.46+-0.54(theo.))*10^-13/cm^2/s/sr. The observation is in agreement with the prediction within the errors. The zenith angle dependence of the observed upward through-going muons supports the previous indication of neutrino oscillations made by Kamiokande using sub- and multi-GeV atmospheric neutrino events.']",['1998-07-01']
1776,['eng'],"['Akhmadaliev, S Z', 'Kezerashvili, G Ya', 'Klimenko, S G', 'Malyshev, V M', 'Maslennikov, A M', 'Milov, A M', 'Milshtein, A I', 'Muchnoi, N Yu', 'Naumenkov, A I', 'Panin, V S', 'Peleganchuk, S V', 'Popov, V G', 'Pospelov, M E', 'Protopopov, I Ya', 'Romanov, L V', 'Shamov, A G', 'Shatilov, D N', 'Simonov, E A', 'Tikhonov, Yu A']",['Delbrück scattering at energies 140/450 MeV'],['Particle Physics - Experimental Results'],"['photon nucleus, elastic scattering', 'crystal, bismuth-germanate', 'intermediate state, (positron electron)', 'scattering, Delbrueck', 'differential cross section, momentum transfer', 'background, Compton scattering', 'photon, angular distribution', 'energy spectrum', 'calorimeter, experimental results', 'Novosibirsk Stor4', '0.14-0.45 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806037'],"['The differential cross section of Delbrück scattering is measured on a bismuth germanate $Bi_4Ge_3O_{12}$ target at photon energies $140 - 450 MeV$ and scattering angles $2.6 - 16.6 mrad$. A good agreement with the theoretical results, obtained exactly in a Coulomb field, is found.']",['1998-06-30']
1777,['eng'],"['Kulchitskii, Yu A', 'Vinogradov, V B']",['Analytical Representation of the Longitudinal Hadronic Shower Development'],['Detectors and Experimental Techniques'],"['showers, hadronic', 'hadron, multiple production', 'spatial distribution', 'parametrization', 'calorimeter, scintillation counter']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903019'],"['The analytical representation of the longitudinal hadronic shower development from the face of a calorimeter is presented and compared with experimental data. The suggested formula is particularly useful at designing, testing and calibration of huge calorimeter complex like in ATLAS at LHC.']",['1999-03-15']
1778,['eng'],"['Abe, F']",['Searches for New Physics in Diphoton Events in $p\\overline{p}$ collisions at $\\sqrt{s} = 1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'photon, pair production', 'jet, associated production', 'lepton, associated production', 'photon, associated production', 'quark, beauty', 'transverse energy, missing-energy', 'electroweak interaction, validity test', 'jet, multiplicity', 'new interaction, search for', 'supersymmetry', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2photon anything', 'anti-p p --> electron positron 2photon anything', 'anti-p p --> (n)jet 2photon anything', 'anti-p p --> beauty 2photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806034'],"['We present a detailed description of a search for anomalous production of missing E$_{\\rm T}$ ($\\mett$), jets, leptons ($e, \\mu, \\tau$), $b$-quarks, or additional photons in events containing two isolated, central consistent with standard model expectations, with the possible exception of one event that has in addition to the two photons a central electron, a high-E$_{\\rm T}$ electromagnetic cluster, and large $\\mett$. We set limits using two specific SUSY scenarios for production of diphoton events with']",['1998-06-29']
1779,['eng'],"['Yu, J']",['DIS Prospects at the Future Muon Collider Facility'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'muon+ muon-, storage ring', 'storage ring, proposed', 'muon- p, deep inelastic scattering', 'neutrino, secondary beam', 'neutrino nucleon, deep inelastic scattering', 'nucleon, structure function', 'small-x', 'Weinberg angle', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806033'],"['We discuss prospects of deep inelastic scattering physics capabilities at the future muon collider facility. In addition to mu^+ mu^- collider itself, the facility provides other possibilities. Among the possibilities, we present muon-proton collider and neutrino fixed target programs at the muon collider facility. This mu-p collider program extends kinematic reach and luminosity by an order of magnitude, increasing the possibility of search for new exotic particles. Perhaps most intriguing DIS prospects come from utilizing high intensity neutrino beam resulting from continuous decays of muons in various sections of the muon collider facility. One of the most interesting findings is a precision measurement of electroweak mixing angle, sin^2theta_W, which can be achieved to the precision equivalent to delta M_W ~ 30 MeV.']",['1998-06-26']
1780,['eng'],"['Yu, J']",['Precision Measurement of $sin^{2}\\theta_{W}$ from $\\nu-N$ Scattering at NuTeV and Direct Measurements of $M_{W}$'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'neutral current', 'charged current', 'cross section, ratio', 'Weinberg angle', 'W, mass', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'mass spectrum, transverse', 'experimental results', 'Batavia TEVATRON PS', 'Batavia TEVATRON Coll', '((4)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806032'],"['We present the preliminary result of sin^2theta_W from nu-N deep inelastic scattering experiment, NuTeV, at Fermilab. This measurement of sin^2theta_W comes from measuring the Paschos-Wolfenstein parameter R-=sigma_NC^nu-sigma_NC^nubar/(sigma_CC^{nu}-sigma_CC^nubar), using separate beams of nu and nubar, utilizing the SSQT. The resulting value of sin^2\\theta_W^(on-shell) is $0.2253\\pm0.0019(stat)\\pm0.0010(syst)$. This value is equivalent to the mass of the W boson, M_W=80.26\\pm0.11 GeV/c^2. We also summarize the direct measurements of M_W from the Tevatron pbar-p collider experiments, DØ and CDF. Combining these two direct measurements yields M_W=80.37\\pm0.08 GeV/c^2.']",['1998-06-26']
1781,['eng'],"['Yu, J']",['Recent QCD results in $\\nu-N$ Deep Inelastic Scattering at CCFR/NuTeV'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'neutrino/mu', 'beryllium, oxygen', 'quantum chromodynamics, perturbation theory', 'strong interaction, coupling constant', 'sum rule, Gross-Llewellyn-Smith', 'nucleon, structure function', 'x-dependence', 'nucleon, strangeness', 'quark, sea', 'quark, charm', 'quark, neutrinoproduction', 'nuclear model', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806031'],"['We present recent QCD results in nu-N scattering at the Fermilab CCFR/NuTeV experiments. We present the latest Next-to-Next-Leading order strong coupling constant, alpha-s, extracted from Gross-Llewellyn-Smith sum rule. The value of alpha-s from this measurement, at the mass of Z boson, is alpha-s^{NNLO}(M_Z**2)=0.114^{+0.009}_{-0.012}. We also present a preliminary result of the CCFR F_2 at large-x. This measurement of F_2 is compared to other experiments and various models that provide nuclear effects. We discuss the previous strange sea quark measurement from the CCFR experiment and the prospects for improvements of the measurement in the NuTeV experiment.']",['1998-06-26']
1782,['eng'],"['Yu, J']",['Strange Sea and $\\alpha_{s}$ Measurements from $\\nu-N$ Deep Inelastic Scattering at CCFR/NuTeV'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1998/03/21', 'neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'neutrino/mu', 'beryllium, oxygen', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'sum rule, Gross-Llewellyn-Smith', 'nucleon, strangeness', 'quark, sea', 'quark, charm', 'quark, neutrinoproduction', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806030'],"['We present the latest Next-to-Next-Leading order strong coupling constant, alpha-s, extracted from Gross-Llewellyn-Smith sum rule. The value of alpha-s from this measurement, at the mass of Z boson, is alpha-s^{NNLO}(M_Z**2)=0.114^{+0.009}_{-0.012}. We discuss the previous strange sea quark measurement from the CCFR experiment and the prospects for improvements of the measurement in the NuTeV experiment.']",['1998-06-26']
1783,['eng'],"['Adloff, C']",['Dijet Event Rates in Deep-Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'small-x', 'jet, pair production', 'yield, (2jet)', 'transverse energy, energy flow', 'dependence, momentum transfer', 'transverse momentum, high', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'photon, resolved', 'color, dipole', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806029'],"['Di-jet event rates have been measured for deep-inelastic scattering in the kinematic domain ~5 < Q^2 < ~100 GeV^2 and ~10^(-4) < x_Bj < ~10^(-2), and for jet transverse momenta squared p_t^2 > ~Q^2. The analysis is based on data collected with the H1 detector at HERA in 1994 corresponding to an integrated luminosity of about 2 pb^(-1). Jets are defined using a cone algorithm in the photon-proton centre of mass system requiring jet transverse momenta of at least 5 GeV. The di-jet event rates are shown as a function of Q^2 and x_Bj. Leading order models of point-like interacting photons fail to describe the data. Models which add resolved interacting photons or which implement the colour dipole model give a good description of the di-jet event rate. This is also the case for next-to-leading order calculations including contributions from direct and resolved photons.']",['1998-06-26']
1784,['eng'],"['Adloff, C']",['Differential (2+1) Jet Event Rates and Determination of $\\alpha_{s}$ in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'yield, (3jet)', 'jet, particle identification', 'correction, hadronization', 'counters and detectors, effect', 'quantum chromodynamics, perturbation theory', 'strong interaction, coupling constant', 'renormalization, dependence', 'dependence, factorization', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806028'],"['Events with a (2+1) jet topology in deep-inelastic scattering at HERA are studied in the kinematic range 200 < Q^2< 10,000 GeV^2. The rate of (2+1) jet events has been determined with the modified JADE jet algorithm as a function of the jet resolution parameter and is compared with the predictions of Monte Carlo models. In addition, the event rate is corrected for both hadronization and detector effects and is compared with next-to-leading order QCD calculations. A value of the strong coupling constant of alpha_s(M_Z^2)= 0.118+- 0.002 (stat.)^(+0.007)_(-0.008) (syst.)^(+0.007)_(-0.006) (theory) is extracted. The systematic error includes uncertainties in the calorimeter energy calibration, in the description of the data by current Monte Carlo models, and in the knowledge of the parton densities. The theoretical error is dominated by the renormalization scale ambiguity.']",['1998-06-26']
1785,['eng'],"['Bourilkov, D']",['Fermion-pair Production above the Z and Search for New Phenomena'],['Particle Physics - Experimental Results'],"['review, Les Arcs 1997/03/15', 'electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'quark, pair production', 'angular distribution, asymmetry', 'new interaction, search for', 'model, composite', 'sparticle, exchange', 'R parity, violation', ""Z'"", 'electroweak interaction, validity test', 'experimental results', 'CERN LEP Stor', '130-183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806027'],"[""A review of the measurements of hadron, flavour-tagged and lepton-pair production cross-sections and lepton-pair forward-backward asymmetries performed by the four LEP experiments ALEPH, DELPHI, L3 and OPAL at energies between 130 and 183 GeV is given. All 183 GeV results are preliminary. The searches by the four collaborations for new physics phenomena like contact interactions and compositeness, exchange of R-parity violating sneutrinos or squarks, leptoquarks or additional heavy gauge bosons Z' are summarized. No evidence for deviations from the Standard Model expectations is found and new or improved limits are derived.""]",['1998-06-26']
1786,['eng'],"['Abe, F']",['Measurement of the $B^{0}_{d} - \\overline{B}^{0}_{d}$ flavor oscillation frequency and study of same side flavor tagging of $B$ mesons in $p\\overline{p}$ collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, oscillation', 'particle identification, flavor', 'B0, semileptonic decay', 'B, hadronic decay', 'B0, mass difference', 'charge correlation, flavor', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'B0 --> charmed meson lepton neutrino', 'B0 --> J/psi(3100) K*(892)', 'B+ --> J/psi(3100) K+', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806026'],"[""$B^0_d$-$\\bar{B}{}^0_d$ oscillations are observed in ``self-tagged'' samples of partially reconstructed $B$ mesons decaying into a lepton and a charmed meson collected in $p\\bar p$ collisions at $\\sqrt{s} = 1.8$ TeV. A flavor tagging technique is employed which relies upon the correlation between the flavor of $B$ mesons and the charge of nearby particles. We measure the flavor oscillation frequency to be $\\Delta m_d = 0.471 ^{+0.078}_{-0.068} \\pm 0.034 ps^{-1}$. The tagging method is also demonstrated in exclusive samples of $B^+_u \\to J/\\psi K^+$ and $B^0_d \\to J/\\psi K^{*0}(892)$, where similar flavor-charge correlations are observed. The tagging characteristics of the various samples are compared with each other, and with Monte Carlo simulations.""]",['1998-06-26']
1787,['eng'],"['Abe, F']",['Measurement of the CP-Violation Parameter sin$(2\\beta)$ in $B^{0}_{d}/\\overline{B}^{0}_{d} \\rightarrow J/\\psi K^{0}_{S}$ Decays'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0, hadronic decay', 'anti-B0, hadronic decay', 'asymmetry, time dependence', 'violation, CP', 'particle identification, flavor', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B0 --> J/psi(3100) K0(S)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806025'],['We present a measurement of the time-dependent asymmetry in the rate for Standard Model this is interpreted as a measurement of the CP-violation parameter $\\sin(2\\beta)$. A total of $198\\pm 17$ $B^0_d/\\bar{B}{^0_d}$ decays were observed in $p\\bar{p}$ collisions at $\\sqrt{s} = 1.8$ TeV by the CDF detector at the Fermilab Tevatron. The initial $b$-flavor is determined by a same side flavor tagging technique. Our analysis results in $\\sin(2\\beta) = 1.8\\pm 1.1(stat)\\pm 0.3(syst)$.'],['1998-06-25']
1788,['eng'],"['Armbruster, B', 'Blair, I M', 'Bodmann, B A', 'Booth, N E', 'Drexlin, G', 'Eberhard, V', 'Edgington, J A', 'Eichner, C', 'Eitel, K', 'Finckh, E', 'Gemmeke, H', 'Hössel, J G', 'Jannakos, T', 'Jünger, P', 'Kleifges, M', 'Kleinfeller, J', 'Kretschmer, W', 'Maschuw, R', 'Oehler, C', 'Plischke, P', 'Rapp, J', 'Ruf, C', 'Steidl, M', 'Stumm, O', 'Wolf, J', 'Zeitnitz, B']",['Measurement of the energy spectrum of $\\nu_{e}$ from muon decay and implications for the Lorentz structure of the weak interaction'],['Particle Physics - Experimental Results'],"['muon+, secondary beam', 'muon+, leptonic decay', 'neutrino/e, energy spectrum', 'neutrino/e, flux', 'neutrino nucleus, nuclear reaction', 'carbon', 'charged current', 'coupling constant, scalar', 'coupling constant, tensor', 'model, weak interaction', 'Michel parameter', 'calorimeter, experimental results', 'Rutherford ISIS PS', '0.8 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806024'],"['The KARMEN experiment uses the reaction 12C(\\nu_e,e-)12N to measure the energy distribution of \\nu_e emitted in muon decay at rest. The \\nu_e analog maximum-likelihood analysis of events near the kinematic end point, E_max. The result, ømega_l = (2.7^{+3.8}_{-3.3}\\pm 3.1) * 10^{-2}, is in good agreement with the standard model prediction ømega_l= 0. We deduce a 90% confidence upper limit of ømega_l <= 0.113, which corresponds to a limit of |g^S_RL + 2 g^T_RL| <= 0.78 on the interference term between scalar and tensor coupling constants.']",['1998-06-25']
1789,['eng'],"['Yang, U K', 'McNulty, C', 'Arroyo, C G', 'Bazarko, A O', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Budd, H S', 'Conrad, J', 'Harris, D A', 'Johnson, R A', 'Kim, J H', 'King, B J', 'Kinnel, T', 'Lamm, M J', 'Lefmann, W C', 'Marsh, W', 'McFarland, K S', 'Mishra, S R', 'Naples, D', 'Quintas, P Z', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Sciulli, F J', 'Seligman, W G', 'Shaevitz, M H', 'Smith, W H', 'Spentzouris, P', 'Stern, E G', 'Vakili, M']",['Measurements of the longitudinal structure function and |$V_{cs}$| in the CCFR experiment'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'neutrino nucleon, interaction', 'antineutrino nucleon, interaction', 'charged current', 'nucleon, structure function', 'structure function, longitudinal', 'structure function, transverse', 'structure function, ratio', 'gluon, momentum spectrum', 'x-dependence', 'momentum transfer, dependence', 'Kobayashi-Maskawa angle', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806023'],"['Measurements of charged current neutrino and anti-neutrino nucleon interactions in the CCFR detector are used to extract the structure functions, F_2, xF_3(nu), xF_3(nubar) and R(longitudinal) in the kinematic region 0.01<x<0.6 and 1<Q^2<300 GeV^2. The new measurements of R in the x<0.1 region provide a constraint on the level of the gluon distribution. The x and Q^2 dependence of R is compared with a QCD based fit to previous data. The CKM matrix element |V_cs| is extracted from a combined analysis of xF_3 and dimuon data.']",['1998-06-25']
1790,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Bose-Einstein correlations of three charged pions in hadronic $Z^{0}$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'correlation, (3pi+)', 'correlation, (3pi-)', 'boson, statistics', 'correction, Coulomb', 'pi, particle source', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806036'],"['Bose-Einstein Correlations (BEC) of three identical charged pions were studied in 4 x 10^6 hadronic Z^0 decays recorded with the OPAL detector at LEP. The genuine three-pion correlations, corrected for the Coulomb effect, were separated from the known two-pion correlations by a new subtraction procedure. A significant genuine three-pion BEC enhancement near threshold was observed having an emitter source radius of r_3 = 0.580 +/- 0.004 (stat.) +/- 0.029 (syst.) fm and a strength of \\lambda_3 = 0.504 +/- 0.010 (stat.) +/- 0.041 (syst.). The Coulomb correction was found to increase the \\lambda_3 value by 0.707 +/- 0.014 (stat.) +/- 0.078 (syst.) when one takes into account the three-pion sample purity. A relation between the two-pion and the three-pion source parameters is discussed.']",['1998-06-30']
1791,['eng'],"['Dorigo, T']",['Observation of Z Decays to b Quark Pairs at the Tevatron Collider'],['Particle Physics - Experimental Results'],"['talk, Vancouver 1998/07/23', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Z0, hadroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'mass spectrum, (2jet)', 'track data analysis, vertex', 'muon, final state', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806022'],"['A search for Z boson decays to pairs of b-quark jets has been performed in the full dataset collected with the CDF detector at the Tevatron proton-antiproton collider. After the selection of a pure sample of bb events by means of the identification of secondary vertices from b-quark decays, we have used two kinematic variables to further discriminate the electroweak bb production from QCD processes, and sought evidence for the Z decay in the dijet invariant mass distribution. An absolute background prediction allows the extraction of an excess of events inconsistent with the background predictions by 3.23 sigma but in good agreement with the amount and characteristics of the expected signal. We then fit the mass distribution with an unbinned likelihood technique, and obtain a Z -> bb signal amounting to 91+-30+-19 events.']",['1998-06-24']
1792,['eng'],"['Bornheim, A']",['Total Cross Section Measurements in $\\gamma-p$ and $\\gamma\\star-p$ at HERA'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 1998/02/16', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon p, interaction', 'total cross section, energy dependence', 'Regge poles', 'quantum chromodynamics, perturbation theory', 'p, structure function', 'x-dependence', 'momentum transfer, dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806021'],['Measurements of the total cross section for real and virtual photons on protons at center-of-mass energies in the range from 20 GeV to 270 GeV with photon virtualities up to 5000 GeV^2 are presented. For real photons this cross section can be described by Regge-motivated models while for virtual photons perturbative QCD can be applied. The measurements of the two HERA collider experiments ZEUS and H1 open the possibility to investigate the interplay between the two theoretical approaches in the transition region as well as the high-energy behavior of the cross sections. The results of total cross section measurements are discussed in the above context.'],['1998-06-22']
1793,['eng'],"['Crittenden, J A']",['Scale Issues in High-Energy Diffractive Vector-Meson Production'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 1998/02/16', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon p, interaction', 'diffraction', 'vector meson, photoproduction', 'rho(770)', 'omega(783)', 'Phi(1020)', 'J/psi(3100)', 'quantum chromodynamics, perturbation theory', 'channel cross section, energy dependence', 'vector meson, mass', 'Upsilon(9460)', 'momentum transfer, spectra', 'slope', 'yield, ratio', 'helicity, conservation law', 'spin, density matrix', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806020'],"['Recent measurements of diffractive vector-meson production with the general-purpose detectors H1 and ZEUS in electron-proton interactions with 300 GeV center-of-mass energy at the HERA accelerator complex have stimulated great interest in the question of whether perturbative QCD (pQCD) can provide an accurate description of such diffractive processes. The high flux of quasi-real photons from the 27.5 GeV electron beam has allowed high-statistics studies of vector-meson photoproduction to be compared to the deeply inelastic processes at high photon virtuality Q^2 >> \\Lambda^2_QCD. Special-purpose electron detectors at small scattering angle have been used to identify a transition region, 0.2 < Q^2 < 2 GeV^2, where the pQCD prediction for the dominance of point-like configurations of qqbar-pairs is verified. Data samples characterized by high momentum transfer to the 820 GeV initial-state proton, 1 < |t| < 13 GeV^2, have now become available, and the results lend support to the proposition that pQCD calculations should accurately describe the inelastic vector-meson production processes in high-|t| photoproduction. Measurements of the energy dependence and the t-dependence of the elastic cross sections for rho, omega, phi, and J/psi production have provided tests of the proposal that the mass (or size) of the vector meson provides a third scaling variable for studying the transition to the domain of pQCD applicability. A preliminary result on elastic upsilon production has also been announced by the ZEUS collaboration. These issues of scale will be discussed in the context of topical phenomenological models, comparing the HERA results and those from fixed-target experiments at lower energy to the wealth of calculations available in the contemporary literature.']",['1998-06-22']
1794,['eng'],[],['Search for Selectron and Squark Production in $e^+ p$ Collisions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'sparticle, search for', 'decay, squark', 'decay, selectron', 'neutralino', 'R parity, invariance', 'sparticle, mass', 'channel cross section, branching ratio', 'upper limit', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> sparticle anything', 'squark --> quark neutralino', 'selectron --> electron neutralino', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806019'],['We have searched for the production of a selectron and a squark in $e^+p$ collisions at a center-of-mass energy of 300 GeV using the ZEUS detector at HERA. The selectron and squark are sought in the direct decay into the lightest neutralino in the framework of supersymmetric extensions to the Standard Model which conserve R-parity. No evidence for the production of supersymmetric particles has been found in a data sample corresponding to 46.6~pb$^{-1}$ of integrated luminosity. We express upper limits on the product of the cross section times the decay branching ratios as excluded regions in the parameter space of the Minimal Supersymmetric Standard Model.'],['1998-06-22']
1795,['eng'],"['Toback, D']",['CDF Searches for New Phenomena'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1998/03/01', 'anti-p p, colliding beams', 'new particle, search for', 'Higgs particle, radiative decay', 'Higgs particle, hadronic decay', 'photon, pair production', 'quark, beauty', 'quark, pair production', 'squark, truth', 'vector meson, technicolor', 'transverse energy, missing-energy', 'intermediate boson', 'jet, multiple production', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2photon anything', 'anti-p p --> positron electron 2photon missing-energy anything', 'anti-p p --> (n)jet 2photon anything', 'anti-p p --> beauty photon anything', 'anti-p p --> intermediate boson anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807002'],"['We present results of recent searches for new physics using the CDF detector at the Fermilab Tevatron. Presented are searches for Higgs -> gammagamma, as well as more general searches in gammagamma + X where X is missing Et, jets, charged leptons, b-quarks or extra photons. The CDF eegammagamma-mett candidate event is discussed along with estimates of the expected rates in the Standard Model. Other searches for SUSY, Higgs and Technicolor look for particles which decay to vector bosons and b-quarks.']",['1998-07-06']
1796,['eng'],"['Brook, N H']",['QCD at HERA'],['Particle Physics - Experimental Results'],"['talk, San Juan 1998/04/08', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'p, structure function', 'x-dependence', 'dependence, momentum transfer', 'gluon, momentum spectrum', 'jet, electroproduction', 'production, small-angle', 'Altarelli-Parisi equation', 'Lipatov equation', 'fragmentation function', 'quantum chromodynamics, perturbation theory', 'scaling, violation', 'charged particle, spectra', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805031'],"['A review of HERA measurements of structure functions, fragmentation functions and forward jet production is presented.']",['1998-05-28']
1797,['eng'],"['Abe, F']",['Measurement of the $B^{-}$ and $\\overline{B}^{0}$ meson lifetimes using semileptonic decays'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B, semileptonic decay', 'B-, lifetime', 'anti-B0, lifetime', 'final state, (D0 lepton-)', 'final state, (D*(2010) lepton-)', 'charmed meson, hadronic decay', 'decay, path length', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806018'],"['The lifetimes of the B- and B0-bar mesons are measured using the partially reconstructed semileptonic decays B-bar -> D l- nu-bar X, where D is either a D0 or D*+ meson. The data were collected by the CDF detector at the Fermilab Tevatron collider during 1992-95 and correspond to about 110 pb-1 of p-bar p collisions at sqrt(s)=1.8 TeV. We measure decay lengths and extract the lifetimes to be tau(B-) = 1.637 +/- 0.058 +0.045 -0.043 ps, tau(B0) = 1.474 +/- 0.039 +0.052 -0.051 ps, and the ratio of the lifetimes to be tau(B-)/tau(B0) = 1.110 +/- 0.056 +0.033 -0.030, where the first uncertainties are statistical and the second are systematic.']",['1998-06-19']
1798,['eng'],"['Alberico, V', 'Bertin, A']",['Measurements of the reaction $\\overline{p}p \\to \\phi \\eta$ of antiproton annihilation at rest at three hydrogen target densities'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'at rest', 'hydrogen, density', 'Phi(1020), hadroproduction', 'eta, hadroproduction', 'anti-p p, bound state', 'p, baryonium', 'partial wave', 'channel cross section, branching ratio', 'mass spectrum', 'magnetic spectrometer, experimental results', 'CERN LEAR', 'anti-p p --> Phi(1020) eta', 'anti-p p --> K+ K- eta', '0 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806017'],"['The proton-antiproton annihilation at rest into the $\\phi\\eta$ final state was measured for three different target densities: liquid hydrogen, gaseous hydrogen at NTP and at a low pressure of 5 mbar. The yield of this reaction in the liquid hydrogen target is smaller than in the low-pressure gas target. The branching ratios of the $\\phi\\eta$ channel were calculated on the basis of simultaneous analysis of the three data samples. The branching ratio for annihilation into $\\phi\\eta$ from the $^3S_1$ protonium state turns out to be about ten times smaller as compared to the one from the $^1P_1$ state.']",['1998-06-18']
1799,['eng'],"['Wengler, T']",['Forward $\\pi^0$ -Meson and Charged Particle Production in Deep Inelastic Scattering at low Bjorken-x'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'small-x', 'pi0, electroproduction', 'charged particle, electroproduction', 'production, small-angle', 'Altarelli-Parisi equation', 'Lipatov equation', 'quantum chromodynamics', 'spectra, x-dependence', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806016'],"[""High transverse momentum pi^0 -mesons and charged particles are measured in deep inelastic e-p scattering events at low Bjorken-x taken with the H1 detector at HERA. The production of high-pt particles is strongly correlated to the emission of hard partons in QCD and is therefore sensitive to the dynamics of the strong interaction. For the first time the measurement of single particles has been extended to the region of small angles w.r.t. the proton remnant (forward region). This region is expected to be particularly sensitive to QCD evolution effects in final states. Results are presented as a function of Bjorken-x and x_i, the fraction of the incident proton's energy carried by the particle, and are compared to different QCD models.""]",['1998-06-17']
1800,['eng'],"['Minowa, M', 'Moriyama, S', 'Inoue, Y', 'Namba, T', 'Takasu, Y', 'Yamamoto, A']",['The Tokyo Axion Helioscope Experiment'],['Particle Physics - Experimental Results'],"['talk, Gainsville 1998/03/13', 'search for, axion', 'axion, solar', 'magnet, superconducting', 'magnetic field, high', 'coupling, (axion 2photon)', 'photon, counters and detectors', 'mass, axion', 'upper limit', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806015'],['A preliminary result of the solar axion search experiment at the University of Tokyo is presented. We searched for axions which could be produced in the solar core by exploiting the axion helioscope. The helioscope consists of a superconducting magnet with field strength of 4 Tesla over 2.3 meters. From the absence of the axion signal we set a 95 % confidence level upper limit on the axion coupling to two photons $g_{a\\gamma\\gamma} < 6.0 \\times 10^{-10} GeV^{-1}$ for the axion mass $m_a < 0.03$ eV. This is the first solar axion search experiment whose sensitivity to $g_{a\\gamma\\gamma}$ exceeds the limit inferred from the solar age consideration.'],['1998-06-17']
1801,['eng'],"['Shiozawa, M']",['Search for Proton Decay via $p \\to e^{+} \\pi^0$ in a Large Water Cherenkov Detector'],['Particle Physics - Experimental Results'],"['p, semileptonic decay', 'p, lifetime', 'lower limit', 'Cherenkov counter, water', 'deep underground detector, KAMIOKANDE', 'experimental results', 'p --> pi0 positron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806014'],"['We have searched for proton decay via p -> e+ pi0 using data from a 25.5 kton-year exposure of the Super-Kamiokande detector. We find no candidate events with an expected background induced by atmospheric neutrinos of 0.1 events. From these data, we set a lower limit on the partial lifetime of the proton to be 1.6E33 years at a 90% confidence level.']",['1998-06-17']
1802,['eng'],"['McFarland, K S', 'Adams, T', 'Alton, A', 'Avvakumov, S', 'De Barbaro, L', 'De Barbaro, P', 'Bernstein, R H', 'Bodek, Arie', 'Bolton, T', 'Brau, J E', 'Buchholz, D A', 'Budd, H S', 'Bugel, L', 'Conrad, J', 'Drucker, R B', 'Frey, R', 'Goldman, J', 'Goncharov, M', 'Harris, D A', 'Johnson, R A', 'Koutsoliotas, S', 'Kim, J H', 'Lamm, M J', 'Marsh, W', 'Mason, D', 'McNulty, C', 'Naples, D', 'Nienaber, P', 'Romosan, A', 'Sakumoto, W K', 'Schellman, H', 'Shaevitz, M H', 'Spentzouris, P', 'Stern, E G', 'Vakili, M', 'Vaitaitis, A G', 'Wu, V', 'Yang, U K', 'Yu, J', 'Zeller, G P']",['Measurement of $sin^{2}\\theta_{W}$ from Neutrino-Nucleon Scattering at NuTeV'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1998/03/14', 'neutrino nucleon, deep inelastic scattering', 'antineutrino nucleon, deep inelastic scattering', 'neutral current', 'charged current', 'Weinberg angle', 'channel cross section, ratio', 'W, mass', 'calorimeter, target', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806013'],"['We report the measurement of sin2thetaW in neutrino-nucleon deep inelastic scattering from the NuTeV experiment. Using separate neutrino and anti-neutrino beams, NuTeV is able to determine sin2thetaW with low systematic errors by measuring the Paschos-Wolfenstein variable R-minus, a ratio of differences of neutrino and anti-neutrino neutral-current and charged-current cross-sections. NuTeV measures sin2thetaW(on-shell)= 0.2253+/-0.0019(stat)+/-0.0010(syst), which implies a W mass of 80.26+/-0.11 GeV.']",['1998-06-12']
1803,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['An upper limit for the $\\tau$-neutrino mass from $\\tau \\to 5\\pi^{\\pm} \\nu_{\\tau}$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, leptonic decay', 'tau, pair production', 'tau, semileptonic decay', 'mass spectrum, (5pi)', 'energy spectrum', 'neutrino/tau, mass', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau --> 5pi neutrino/tau', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806035'],"[""An upper limit for the tau-neutrino mass has been determined from the decay tau -> 5pi+- \\nu_tau using data collected with the OPAL detector from 1991 to 1995 in e+e- collisions at \\sqrt{s} ~ M_Z. A limit of 43.2 MeV at 95% CL is obtained using a two-dimensional method in the 5pi invariant mass and energy distribution from 22 selected events. Combining this result with OPAL's previously published measurement using tau+tau- -> 3h+- \\bar{nu}_tau 3h-+ obtained.""]",['1998-06-30']
1804,['eng'],"['Bai, J Z']",['Determination of the $J/\\psi$ leptonic branching fraction via $\\psi(2S) \\to \\pi ^{+} \\pi^{-} J/\\psi$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), hadronic decay', 'J/psi(3100), leptonic decay', 'J/psi(3100), branching ratio', 'lepton, universality', 'quantum chromodynamics, Lambda parameter', 'coupling constant, strong interaction', 'magnetic spectrometer, BES', 'experimental results', 'Beijing Stor', 'electron positron --> psi(3685)', 'psi(3685) --> J/psi(3100) pi+ pi-', 'J/psi(3100) --> electron positron', 'J/psi(3100) --> muon+ muon-', '3.7 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806012'],"['A comparison of the rates for psi(2S) -> pi^+ pi^- J/psi, J/psi -> l^+l^- and J/psi -> anything is used to determine the J/psi leptonic branching fractions. The results are B(J/psi -> e^+e^-) = (5.90 +/- 0.05 +/- 0.10)% and B(J/psi -> mu^+ mu^-) = (5.84 +/- 0.06 +/- 0.10)%, where the first error is statistical and the second is systematic. Assuming lepton universality, the leptonic branching fraction of the J/psi is B(J/psi -> l^+ l^-) = (5.87 +/- 0.04 +/- 0.09)% per species. This result is used to estimate the QCD scale factor Lambda_MSbar and the strong coupling constant alpha_s.']",['1998-06-11']
1805,['eng'],"['Qian, J']",['New New-Phenomena Results from D0'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1998/03/01', 'anti-p p, colliding beams', 'photon, pair production', 'jet, multiple production', 'transverse energy, missing-energy', 'supersymmetry', 'sparticle, pair production', 'channel cross section, branching ratio', 'upper limit', 'neutralino, radiative decay', 'photon photon, multiple scattering', 'magnetic monopole, effect', 'magnetic monopole, mass', 'lower limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2photon anything', 'anti-p p --> (n)jet 2photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806011'],"['We have searched for diphoton events (\\ggmet) with large missing transverse momentum, $\\gamma\\rlap{\\kern0.25em/}E_T$ events (\\gmetjj) with two or more jets, and diphoton events ($\\gamma\\gamma$) with high transverse energies in $p\\bar p$ collisions at $\\sqrt{s} = 1.8$ TeV using approximately 100~pb$^{-1}$ of data collected with the DØ detector at the Fermilab Tevatron in 1992--1996. No excess of events beyond the expected backgrounds is observed. The null results are interpreted in supersymmetric models with a dominant monopole production.']",['1998-06-11']
1806,['eng'],"['Schneekloth, U']",['Recent HERA Results and Future Prospects'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'electron p, colliding beams', 'electron p, deep inelastic scattering', 'p, structure function', 'structure function, charm', 'lepton, final state', 'transverse momentum, missing-energy', 'mass spectrum, transverse', 'charged current', 'W, mass', 'coupling, (2W photon)', 'sparticle, search for', 'squark', 'selectron', 'sparticle, mass', 'luminosity', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'upgrade, proposed', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806010'],"['A few selected HERA results are presented and the prospects for future measurements with high luminosity are discussed, which will become available after the planned luminosity upgrade of the HERA storage ring planned for 2000.']",['1998-06-11']
1807,['eng'],"['Adloff, C']",['Observation of Events with an Isolated High Energy Lepton and Missing Transverse Momentum at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'transverse momentum, missing-energy', 'lepton, electroproduction', 'transverse momentum, high', 'kinematics, phase space', 'event shape analysis, planarity', 'W, electroproduction', 'W, leptonic decay', 'electroweak interaction, validity test', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> muon anything', 'positron p --> electron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806009'],"['A search for events with an imbalance in transverse momentum and with isolated high energy leptons has been carried out at the positron-proton collider HERA. One event with an e^- and five events with a mu^+- are found together with evidence for undetected particles carrying transverse momentum. Within the Standard Model the dominant origin of events with this kind of topology is the production of W bosons with subsequent leptonic decay. Three of the six events are within measurement errors found in a region of phase space likely to be populated by this process, while the remaining events show kinematic properties which are atypical of all Standard Model processes considered.']",['1998-06-11']
1808,['eng'],"['Ackerstaff, K']",['The HERMES Spectrometer'],['Detectors and Experimental Techniques'],"['tracks', 'drift chamber', 'proportional chamber', 'electrode, microstrip', 'particle identification', 'Cherenkov counter, threshold', 'transition radiation detector', 'calorimeter, lead-glass', 'alignment', 'scintillation counter, hodoscope', 'luminosity, beam monitoring', 'trigger', 'data acquisition', 'electronics, readout', 'magnetic spectrometer, HERMES', 'DESY HERA Stor', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806008'],"['The HERMES experiment is collecting data on inclusive and semi-inclusive deep inelastic scattering of polarised positrons from polarised targets of H, D, and He. These data give information on the spin structure of the nucleon. This paper describes the forward angle spectrometer built for this purpose. The spectrometer includes numerous tracking chambers (micro-strip gas chambers, drift and proportional chambers) in front of and behind a 1.3 T.m magnetic field, as well as an extensive set of detectors for particle identification (a lead-glass calorimeter, a pre-shower detector, a transition radiation detector, and a threshold Cherenkov detector). Two of the main features of the spectrometer are its good acceptance and identification of both positrons and hadrons, in particular pions. These characteristics, together with the purity of the targets, are allowing HERMES to make unique contributions to the understanding of how the spins of the quarks contribute to the spin of the nucleon.']",['1998-06-11']
1809,['eng'],"['Barate, R', 'Buskulic, D', 'Décamp, D', 'Ghez, Philippe', 'Goy, C', 'Jézéquel, S', 'Lees, J P', 'Lucotte, A', 'Martin, F', 'Merle, E', 'Minard, M N', 'Nief, J Y', 'Pietrzyk, B', 'Alemany, R', 'Boix, G', 'Casado, M P', 'Chmeissani, M', 'Crespo, J M', 'Delfino, M C', 'Fernández, E', 'Fernández-Bosman, M', 'Garrido, L', 'Graugès, E', 'Juste, A', 'Martínez, M', 'Merino, G', 'Miquel, R', 'Mir, L M', 'Morawitz, P', 'Park, I C', 'Pascual, A', 'Riu, I', 'Sánchez, F', 'Colaleo, A', 'Creanza, D', 'De Palma, M', 'Gelao, G', 'Iaselli, Giuseppe', 'Maggi, G', 'Maggi, M', 'Nuzzo, S', 'Ranieri, A', 'Raso, G', 'Ruggieri, F', 'Selvaggi, G', 'Silvestris, L', 'Tempesta, P', 'Tricomi, A', 'Zito, G', 'Huang, X', 'Lin, J', 'Ouyang, Q', 'Wang, T', 'Xie, Y', 'Xu, R', 'Xue, S', 'Zhang, J', 'Zhang, L', 'Zhao, W', 'Abbaneo, D', 'Becker, U', 'Bright-Thomas, P G', 'Casper, David William', 'Cattaneo, M', 'Ciulli, V', 'Dissertori, G', 'Drevermann, H', 'Forty, Roger W', 'Frank, M', 'Gianotti, F', 'Hagelberg, R', 'Hansen, J B', 'Harvey, J', 'Janot, P', 'Jost, B', 'Lehraus, Ivan', 'Maley, P', 'Mato, P', 'Minten, A', 'Moneta, L', 'Qi, N', 'Pacheco, A', 'Ranjard, F', 'Rolandi, Luigi', 'Rousseau, D', 'Schlatter, D', 'Schmitt, M', 'Schneider, O', 'Tejessy, W', 'Teubert, F', 'Tomalin, I R', 'Vreeswijk, M', 'Wachsmuth, Horst Werner', 'Ajaltouni, Ziad J', 'Badaud, F', 'Chazelle, G', 'Deschamps, O', 'Falvard, A', 'Ferdi, C', 'Gay, P', 'Guicheney, C', 'Henrard, P', 'Jousset, J', 'Michel, B', 'Monteil, S', 'Montret, J C', 'Pallin, D', 'Perret, P', 'Podlyski, F', 'Proriol, J', 'Rosnet, P', 'Hansen, J D', 'Hansen, J R', 'Hansen, P H', 'Nilsson, B S', 'Rensch, B', 'Wäänänen, A', 'Daskalakis, G', 'Kyriakis, A', 'Markou, C', 'Simopoulou, Errietta', 'Vayaki, Anna', 'Blondel, Alain', 'Brient, J C', 'Machefert, F P', 'Rougé, A', 'Rumpf, M', 'Tanaka, R', 'Valassi, A', 'Videau, H L', 'Focardi, E', 'Parrini, G', 'Zachariadou, K', 'Cavanaugh, R J', 'Corden, M', 'Georgiopoulos, C H', 'Hühn, T', 'Jaffe, D E', 'Antonelli, A', 'Bencivenni, G', 'Bologna, G', 'Bossi, F', 'Campana, P', 'Capon, G', 'Cerutti, F', 'Chiarella, V', 'Felici, G', 'Laurelli, P', 'Mannocchi, G', 'Murtas, F', 'Murtas, G P', 'Passalacqua, L', 'Pepé-Altarelli, M', 'Chalmers, M', 'Curtis, L', 'Halley, A W', 'Lynch, J G', 'Negus, P', ""O'Shea, V"", 'Raine, C', 'Scarr, J M', 'Smith, K', 'Teixeira-Dias, P', 'Thompson, A S', 'Thomson, E', 'Ward, J J', 'Buchmüller, O L', 'Dhamotharan, S', 'Geweniger, C', 'Graefe, G', 'Hanke, P', 'Hansper, G', 'Hepp, V', 'Kluge, E E', 'Putzer, A', 'Sommer, J', 'Tittel, K', 'Werner, S', 'Wunsch, M', 'Beuselinck, R', 'Binnie, David M', 'Cameron, W', 'Dornan, Peter J', 'Girone, M', 'Goodsir, S M', 'Martin, E B', 'Marinelli, N', 'Moutoussi, A', 'Nash, J', 'Sedgbeer, J K', 'Spagnolo, P', 'Williams, M D', 'Ghete, V M', 'Girtler, P', 'Kneringer, E', 'Kuhn, D', 'Rudolph, G', 'Bowdery, C K', 'Buck, P G', 'Colrain, P', 'Crawford, G', 'Finch, A J', 'Foster, F', 'Hughes, G', 'Jones, R W L', 'Robertson, N A', 'Williams, M I', 'Giehl, I', 'Hoffmann, C', 'Jakobs, K', 'Kleinknecht, K', 'Kröcker, M', 'Nürnberger, H A', 'Quast, G', 'Renk, B', 'Rohne, E', 'Sander, H G', 'Van Gemmeren, P', 'Zeitnitz, C', 'Ziegler, T', 'Aubert, Jean-Jacques', 'Benchouk, C', 'Bonissent, A', 'Bujosa, G', 'Carr, J', 'Coyle, P', 'Ealet, A', 'Fouchez, D', 'Leroy, O', 'Motsch, F', 'Payre, P', 'Talby, M', 'Sadouki, A', 'Thulasidas, M', 'Tilquin, A', 'Trabelsi, K', 'Aleppo, M', 'Antonelli, M', 'Ragusa, F', 'Berlich, R', 'Büscher, V', 'Cowan, G D', 'Dietl, H', 'Ganis, G', 'Lütjens, G', 'Mannert, C', 'Männer, W', 'Moser, H G', 'Schael, S', 'Settles, Ronald', 'Seywerd, H C J', 'Stenzel, H', 'Wiedenmann, W', 'Wolf, G', 'Boucrot, J', 'Callot, O', 'Chen, S', 'Davier, M', 'Duflot, L', 'Grivaz, J F', 'Heusse, P', 'Höcker, A', 'Jacholkowska, A', 'Kado, M', 'Kim, D W', 'Le Diberder, F', 'Lefrançois, J', 'Serin, L', 'Tournefier, E', 'Veillet, J J', 'Videau, I', 'Zerwas, D', 'Azzurri, P', 'Bagliesi, G', 'Bettarini, S', 'Boccali, T', 'Bozzi, C', 'Calderini, G', ""Dell'Orso, R"", 'Fantechi, R', 'Ferrante, I', 'Giassi, A', 'Gregorio, A', 'Ligabue, F', 'Lusiani, A', 'Marrocchesi, P S', 'Messineo, A', 'Palla, Fabrizio', 'Rizzo, G', 'Sanguinetti, G', 'Sciabà, A', 'Sguazzoni, G', 'Tenchini, Roberto', 'Vannini, C', 'Venturi, A', 'Verdini, P G', 'Blair, G A', 'Bryant, L M', 'Chambers, J T', 'Coles, J', 'Green, M G', 'Medcalf, T', 'Perrodo, P', 'Strong, J A', 'Von Wimmersperg-Töller, J H', 'Botterill, D R', 'Clifft, R W', 'Edgecock, T R', 'Haywood, S', 'Norton, P R', 'Thompson, J C', 'Wright, A E', 'Bloch-Devaux, B', 'Colas, P', 'Fabbro, B', 'Faïf, G', 'Lançon, E', 'Lemaire, M C', 'Locci, E', 'Pérez, P', 'Przysiezniak, H', 'Rander, J', 'Renardy, J F', 'Rosowsky, A', 'Roussarie, A', 'Trabelsi, A', 'Vallage, B', 'Black, S N', 'Dann, J H', 'Kim, H Y', 'Konstantinidis, N P', 'Litke, A M', 'McNeil, M A', 'Taylor, G', 'Booth, C N', 'Cartwright, S L', 'Combley, F', 'Kelly, M S', 'Lehto, M H', 'Thompson, L F', 'Affholderbach, K', 'Böhrer, A', 'Brandt, S', 'Foss, J', 'Grupen, Claus', 'Smolik, L', 'Stephan, F', 'Giannini, G', 'Gobbo, B', 'Musolino, G', 'Pütz, J', 'Rothberg, J E', 'Wasserbaech, S R', 'Williams, R W', 'Armstrong, S R', 'Betteridge, A P', 'Charles, E', 'Elmer, P', 'Ferguson, D P S', 'Gao, Y', 'González, S', 'Greening, T C', 'Hayes, O J', 'Hu, H', 'Jin, S', 'McNamara, P A', 'Nachtman, J M', 'Nielsen, J', 'Orejudos, W', 'Pan, Y B', 'Saadi, Y', 'Scott, I J', 'Walsh, J', 'Wu Sau Lan', 'Wu, X', 'Zobernig, G']",['Scalar quark searches in $e^+ e^-$ collisions at $\\sqrt{s}$ = 181-184 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'squark, search for', 'squark, truth', 'squark, beauty', 'squark, decay modes', 'squark, mass', 'lower limit', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '181-184 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ep-98-076', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9810028']","[""Searches for scalar top, scalar bottom and degenerate scalar quarks have been performed with data collected with the ALEPH detector at LEP. The data sample consists of 57~$\\mathrm{pb}^{-1}$ taken at $\\rts$ = 181--184~GeV. No evidence for scalar top, scalar bottom or degenerate scalar quarks was found in the channels $\\stop \\rightarrow \\mathrm{c}\\neu$, $\\stop \\rightarrow \\mathrm{b}\\ell\\sn u$, $\\sbot \\rightarrow \\mathrm{b}\\neu$, and $\\mathrm{\\tilde{q}} \\rightarrow \\mathrm{q}\\neu$. From the channel $\\stop \\rightarrow \\mathrm{c}\\neu$ a limit of 74~$\\gev$ has been set on the scalar top quark mass, independent of the mixing angle. This limit assumes a mass difference between the $\\stop$ and the $\\neu$ in the range 10--40~$\\gev$. From the channel $\\stop \\rightarrow \\mathrm{b}\\ell\\ snu$ the mixing-angle-independent scalar top limit is 82~$\\gev$, assuming $m_{\\mathrm{\\tilde{t}}}-m_{\\tilde{\\nu}}$ $>$ 10~$\\gev$. From the channel $\\sbot \\rightarrow \\mathrm{b}\\neu$, a limit of 79 ~$\\gev$ has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid for $m_{\\mathrm{\\tilde{b}}}-m_{\\neu}$ $>$ 10~$\\gev$. From the chan nel $\\mathrm{\\tilde{q}} \\rightarrow \\mathrm{q}\\neu$, a limit of 87~$\\gev$ has been set on the mass of supersymmetric partners of light quarks assuming five degenerate flavours and the production o f both ``left-handed'' and ``right-handed'' squarks. This limit is valid for $m_{\\mathrm{\\tilde{q}}}-m_{\\neu}$ $>$ 5~$\\gev$.""]",['1998-06-04']
1810,['eng'],"['Adams, J']",['Search for the decay $K_{L}\\to \\pi ^{0} \\nu \\overline {\\nu}$'],['Particle Physics - Experimental Results'],"['K0(L), semileptonic decay', 'K0(L), rare decay', 'pi0, radiative decay', 'K0(L), branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0(L) --> pi0 neutrino antineutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806007'],"['We report on a search for the rare decay K_L -> pi^0 nu nubar in the KTeV experiment at Fermilab. We searched for two-photon events whose kinematics were consistent with an isolated pi^0 coming from the decay K_L -> pi^0 nu nubar. One candidate event was observed, which was consistent with the expected level of background. An upper limit on the branching ratio was determined to be B(K_L -> pi^0 nu nubar) < 1.6E-6 at the 90% confidence level.']",['1998-06-10']
1811,['eng'],"['Ackerstaff, K']",['Beam-Induced Nuclear Depolarisation in a Gaseous Polarised Hydrogen Target'],['Detectors and Experimental Techniques'],"['target, internal', 'hydrogen, polarized target', 'depolarization', 'positron, beam', 'magnetic spectrometer, HERMES', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806006'],"['Spin-polarised atomic hydrogen is used as a gaseous polarised proton target in high energy and nuclear physics experiments operating with internal beams in storage rings. When such beams are intense and bunched, this type of target can be depolarised by a resonant interaction with the transient magnetic field generated by the beam bunches. This effect has been studied with the HERA positron beam in the HERMES experiment at DESY. Resonances have been observed and a simple analytic model has been used to explain their shape and position. Operating conditions for the experiment have been found where there is no significant target depolarisation due to this effect.']",['1998-06-10']
1812,['eng'],"['Ellison, J']",['Measurements of the W Boson Mass and Trilinear Gauge Boson Couplings at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1998/03/14', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'W, mass', 'W, pair production', 'photon, associated production', 'coupling, (2W photon)', 'coupling, (2W Z0)', 'form factor, dipole', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'anti-p p --> 2W anything', 'anti-p p --> W photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806004'],"['We present measurements of the W boson mass at the Tevatron based on $W \\to Ib (1994--95). The W boson mass measured in the preliminary CDF analysis is 80.43 \\pm 0.10 (stat) \\pm 0.12 (syst) GeV/c^2. The D0 measured value is 80.44 trilinear gauge boson couplings. The limits obtained on the WW\\gamma and WWZ anomalous couplings from a combined D0 analysis using $W\\gamma$, $WW \\to \\ell for a dipole form factor scale of 2 TeV. Improved limits have been obtained by combining these results with the limits derived from the LEP experiments.']",['1998-06-08']
1813,['eng'],"['Jungmann, K P']",['Lepton Flavour Violation Experiments'],['Particle Physics - Experimental Results'],"['review, San Juan 1998/04/01', 'violation, flavor', 'double-beta decay, (0neutrino)', 'K, semileptonic decay', 'K0(L), leptonic decay', 'muon, radiative decay', 'muon- nucleus, interaction', 'transition, muon- electron', 'muonium, transition', 'muonium, antiparticle', 'experimental methods', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806003'],"['Dedicated experiments searching for lepton flavour violation can be performed very sensitively using K-decays and $\\mu$-decays as well as neutrinoless double confirmed signal reported yet, stringent limits for parameters in speculative extensions to the standard model can be set. Some models could recently be ruled out.']",['1998-06-04']
1814,['eng'],"['Bai, J Z']","[""Branching Fractions for $\\psi(2S)$ to $\\gamma \\eta'$ and $\\gamma \\eta$""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'psi(3685), electroproduction', 'psi(3685), radiative decay', 'psi(3685), branching ratio', 'eta(958), hadronic decay', 'eta, hadronic decay', 'interference, (eta/c(2980) eta)', 'mass spectrum', 'magnetic detector, BES', 'experimental results', 'Beijing Stor', 'electron positron --> psi(3685)', 'psi(3685) --> eta(958) photon', 'psi(3685) --> eta photon', 'eta(958) --> rho(770) photon', 'eta(958) --> eta pi+ pi-', 'eta --> pi+ pi- pi0', '3.685 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806002'],"[""We report the first measurements of the branching fractions: $B(\\psi(2S) -> result is consistent with expectations of a model that considers the possibility of $\\eta' - \\eta$ mixing. The ratio of the $\\psi(2S)$ to $\\gamma pseudoscalar octet-singlet mixing angle.""]",['1998-06-04']
1815,['eng'],"['Aglietta, M']","['Muon ""Depth-Intensity"" Relation Measured by LVD Underground Experiment and Cosmic-Ray Muon Spectrum at Sea Level']",['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'cosmic radiation, energy spectrum', 'muon, multiplicity', 'muon, flux', 'angular distribution', 'spatial distribution', 'deep underground detector, Gran Sasso', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9806001'],"[""We present the analysis of the muon events with all muon multiplicities collected during 21804 hours of operation of the first LVD tower. The measured angular distribution of muon intensity has been converted to the `depth -- vertical intensity' relation in the depth range from 3 to 12 km w.e.. The analysis of this relation allowed to derive the power index, $\\gamma$, of the primary all-nucleon spectrum: $\\gamma=2.78 \\pm 0.05$. The `depth -- vertical intensity' relation has been converted to standard rock and the comparison with the data of other experiments has been done. We present also the derived vertical muon spectrum at sea level.""]",['1998-06-04']
1816,['eng'],"['Abe, F']",['Observation of the $B_{c}$ Meson in $p\\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B/c, hadroproduction', 'B/c, semileptonic decay', 'mass spectrum, (J/psi(3100) lepton)', 'B/c, mass', 'B/c, lifetime', 'channel cross section, branching ratio', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B/c --> J/psi(3100) lepton neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805034'],['We have observed bottom-charm mesons B_c via the decay mode Bc -> J/psi lepton neutrino in 1.8 TeV p-bar p collisions using the CDF detector at the Fermilab Tevatron. A fit of background and signal contributions to the J/psi + lepton mass distribution yielded 20.4 +6.2 -5.5 events from B_c mesons. A fit to the same distribution with background alone was rejected at the level of 4.8 standard deviations. We measured the B_c mass to be 6.40 +- 0.39 +- 0.13 GeVc^2 and the B_c lifetime to be tau(B_c) = 0.46 +0.18 -0.16 +- 0.03 ps. We measured the production cross section times branching ratio for B_c -> J/psi lepton neutrino relative to that for B+ -> J/psi K to be 0.132 +0.041 -0.037 (stat) +- 0.031 (syst) +0.032 -0.020 (lifetime).'],['1998-05-29']
1817,['eng'],"['Alam, M S']",['Further Search for the Two-Photon Production of the Glueball Candidate $f_{J}(2220)$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'search for, f4(2220)', 'f4(2220), hadronic decay', 'mass spectrum, (pi+ pi-)', 'K, pair production', 'width, branching ratio', 'upper limit', 'glueball', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> f4(2220) positron electron', 'f4(2220) --> pi+ pi-', 'f4(2220) --> 2K0(S)', 'f4(2220) --> K+ K-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805033'],"[""The CLEOII detector at the Cornell e+ e- storage ring CESR has been used to search for the two-photon production of the $f_J(2220)$ decaying into pi+ pi-. No evidence for a signal is found in data corresponding to an integrated luminosity of 4.77/fb and a 95% CL upper limit on $\\Gamma_{two-photon} * BR{pi+ pi-}$ of 2.5 eV is set. If this result is combined with the BES Collaboration's measurement of $f_J(2220) -> pi+ pi-$ in radiative $J/\\psi$ decay, a 95% CL lower limit on the stickiness of the $f_J(2220)$ of 73 is obtained. If the recent CLEO result for $\\Gamma_{two-photon} * BR{\\K_S K_S}$ is combined with the present result, the stickiness of the $f_J(2220)$ is found to be larger than 102 at the 95% CL. These results for the stickiness (the ratio of the probabilities for two-gluon coupling and two-photon coupling) provide further support for a substantial neutral parton content in the $f_J(2220)$.""]",['1998-05-29']
1818,['eng'],"['Agababian, N M']",['Self-affine scaling from non-integer phase-space partition in $\\pi^{+}p$ and $K^{+}p$ Collisions at 250 GeV/$c$'],['Particle Physics - Experimental Results'],"['pi+ p, interaction', 'K+ p, interaction', 'hadron, multiple production', 'scaling', 'phase space', 'multiplicity, moment', 'transformation, affine', 'bubble chamber(hydrogen)', 'magnetic spectrometer, experimental results', 'CERN SPS', '250 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805030'],['A factorial-moment analysis with real (integer and non-integer) phase space partition is applied to $\\pi^+$p and K$^+$p collisions at 250 GeV/$c$. Clear evidence is shown for self-affine rather than self-similar power-law scaling in multiparticle production. The three-dimensional self-affine second-order scaling exponent is determined to be 0.061$\\pm$0.010.'],['1998-05-26']
1819,['eng'],"['Chkhaidze, L V', 'Djobava, T', 'Kharkhelauri, L L', 'Mosidze, M D']",['The comparison of characteristics of $\\pi ^{-}$ mesons produced in central Mg-Mg interactions with the quark gluon string model predictions'],['Particle Physics - Experimental Results'],"['nucleus nucleus, nuclear reaction', 'magnesium', 'central region', 'pi-, hadroproduction', 'pi-, multiplicity', 'pi-, momentum spectrum', 'transverse momentum, spectra', 'rapidity dependence', 'pi-, angular distribution', 'quark gluon, string model', 'nuclear reaction, temperature', 'anisotropy', 'four-pi-detector, experimental results', 'Dubna PS', '4.3 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805028'],"[""A detailed study of pion production in central Mg-Mg collisions at a momentum of 4.3 GeV/c per incident nucleon was carried out with use of the setup GIBS. The average kinematical characteristics of pions (multiplicity n_, momentum P, transverse momentum P_{T}, emission angle Q, rapidity Y) and corresponding distributions had been obtained. The experimental results had been compared with the predictions of the Quark Gluon String Model (QGSM) and satisfactory agreement between the experimental data and the model have been found. The QGSM reproduces also the dependence of average P_{T} on n_{-}. The temperatures of pi^{-} mesons have been estimated in the rapidity interval of 0.5<=Y<=2.1. A satisfactory fit for pi^{-} mesons had been achieved by using a form involving two temperatures T_{1} and T_{2}. It was found that the QGSM underestimates T_{2} by (10-15)%. The data have been analyzed using the transverse momentum technique. The observed dependence of the <P_{x'}(Y)> on Y shows the S-shape behaviour. The slope at midrapidity F had been determined. The QGSM reproduces the <P_{x}> distribution satisfactorily, but underestimates the parameter F.""]",['1998-05-26']
1820,['eng'],"['Anderson, S']",['First Search for CP Violation in $\\tau$ Lepton Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau+, semileptonic decay', 'tau-, semileptonic decay', 'invariance, CP', 'angular distribution', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> K0(S) pi- neutrino/tau', 'K0(S) --> pi+ pi-', '10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805027'],['Using the CLEO II detector we have performed the first search for $CP$ violation in tau lepton decay. CP violation in lepton decay does not occur in the minimal standard model but can occur in extensions such as the multi-Higgs doublet model. It appears as a characteristic difference between the $\\tau^+$ and $\\tau^-$ decay angular distributions for the semi-leptonic decay modes such as $\\tau^- \\to K^0 \\pi^- \\nu$. We define an observable asymmetry to exploit this and find no evidence for any CP violation.'],['1998-05-25']
1821,['eng'],"['Moriyama, S', 'Minowa, M', 'Namba, T', 'Inoue, Y', 'Takasu, Y', 'Yamamoto, A']",['Direct search for solar axions by using strong magnetic field and X-ray detectors'],['Particle Physics - Experimental Results'],"['search for, axion', 'axion, solar', 'transition, axion photon', 'magnetic field, high', 'coupling, (axion 2photon)', 'upper limit', 'magnet, superconducting', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805026'],"['We have searched for axions which could be produced in the solar core by exploiting their conversion to X rays in a strong laboratory magnetic field. The signature of the solar axion is an increase in the rate of the X rays detected in a magnetic helioscope when the sun is within its acceptance. From the absence of such a signal we set a 95% confidence level limit on the axion coupling to two photons $g_{a\\gamma\\gamma}\\equiv 1/M < 6.0\\times 10^{-10}$ GeV$^{-1}$, provided the axion mass $m_a<0.03$ eV. The limit on the coupling is factor 4.5 more stringent than the recent experimental result. This is the first experiment whose sensitivity to $g_{a\\gamma\\gamma}$ is higher than the limit constrained by the solar age consideration.']",['1998-05-25']
1822,['eng'],"['Blusk, S R']",['Measurement of the Top Quark Mass'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1998/03/21', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'mass, truth', 'quark, decay', 'final state, dilepton', 'final state, ((n)jet lepton)', 'final state, ((n)jet)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805035', 'http://www-lib.fnal.gov/archive/1998/conf/Conf-98-151-E.html']","['In this paper, we report on the most recent measurements of the top quark mass, performed by the CDF and D0 collaborations at the Fermilab Tevatron. The CDF collaboration has performed measurements of the top quark mass in three decay channels from which the top quark mass is measured to be 175.5 +- 6.9 GeV/c^2. The D0 collaboration combines measurements from two decay channels to obtain a top quark mass of 172.1 +- 7.1 GeV/c^2. Combining the measurements from the two experiments, assuming a 2 GeV/c^2 correlated systematic uncertainty, the measurement of the top quark mass at the Tevatron is 173.9 +- 5.2 GeV/c^2. This report presents the measurements of the top quark mass from each of the decay channels which contribute to this measurement.']",['2000-01-20']
1823,['eng'],"['Wong, H T', 'Li, J']",['A Pilot Experiment with Reactor Neutrinos in Taiwan'],['Particle Physics - Experimental Results'],"['antineutrino nucleus, interaction', 'antineutrino/e', 'deuteron', 'boron', 'charged current', 'neutral current', 'neutrino electron, elastic scattering', 'fission, particle source', 'neutrino, oscillation', 'scintillation counter, crystal', 'cesium, iodine', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805024'],['A Collaboration comprising Taiwan and mainland Chinese scientists has been built up since 1996 to pursue a experimental program in neutrino and astro-particle physics in Taiwan. A pilot experiment to be performed at the Nuclear Power Station II in Taiwan is now under intense preparation. It will make use of a 600 kg CsI(Tl) crystal calorimeter to study various neutrino interactions. The feasibility of performing a long baseline reactor neutrino experiment will also be investigated. The conceptual design and the physics to be addressed by the pilot experiment are presented.'],['1998-05-22']
1824,['eng'],"['Willocq, S']",['B Physics at SLD'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1998/03/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'quark, decay modes', 'B+, lifetime', 'B0, lifetime', 'B/s0 anti-B/s0, interference', 'B/s0, mass difference', 'decay, path length', 'track data analysis, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'beauty --> strangeness gluon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805022'],"['We report new preliminary B Physics results obtained with 300,000 hadronic Z0 decays collected by the SLD experiment at the SLC between 1993 and 1997. Three analyses are presented: a measurement of B+ and B0 lifetimes, a study of the time dependence of Bs - Bs-bar mixing, and a search for decays of the type b --> sg. All analyses benefit from the small and stable interaction point and the excellent resolution and efficiency provided by the pixel-based CCD Vertex Detector. The b --> sg analysis also exploits the particle identification capabilities of the Cherenkov Ring Imaging Detector.']",['1998-05-21']
1825,['eng'],"['Fukuda, Y']","[""Measurements of the Solar Neutrino Flux from Super-Kamiokande's First 300 Days""]",['Particle Physics - Experimental Results'],"['neutrino, solar', 'neutrino, flux', 'flux, time variation', 'neutrino electron, elastic scattering', 'Cherenkov counter, water', 'experimental results', 'deep underground detector, KAMIOKANDE']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805021'],"['The first results of the solar neutrino flux measurement from Super-Kamiokande are presented. The results shown here are obtained from data taken between the 31st of May, 1996, and the 23rd of June, 1997. Using our measurement of recoil electrons with energies above 6.5 MeV, we infer the total flux of 8B solar neutrinos to be 2.42+-0.06(stat.)+0.10-0.07(syst.)*10^6/cm^2/s. This result is consistent with the Kamiokande measurement and is 36% of the flux predicted by the BP95 solar model. The flux is also measured in 1.5 month subsets and shown to be consistent with a constant rate.']",['1998-05-21']
1826,['eng'],"['Glenzinski, D A']",['Measurement of $M_{W}$ from LEP2'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1997/03/22', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, mass', 'W, leptonic decay', 'W, hadronic decay', 'experimental results', 'CERN LEP Stor', '161, 172, 183 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805020'],"['In 1997 each LEP experiment collected approximately 55 inv. pb of data at a center-of-mass energy of 183 GeV. These data yield a sample of candidate e+e- -> WW events from which the mass of the W boson, Mw, is measured. The LEP combined result, including data taken at roots = 161 and 172 GeV and assuming the Standard Model relation between the W decay width and mass, is Mw = 80.35 +/- 0.07 (exp) +/- 0.04 (CR) +/- 0.03 (E_beam) GeV, where the errors correspond to experimental, colour-reconnection/Bose-Einstein, and LEP beam energy uncertainties respectively.']",['1998-05-21']
1827,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Böhme, J', 'Boutemeur, M', 'Braibant, S', 'Bright-Thomas, P G', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Ciocca, C', 'Clarke, P E L', 'Clay, E', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Dubbert, J', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Evans, H G', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jacob, F R', 'Jawahery, A', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Liebisch, R', 'List, B', 'Littlewood, C', 'Lloyd, A W', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Polok, J', 'Przybycien, M B', 'Rembser, C', 'Rick, Hartmut', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Roscoe, K', 'Rossi, A M', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schörner-Sadenius, T', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Seuster, R', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Sproston, M', 'Stahl, A', 'Stephens, K', 'Steuerer, J', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Production of $K^{0}_{S}$ and $\\Lambda$ in Quark and Gluon Jets from $Z^{0}$ Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'quark, jet', 'gluon, jet', 'K0(S), hadronic decay', 'Lambda, hadronic decay', 'yield, (Lambda K0(S))', 'jet, energy spectrum', 'energy flow', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=EP-98-058', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805025']","['The production of K^0_S mesons and Lambda baryons in quark and gluon jets has been investigated using two complementary techniques. In the first approach, which provides high statistical accuracy, jets were selected using different jet finding algorithms and ordered according to their energy. Production rates were determined taking into account the dependences of quark and gluon compositions as a function of jet energy as predicted by Monte Carlo models. Selecting three-jet events with the k_perp (Durham) jet finder (y_cut = 0.005), the ratios of K^0_S and Lambda production rates in gluon and quark jets relative to the mean charged particle multiplicity were found to be 1.10 +/- 0.02 +/- 0.02 and 1.41 +/- 0.04 +/- 0.04, respectively, where the first uncertainty is statistical and the second is systematic. In the second approach, a new method of identifying quark jets based on the collimation of energy flow around the jet axis is introduced and was used to anti-tag gluon jets in symmetric (Y-shaped) three-jet events. Using the cone jet finding algorithm with a cone size of 30 degrees, the ratios of relative production rates in gluon and quark jets were determined to be 0.94 +/- 0.07 +/- 0.07 for K^0_S and 1.18 +/- 0.10 +/- 0.17 for Lambda. The results of both analyses are compared to the predictions of Monte Carlo models.']",['1998-05-13']
1828,['eng'],"['Vossebeld, J H']",['Photon Structure in Photon Proton Interactions'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'positron p, colliding beams', 'photon p, interaction', 'jet, photoproduction', 'final state, (2jet)', 'photon, structure function', 'photon, resolved', 'hard scattering', 'particle identification, jet', 'quantum chromodynamics, perturbation theory', 'transverse energy, energy flow', 'differential cross section, transverse energy', 'rapidity dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805019'],"['Photoproduction of jets at HERA provides information on the partonic structure of the photon. We report on the latest dijet photoproduction results, for real photons and for photons at low virtualities, measured with the ZEUS detector.']",['1998-05-20']
1829,['eng'],"['Barberis, D']",['A study of the centrally produced $\\phi \\phi$ system in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'Phi(1020), pair production', 'K, multiple production', 'exchange, (2pomeron)', 'mass spectrum', 'spectra, x-dependence', 'momentum transfer, dependence', 'glueball', 'spin, parity', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p 2K+ 2K-', 'p p --> 2Phi(1020)', 'p p --> Phi(1020) K+ K-', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805018'],['The reaction pp to pfps(K+K-K+K-) in which the K+K-K+K- system is centrally produced has been studied at 450 GeV/c. Phi phi production has been found to dominate this reaction and is compatible with being produced by double Pomeron exchange. An angular analysis of the phi phi system favours JPC = 2++ and its dPT dependence is similar to that observed for glueball candidates.'],['1998-05-19']
1830,['eng'],"['Abe, F']",['Search for Long-Lived Parents of $Z^{0}$ Bosons in $p\\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'new particle, lifetime', 'quark, pair production', 'quark, decay', 'family, 4', 'Z0, leptonic decay', 'channel cross section, branching ratio', 'upper limit', 'track data analysis, vertex', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805017'],"['We search for new long-lived particles which decay to Z bosons by looking for Z->e+e- decays with displaced vertices. We find no evidence for parent particles of the Z with long lifetimes in 90 pb-1 of data from the CDF experiment at Fermilab. We set a cross section limit as a function of the lifetime of the parent particle for both a generic Z parent and a fourth-generation, charge -1/3 quark that decays into Z+b.']",['1998-05-18']
1831,['eng'],"['Breitweg, J']",['Forward Jet Production in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'production, small-angle', 'small-x', 'showers, parton', 'Lipatov equation', 'Altarelli-Parisi equation', 'color, dipole', 'quantum chromodynamics, perturbation theory', 'channel cross section, x-dependence', 'numerical calculations, Monte Carlo', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805016'],"['The inclusive forward jet cross section in deep inelastic $e^+p$ scattering has been measured in the region of $x$--Bjorken, ~$4.5 \\cdot 10^{-4}$~ to ~$4.5 BFKL--like parton shower evolution. The cross section at hadron level as a function of \\xbj is compared to cross sections predicted by various Monte Carlo models. An excess of forward jet production at small \\xbj is observed, which is not reproduced by models based on DGLAP parton shower evolution. The Colour Dipole model describes the data reasonably well. Predictions of perturbative QCD calculations at the parton level based on BFKL and DGLAP parton evolution are discussed in the context of this measurement.']",['1998-05-18']
1832,['eng'],"['Jungmann, K']",['Searching New Physics in Muonium Atom'],['Particle Physics - Experimental Results'],"['muon+ nucleus, interaction', 'silicon, oxygen', 'muonium, production', 'muonium, transition', 'muonium, antiparticle', 'upper limit', 'muon, magnetic moment', 'gauge boson, dilepton', 'mass, lower limit', 'grand unified theory', 'supersymmetry', 'magnetic spectrometer, experimental results', 'PSI Cycl']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805015'],"['Quantum Electrodynamics describes electromagnetic interactions of free muons and of muon and electron in the muonium atom to very high accuracy. Contributions of other and yet unknown interactions can be investigated in precision experiments, e.g. by searching for muonium-antimuonium conversion and by measuring the muon magnetic anomaly.']",['1998-05-15']
1833,['eng'],"['Jungmann, K']",['Results from recent searches for muonium-antimuonium conversion and future perspectives'],['Particle Physics - Experimental Results'],"['talk, Tsukuba 1998/03/04', 'muon+ nucleus, interaction', 'silicon, oxygen', 'muonium, production', 'muonium, transition', 'upper limit', 'muonium, antiparticle', 'particle identification, (muon- positron)', 'gauge boson, dilepton', 'mass, lower limit', 'grand unified theory', 'supersymmetry', 'R parity, violation', 'neutrino/mu, mass', 'magnetic spectrometer, experimental results', 'PSI Cycl']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805014'],"['A positive muon ($\\mu^+$) and an electron ($e^-$) form the the hydrogen-like muonium atom ($M$=$\\mu^+ e^-$). Since it consists of two leptonic particles which are according to present knowledge point-like, accurate calculations of its level energies can be performed in the framework of standard theory. In particular, the theoretical description of this system is possible almost exclusively by Quantum Electrodynamics (QED) which has been verified in various very high precision experiments. Due to the close confinement of the bound state the muonium atom renders in addition the possibility for sensitive searches for electron--muon interactions not included in the standard model. Such exotic processes could affect the energy of the quantum states at a level of the same order of magnitude as the precision achievable in modern spectroscopic experiments.Oscillations between muonium and antimuonium ($\\bar{M}$=$\\mu^- e^+$) would violate separate additive lepton number conservation which is a purely empirical law.']",['1998-05-15']
1834,['eng'],"['Willmann, L', 'Jungmann, K']",['The Muonium Atom as a Probe of Physics beyond the Standard Model'],['Particle Physics - Experimental Results'],"['muonium, transition', 'muonium, antiparticle', 'time dependence', 'electroweak interaction, validity test', 'violation, flavor', 'four-fermion interaction, coupling constant', 'Higgs particle, exchange', 'neutrino, Majorana', 'neutrino, mass', 'supersymmetry', 'tau, sneutrino', 'gauge boson, dilepton', 'muon+ nucleus, interaction', 'muonium, production', 'argon', 'silicon, oxygen', 'aluminum', 'electron electron, interaction', 'muon-, pair production', 'muonium, particle identification', 'particle identification, (muon- positron)', 'muon-, leptonic decay', 'experimental methods', 'interpretation of experiments', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805013'],['The observed interactions between particles are not fully explained in the successful theoretical description of the standard model to date. Due to the close confinement of the bound state muonium ($M = \\mu^+ e^-$) can be used as an ideal probe of quantum electrodynamics and weak interaction and also for a search for additional interactions between leptons. Of special interest is the lepton number violating process of sponteanous conversion of muonium to antimuonium.'],['1998-05-15']
1835,['eng'],"['Meyer, V', 'Grossmann, A', 'Jungmann, K', 'Merkel, J', 'zu Putlitz, G', 'Reinhard, I', 'Träger, K', 'Schmidt, P V', 'Willmann, L', 'Engfer, R', 'Wirtz, H P', 'Abela, R', 'Bertl, W', 'Renker, D', 'Walter, H K', 'Karpukhin, V V', 'Kisel, I V', 'Korenchenko, A S', 'Korenchenko, S M', 'Kravchuk, N', 'Kuchinskii, N A', 'Moiseenko, A', 'Bagaturia, Yu S', 'Mzhavia, D A', 'Sakhelashvili, T M', 'Hughes, V W']",['Increased Sensitivity to Possible Muonium to Antimuonium Conversion'],['Particle Physics - Experimental Results'],"['muon+ nucleus, interaction', 'silicon, oxygen', 'muonium, production', 'muonium, transition', 'upper limit', 'muonium, antiparticle', 'particle identification, (muon- positron)', 'gauge boson, dilepton', 'mass, lower limit', 'supersymmetry', 'symmetry, left-right', 'muon+, leptonic decay', 'violation, flavor', 'magnetic spectrometer, experimental results', 'PSI Cycl']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805012'],"['A new experimental search for muonium-antimuonium conversion was conducted at the Paul Scherrer Institute, Villigen, Switzerland. The preliminary analysis yielded one event fulfilling all required criteria at an expected background of 1.7(2) events due to accidental coincidences. An upper limit for the conversion probability in 0.1 T magnetic field is extracted as $8 \\cdot 10^{-11}$ (90% CL).']",['1998-05-15']
1836,['eng'],"['Sinclair, L E']",['Dynamics of Multijet Processes in Photoproduction'],['Particle Physics - Experimental Results'],"['talk, Brussels 1998/04/04', 'positron p, colliding beams', 'momentum transfer, low', 'jet, hadroproduction', 'jet, multiple production', 'angular distribution, (3jet)', 'mass spectrum, (3jet)', 'transverse energy, high', 'phase space', 'showers, parton', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805010'],"['The cross section for producing three high transverse energy jets with a three-jet invariant mass of M_3J > 50 GeV has been measured in photoproduction at HERA. The angular distribution of the three jets is presented and found to be inconsistent with a uniform population of the available phase space. In contrast, parton shower models and O(alpha alpha_s^2) pQCD calculations are able to describe the three jet dynamics.']",['1998-05-14']
1837,['eng'],"['Abbott, B']",['Determination of the Absolute Jet Energy Scale in the D0 Calorimeters'],['Detectors and Experimental Techniques'],"['anti-p p, colliding beams', 'jet, hadroproduction', 'jet, energy', 'calorimeter, liquid argon', 'uranium', 'energy, calibration', 'transverse energy, missing-energy', 'energy dependence', 'rapidity dependence', 'numerical calculations, Monte Carlo', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll', '630, 1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805009'],"['The DZERO detector is used to study proton-antiproton collisions at the 1800 GeV and 630 GeV center-of-mass energies available at the Fermilab Tevatron. To measure jets, the detector uses a sampling calorimeter composed of uranium and liquid argon as the passive and active media respectively. Understanding the jet energy calibration is not only crucial for precision tests of QCD, but also for the measurement of particle masses and the determination of physics backgrounds associated with new phenomena. This paper describes the energy calibration of jets observed with the DZERO detector at the two proton-antiproton center-of-mass energies in the transverse energy and pseudorapidity range ET>8 GeV and pseudorapidity<3.']",['1998-05-13']
1838,['eng'],"['Söldner-Rembold, S']",['Testing QCD in Photon-Photon Interactions'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 1998/02/15', 'electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'exchange, two-photon', 'photon photon, interaction', 'photon, structure function', 'momentum transfer, dependence', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'jet, photoproduction', 'final state, (2jet)', 'hadron, photoproduction', 'differential cross section, transverse momentum', 'cross section, energy dependence', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805008'],['At high energies photon-photon interactions are dominated by quantum fluctuations of the photons into fermion-antifermion pairs and into vector mesons. This is called photon structure. Electron-positron collisions at LEP are an ideal laboratory for studying photon structure and for testing QCD.'],['1998-05-13']
1839,['eng'],"['Erhan, S']","[""Beauty '97 Conference Summary""]",['Particle Physics - Experimental Results'],"['conference, review', 'Santa Monica 1997/10/13', 'violation, CP', 'B, decay', 'B0 anti-B0, oscillation', 'Kobayashi-Maskawa angle', 'unitarity', 'particle identification, beauty', 'B0, mass difference', 'electron positron, annihilation', 'B, pair production', 'energy, asymmetry', 'anti-p p, colliding beam detector', 'electron p, interaction', 'counters and detectors, gas', 'readout, microstrip', 'semiconductor detector, vertex', 'trigger', 'B, particle source', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805007'],"['CP-violation is one of the least understood phenomena in our field. There are major experimental programs in all high energy laboratories around the world which will hopefully remedy this within the next decade. The study of CP-violating effects in B meson decays will allow stringent tests of the Standard Model to be made and may point the way to New Physics. The Beauty97 conference provided a forum for these experiments to discuss their physics potential and experimental challenges relating to these studies. This paper reviews the ongoing and future experimental B-physics projects. I will summarize the status and future plans of these projects, as well as the highlights of the physics and key R&D results presented at the conference. At the end, a critical comparison of the CP-violation B experiments will be given.']",['1998-05-12']
1840,['eng'],"['Fukuda, Y', 'Hayakawa, T', 'Ichihara, E', 'Inoue, K', 'Ishihara, K', 'Ishino, H', 'Itow, Y', 'Kajita, T', 'Kameda, J', 'Kasuga, S', 'Kobayashi, K', 'Kobayashi, Y', 'Koshio, Y', 'Martens, K', 'Miura, M', 'Nakahata, M', 'Nakayama, S', 'Okada, A', 'Oketa, M', 'Okumura, K', 'Ota, M', 'Sakurai, N', 'Shiozawa, M', 'Suzuki, Y', 'Takeuchi, Y', 'Totsuka, Y', 'Yamada, S', 'Earl, M A', 'Habig, A', 'Kearns, E T', 'Kim, S B', 'Messier, M D', 'Scholberg, K', 'Stone, J L', 'Sulak, Lawrence R', 'Walter, C W', 'Goldhaber, M', 'Barszczak, T', 'Gajewski, W', 'Halverson, P G', 'Hsu, J', 'Kropp, W R', 'Price, L R', 'Reines, F', 'Sobel, H W', 'Vagins, M R', 'Ganezer, K S', 'Keig, W E', 'Ellsworth, R W', 'Tasaka, S', 'Flanagan, J W', 'Kibayashi, A', 'Learned, J G', 'Matsuno, S', 'Stenger, Victor J', 'Takemori, D', 'Ishii, T', 'Kanzaki, J I', 'Kobayashi, T', 'Nakamura, K', 'Nishikawa, K', 'Oyama, Y', 'Sakai, A', 'Sakuda, M', 'Sasaki, O', 'Echigo, S', 'Kohama, M', 'Suzuki, A T', 'Haines, T J', 'Blaufuss, E', 'Sanford, R', 'Svoboda, R', 'Chen, M L', 'Conner, Z', 'Goodman, J A', 'Sullivan, G W', 'Mori, M', 'Hill, J', 'Jung, C K', 'Mauger, C', 'McGrew, C', 'Sharkey, E', 'Viren, B M', 'Yanagisawa, C', 'Doki, W', 'Ishizuka, T', 'Kitaguchi, Y', 'Koga, H', 'Miyano, K', 'Okazawa, H', 'Saji, C', 'Takahata, M', 'Kusano, A', 'Nagashima, Y', 'Takita, M', 'Yamaguchi, T', 'Yoshida, M', 'Etoh, M', 'Fujita, K', 'Hasegawa, A', 'Hasegawa, T', 'Hatakeyama, S', 'Iwamoto, T', 'Kinebuchi, T', 'Koga, M', 'Maruyama, T', 'Ogawa, H', 'Suzuki, A', 'Tsushima, F', 'Koshiba, M', 'Nemoto, M', 'Nishijima, K', 'Futagami, T', 'Hayato, Y', 'Kanaya, Y', 'Kaneyuki, K', 'Watanabe, Y', 'Kielczewska, D', 'Doyle, R A', 'George, J', 'Stachyra, A', 'Wai, L', 'Wilkes, J', 'Young, K']",['Study Of The Atmospheric Neutrino Flux In The Multi-gev Energy Range'],['Particle Physics - Experimental Results'],"['neutrino/mu, cosmic radiation', 'neutrino/e, cosmic radiation', 'cosmic radiation, energy', 'cosmic radiation, flux', 'flux, ratio', 'angular dependence', 'neutrino nucleon, interaction', 'charged current', 'yield, (muon electron)', 'momentum dependence', 'Cherenkov counter, experimental results', 'deep underground detector, KAMIOKANDE']","['http://www-lib.kek.jp/cgi-bin/img_index?199827041', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805006']","['The atmospheric neutrino flux ratio $\\nu_\\mu/\\nu_e$ and its zenith angle dependence have been measured in the multi-GeV energy range using an exposure of 25.5 kiloton-years of the Super-Kamiokande detector. By comparing the data to a detailed Monte Carlo simulation, the ratio $(\\mu/e)_{DATA}/(\\mu/e)_{MC}$ was measured to be $0.66\\pm0.06(stat.)\\pm0.08(sys.)$. In addition, a strong distortion in the shape of the event zenith angle distribution was observed. The ratio of the number of upward to downward $\\mu$-like events was found to be 0.52$^{+0.07}_{-0.06}(stat.)\\pm0.01(sys.)$, with an expected value of $0.98\\pm0.03(stat.)\\pm0.02(sys.)$, while the same ratio for the $e$-like events was consistent with unity.']",['1998-05-12']
1841,['eng'],"['Abe, K']",['An Improved Test of the Flavor Independence of Strong Interactions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'coupling constant, strong interaction', 'dependence, flavor', 'particle identification, flavor', 'final state, (2jet)', 'final state, (3jet)', 'track data analysis, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.28 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805023'],"['We present an improved comparison of the strong coupling of the gluon to light (q_l=u+d+s), c, and b quarks, determined from multijet rates in flavor-tagged samples of hadronic Z0 decays recorded with the SLC Large Detector at the SLAC Linear Collider between 1993 and 1995. Flavor separation among primary q_l q_l-bar, c c-bar, and b b-bar final states was made on the basis of the reconstructed mass of long-lived heavy-hadron decay vertices, yielding tags with high purity and low bias against >= 3-jet final states. We find alpha_s^c/alpha_s^uds = 1.036+-0.043 (stat) +0.041-0.045 (syst) +0.020-0.018 (theory) and alpha_s^b/alpha_s^uds = 1.004+-0.018 (stat) +0.026-0.031 (syst) +0.018-0.029 (theory).']",['1998-05-21']
1842,['eng'],"['Dreis, H B', 'Eisele, Franz', 'Hildebrandt, M', 'Schmidt, B', 'Sponsel, A', 'Ziegler, M']",['Development of a Scintillating Fibre Detector for HERA-B'],['Detectors and Experimental Techniques'],"['scintillation counter, fibre', 'electrode, readout', 'photoelectron, amplifier', 'radiation, yield', 'radiation, damage', 'performance', 'magnetic detector, HERA-B', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805004'],['A fibre detector with multianode PM readout for high rate applications was developed for the HERA-B spectometer to cover the area near the beampipe. Such a detector has to operate at particle rates up to 2*10**4 mm**(-2) s**(-1) and has to tolerate a radiation dosis up to 1 Mrad/y. The light output of test detectors with different scintillating fibres was measured as well as the light transport through clear fibres to the PM as a function of radiation dosis and different conditions of irradiation. The geometry of the detector is described and results for a full size prototype are presented.'],['1998-05-07']
1843,['eng'],"['Saitô, N']",['Spin Physics with the PHENIX Detector System'],['Detectors and Experimental Techniques'],"['p p, colliding beams', 'p, polarized beam', 'p, structure function', 'structure function, spin', 'cross section, helicity', 'photon, direct production', 'W, hadroproduction', 'W, leptonic decay', 'muon, transverse momentum', 'gluon, polarization', 'antiquark, polarization', 'parity, violation', 'numerical calculations, Monte Carlo', 'magnetic detector, PHENIX', 'efficiency', 'proposed experiment, Brookhaven RHIC Coll', '200, 500 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805003'],['The PHENIX experiment at RHIC has extended its scope to cover spin physics using polarized proton beams. The major goals of the spin physics at RHIC are elucidation of the spin structure of the nucleon and precision tests of the symmetries. Sensitivities of the spin physics measurements with the PHENIX detector system are reviewed.'],['1998-05-05']
1844,['eng'],"['Asaoka, Y', 'Abe, K', 'Yoshimura, K', 'Ishino, M', 'Fujikawa, M', 'Orito, S']",['Development of a Large-Area Aerogel Cherenkov Counter Onboard BESS'],['Detectors and Experimental Techniques'],"['anti-p, cosmic radiation', 'Cherenkov counter, aerogel', 'Cherenkov counter, threshold', 'photoelectron, amplifier', 'magnetic spectrometer', 'tracks, energy loss', 'efficiency', 'particle identification, (anti-p muon)', 'optics, dispersion']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805001'],"['This paper describes the development of a threshold type aerogel Cherenkov counter with a large sensitive area of 0.6 m$^2$ to be carried onboard the BESS rigidity spectrometer to detect cosmic-ray antiprotons. The design incorporates a large diffusion box containing 46 finemesh photomultipliers, with special attention being paid to achieving good performance under a magnetic field and providing sufficient endurance while minimizing material usage. The refractive index of the aerogel was chosen to be 1.03. By utilizing the muons and protons accumulated during the cosmic-ray measurements at sea level, a rejection factor of 10$^4$ was obtained against muons with $\\beta \\approx 1$, while keeping 97% efficiency for protons below the threshold.']",['1998-05-04']
1845,['eng'],"['Abe, K']","['Production of $\\pi^{+}, K^{+}, K^{0}, K^{*0}, \\phi, p$ and $\\Lambda^{0}$ in Hadronic $Z^{0}$ Decays']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'hadron, multiple production', 'pi', 'K', 'K*(892)', 'Phi(1020)', 'p', 'Lambda', 'dependence, flavor', 'differential cross section, momentum dependence', 'quantum chromodynamics, perturbation theory', 'duality, parton hadron', 'leading logarithm approximation', 'channel cross section', 'model, fragmentation', 'yield, ratio', 'yield, (particle antiparticle)', 'production, strangeness', 'quark, jet', 'effect, leading particle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'tables', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805029'],"['We have measured the differential production cross sections as a function of scaled momentum x_p=2p/E_cm of the identified hadron species pi+, K+, K0, K*0, phi, p, Lambda0, and of the corresponding antihadron species in inclusive hadronic Z0 decays, as well as separately for Z0 decays into light (u, d, s), c and b flavors. Clear flavor dependences are observed, consistent with expectations based upon previously measured production and decay properties of heavy hadrons. These results were used to test the QCD predictions of Gribov and Lipatov, the predictions of QCD in the Modified Leading Logarithm Approximation with the ansatz of Local Parton-Hadron Duality, and the predictions of three fragmentation models. Ratios of production of different hadron species were also measured as a function of x_p and were used to study the suppression of strange meson, strange and non-strange baryon, and vector meson production in the jet fragmentation process. The light-flavor results provide improved tests of the above predictions, as they remove the contribution of heavy hadron production and decay from that of the rest of the fragmentation process. In addition we have compared hadron and antihadron production as a function of x_p in light quark (as opposed to antiquark) jets. Differences are observed at high x_p, providing direct evidence that higher-momentum hadrons are more likely to contain a primary quark or antiquark. The differences for pseudoscalar and vector kaons provide new measurements of strangeness suppression for high-x_p fragmentation products.']",['1998-05-26']
1846,['eng'],"['Browder, T E']","[""Observation of High Momentum $\\eta'$ Production in B Decay""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'eta(958), momentum', 'mass spectrum', 'production, strangeness', 'B, branching ratio', 'Feynman graph, penguin', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> eta(958) anything', 'B --> eta(958) K (n)pi', 'beauty --> strangeness gluon', 'approx. 10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804018'],"[""We report the first observation of $B\\to \\eta' X$ transitions with high momentum $\\eta'$ mesons. We observe $39.0\\pm 11.6$ $B$ decay events with $2.0< p_{\\eta'} < 2.7$ GeV/c, the high momentum region where background from $b\\to c$ processes is suppressed. We discuss the physical interpretation of the signal, including the possibility that it is due to $b\\to s g^*$ transitions. Given that interpretation, we find ${\\cal B}(B\\to \\eta' X_s) = (6.2 \\pm 1.6(stat) \\pm 1.3(sys)^{+0.0}_{-1.5}(bkg))\\times 10^{-4} $ for $2.0<p_{\\eta'}<2.7$ GeV/c.""]",['1998-05-01']
1847,['eng'],"['Klima, B']",['D0 Findings on the Top Quark'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1998/03/01', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay modes', 'final state, dilepton', 'final state, ((n)jet lepton)', 'final state, ((n)jet)', 'mass, truth', 'channel cross section', 'Higgs particle, search for', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'truth --> W beauty', 'truth --> Higgs particle+ beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804017'],"['Recent results on top quark physics with the D0 experiment in pbar-p collisions at sqrt(s) = 1.8 TeV for an integrated luminosity of 125 pb**-1 are reported. The direct measurement of the top quark mass uses single lepton and dilepton events, giving the result m(top) = 172.1 +/- 7.1 GeV/c**2. The measurement of the t-tbar production cross section includes analyses from 9 top decay channels: dilepton (t-tbar --> e+mu, e+e, and mu+mu), electron and neutrino (t-tbar --> e+nu), single leptons (t-tbar --> e + jets, t-tbar --> mu + jets) with and without b tagging, and all-jets (t-tbar --> 6 jets). We measure the t-tbar production cross section to be 5.9 +/- 1.7 pb at m(top) = 172.1 GeV/c**2. Combining the D0 and the CDF measurements of the top quark mass and combining their t-tbar cross sections, in both cases taking into account error correlations, yields unofficially sigma(t-tbar) = 6.7 +/- 1.3 pb at an averaged top quark mass of m(top) = 173.8 +/- 5.2 GeV/c**2. Preliminary results on a search for charged Higgs production in top events, t --> Higgs + b, are presented.']",['1998-04-30']
1848,['eng'],"['Hofer, H', 'Pohl, M']",['Charge Determination of High Energy Electrons and Nuclei by Synchrotron Radiation with AMS'],['Detectors and Experimental Techniques'],"['positron, cosmic radiation', 'electron, cosmic radiation', 'nucleus, cosmic radiation', 'cosmic radiation, momentum spectrum', 'charge, measurement', 'magnetic field, geophysics', 'synchrotron radiation', 'photon, energy spectrum', 'photon, yield', 'momentum dependence', 'magnetic spectrometer, satellite', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804016'],"[""We investigate the possibilities to identify the charge of TeV electrons and PeV nuclei using their synchrotron radiation in the earth's magnetic field. Characteristics of synchrotron radiation photons are evaluated and methods of detection are discussed.""]",['1998-04-29']
1849,['eng'],"['Warburton, A T']",['A Study of Exclusive Nonleptonic Decays of B Mesons into Final States of Strange Mesons and 1S or 2S Charmonia'],['Particle Physics - Experimental Results'],"['thesis', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B, hadronic decay', 'B0, branching ratio', 'B+, branching ratio', 'J/psi(3100)', 'psi(3685)', 'K*(892)', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', 'B0 --> psi mesons K*(892)', 'B+ --> psi mesons K+', 'psi mesons --> muon+ muon-', 'psi(3685) --> J/psi(3100) pi+ pi-', 'K*(892) --> K+ pi-', '1800 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0108046'],"['[abridged] Bound states of heavy quarks can serve as a laboratory for inquiry into the behaviour of the fundamental strong and electroweak interactions. This thesis examines observations of B0, B0bar, and B+- mesons produced in proton-antiproton collisions at centre-of-mass energies of sqrt{s}=1.8 TeV. The B-meson decay products are recorded using the Collider Detector at Fermilab (CDF) located on the Tevatron collider at Fermilab, USA. Four B-meson decays and their charge conjugates are studied: B+ -> J/psi K+, B0 -> J/psi K*(892)0, B+ -> psi(2S) K+, and B0 -> psi(2S) K*(892)0. Using a data sample corresponding to a time-integrated luminosity of (109 +- 7)/pb, statistically significant signals are observed in all the channels. Topological similarities between the B decays are exploited to measure the six relative branching fractions (Br) of each channel with respect to the other channels. The ratios involving the B+ -> J/psi K+ mode are Br(B0 -> J/psi K*(892)0) / Br(B+ -> J/psi K+) = 1.76 +- 0.14[stat] +- 0.15[syst], Br(B+ -> psi(2S) K+) / Br(B+ -> J/psi K+) = 0.558 +- 0.082[stat] +- 0.056[syst], and Br(B0 -> psi(2S) K*(892)0) / Br(B+ -> J/psi K+) = 0.908 +- 0.194[stat] +- 0.100[syst]. The indicated uncertainties are statistical and systematic, respectively. In ratios involving unlike B-meson species, equal production rates for B+ and B0 mesons have been assumed. The B+ -> psi(2S) K+ and B0 -> psi(2S) K*(892)0 reconstructions are the first observations of these processes at a hadron collider. The branching-fraction ratio measurements are consistent with phenomenological predictions that employ the factorization Ansatz, and the derived absolute branching-fraction measurements are consistent with previous world-average limits and values from e+e- colliders. [abridged]']",['2001-08-31']
1850,['eng'],"['Breitweg, J']",['Diffractive Dijet Cross Sections in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'final state, (2jet)', 'rapidity, gap', 'diffraction, structure function', 'hard scattering', 'differential cross section, momentum dependence', 'transverse energy, dependence', 'rapidity dependence', 'photon, momentum spectrum', 'photon, resolved', 'momentum spectrum, pomeron', 'structure function, pomeron', 'quark', 'gluon', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804013'],['Differential dijet cross sections have been measured with the ZEUS detector for photoproduction events in which the hadronic final state containing the jets is separated with respect to the outgoing proton direction by a large rapidity gap. The cross section has been measured as a function of the fraction of the photon (x_gamma^OBS) and pomeron (beta^OBS) momentum participating in the production of the dijet system. The observed x_gamma^OBS dependence shows evidence for the presence of a resolved- as well as a direct-photon component. The measured cross section d(sigma)/d(beta^OBS) increases as beta^OBS increases indicating that there is a sizeable contribution to dijet production from those events in which a large fraction of the pomeron momentum participates in the hard scattering. These cross sections and the ZEUS measurements of the diffractive structure function can be described by calculations based on parton densities in the pomeron which evolve according to the QCD evolution equations and include a substantial hard momentum component of gluons in the pomeron.'],['1998-04-24']
1851,['eng'],"['Abe, F']",['Observation of $B_c$ Mesons in $p\\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B/c, hadroproduction', 'B/c, semileptonic decay', 'mass spectrum, (J/psi(3100) lepton)', 'mass, B/c', 'final state, (3lepton)', 'B/c, lifetime', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> B/c anything', 'B/c --> J/psi(3100) lepton anything', 'B/c --> J/psi(3100) lepton neutrino', 'B/c --> J/psi(3100) K+', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804014'],"['We report the observation of bottom-charmed mesons B_c in 1.8 TeV p-bar p collisions using the CDF detector at the Fermilab Tevatron. The B_c mesons were found through their semileptonic decays, B_c -> J/psi lepton X. A fit to the J/psi lepton mass distribution yielded 20.4 +6.2 -5.5 events from B_c mesons. A test of the null hypothesis, i.e. an attempt to fit the data with background alone, was rejected at the level of 4.8 standard deviations. By studying the quality of the fit as a function of the assumed B_c mass, we determined M(B_c) = 6.40 +- 0.39 +- 0.13 GeV/c^2. From the distribution of trilepton intersection points in the plane transverse to the beam direction we measured the B_c lifetime to be tau(B_c) = 0.46 +0.18 -0.16 +- 0.03 ps. We also measured the ratio of production cross section times branching fraction for B_c -> J/psi lepton neutrino relative to that for B+ -> J/psi K to be: 0.132 +0.041 -0.037 (stat) +- 0.031 (syst) +0.032 -0.020 (lifetime)']",['1998-04-24']
1852,['eng'],"['Lingel, K', 'Skwarnicki, T', 'Smith, J G']",['Penguin decays of B mesons'],['Particle Physics - Experimental Results'],"['review, experimental results', 'B, decay modes', 'B/s0, decay modes', 'Feynman graph, penguin', 'neutral current, flavor changing', 'Kobayashi-Maskawa angle', 'anti-p p, interaction', 'electron positron, annihilation', 'quark, beauty', 'quark, pair production', 'quark, radiative decay', 'quark, semileptonic decay', 'quark, hadronic decay', 'beautiful meson, branching ratio', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804015'],"[""Penguin, or loop, decays of B mesons induce effective flavor-changing neutral currents, which are forbidden at tree level in the Standard Model. These decays give special insight into the CKM matrix and are sensitive to non-standard model effects. In this review, we give a historical and theoretical introduction to penguins and a description of the various types of penguin processes: electromagnetic, electroweak, and gluonic. We review the experimental searches for penguin decays, including the measurements of the electromagnetic penguins b -> s gamma and B -> K* gamma and gluonic penguins B -> K pi, B+ -> omega K+ and B -> eta' K, and their implications for the Standard Model and New Physics. We conclude by exploring the future prospects for penguin physics.""]",['1998-04-28']
1853,['eng'],"['Adloff, C']",['Multiplicity Structure of the Hadronic Final State in Diffractive Deep-Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, photoproduction', 'charged particle, multiplicity', 'mass, dependence', 'multiplicity, spectra', 'multiplicity, moment', 'rapidity spectrum', 'rapidity, gap', 'angular correlation', 'photon, dissociation', 'quantum chromodynamics', 'Regge poles', 'diffraction, structure function', 'color, singlet', 'gluon', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 Gev-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804012'],"['The multiplicity structure of the hadronic system X produced in deep-inelastic processes at HERA of the type ep -> eXY, where Y is a hadronic system with mass M_Y< 1.6 GeV and where the squared momentum transfer at the pY vertex, t, is limited to |t|<1 GeV^2, is studied as a function of the invariant mass M_X of the system X. Results are presented on multiplicity distributions and multiplicity moments, rapidity spectra and forward-backward correlations in the centre-of-mass system of X. The data are compared to results in e+e- annihilation, fixed-target lepton-nucleon collisions, hadro-produced diffractive final states and to non-diffractive hadron-hadron collisions. The comparison suggests a production mechanism of virtual photon dissociation which involves a mixture of partonic states and a significant gluon content. The data are well described by a model, based on a QCD-Regge analysis of the diffractive structure function, which assumes a large hard gluonic component of the colourless exchange at low Q^2. A model with soft colour interactions is also successful.']",['1998-04-23']
1854,['eng'],[],['The D0 Detector at TeV33'],['Detectors and Experimental Techniques'],"['four-pi-detector, DZERO', 'calorimeter', 'scintillation counter, fibre', 'muon, counters and detectors', 'semiconductor detector, vertex', 'trigger', 'luminosity', 'Batavia TEVATRON Coll', 'upgrade, proposed']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804011'],"['The physics that can be done with 30 fb$^{-1}$ of data at the Tevatron (TeV33) will significantly advance our understanding of particle physics. In this document we consider the potential of the DO detector for running with the TeV33 Collider. In that era, the instantaneous luminosity is expected to rise by a factor of two to five. We show that the DO detector will perform well with some relatively modest modifications.']",['1998-04-23']
1855,['eng'],"['Harris, D A', 'McFarland, K S']",['A small target neutrino deep-inelastic scattering experiment at the first Muon Collider'],['Detectors and Experimental Techniques'],"['talk, Batavia 1997/11/06', 'muon+ muon-, storage ring', 'storage ring, proposed', 'neutrino, secondary beam', 'neutrino, flux', 'neutrino nucleus, deep inelastic scattering', 'strong interaction, coupling constant', 'polarized target', 'quark, spin', 'nucleon, structure function', 'dependence, mass number', 'neutral current, coupling', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804010'],"['Several different scenarios for neutrino scattering experiments using a neutrino beam from the muon collider complex are discussed. The physics reach of a neutrino experiment at the front end of a muon collider is shown to extend far beyond that of current neutrino experiments, since the high intensity neutrino beams one would see at the muon collider allow for a large flexibility in choosing neutrino targets. Measurements of quark spin, A-dependence of the structure function $xF_3$ and neutral current chiral couplings to quarks are outlined.']",['1998-04-21']
1856,['eng'],"['Harris, D A', 'McFarland, K S']",['Detectors for Neutrino Physics at the First Muon Collider'],['Detectors and Experimental Techniques'],"['talk, Batavia 1997/11/06', 'muon+ muon-, storage ring', 'storage ring, proposed', 'neutrino, secondary beam', 'neutrino, flux', 'neutrino nucleus, deep inelastic scattering', 'counters and detectors, proposed', 'neutrino, oscillation', 'muon, background', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804009'],"[""We consider possible detector designs for short-baseline neutrino experiments using neutrino beams produced at the First Muon Collider complex. The high fluxes available at the muon collider make possible high statistics deep-inelastic scattering neutrino experiments with a low-mass target. A design of a low-energy neutrino oscillation experiment on the ``tabletop'' scale is also discussed.""]",['1998-04-21']
1857,['eng'],"['Halzen, Francis']",['The AMANDA Neutrino Telescope and the Indirect Search for Dark Matter'],['Detectors and Experimental Techniques'],"['talk, Santa Monica 1998/02/18', 'astrophysics, missing-mass', 'WIMP, annihilation', 'neutrino, counters and detectors', 'neutrino nucleon, interaction', 'charged current', 'muon, cosmic radiation', 'angular distribution', 'Cherenkov counter, water', 'deep underground detector, AMANDA', 'performance']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804007'],"['With an effective telescope area of order 10^4 m^2, a threshold of ~50 GeV and a pointing accuracy of 2.5 degrees, the AMANDA detector represents the first of a new generation of high energy neutrino telescopes, reaching a scale envisaged over 25 years ago. We describe its performance, focussing on the capability to detect halo dark matter particles via their annihilation into neutrinos.']",['1998-04-17']
1858,['eng'],"['Morrison, D P']",['The PHENIX Experiment at RHIC'],['Particle Physics - Experimental Results'],"['scattering, heavy ion', 'critical phenomena, confinement', 'symmetry, chiral', 'J/psi(3100), hadroproduction', 'photon, direct production', 'lepton, pair production', 'correlation', 'magnetic detector, PHENIX', 'proposed experiment, Brookhaven RHIC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804004'],['The physics emphases of the PHENIX collaboration and the design and current status of the PHENIX detector are discussed. The plan of the collaboration for making the most effective use of the available luminosity in the first years of RHIC operation is also presented.'],['1998-04-07']
1859,['eng'],"['Altegoer, J', 'Astier, P', 'Autiero, D', 'Baldisseri, A', 'Baldo-Ceolin, Massimilla', 'Ballocchi, G', 'Banner, M', 'Basa, S', 'Bassompierre, Gabriel', 'Benslama, K', 'Besson, N', 'Bird, I G', 'Blumenfeld, B', 'Bobisut, F', 'Bouchez, J', 'Boyd, S', 'Bueno, A G', 'Bunyatov, S A', 'Camilleri, L L', 'Cardini, A', 'Castera, A', 'Cattaneo, Paolo Walter', 'Cavasinni, V', 'Cervera-Villanueva, A', 'Collazuol, G', 'Conforto, G', 'Conta, C', 'Contalbrigo, M', 'Cousins, R D', 'Daniels, D C', 'De Santo, A', 'Del Prete, T', 'Dignan, T', 'Di Lella, Luigi', 'do Couto e Silva, E', 'Donnelly, I J', 'Dumarchez, J', 'Fazio, T', 'Feldman, G J', 'Ferrari, R', 'Ferrère, D', 'Flaminio, Vincenzo', 'Fraternali, M', 'Gaillard, Jean-Marc', 'Galumian, P I', 'Gangler, E', 'Geiser, A', 'Geppert, D', 'Gibin, D', 'Gninenko, S N', 'Gómez-Cadenas, J J', 'Gosset, J', 'Gössling, C', 'Gouanère, M', 'Grant, A', 'Graziani, G', 'Guglielmi, A M', 'Hagner, C', 'Hernando, J', 'Hubbard, D B', 'Hurst, P', 'Hyett, N', 'Iacopini, E', 'Joseph, C L', 'Kekez, D', 'Kirsanov, M M', 'Klimov, O L', 'Kokkonen, J', 'Kovzelev, A', 'Kuznetsov, V E', 'Lacaprara, S', 'Lanza, A', 'La Rotonda, L', 'Laveder, M', 'Letessier-Selvon, A A', 'Lévy, J M', 'Linssen, L', 'Ljubicic, A', 'Long, J', 'Lupi, A', 'Manola-Poggioli, E', 'Marchionni, A', 'Martelli, F', 'Méchain, X', 'Mendiburu, J P', 'Meyer, J P', 'Mezzetto, M', 'Mishra, S R', 'Moorhead, G F', 'Mossuz, L', 'Nédélec, P', 'Nefedov, Yu A', 'Nguyen-Mau, C', 'Orestano, D', 'Pastore, F', 'Peak, L S', 'Pennacchio, E', 'Perroud, J P', 'Pessard, H', 'Petti, R', 'Placci, Alfredo', 'Plothow-Besch, Hartmute', 'Pluquet, A', 'Polesello, G', 'Pollmann, D', 'Pope, B G', 'Popov, B A', 'Poulsen, C', 'Rathouit, P', 'Roda, C', 'Rubbia, André', 'Salvatore, F', 'Scannicchio, D', 'Schahmaneche, K', 'Schmidt, B', 'Sconza, A', 'Serrano, M', 'Sevior, M E', 'Sillou, D', 'Soler, F J P', 'Sozzi, G', 'Steele, D', 'Steffen, P', 'Steininger, M', 'Stiegler, U', 'Stipcevic, M', 'Stolarczyk, T', 'Tareb-Reyes, M', 'Taylor, G N', 'Tereshchenko, S', 'Toropin, A N', 'Touchard, A M', 'Tovey, S N', 'Tran, M T', 'Tsesmelis, Emmanuel', 'Ulrichs, J', 'Urós, V', 'Valdata-Nappi, M', 'Valuev, V Yu', 'Vannucci, François', 'Varvell, K E', 'Veltri, M', 'Vercesi, V', 'Verkindt, D', 'Vieira, J M', 'Vinogradova, T G', 'Vo, M K', 'Volkov, S', 'Weber, F', 'Weisse, T', 'Werlen, M', 'Wilson, F F', 'Winton, L J', 'Yabsley, B D', 'Zaccone, H', 'Zuber, K']",['Search for a new gauge boson in $\\pi^{0}$ decays'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'pi0, hadroproduction', 'pi0, radiative decay', 'gauge boson, search for', 'scattering, gauge boson nucleus', 'Primakoff effect', 'pi0, branching ratio', 'coupling, (gauge boson quark)', 'upper limit', 'experimental results', 'CERN SPS', 'pi0 --> gauge boson photon', 'gauge boson nucleus --> nucleus pi0', '450 GeV']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804003', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ep-98-047']","[""A search was made for a new light gauge boson $X$ which might be produced in $\\pi^{0}\\rightarrow\\gamma + X$ decay from neutral pions generated by 450-GeV protons in the CERN SPS neutrino target. Th e X's would penetrate the downstream shielding and be observed in the NOMAD detector via the Primakoff effect, in the process of $X \\rightarrow\\pi^{0}$ conversion in the external Coulomb field of a nucleus.\\ With $1.45\\times10^{18}$ protons on target, 20 candidate events with energy between 8 and 140 GeV were found from the analysis of neutrino data.\\ This number is in agreement with the e xpectation of 18.1$\\pm$2.8 background events from standard neutrino processes.\\ A new 90 $\\% ~C.L.$ upper limit on the branching ratio $Br(\\pi^{0}\\rightarrow\\gamma + X)<$ (3.3~to~1.9)$\\times10^{-5}$ for $X$ masses ranging from 0 to 120 MeV/c$^{2}$ is obtained.""]",['1998-04-16']
1860,['eng'],"['Achasov, M N', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Koshuba, S V', 'Lysenko, A P', 'Pakhtusova, E V', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Serednyakov, S I', 'Valishev, A A', 'Usov, Yu V']",['Study of $\\Delta(1232)$ isobar electroproduction at VEPP-2M $e^{+}e^-$ collider'],['Particle Physics - Experimental Results'],"['electron positron, storage ring', 'electron nucleus, inclusive reaction', 'gas, background', 'Delta(1232)+, electroproduction', 'Delta(1232)+, hadronic decay', 'mass spectrum, (p pi0)', 'pi0, angular distribution', 'experimental results', 'Novosibirsk Stor2']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804002'],"['Results from the Spherical Nonmagnetic Detector (SND) on $\\Delta (1232)$ isobar electroproduction in the collisions of beam electrons (positrons) and residual gas nuclei in the VEPP-2M $e^+e^-$ collider are presented. On the basis of the obtained data the expected counting rate of this process in future high luminosity $e^+e^-$ colliders (~$\\phi$-, $c$-$\\tau$- and $b$-factories) was estimated.']",['1998-04-03']
1861,['eng'],"['Breitweg, J']",['Measurement of Jet Shapes in High-$Q^2$ Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'momentum transfer, high', 'event shape analysis', 'transverse energy, dependence', 'neutral current', 'charged current', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804001'],"['The shapes of jets with transverse energies, E_T(jet), up to 45 GeV produced in neutral- and charged-current deep inelastic e+p scattering (DIS) at Q**2 > 100 GeV**2 have been measured with the ZEUS detector at HERA. Jets are identified using a cone algorithm in the eta-phi plane with a cone radius of one unit. The jets become narrower as E_T(jet) increases. The jet shapes in neutral- and charged-current DIS are found to be very similar. The jets in neutral-current DIS are narrower than those in resolved processes in photoproduction and closer to those in direct-photon processes for the same ranges in E_T(jet) and jet pseudorapidity. The jet shapes in DIS are observed to be similar to those in e+e- interactions and narrower than those in pbarp collisions for comparable E_T(jet). Since the jets in e+e- interactions and e+p DIS are predominantly quark initiated in both cases, the similarity in the jet shapes indicates that the pattern of QCD radiation within a quark jet is to a large extent independent of the hard scattering process in these reactions.']",['1998-04-02']
1862,['eng'],"['Milstene, C', 'Cooper, P S', 'Moinester, M A']",['Kaon Radiative Decay $K^{\\pm} \\to \\mu\\nu\\gamma$ at CKM at the Fermilab Main Injector'],['Particle Physics - Experimental Results'],"['talk, Batavia 1997/05/01', 'K-, radiative decay', 'K-, rare decay', 'Dalitz plot', 'background', 'spectrometer', 'Cherenkov counter, ring imaging', 'acceptance', 'numerical calculations', 'proposed experiment, Fermilab', 'K- --> muon- neutrino photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803033'],"['High statistics data for the K+ -> mu+ nu gamma decay can allow the precision determination of the kaon structure dependent form factors and the kaon polarizability. This study is possible at the proposed FNAL CKM experiment. CKM (Charged Kaons at the Main injector) is a decay-in-flight spectrometer with two RICH, and designed to run at the main injector with a high kaon flux. The radiative decay data will be taken complementary to the primary CKM effort to study the rare kaon decay (K to pi nu nubar) for which CKM was primarily designed. We summarize here the underlying physics of K ->mu nu gamma, the experimental status, and how the CKM spectrometer will be adapted for this study.']",['1998-04-01']
1863,['eng'],"['Adloff, C']",['Hadron Production in Diffractive Deep-Inelastic Scattering'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'diffraction', 'photon, dissociation', 'energy flow, hadronic', 'charged particle, transverse momentum', 'spectra, x-dependence', 'flux, pomeron', 'structure function, pomeron', 'gluon', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803032'],"['Characteristics of hadron production in diffractive deep-inelastic positron-proton scattering are studied using data collected in 1994 by the H1 experiment at HERA. The following distributions are measured in the centre-of-mass frame of the photon dissociation system: the hadronic energy flow, the Feynman-x (x_F) variable for charged particles, the squared transverse momentum of charged particles (p_T^{*2}), and the mean p_T^{*2} as a function of x_F. These distributions are compared with results in the gamma^* p centre-of-mass frame from inclusive deep-inelastic scattering in the fixed-target experiment EMC, and also with the predictions of several Monte Carlo calculations. The data are consistent with a picture in which the partonic structure of the diffractive exchange is dominated at low Q^2 by hard gluons.']",['1998-04-01']
1864,['eng'],"['Ammar, R']",['A Limit on the Mass of the $\\nu_{\\tau}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, semileptonic decay', 'neutrino/tau, mass', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> tau+ tau-', 'tau- --> 5pi neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803031'],"['A limit on the mass of the tau neutrino is derived from 4.5 million tau pairs produced in an integrated luminosity of 5.0 fb^{-1} of electron-positron annihilation to tau pairs at center of mass energies near 10.6 GeV. The measurement technique involves a two-dimensional extended likelihood analysis, including the dependence of the end-point population on the neutrino mass, and allows for the first time an explicit background contribution. We use the decays of the tau to five charged pions and a neutrino as well as the decay to three charged pions, two neutral pions and a neutrino to obtain an upper limit of 30 MeV/c^2 at 95% C.L.']",['1998-04-01']
1865,['eng'],"['Allison, W W M']",['Search for the Proton Decay Mode $p\\rightarrow \\nu K^{+}$ in Soudan 2'],['Particle Physics - Experimental Results'],"['p, semileptonic decay', 'p, branching ratio', 'lower limit', 'K+, decay modes', 'calorimeter, experimental results', 'deep underground detector, Soudan', 'p --> K+ neutrino', 'K+ --> muon+ neutrino', 'K+ --> pi+ pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803030'],"['We have searched for the proton decay mode proton to neutrino K+ using the one-kiloton Soudan 2 high resolution calorimeter. Contained events obtained from a 3.56 kiloton-year fiducial exposure through June 1997 are examined for occurrence of a visible K+ track which decays at rest into mu+ nu or pi+ pi0. We found one candidate event consistent with background, yielding a limit, tau/B > 4.3 10^{31} years at 90% CL with no background subtraction.']",['1998-03-31']
1866,['eng'],"['Barberis, D']",['A study of pseudoscalar states produced centrally in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'central region', 'pseudoscalar meson, hadroproduction', 'pi0, radiative decay', 'eta, radiative decay', 'eta(958), hadronic decay', 'mass spectrum', 'spectra, x-dependence', 'transverse momentum, difference', 'momentum transfer, spectra', 'angular correlation, (2p)', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p pseudoscalar meson', 'eta --> 2photon', 'eta(958) --> pi+ pi- pi0', 'eta(958) --> eta pi+ pi-', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803029'],['A study has been made of pseudoscalar mesons produced centrally in pp interactions. The results show that the eta and etaprime appear to have a similar production mechanism which differs from that of the pi0. The production properties of the eta and etaprime are not consistent with what is expected from double Pomeron exchange. In addition the production mechanism for the eta and etaprime is such that the production cross section are greatest when the azimuthal angle between the pT vectors of the two protons is 90 degrees.'],['1998-03-31']
1867,['eng'],"['Behnke, T', 'Hüntemeyer, P', 'Oh, A', 'Steuerer, J', 'Wagner, A', 'Zeuner, W']",['The Charge Collection Properties of CVD Diamond'],['Detectors and Experimental Techniques'],"['solid-state counter, position sensitive', 'carbon, crystal', 'charge, yield', 'efficiency, time variation']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804006'],"['The charge collection properties of CVD diamond have been investigated with ionising radiation. In this study two CVD diamond samples, prepared with electrical contacts have been used as solid state ionisation chambers. The diamonds have been studied with beta particles and 10 keV photons, providing a homogeneous ionisation density and with protons and alpha particles which are absorbed in a thin surface layer. For the latter case a strong decrease of the signal as function of time is observed, which is attributed to polarisation effects inside the diamond. Spatially resolved measurements with protons show a large variation of the charge collection efficiency, whereas for photons and minimum ionising particles the response is much more uniform and in the order of 18%. These results indicate that the applicability of CVD diamond as a position sensitive particle detector depends on the ionisation type and appears to be promising for homogeneous ionisation densities as provided by relativistic charged particles.']",['1998-04-16']
1868,['eng'],"['Smith, J G']",['First observation of five charmless hadronic B decays'],['Particle Physics - Experimental Results'],"['talk, Santa Barbara 1997/07/07', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charmed particle)', 'Feynman graph, penguin', 'eta(958)', 'omega(783)', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> 2meson', 'B0 --> K pi', 'B0 --> eta(958) K', 'B0 --> omega(783) K', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803028'],"['There has been much progress in measurements of charmless hadronic B decays during 1997. Building on the previous indications from CLEO and LEP, CLEO now has clear signals in five exclusive final states: K^+\\pi^, K^0\\pi^+, etapr K^+, etapr K^0, and omega K^+. The branching fractions for the etapr K modes are several times larger than the others. A similar strikingly large signal has been seen in the inclusive decay, B->etapr X_S. All of these signals would appear to be dominated by hadronic penguin processes. (Invited talk presented at the Seventh International Symposium On Heavy Flavor Physics, Santa Barbara, CA, July 7-11, 1997.)']",['1998-03-30']
1869,['eng'],"['Prinz, A', 'Baggs, R', 'Ballam, J', 'Ecklund, S D', 'Fertig, C', 'Jaros, J A', 'Kase, K', 'Kulikov, A', 'Langeveld, W G J', 'Leonard, R', 'Marvin, T P', 'Nakashima, T', 'Nelson, W R', 'Odian, A C', 'Pertsova, M', 'Putallaz, G', 'Weinstein, A']",['Search for Millicharged Particles at SLAC'],['Particle Physics - Experimental Results'],"['electron nucleus, interaction', 'tungsten, rhenium', 'new particle, search for', 'charge, low', 'charge, fractional', 'matter, ionization', 'energy loss', 'charge, mass', 'production, upper limit', 'scintillation counter, experimental results', 'SLAC Lab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9804008'],"['Particles with electric charge q < 10^(-3)e and masses in the range 1--100 MeV/c^2 are not excluded by present experiments. An experiment uniquely suited to the production and detection of such ""millicharged"" particles has been carried out at SLAC. This experiment is sensitive to the infrequent excitation and ionization of matter expected from the passage of such a particle. Analysis of the data rules out a region of mass and charge, establishing, for example, a 95%-confidence upper limit on electric charge of 4.1X10^(-5)e for millicharged particles of mass 1 MeV/c^2 and 5.8X10^(-4)e for mass 100 MeV/c^2.']",['1998-04-20']
1870,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'List, B', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Utzat, P', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for stable and long-lived massive charged particles in $e^{+} e^{-}$ collisions at $\\sqrt{s}$ = 130-183 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'postulated particle, massive', 'postulated particle, pair production', 'supersymmetry', 'smuon', 'stau', 'lepton, charged particle', 'chargino', 'charge, fractional', 'mass, lower limit', 'channel cross section, upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '130-183 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=EP-98-039', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803026']","['A search for stable and long-lived massive particles of electric charge |Q/e| = 1 or 2/3, pair-produced in e+e- collisions at centre-of-mass energies from 130 to 183 GeV, is reported by the OPAL collaboration at LEP. No evidence for production of these particles was observed in a mass range between 45 and 89.5 GeV. Model-independent upper limits on the production cross-section between 0.05 and 0.19 pb have been derived for scalar and spin-1/2 particles with charge +/-1. Within the framework of the minimal supersymmetric model (MSSM), this implies a lower limit of 82.5 (83.5) GeV on the mass of long-lived right- (left-)handed scalar muons and scalar taus. Long-lived charged leptons and charginos are excluded for masses below 89.5 GeV. For particles with charge +/-2/3 the upper limits on the production cross-section vary between 0.05 and 0.2 pb. All limits, on masses and on cross-sections, are valid at the 95% confidence level for particles with lifetimes longer than 10^{-6} s.']",['1998-03-18']
1871,['eng'],"['Petrera, S']",['Experiments at Large Underground Detectors'],['Particle Physics - Experimental Results'],"['review, Gran Sasso 1997/09/07', 'nucleon, semileptonic decay', 'grand unified theory', 'search for, magnetic monopole', 'neutrino, solar', 'neutrino, astrophysics', 'astrophysics, missing-mass', 'astrophysics, supernova', 'cosmic radiation, flux', 'deep underground detector, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803025'],"['This talk reports a subset of the topics discussed at TAUP97. The topics are: nucleon decay, supermassive monopoles, Neutrino Astrophysics and Cosmic Ray Physics.']",['1998-03-25']
1872,['eng'],"['Kirk, A']",['A search for non-$q\\bar{q}$ mesons at the CERN Omega Spectrometer'],['Particle Physics - Experimental Results'],"['p p, inelastic scattering', 'meson resonance, hadroproduction', 'meson, hybrid', 'glueball', 'gluon, exchange', 'quark, exchange', 'exchange, (2pomeron)', 'transverse momentum, difference', 'mass spectrum, (pi+ pi-)', 'mass spectrum, (K+ K-)', 'mass spectrum, (2pi+ 2pi-)', 'f0(1500)', 'f0(1710)', 'postulated particle, f2(1900)', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p meson', '85, 300, 450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803024'],"['The non-Abelian nature of QCD suggests that particles that have a gluon constituent, such as glueballs or hybrids, should exist. Experiments WA76, WA91 and WA102 have performed a dedicated search for these states in central production using the CERN Omega Spectrometer. Several non-qqbar candidates have been observed. This paper presents a study of central meson production as a function of the difference in transverse momentum (dPT) of the exchanged particles which shows that undisputed qqbar mesons are suppressed at small dPT whereas the glueball candidates are enhanced.']",['1998-03-25']
1873,['eng'],"['Ambrosio, M']",['The Observation of Up-going Charged Particles Produced by High Energy Muons in Underground Detectors'],['Particle Physics - Experimental Results'],"['muon, cosmic radiation', 'muon nucleus, interaction', 'pi, electroproduction', 'angular distribution', 'pi, particle identification', 'efficiency', 'neutrino/mu, particle identification', 'background', 'numerical calculations, Monte Carlo', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9807032'],"['An experimental study of the production of up-going charged particles in inelastic interactions of down-going underground muons is reported, using data obtained from the MACRO detector at the Gran Sasso Laboratory. In a sample of 12.2 10^6 single muons, corresponding to a detector livetime of 1.55 y, 243 events are observed having an up-going particle associated with a down-going muon. These events are analysed to determine the range and emission angle distributions of the up-going particle, corrected for detection and reconstruction efficiency. Measurements of the muon neutrino flux by underground detectors are often based on the observation of through-going and stopping muons produced in $\\nu_\\mu$ interactions in the rock below the detector. Up-going particles produced by an undetected down-going muon are a potential background source in these measurements. The implications of this background for neutrino studies using MACRO are discussed.']",['1998-08-03']
1874,['eng'],"['Abbott, B']",['Search For Heavy Point-like Dirac Monopoles'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, magnetic monopole', 'photon, pair production', 'transverse energy, high', 'Feynman graph, higher-order', 'mass, magnetic monopole', 'lower limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803023'],"['We have searched for central production of a pair of photons with high transverse energies in $p\\bar p$ collisions at $\\sqrt{s} = 1.8$ TeV using $70 pb^{-1}$ of data collected with the DØ detector at the Fermilab Tevatron in 1994--1996. If they exist, virtual heavy pointlike Dirac monopoles could rescatter pairs of nearly real photons into this final state via a box diagram. We observe no excess of events above background, and set lower 95% C.L. limits of $610, 870, or 1580 GeV/c^2$ on the mass of a spin 0, 1/2, or 1 Dirac monopole.']",['1998-03-24']
1875,['eng'],"['Asner, D M']",['Radiative Decay Modes of the $D^{0}$ Meson'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D0, electroproduction', 'D0, radiative decay', 'vector meson, production', 'Phi(1020)', 'omega(783)', 'rho(770)0', 'K*(892)', 'mass spectrum', 'D0, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D0 --> vector meson photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803022'],"['Using data recorded by the CLEO-II detector at CESR we have searched for four radiative decay modes of the $D^0$ meson: $D^0\\to\\phi\\gamma$, $D^0\\to\\omega\\gamma$, $D^0\\to\\bar{K}^{*}\\gamma$, and $D^0\\to\\rho^0\\gamma$. We obtain 90% CL upper limits on the branching ratios of these modes of $1.9\\times 10^{-4}$, $2.4\\times 10^{-4}$, $7.6\\times 10^{-4}$ and $2.4\\times 10^{-4}$ respectively.']",['1998-03-24']
1876,['eng'],"['Adamovich, M I', 'Alexandrov, Yu A', 'Barberis, D', 'Beck, M', 'Bérat, C', 'Beusch, Werner', 'Boss, M', 'Brons, S', 'Brückner, W', 'Buénerd, M', 'Busch, C', 'Büscher, C', 'Charignon, F', 'Chauvin, J', 'Chudakov, E A', 'Dersch, U', 'Dropmann, F', 'Engelfried, J', 'Faller, F', 'Fournier, A', 'Gerassimov, S G', 'Godbersen, M', 'Grafström, P', 'Haller, T', 'Heidrich, M', 'Hubbard, E', 'Hurst, R B', 'Königsmann, Kay C', 'Konorov, I', 'Keller, N', 'Martens, K', 'Martin, P', 'Masciocchi, S', 'Michaels, R', 'Müller, U', 'Neeb, H', 'Newbold, D', 'Newsom, C R', 'Paul, S', 'Pochodzalla, J', 'Potashnikova, I K', 'Povh, B', 'Ren, Z', 'Rey-Campagnolle, M', 'Rosner, G', 'Rossi, L', 'Rudolph, H', 'Scheel, C V', 'Schmitt, L', 'Siebert, Hans-Wolfgang', 'Simon, A', 'Smith, V J', 'Thilmann, O', 'Trombini, A', 'Vesin, E', 'Volkemer, B', 'Vorwalter, K', 'Walcher, T', 'Wälder, G', 'Werding, R', 'Wittmann, E', 'Zavertyaev, M V']","['Charge Asymmetries for $D, D_{s}$ and $\\Lambda_{c}$ Production in $\\Sigma^{-}$ - Nucleus Interactions at 340 GeV/c']",['Particle Physics - Experimental Results'],"['Sigma nucleus, inclusive reaction', 'charmed particle, hadroproduction', 'charmed particle, hadronic decay', 'D', 'D/s', 'Lambda/c+', 'charge, asymmetry', 'x-dependence', 'experimental results', 'CERN SPS', 'Sigma- nucleus --> charmed particle anything', '340 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803021'],"['CERN experiment WA89 has studied charmed particles produced by a Sigma^- beam at 340 GeV/c on nuclear targets. Production of particles which have light quarks in common with the beam is compared to production of those which do not. Considerable production asymmetries between D^- and D^p, D_s^ and D_s^+ and Lambda_c and Antilambda_c are observed. The results are compared with pion beam data and with theoretical calculations.']",['1998-03-24']
1877,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'List, B', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Sieberg, R P B', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Utzat, P', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['An upper limit on the anomalous magnetic moment of the $\\tau$ lepton'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, radiative decay', 'tau, pair production', 'current, electromagnetic', 'tau, magnetic moment', 'upper limit', 'form factor, magnetic', 'form factor, electric', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> tau+ tau- photon', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=EP-98-033', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803020']","['Using radiative Z^0 -> \\tau^+ \\tau^- \\gamma events collected with the OPAL detector at LEP at \\sqrt{s}=M_Z during 1990-95, a direct study of the electromagnetic current at the \\tau\\gamma vertex has been performed in terms of the anomalous magnetic form factor F_2 of the \\tau lepton. The analysis is based on a data sample of 1429 e^+ e^- -> \\tau^+ \\tau^- \\gamma events which are examined for a deviation from the expectation with F_2 = 0. From the non-observation of anomalous \\tau^+ \\tau^- \\gamma production a limit of -0.068 < F_2 < 0.065 is obtained. This can also be interpreted as a limit on the electric dipole form factor F_3 as -3.8 x 10^-16 e-cm < eF_3 < 3.6 x 10^-16 e-cm. The above ranges are valid at the 95% confidence level.']",['1998-03-26']
1878,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'List, B', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Utzat, P', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['A search for neutral Higgs bosons in the MSSM and models with two scalar field doublets'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, pair production', 'Higgs particle, neutral particle', 'Higgs particle, multiplet', 'doublet, 2', 'supersymmetry, symmetry breaking', 'Higgs particle, decay modes', 'Higgs particle, mass', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2Higgs particle', 'Higgs particle --> 2beauty', 'Higgs particle --> quark antiquark', 'Higgs particle --> tau+ tau-', '130-172 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=EP-98-029', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803019']","['A search is described for the neutral Higgs bosons h^0 and A^0 predicted by models with two scalar field doublets and, in particular, the Minimal Supersymmetric Standard Model (MSSM). The search in the Z^0 h^0 and h^0 A^0 production channels is based on data corresponding to an integrated luminosity of 25 pb^{-1} from e^+e^- collisions at centre-of-mass energies between 130 and 172GeV collected with the OPAL detector at LEP. The observation of a number of candidates consistent with Standard Model background expectations is used in combination with earlier results from data collected at the Z^0 resonance to set limits on m_h and m_A in general models with two scalar field doublets and in the MSSM. For example, in the MSSM, for tan(beta) > 1, minimal and maximal scalar top quark mixing and soft SUSY-breaking masses of 1 TeV, the 95% confidence level limits m_h > 59.0 GeV and m_A > 59.5 GeV are obtained. For the first time, the MSSM parameter space is explored in a detailed scan.']",['1998-03-18']
1879,['eng'],"['Bergfeld, T']",['Observation of $B^{+}\\to \\omega K^{+}$ and Search for Related $B$ Decay Modes'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'final state, (0charmed particle)', 'omega(783)', 'Phi(1020)', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B+ --> omega(783) K+', 'B --> Phi(1020) K*(892)', 'B --> vector meson meson', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803018'],"['We have searched for two-body charmless decays of B mesons to purely hadronic exclusive final states including $\\omega$ or $\\phi$ mesons using data collected with the CLEO II detector. With this sample of $6.6 \\times 10^6$ B mesons we observe a signal for the $\\omega K^+$ final state, and measure a branching fraction of B($B^+ \\to \\omega K^+$) = 1.5 +0.7 -0.6 +-0.2 $\\times 10^{-5}$. We also observe some evidence for the $\\phi K^*$ final state, and upper limits are given for 22 other decay modes. These results provide the opportunity for studies of theoretical models and physical parameters.']",['1998-03-23']
1880,['eng'],"['Abbott, B', 'Abolins, M']",['Limits on Anomalous $WW\\gamma$ and $WWZ$ Couplings'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'photon, hadroproduction', 'gauge boson, pair production', 'coupling, (3gauge boson)', 'intermediate boson, hadronic decay', 'W, leptonic decay', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', 'anti-p p --> Z0 W anything', 'anti-p p --> W photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803017'],"['Limits on the anomalous WWgamma and WWZ couplings are presented from a simultaneous fit to the data samples of three gauge boson pair final states in pbar-p collisions at sqrt(s)=1.8 TeV: Wgamma production with the W boson decaying to enu or munu, W boson pair production with both of the W bosons decaying to enu or munu, and WW or WZ production with one W boson decaying to enu and the other W boson or the Z boson decaying to two jets. Assuming identical WWgamma and WWZ couplings, 95 % C.L. limits on the anomalous couplings of -0.30<Delta kappa<0.43 (lambda = 0) and -0.20<lambda<0.20 (Delta kappa = 0) are obtained using a form factor scale Lambda = 2.0 TeV. Limits found under other assumptions on the relationship between the WWgamma and WWZ couplings are also presented.']",['1998-03-20']
1881,['eng'],"['Grigalashvili, T', 'Chikovani, L D', 'Ioramashvili, E S', 'Dzhavrishvili, A K', 'Khisanishvili, L A', 'Mailian, E S', 'Nickoladze, M', 'Shalamberidze, L B']",['A-Dependencies of Neutral Strange Particle Yields at $40 GeV/c \\overline {p}$ -Nuclei Collisions'],['Particle Physics - Experimental Results'],"['anti-p nucleus, inclusive reaction', 'K0, hadroproduction', 'Lambda, hadroproduction', 'yield, (Lambda Antilambda K0)', 'dependence, mass number', 'strange particle, hadronic decay', 'mass spectrum', 'angular distribution', 'string model, fragmentation', 'magnetic spectrometer, experimental results', 'Serpukhov PS', '40 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803016'],"['The interactions of $\\bar p$ with D(2), Li(7), C(12), S(32), Cu(64) and Pb(207) nuclei at $40 GeV/c$ were studied by RISC-streamer chamber spectrometer. The yields of $K^0$ mesons and $\\Lambda$ and $\\bar\\Lambda$ hyperons as functions of the target nucleus mass numbers are investigated. The experimental results are compared with model predictions using $FRITIOF-7.02$ program package.']",['1998-03-20']
1882,['eng'],"['Kulchitskii, Yu A']",['Study of the Hadron Shower Profiles with the Tile Hadron Calorimeter'],['Detectors and Experimental Techniques'],"['talk, Geneva 1997/09', 'calorimeter, hadronic', 'iron', 'scintillation counter', 'showers, hadronic', 'magnetic detector, ATLAS', 'CERN LHC Coll', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9903052'],['The lateral and longitudinal profiles of the hadronic showers detected by iron-scintillator tile hadron calorimeter with longitudinal tile configuration have been investigated. The results are based on 100 GeV pion beam data. Due to the beam scan provided many different beam impact locations with cells it is succeeded to obtain detailed picture of transverse shower behavior. The underlying radial energy densities for four depths and for overall calorimeter have been reconstructed. The three-dimensional hadronic shower parametrisation have been suggested.'],['1999-03-23']
1883,['eng'],"['Abe, F']",['Observation of $B^{+}\\rightarrow \\psi (2S) K^{+}$ and $B^{0}\\rightarrow \\psi(2S) K^{*}(892)^0$ decays and measurements of B-meson branching fractions into $J/\\psi $ and $\\psi (2S)$ final states'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B, hadroproduction', 'B, hadronic decay', 'B+, branching ratio', 'B0, branching ratio', 'J/psi(3100), leptonic decay', 'psi(3685), decay modes', 'factorization', 'mass spectrum', 'transverse momentum, spectra', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> B anything', 'B+ --> psi mesons K+', 'B0 --> psi mesons K*(892)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803013'],"['We report the observations of the decays B^+ -> psi(2S) K^+ and B^0 -> psi(2S) K^*(892)^0 in ppbar collisions at a center-of-mass energy of 1.8 TeV using a 110 pb^{-1} data sample recorded by the Collider Detector at Fermilab. We also reconstruct the decays B^+ -> J/psi K^+ and B^0 -> J/psi K^*(892)^0 and measure the six ratios of branching fractions of these four decays. The relative branching-fraction results are shown to be consistent with phenomenological factorization calculations of hadronic B-meson decays. We use the world-average branching fraction Br(B^+ -> J/psi K^+) to derive Br(B^+ -> psi(2S) K^+) = (0.56 +/- 0.08 +/- 0.10) x 10^{-3}, Br(B^0 -> psi(2S) K^*(892)^0) = (0.92 +/- 0.20 +/- 0.16) x 10^{-3}, and Br(B^0 -> J/psi K^*(892)^0) = (1.78 +/- 0.14 +/- 0.29) x 10^{-3}, where the first and second uncertainties are statistical and systematic, respectively.']",['1998-03-17']
1884,['eng'],"['Kasper, P A']",['Physics Prospects at BTeV'],['Particle Physics - Experimental Results'],"['talk, Santa Monica 1997/10/13', 'anti-p p, colliding beams', 'colliding beam detector, proposed', 'production, beauty', 'particle identification, beauty', 'B, decay constant', 'beautiful meson, hadronic decay', 'Kobayashi-Maskawa angle', 'unitarity', 'B0 anti-B0, oscillation', 'B/s0 anti-B/s0, oscillation', 'violation, CP', 'proposed experiment, Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803012'],"['BTeV is a proposed forward collider program at the Fermilab Tevatron dedicated to precision studies of CP violation, mixing and rare decays of beauty and charm hadrons. A description of the proposed detector and results of simulations of several physics channels are presented.']",['1998-03-13']
1885,['eng'],"['Hawker, E A', 'Awes, T C', 'Beddo, M E', 'Brown, C N', 'Bush, J D', 'Carey, T A', 'Chang, T H', 'Cooper, W E', 'Gagliardi, C A', 'Garvey, G T', 'Geesaman, D F', 'He Xiao Chun', 'Isenhower, L D', 'Kaufman, S B', 'Kaplan, D M', 'Kirk, P N', 'Koetke, D D', 'Kyle, G S', 'Lee, D M', 'Lee, W M', 'Leitch, M J', 'Makins, N C R', 'McGaughey, P L', 'Moss, J M', 'Müller, B A', 'Nord, P M', 'Park, B K', 'Papavassiliou, V', 'Peng, J C', 'Petitt, G', 'Reimer, P E', 'Sadler, M E', 'Selden, J', 'Stankus, P', 'Sondheim, W E', 'Thompson, T N', 'Towell, R S', 'Tribble, R E', 'Vasilev, M A', 'Wang, Y C', 'Wang, Z F', 'Webb, J C', 'Willis, J L', 'Wise, D K', 'Young, G R']",['Measurement of the Flavour Asymmetry in the Nucleon Sea'],['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'p deuteron, inclusive reaction', 'muon, pair production', 'Drell-Yan process', 'channel cross section, ratio', 'quark, sea', 'quark, up', 'quark, down', 'antiquark, ratio', 'flavor, asymmetry', 'x-dependence', 'momentum spectrum, parton', 'parametrization', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'p nucleon --> muon+ muon- anything', '800 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803011'],"['A precise measurement of the ratio of Drell-Yan yields from an 800 GeV/c proton beam incident on hydrogen and deuterium targets is reported. Over 140,000 Drell-Yan muon pairs with dimuon mass M_{mu+ mu-} >= 4.5 GeV/c^2 were recorded. From these data, the ratio of anti-down (dbar) to anti-up (ubar) quark distributions in the proton sea is determined over a wide range in Bjorken-x. A strong x dependence is observed in the ratio dbar/ubar, showing substantial enhancement of dbar with respect to ubar for x<0.2. This result is in fair agreement with recent parton distribution parameterizations of the sea. For x>0.2, the observed dbar/ubar ratio is much nearer unity than given by the parameterizations.']",['1998-03-13']
1886,['eng'],"['Edwards, K']","['Measurement of the Mass Splittings between the $b\\overline{b}\\chi_{b,J}(1P)$ States']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10020), electroproduction', 'Upsilon(10020), radiative decay', 'chi mesons, beauty', 'chi mesons, mass', 'photon, energy spectrum', 'mass difference, ratio', 'potential, confinement', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Upsilon(10020) --> chi mesons photon', '10.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803010'],"['We present new measurements of photon energies and branching fractions for the radiative transitions: Upsilon(2S)->gamma+chi_b(J=0,1,2). The masses of the chi_b states are determined from the measured radiative photon energies. The ratio of mass splittings between the chi_b substates, r==(M[J=2]-M[J=1])/(M[J=1]-M[J=0]) with M the chi_b mass, provides information on the nature of the bbbar confining potential. We find r(1P)=0.54+/-0.02+/-0.02. This value is in conflict with the previous world average, but more consistent with the theoretical expectation that r(1P)<r(2P); i.e., that this mass splittings ratio is smaller for the chi_b(1P) triplet than for the chi_b(2P) triplet.']",['1998-03-13']
1887,['eng'],"['Khan, M H R', 'Murakami, A', 'Sumiyoshi, T', 'Kuniya, T', 'Adachi, I', 'Enomoto, R', 'Hattori, H', 'Iijima, T', 'Kaneda, K', 'Kawabata, R', 'Ooba, T', 'Suda, R', 'Suzuki, K', 'Watanabe, M']",['The monitoring system for the aerogel Cherenkov counter of the BELLE detector'],['Particle Physics - Experimental Results'],"['particle identification', 'Cherenkov counter, aerogel', 'Cherenkov counter, threshold', 'monitoring', 'optics, fibre', 'stability', 'magnetic detector, BELLE', 'KEK TRISTAN Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803027'],"['We report on a design and performances of a monitoring system developed for the aerogel Cherenkov counters (ACC) of the BELLE detector. The system consists of blue LEDs, a diffuser box, and optical distributors which distribute the LED light to the ACC modules. The employed LED (NSPB series) has been observed to have high reliability on the long term stability and the temprature dependence. The diffuser box is employed to reduce the intrinsic non-uniformity of the LED light intensity. The overall performances of the present monitoring system on uniformity and intensity of the light output have been found to satisfy all the requirements for the monitoring.']",['1998-03-30']
1888,['eng'],"['Achasov, M N', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Korol, A A', 'Koshuba, S V', 'Nesterenko, I N', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Velikzhanin, Yu S']",['Upper limit on the $\\eta \\rightarrow \\pi^{0} \\pi^{0}$ decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'eta, hadronic decay', 'eta, branching ratio', 'upper limit', 'calorimeter, experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> eta photon', 'eta --> 2pi0', '10.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803008'],['Upper bound 6*10^{-4} with 90% confidence is reported for the eta -> pi^0 pi^0 decay from the SND experiment at the VEPP-2M collider.'],['1998-03-12']
1889,['eng'],"['Abe, F']",['Search for Chargino-Neutralino Associated Production at the Fermilab Tevatron Collider'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'sparticle, search for', 'sparticle, associated production', 'sparticle, decay', 'final state, (3lepton)', 'chargino, mass', 'neutralino, mass', 'lower limit', 'transverse energy, missing-energy', 'channel cross section, branching ratio', 'upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> chargino neutralino anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803015'],"['We have searched in $p \\bar{p}$ collisions at $\\sqrt{s}$ = 1.8 TeV for events with three charged leptons and missing transverse energy. In the Minimal Supersymmetric Standard Model, we expect trilepton events from chargino-neutralino ($\\chione \\chitwo$) pair production, with subsequent decay into leptons. We observe no candidate $e^+e^-e^\\pm$, $e^+e^-\\mu^\\pm$, $e^\\pm\\mu^+\\mu^-$ or $\\mu^+\\mu^-\\mu^\\pm$ events in 106 pb$^{-1}$ integrated luminosity. We present limits on the sum of the branching ratios times cross section for the four channels: $\\sigma_{\\chione\\chitwo}\\cdot $BR$(\\chione\\chitwo\\to 3\\ell+X) < 0.34$~pb, M$_\\chione > $ 81.5 \\mgev\\sp and M$_\\chitwo > $ 82.2 \\mgev\\sp for $\\tan\\beta=2$, $\\mu =-600$~\\mgev\\sp and M$_\\squark=$ M$_\\gluino$.']",['1998-03-18']
1890,['eng'],"['Kearns, E T']",['Experimental Measurements of Atmospheric Neutrinos'],['Particle Physics - Experimental Results'],"['talk, Gran Sasso 1997/09/07', 'neutrino, cosmic radiation', 'neutrino/mu, flux', 'neutrino/e, flux', 'flux, ratio', 'angular dependence', 'deep underground detector, Soudan', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803007'],"['This talk reports the latest indications of an anomaly in the measurements of atmospheric neutrinos. New results from Soudan-2 and Super-Kamiokande provide evidence that the ratio of nu_mu to nu_e interactions is not as expected. High energy Super-Kamiokande data indicates the cause is a deficit of upward-going nu_mu, and the zenith angle dependence of the effect is consistent with neutrino oscillations. Upward-going muon measurements by several detectors are discussed, but in total they provide inconclusive evidence for the anomaly.']",['1998-03-10']
1891,['eng'],"['Fukuda, Y']",['Measurement of a small atmospheric $\\nu_{\\mu}/\\nu_{e}$ ratio'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'neutrino/mu, flux', 'neutrino/e, flux', 'flux, ratio', 'momentum spectrum', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803006'],"['From an exposure of 25.5~kiloton-years of the Super-Kamiokande detector, 900 muon-like and 983 electron-like single-ring atmospheric neutrino interactions were detected with momentum $p_e > 100$ MeV/$c$, $p_\\mu > 200$ MeV/$c$, and with visible energy less than 1.33 GeV. Using a detailed Monte Carlo simulation, the ratio $(\\mu/e)_{DATA}/(\\mu/e)_{MC}$ was measured to be $0.61 Kamiokande, IMB and Soudan-2 experiments, and smaller than expected from theoretical models of atmospheric neutrino production.']",['1998-03-09']
1892,['eng'],"['Bernreuther, S']",['The HERMES Back Drift Chambers'],['Detectors and Experimental Techniques'],"['drift chamber, gas', 'argon, organic compounds', 'carbon, fluorine', 'spatial resolution', 'efficiency', 'alignment', 'calibration', 'magnetic spectrometer, HERMES', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803005'],"['The tracking system of the HERMES spectrometer behind the bending magnet consists of two pairs of large planar 6-plane drift chambers. The design and performance of these chambers is described. This description comprises details on the mechanical and electronical design, information about the gas mixture used and its properties, results on alignment, calibration, resolution, and efficiencies, and a discussion of the experience gained through the first three years of operation.']",['1998-03-06']
1893,['eng'],"['Abbott, B']",['Limits on $WW\\gamma$ and $WWZ$ Couplings from $W$ Boson Pair Production'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, pair production', 'W, leptonic decay', 'coupling, (2W photon)', 'coupling, (Z0 2W)', 'transverse energy, spectra', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803004'],"['The results of a search for W boson pair production in pbar-p collisions at sqrt{s}=1.8 TeV with subsequent decay to emu, ee, and mumu channels are presented. Five candidate events are observed with an expected background of 3.1+-0.4 events for an integrated luminosity of approximately 97 pb^{-1}. Limits on the anomalous couplings are obtained from a maximum likelihood fit of the E_T spectra of the leptons in the candidate events. Assuming identical WWgamma and WWZ couplings, the 95 % C.L. limits are -0.62<Delta_kappa<0.77 (lambda = 0) and -0.53<lambda<0.56 (Delta_kappa = 0) for a form factor scale Lambda = 1.5 TeV.']",['1998-03-04']
1894,['eng'],"['Abbott, B']",['Measurement of the Shape of the Transverse Momentum Distribution of W Bosons Produced in $p\\overline{p}$ Collisions at $\\sqrt{s}$= 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'transverse momentum, spectra', 'quantum chromodynamics, perturbation theory', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803003'],['The shape of the transverse momentum distribution of W bosons (p_T(W)) produced in pbarp collisions at sqrt(s)= 1.8 TeV is measured with the DO detector at Fermilab. The result is compared to QCD perturbative and resummation calculations over the p_T(W) range from 0-200 GeV/c. The shape of the distribution is consistent with the theoretical prediction.'],['1998-03-04']
1895,['eng'],"['Luk, K B']",['Hunting For Direct CP Violation in Strange-Baryon Decays'],['Particle Physics - Experimental Results'],"['talk, Nanjing 1997/08/16', 'hyperon, hadronic decay', 'violation, CP', 'anti-p p, annihilation', 'Lambda, pair production', 'p nucleus, inclusive reaction', 'Antixi-, hadroproduction', 'Xi-, hadroproduction', 'Lambda, polarization', 'angular distribution', 'helicity', 'magnetic spectrometer', 'proposed experiment, Fermilab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803002'],"['Although CP-symmetry breaking has only been seen in neutral kaon decays, this mysterious phenomenon is expected to occur elsewhere. In this talk, how CP violation can arise in strange-baryon decays is briefly reviewed. The current status and prospects for searching for such an effect will be presented.']",['1998-03-03']
1896,['eng'],"['Kaplan, D M']",['BTeV/C0'],['Particle Physics - Experimental Results'],"['talk, Batavia 1997/09/22', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'quark, decay', 'Kobayashi-Maskawa angle', 'unitarity', 'violation, CP', 'neutral current, flavor changing', 'magnetic spectrometer, proposed', 'semiconductor detector, vertex', 'proposed experiment, Batavia TEVATRON Coll', '2000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9803001'],"['The physics goals and techniques of the proposed BTeV experiment at the C0 Tevatron interaction area are summarized, with emphasis on aspects of the experiment that depend on near-beam issues. BTeV aims to carry out a comprehensive study of rare processes (especially CP violation) in charm and beauty decay starting in collider Run II. Vertex detectors will be deployed within a few mm of the beam. Early running may employ a wire target in the beam halo.']",['1998-03-03']
1897,['eng'],"['Alexander, J']",['The Hadronic Transitions $\\Upsilon(2S)\\to \\Upsilon(1S)$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10020), electroproduction', 'Upsilon(10020), hadronic decay', 'Upsilon(10020), branching ratio', 'Upsilon(9460), leptonic decay', 'Upsilon(9460), decay modes', 'Upsilon(9460), branching ratio', 'mass spectrum, two-pion', 'eta', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Upsilon(10020) --> Upsilon(9460) pi+ pi-', 'Upsilon(10020) --> Upsilon(9460) 2pi0', 'Upsilon(9460) --> muon+ muon-', 'Upsilon(9460) --> positron electron', 'Upsilon(10020) --> Upsilon(9460) eta', 'Upsilon(10020) --> Upsilon(9460) pi0', '10.02 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802024'],"[""Using a data sample of $\\Upsilon(2S)$ events collected with the CLEO II detector at the Cornell Electron Storage Ring, we have investigated the hadronic transitions between the $\\Upsilon(2S)$ and the $\\Upsilon(1S)$. The charged dipion transition $\\Upsilon(2S)\\to \\Upsilon(1S)\\pi^+\\pi^-$ was studied using two different analysis techniques. Selecting events in which analysis), we measured the branching fraction of B=0.189+-0.004+-0.009, while using a method allowing $\\Upsilon(1S)$ to decay into anything (``inclusive'' analysis) we found B=0.0196+-0.002+-0.010. The appropriate average of the two measurements gives B=0.0192+-0.002+-0.010. Combining the exclusive and inclusive results we derive the $\\Upsilon(1S)$ leptonic branching ratios B_{ee}=0.0229+-0.0008+-0.0011 and B_{\\mu\\mu}=0.0249+-0.0008+-0.0013 We also studied $\\Upsilon(2S)\\to \\Upsilon(1S)\\pi^0\\pi^0$ and obtained the branching fraction of B=0.092+-0.006+-0.007. Parameters of the $\\pi\\pi$ system (dipion invariant mass spectra, angular distributions) were analyzed and found to be consistent with current theoretical models. Lastly, we searched for the $\\eta$ and single $\\pi^0$ transitions and obtained the upper limits of 0.0028 and 0.0011 respectively.""]",['1998-03-02']
1898,['eng'],"['Athanas, M']",['First Observation of the Cabibbo Suppressed Decay $B^{+}\\to \\overline{D}^{0}K^{+}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B+, hadronic decay', 'B+, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B+ --> anti-D0 K+', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802023'],"['We have observed the decay of the $B^-$ meson into $D^0 K^-$, using 3.3 million $B\\bar B$ pairs collected with the CLEO II detector at the Cornell Electron Storage Ring. We find the branching fractions of this decay to be suppressed relative to the decay into $D^0 \\pi^-$ by $0.055 \\pm 0.014 \\pm 0.005$.']",['1998-02-27']
1899,['eng'],"['Brandenburg, G']",['Continuum Charged $D^{*}$ Spin Alignment at $\\sqrt{s}$ = 10.5 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, charm', 'quark, pair production', 'quark, hadronization', 'D*(2010), electroproduction', 'spin, alignment', 'D*(2010), hadronic decay', 'mass spectrum', 'angular distribution', 'electron positron --> D*(2010) anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K- pi+ pi0', 'approx. 10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802022'],['A measurement of the spin alignment of charged D^* mesons produced in continuum e^+ e^- \\to c \\bar{c} events at \\sqrt{s}=10.5 GeV is presented. This study using 4.72 fb^{-1} of CLEO II data shows that there is little evidence of any D^* spin alignment.'],['1998-02-27']
1900,['eng'],"['Evangelista, C', 'Palano, A', 'Drijard, Daniel', 'Hamann, N H', 'Jones, R T', 'Mouëllic, B', 'Ohlsson, S', 'Perreau, J M', 'Eyrich, W', 'Moosburger, M', 'Pomp, S', 'Stinzing, F', 'Fischer, H', 'Franz, J', 'Rössle, E', 'Schmitt, H', 'Wirth, H', 'Buzzo, A', 'Kirsebom, K', 'Lo Vetere, M', 'Macri, M', 'Marinelli, M', 'Passaggio, S', 'Pia, M G', 'Pozzo, A', 'Robutti, E', 'Santroni, A', 'Debevec, P T', 'Eisenstein, R A', 'Harris, P G', 'Hertzog, D W', 'Hughes, S A', 'Reimer, P E', 'Ritter, J B', 'Geyer, R', 'Kilian, K', 'Oelert, Walter', 'Röhrich, K', 'Rook, M', 'Steinkamp, O', 'Korsmo, H', 'Stugu, B', 'Johansson, T']",['Study of the reaction $p\\bar{p} \\to \\phi \\phi$ from 1.1 to 2.0 GeV/c'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'jet, target', 'Phi(1020), pair production', 'Phi(1020), hadronic decay', 'channel cross section, momentum dependence', 'search for, f4(2220)', 'branching ratio, upper limit', 'Iizuka-Okubo-Zweig rule, violation', 'model, production', 'experimental results', 'CERN LEAR', 'anti-p p --> 2Phi(1020)', 'anti-p p --> 2K+ 2K-', '1.1-2.0 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802016'],"['A study has been performed of the reaction pbar p -> 4K using in-flight antiprotons from 1.1 to 2.0 GeV/c incident momentum interacting with a hydrogen jet target. The reaction is dominated by the production of a pair of phi mesons. The pbar p -> phi phi cross section rises sharply above threshold and then falls continuously as a function of increasing antiproton momentum. The overall magnitude of the cross section exceeds expectations from a simple application of the OZI rule by two orders of magnitude. In a fine scan around the xi/f_J(2230) resonance, no structure is observed. A limit is set for the double branching ratio B(xi -> pbar p) * B(xi -> phi phi) < 6e-5 for a spin 2 resonance of M = 2.235 GeV and Width = 15 MeV.']",['1998-02-19']
1901,['eng'],"['Nayak, T K']",['Present Status and Future of DCC Analysis'],['Particle Physics - Experimental Results'],"['talk, Tsukuba 1997/12/01', 'scattering, heavy ion', 'lead', 'quark gluon, plasma', 'condensation, chiral', 'critical phenomena', 'centauro', 'event shape analysis', 'photon, multiplicity', 'charged particle, multiplicity', 'transformation, wavelet', 'multiplicity, moment', 'experimental results', 'CERN SPS', '158 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802019'],['Disoriented Chiral Condensates (DCC) have been predicted to form in high energy heavy ion collisions where the approximate chiral symmetry of QCD has been restored. This leads to large imbalances in the production of charged to neutral pions. Sophisticated analysis methods are being developed to disentangle DCC events out of the large background of events with conventionally produced particles. We present a short review of current analysis methods and future prospects.'],['1998-02-24']
1902,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'List, B', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Utzat, P', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for an excess in the production of four-jet events from $e^+ e^-$ collisions at $\\sqrt{s}$ = 130-184 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'final state, (4jet)', 'mass spectrum, (2jet)', 'electroweak interaction, validity test', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 4jet', '130-184 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=EP-98-013', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802015']","[""Events with four distinct jets from e^+e^- collisions, collected by the OPAL detector at centre-of-mass energies between 130 and 184 GeV, are analysed for a peak in the sum of dijet masses. This search is motivated by the ALEPH Collaboration's observation of a clear excess of events with dijet mass sums close to 105 GeV in data taken at centre-of-mass energies of 130 and 136 GeV in 1995. We have observed no significant excess of four-jet events compared to the Standard Model expectation for any dijet mass sum at any energy. Our observation is inconsistent with the excess observed by ALEPH in 1995. Upper limits are determined on the production cross-section as a function of the dijet mass sum.""]",['1998-02-16']
1903,['eng'],"['Littenberg, L S']",['BNL Future Plans'],['Particle Physics - Experimental Results'],"['talk, Tsukuba 1997/10/31', 'proton synchrotron', 'secondary beam', 'muon- nucleus, interaction', 'transition, muon- electron', 'violation, flavor', 'K, semileptonic decay', 'neutral current, flavor changing', 'time reversal, violation', 'neutrino/mu, mass', 'muon, electric moment', 'proposed experiment, Brookhaven PS', 'K --> pi neutrino antineutrino', 'K+ --> pi0 muon+ neutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802014'],['I discuss the prospects for a fixed target physics program at the AGS in the RHIC era.'],['1998-02-18']
1904,['eng'],"['Breitweg, J', 'Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Yoshida, R', 'Zhang, H', 'Mattingly, M C K', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'De Pasquale, S', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Ricci, F', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Brock, I C', 'Coboken, K', 'Crittenden, J A', 'Deffner, R', 'Eckert, M', 'Grothe, M', 'Hartmann, H', 'Heinloth, K', 'Heinz, L', 'Hilger, E', 'Jakob, H P', 'Kappes, A', 'Katz, U F', 'Kerger, R', 'Paul, E', 'Pfeiffer, M', 'Stamm, J', 'Wedemeyer, R', 'Wieber, H', 'Bailey, D S', 'Campbell-Robson, S', 'Cottingham, W N', 'Foster, B', 'Hall-Wilton, R', 'Heath, G P', 'Heath, H F', 'McFall, J D', 'Piccioni, D', 'Roff, D G', 'Tapper, R J', 'Ayad, R', 'Capua, M', 'Garfagnini, A', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Kim, J Y', 'Lee, J H', 'Lim, I T', 'Pac, M Y', 'Caldwell, A', 'Cartiglia, N', 'Jing, Z', 'Liu, W', 'Mellado, B', 'Parsons, J A', 'Ritz, S', 'Sampson, S', 'Sciulli, F', 'Straub, P B', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Figiel, J', 'Klimek, K H', 'Przybycien, M B', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Bukowy, M', 'Czermak, A', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Dulinski, Z', 'Kotanski, Andrzej', 'Abbiendi, G', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Cases, G', 'Desler, K', 'Drews, G', 'Fricke, U', 'Goebel, F', 'Göttlicher, P', 'Graciani, R', 'Haas, T', 'Hain, W', 'Hasell, D', 'Hebbel, K', 'Johnson, K F', 'Kasemann, M', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Lindemann, L', 'Löhr, B', 'Milewski, J', 'Monteiro, T', 'Ng, J S T', 'Notz, D', 'Park, I H', 'Pellegrino, A R', 'Pelucchi, F', 'Piotrzkowski, K', 'Rohde, M', 'Roldán, J', 'Ryan, J J', 'Savin, A A', 'Schneekloth, U', 'Schwarzer, O', 'Selonke, F', 'Surrow, B', 'Tassi, E', 'Westphal, D', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Burow, B D', 'Coldewey, C', 'Grabosch, H J', 'Meyer, A', 'Schlenstedt, S', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Markun, P', 'Trefzger, T M', 'Wölfle, S', 'Bromley, J T', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'MacDonald, N', 'Saxon, D H', 'Sinclair, L E', 'Strickland, E', 'Waugh, R', 'Bohnet, I', 'Gendner, N', 'Holm, U', 'Meyer-Larsen, A', 'Salehi, H', 'Wick, K', 'Gladilin, L K', 'Horstmann, D', 'Kcira, D', 'Klanner, R', 'Lohrmann, E', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Cole, J E', 'Howell, G', 'Lamberti, L', 'Long, K R', 'Miller, D B', 'Pavel, N', 'Prinias, A', 'Sedgbeer, J K', 'Sideris, D', 'Walker, R', 'Mallik, U', 'Wang, S M', 'Wu, J T', 'Cloth, P', 'Filges, D', 'Ishii, T', 'Kuze, M', 'Suzuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamauchi, K', 'Yamazaki, Y', 'Hong, S J', 'Lee, S B', 'Nam, S W', 'Park, S K', 'Barreiro, F', 'Fernández, J P', 'García, G', 'Glasman, C', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Martínez, M', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Murray, W N', 'Ochs, A', 'Riveline, M', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Tsurugai, T', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A']",['High-$E_{T}$ Inclusive Jet Cross Sections in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'jet, photoproduction', 'differential cross section, rapidity dependence', 'jet, transverse energy', 'quantum chromodynamics, perturbation theory', 'jet, particle identification', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802012'],"['Inclusive jet differential cross sections for the reaction e+ p --> e+ + jet + X with quasi-real photons have been measured with the ZEUS detector at HERA. These cross sections are given for the photon-proton centre-of-mass energy interval 134 < W < 277 GeV and jet pseudorapidity in the range -1 < eta(jet) < 2 in the laboratory frame. The results are presented for three cone radii in the eta-phi plane, R=1.0, 0.7 and 0.5. Measurements of dsigma/deta(jet) above various jet-transverse-energy thresholds up to 25 GeV and in three ranges of W are presented and compared to next-to-leading order (NLO) QCD calculations. For jets defined with R=1.0 differences between data and NLO calculations are seen at high eta(jet) and low E_T(jet). The measured cross sections for jets defined with R=0.7 are well described by the calculations in the entire measured range of eta(jet) and E_T(jet). The inclusive jet cross section for E_T(jet) > 21 GeV is consistent with an approximately linear variation with the cone radius R in the range between 0.5 and 1.0, and with NLO calculations.']",['1998-02-15']
1905,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'List, B', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Utzat, P', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']","['Production of $f_{0}(980), f_{2}(1270)$ and $\\phi(1020)$ in hadronic $Z^{0}$ decay']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'f0(975)', 'f2(1270)', 'Phi(1020)', 'mass spectrum, (pi+ pi-)', 'mass spectrum, (K+ K-)', 'final state, (3jet)', 'quark, jet', 'gluon, jet', 'model, coupled channel', 'multiplicity, dependence', 'rapidity, gap', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802013', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=EP-98-010']","['Inclusive production of the f_0(980), f_2(1270) and \\phi(1020) resonances has been studied in a sample of 4.3 million hadronic Z^0 decays from the OPAL experiment at LEP. A coupled channel analysis has been used for the f_0 in simultaneous fits to the resonances in inclusive \\pi+\\pi- and K+K- mass spectra. Fragmentation functions are reported for the three states. Total inclusive rates are measured to be 0.141 +/- 0.007 +/- 0.011 f_0, 0.155 +/- 0.011 +/- 0.018 f_2, and 0.091 +/- 0.002 +/- 0.003 \\phi mesons per hadronic Z^0 decay. The production properties of the f_0, including those in three-jet events, are compared with those of the f_2 and \\phi, and with the Lund string model of hadron production. All measurements are consistent with the hypothesis that the f_0 is a conventional qq(bar) scalar meson.']",['1998-02-15']
1906,['eng'],"['Adler, Stephen Louis', 'Atiya, M S', 'Chiang, I H', 'Frank, J S', 'Haggerty, J S', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'Sambamurti, A K', 'Stevens, A', 'Strand, R C', 'Witzig, C', 'Louis, W C', 'Akerib, D S', 'Ardebili, M', 'Convery, M R', 'Ito, M M', 'Marlow, D R', 'McPherson, R A', 'Meyers, P D', 'Selen, M A', 'Shoemaker, F C', 'Smith, A J S', 'Blackmore, E W', 'Bryman, D A', 'Felawka, L', 'Konaka, A', 'Kuno, Y', 'MacDonald, J A', 'Numao, T', 'Padley, P', 'Poutissou, J M', 'Poutissou, R', 'Roy, J D', 'Turcot, A S', 'Kitching, P', 'Nakano, T', 'Rozon, M', 'Soluk, R A']",['Upper Limit on the Decay $K^{+} \\to e^{+} \\nu \\mu^{+} \\mu^{-}$'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'K+, branching ratio', 'upper limit', 'perturbation theory, chiral', 'experimental results', 'Brookhaven PS', 'K+ --> muon+ muon- positron neutrino', '0.8 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802011'],"['An upper limit on the branching ratio for the decay K+ --> e+ nu mu+ mu- is set at 5.0 x 10^{-7} at 90% confidence level, consistent with predictions from chiral perturbation theory.']",['1998-02-13']
1907,['eng'],"['Lammel, S']",['Supersymmetry at the Tevatron?'],['Particle Physics - Experimental Results'],"['lectures', 'anti-p p, colliding beams', 'supersymmetry', 'sparticle, search for', 'sparticle, mass spectrum', 'transverse energy, missing-energy', 'jet', 'lepton, particle identification', 'sparticle, pair production', 'sparticle, decay modes', 'squark, truth', 'squark, beauty', 'gluino', 'charge, dilepton', 'chargino', 'neutralino', 'lepton, multiplicity', 'R parity, violation', 'final state, (2electron 2photon)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802010'],"['These lectures contain an introduction to the search for supersymmetry at hadron colliders. The Tevatron is one of high-energy physics most sophisticated tools. The high center-of-mass energy of its proton-antiproton collisions makes it an ideal place to search for physics beyond the Standard Model, such as supersymmetry. Two experiments, CDF and DØ, completed a long data taking period in summer of 1995, yielding over $100 p b^{-1}$ of proton-- antiproton interactions. The data recorded by the experiments are still being analysed. The lectures outline the strategies in the search for supersymmetry at the Tevatron and examine the major analyses in detail. Results obtained by the two experiments are included where available.']",['1998-02-09']
1908,['eng'],"['Woods, M']",['Compton Polarimetry at a TeV Collider'],['Particle Physics - Experimental Results'],"['talk, Santa Cruz 1997/09/22', 'talk, Zvenigorod 1997/09/29', 'electron positron, linear collider', 'electron electron, linear collider', 'linear collider, proposed', 'electron, polarized beam', 'polarization, beam monitoring', 'Compton scattering', 'radiation, laser', 'Cherenkov counter', 'SLAC SLC Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802009'],"['An electron beam polarization of 80% or greater will be a key feature of a 1 TeV Linear Collider. Accurate measurements of the beam polarization will therefore be needed. We discuss design considerations and capabilities for a Compton-scattering polarimeter located in the extraction line from the Interaction Point. Polarization measurements with 1% accuracy taken parasitic to collision data look feasible, but detailed simulations are needed. Polarimeter design issues are similar for both electron-positron and electron-electron collider modes, though beam disruption creates more difficulties for the electron-electron mode.']",['1998-02-09']
1909,['eng'],"['Klapdor-Kleingrothaus, H V']",['Double $\\beta$ Decay'],['Detectors and Experimental Techniques'],"['review, experimental results', 'double-beta decay, (0neutrino)', 'neutrino/e, mass', 'supersymmetry', 'R parity, violation', 'neutrino, heavy', 'neutrino, exchange', 'neutrino, Majorana', 'neutrino, sterile', 'B-L number, violation', 'mass, sneutrino', 'leptoquark', 'model, composite', 'W, right-handed', 'W, mass', 'nucleus, lifetime', 'Majoron', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'semiconductor detector, germanium', 'deep underground detector, Gran Sasso', 'proposed experiment', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802007'],"['Nuclear double beta decay provides an extraordinarily broad potential to search for beyond Standard Model physics, probing already now the TeV scale, on which new physics should manifest itself. These possibilities are reviewed here. First, the results of present generation experiments are presented. The most sensitive one of them -- the Heidelberg-Moscow experiment in the Gran Sasso -- probes the electron mass now in the sub eV region and will reach a limit of $\\sim$ 0.1 eV in a few years. Basing to a large extent on the theoretical work of the Heidelberg Double Beta Group in the last two years, results are obtained also for SUSY models (R-parity breaking, sneutrino mass), leptoquarks (leptoquark-Higgs coupling), compositeness, right-handed W boson mass and others. These results are comfortably competitive to corresponding results from high-energy accelerators like TEVATRON, HERA, etc. Second, future perspectives of $\\beta\\beta$ research are discussed. A new Heidelberg experimental proposal (GENIUS) is presented which would allow to increase the sensitivity for Majorana neutrino masses from the present level of at best 0.1 eV down to 0.01 or even 0.001 eV. Its physical potential would be a breakthrough into the multi-TeV range for many beyond standard models. Its sensitivity for neutrino oscillation parameters would be larger than of all present terrestrial neutrino oscillation experiments and of those planned for the future. It could probe directly the atmospheric neutrino problem and even the large angle solution of the solar neutrino problem. It would further, already in a first step, cover almost the full MSSM parameter space for prediction of neutralinos as cold dark matter, making the experiment competitive to LHC in the search for supersymmetry.']",['1998-02-05']
1910,['eng'],"['Carena, M S', 'Culbertson, R J', 'Eno, S', 'Frisch, H J', 'Mrenna, S']",['Perspectives on Supersymmetry'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'supersymmetry, search for', 'supersymmetry, symmetry breaking', 'sparticle, hadroproduction', 'sparticle, pair production', 'sparticle, decay modes', 'supergravity', 'sparticle, mass spectrum', 'R parity, violation', 'chargino', 'neutralino', 'gaugino', 'squark, truth', 'slepton', 'channel cross section, mass', 'channel cross section, branching ratio', 'Higgs particle, decay modes', 'LSP, Higgsino', 'LSP, gravitino', 'transverse energy, missing-energy', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802006'],"['A review of the status of searches for Supersymmetry at the Tevatron Collider as of the Summer of 1997. This is a new version of the previous review, substantially shortened to fit editorial guidelines, and significantly different to warrant a separate posting. To appear in ""Perspectives on Supersymmetry"", ed. G.L. Kane (World Scientific, Singapore).']",['1998-02-04']
1911,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'List, B', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Utzat, P', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for charged Higgs bosons in $e^+ e^-$ collisions at $\\sqrt{s}$ = 130-172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, charged particle', 'Higgs particle, pair production', 'Higgs particle, decay modes', 'channel cross section, branching ratio', 'Higgs particle, mass', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2Higgs particle', 'Higgs particle --> quark antiquark', 'Higgs particle --> tau neutrino/tau', '130-172 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802004', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-168']","[""A search is described to detect charged Higgs bosons via the process e^+e^- -> H^+H^-, using data collected by the OPAL detector at center-of-mass energies of 130-172 GeV with a total integrated luminosity of 25 pb^-1. The decay channels are assumed to be H^+ -> qq'(bar) and H^+ -> \\tau^+ \\nu_{\\tau}. No evidence for charged Higgs boson production is observed. The lower limit for its mass is determined to be 52 GeV at 95% confidence level, independent of the H^+ -> \\tau^+ \\nu_{\\tau} branching ratio.""]",['1998-02-03']
1912,['eng'],"['Telnov, V I']",['Physics goals and parameters of photon colliders'],['Particle Physics - Experimental Results'],"['talk, Santa Cruz 1997/09/22', 'electron positron, linear collider', 'photon electron, colliding beams', 'photon photon, colliding beams', 'colliding beams, proposed', 'radiation, laser', 'Compton scattering, backscatter', 'luminosity', 'Higgs particle, photoproduction', 'Higgs particle, branching ratio', 'channel cross section, mass', 'Higgs particle, decay modes', 'W, pair production', 'beam cooling, laser']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802003'],"['Linear colliders offer a unique possibility to study gamma gamma and gamma electron interactions at the energies 0.1--2 TeV. This option is now included in design reports of NLC, JLC and TESLA/SBLC. This paper includes: status of photon colliders, new possibilities in study of Higgs boson, ways to achieve high luminosities.']",['1998-02-03']
1913,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurements of the $B^{0}_s$ and $\\Lambda^{0}_b$ lifetimes'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Lambda/b0, semileptonic decay', 'Lambda/b0, lifetime', 'B/s0, semileptonic decay', 'B/s0, lifetime', 'D/s-, decay modes', 'K*(892)', 'Phi(1020)', 'Lambda/c+, decay modes', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'Lambda/b0 --> Lambda/c+ lepton-', 'Lambda/c+ --> p K- pi+', 'Lambda/c+ --> Lambda lepton+ neutrino anything', 'B/s0 --> D/s- lepton+', 'D/s- --> Phi(1020) pi-', 'D/s- --> K*(892) K-', 'D/s- --> K0(S) K-', 'D/s- --> Phi(1020) lepton- antineutrino anything', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802002', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-159']","['This paper presents updated measurements of the lifetimes of the B^0_s meson and the \\Lambda_b baryon using 4.4 million hadronic Z^0 decays recorded by the OPAL detector at LEP from 1990 to 1995. A sample of B^0_s decays is obtained using D_s^- \\ell^+ combinations, where the D_s^- is fully reconstructed in the in the \\phi \\ell^- \\nu(bar) X decay mode. A sample of \\Lambda_b decays is obtained using \\Lambda_c^+ \\ell^- combinations, where the \\Lambda_c^+ is fully reconstructed in its decay to a p K^- \\pi^+ final state and partially reconstructed in the \\Lambda \\ell^+ \\nu X decay channel. From 172 +/- 28 D_s^- \\tau(B^0_s) = 1.50 +0.16 -0.15 +/- 0.04 ps, where the errors are statistical and systematic, respectively. From the 129 measured lifetime \\tau(\\Lambda_b) = 1.29 +0.24 -0.22 +/- 0.06 ps, where the errors are statistical and systematic, respectively.']",['1998-02-03']
1914,['eng'],"['Rodríguez, J L']",['$b \\to c$ Hadronic Decays'],['Particle Physics - Experimental Results'],"['review, Honolulu 1997/03/24', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'Z0, electroproduction', 'quark, beauty', 'quark, pair production', 'quark, hadronic decay', 'quantum chromodynamics, parametrization', 'factorization, validity test', 'model, spectator', 'B, pair production', 'B0, hadronic decay', 'B0, branching ratio', 'B-, branching ratio', 'experimental results', 'magnetic detector, CLEO', 'Cornell CESR Stor', 'magnetic detector, OPAL', 'CERN LEP Stor', '10.6, 91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801028'],"['A review of current experimental results on exclusive hadronic decays of bottom mesons to a single or double charmed final state is presented. We concentrate on branching fraction measurements conducted at $e^+e^-$ colliders at the $\\Upsilon(4s)$ and at the $Z^0$ resonance. The experimental results reported are then used in tests of theoretical model predictions, the determination of the QCD parameters $a_1$ and $a_2/a_1$ and tests of factorization']",['1998-01-30']
1915,['eng'],"['Abbott, B', 'Abolins, M', 'Acharya, B S', 'Adam, I', 'Adams, D L', 'Adams, M', 'Ahn, S', 'Aihara, H', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Astur, R', 'Baarmand, M M', 'Baden, A', 'Balamurali, V', 'Balderston, J', 'Baldin, B Yu', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Bartlett, J F', 'Bazizi, K', 'Belyaev, A', 'Beri, S B', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Biswas, N', 'Blazey, G C', 'Blessing, S K', 'Bloom, P', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F O', 'Boswell, C', 'Brandt, A', 'Brock, R L', 'Bross, A D', 'Buchholz, D A', 'Burtovoi, V S', 'Butler, J M', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chang, S M', 'Chekulaev, S V', 'Chen, L P', 'Chen, W', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cobau, W G', 'Cochran, J', 'Coney, L', 'Cooper, W E', 'Cretsinger, C E', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Evdokimov, V N', 'Fahland, T', 'Fatyga, M K', 'Fehér, S', 'Fein, D K', 'Ferbel, T', 'Finocchiaro, G', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Forden, G E', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Geld, T L', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gibbard, B', 'Glenn, S', 'Gobbi, B', 'Goldschmidt, A', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, D R', 'Greenlee, H', 'Grim, G P', 'Grinstein, S', 'Grossman, N L', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Guida, J A', 'Guida, J M', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, P', 'Gutnikov, Yu E', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Hernández-Montoya, R', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hsieh, F', 'Ting Hu Tong Hu', 'Hühn, T', 'Ito, A S', 'James, E', 'Jaques, J', 'Jerger, S A', 'Jesik, R', 'Jiang, J Z Y', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Jun, S Y', 'Jung, C K', 'Kahn, S', 'Kalbfleisch, G R', 'Kang, J S', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kelly, M L', 'Kim, C L', 'Kim, S K', 'Klatchko, A', 'Klima, B', 'Klopfenstein, C', 'Klioukhine, V I', 'Kochetkov, V I', 'Kohli, J M', 'Koltick, D S', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kourlas, J', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kunori, S', 'Lami, S', 'Lander, R', 'Landry, F J', 'Landsberg, G L', 'Lauer, B M', 'Leflat, A', 'Li, H', 'Li, J', 'Li-Demarteau, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Liu, Y C', 'Lobkowicz, F', 'Loken, S C', 'Lökös, S', 'Lueking, L H', 'Lyon, A L', 'Maciel, A K A', 'Madaras, R J', 'Madden, R', 'Magana-Mendoza, L', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Markeloff, R', 'Marshall, T', 'Martin, M I', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McKibben, T', 'McKinley, J', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miettinen, H', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mooney, P', 'Da Motta, H', 'Murphy, C', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Narayanan, A', 'Neal, H A', 'Negret, J P', 'Némethy, P', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Oliveira, E', 'Oltman, E', 'Oshima, N', 'Owen, D', 'Padley, P', 'Para, A', 'Park, Y M', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pishchalnikov, Yu', 'Podstavkov, V M', 'Pope, B G', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramírez, O', 'Rasmussen, L', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Roe, N A', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Sánchez-Hernández, A', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Scully, J R', 'Shabalina, E', 'Shaffer, C', 'Shankar, H C', 'Shivpuri, R K', 'Shupe, M', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Smart, W', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sood, P M', 'Sosebee, M', 'Sotnikova, N', 'Souza, M', 'Spadafora, A L', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stewart, D', 'Stichelbaut, F', 'Stoyanova, D A', 'Stoker, D', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Sznajder, A', 'Tamburello, P D', 'Tarazi, J', 'Tartaglia, M', 'Thomas, T L T', 'Thompson, J', 'Trippe, T G', 'Tuts, P M', 'Varelas, N', 'Varnes, E W', 'Vititoe, D', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, G', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Won, E', 'Wood, D R', 'Xu, H', 'Yamada, R', 'Yamin, P', 'Yang, J', 'Yasuda, T', 'Yepes, P', 'Yoshikawa, C', 'Youssef, S', 'Yu, J', 'Yu, Y', 'Zhu, Z H', 'Zieminska, D', 'Zieminski, A', 'Zverev, E G', 'Zylberstejn, A']",['Search for the Decay $b \\to X_{s} \\mu ^{+} \\mu ^{-}$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'quark, semileptonic decay', 'quark, branching ratio', 'production, strangeness', 'B0, leptonic decay', 'mass spectrum, dimuon', 'yield, dimuon', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'beauty --> strangeness muon+ muon- anything', 'B0 --> muon+ muon-', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801027'],['We have searched for the flavor-changing neutral current decay b -> s mu+ mu- in p pbar collisions at sqrt(s) = 1.8 TeV with the DO detector at Fermilab. We determine the 90% confidence level limit for the branching fraction to be B(b -> X_s mu+ mu-) < 3.2 x 10^{-4}. We argue that this limit is more stringent than the best published limit on this decay rate.'],['1998-01-29']
1916,['eng'],"['Abbott, B', 'Abolins, M', 'Acharya, B S', 'Adam, I', 'Adams, D L', 'Adams, M', 'Ahn, S', 'Aihara, H', 'Alves, G A', 'Amos, N', 'Anderson, E W', 'Astur, R', 'Baarmand, M M', 'Baden, A', 'Balamurali, V', 'Balderston, J', 'Baldin, B Yu', 'Banerjee, S', 'Bantly, J', 'Barberis, E', 'Bartlett, J F', 'Bazizi, K', 'Belyaev, A', 'Beri, S B', 'Bertram, I', 'Bezzubov, V A', 'Bhat, P C', 'Bhatnagar, V', 'Bhattacharjee, M', 'Biswas, N', 'Blazey, G C', 'Blessing, S K', 'Bloom, P', 'Böhnlein, A', 'Bozhko, N', 'Borcherding, F O', 'Boswell, C', 'Brandt, A', 'Brock, R L', 'Bross, A D', 'Buchholz, D A', 'Burtovoi, V S', 'Butler, J M', 'Carvalho, W S', 'Casey, D', 'Casilum, Z', 'Castilla-Valdez, H', 'Chakraborty, D', 'Chang, S M', 'Chekulaev, S V', 'Chen, L P', 'Chen, W', 'Choi, S', 'Chopra, S', 'Choudhary, B C', 'Christenson, J H', 'Chung, M', 'Claes, D', 'Clark, A R', 'Cobau, W G', 'Cochran, J', 'Coney, L', 'Cooper, W E', 'Cretsinger, C E', 'Cullen-Vidal, D E', 'Cummings, M A C', 'Cutts, D', 'Dahl, O I', 'Davis, K', 'De, K', 'Del Signore, K', 'Demarteau, M', 'Denisov, D S', 'Denisov, S P', 'Diehl, H T', 'Diesburg, M', 'DiLoreto, G', 'Draper, P', 'Ducros, Y', 'Dudko, L V', 'Dugad, S R', 'Edmunds, D L', 'Ellison, J', 'Elvira, V D', 'Engelmann, R', 'Eno, S', 'Eppley, G', 'Ermolov, P', 'Eroshin, O V', 'Evdokimov, V N', 'Fahland, T', 'Fatyga, M K', 'Fehér, S', 'Fein, D K', 'Ferbel, T', 'Finocchiaro, G', 'Fisk, H E', 'Fisyak, Yu', 'Flattum, E M', 'Forden, G E', 'Fortner, M R', 'Frame, K C', 'Fuess, S', 'Gallas, E J', 'Galyaev, A N', 'Gartung, P E', 'Geld, T L', 'Genik, R J', 'Genser, K', 'Gerber, C E', 'Gibbard, B', 'Glenn, S', 'Gobbi, B', 'Goldschmidt, A', 'Gómez, B', 'Gómez, G', 'Goncharov, P I', 'González-Solis, J L', 'Gordon, H', 'Goss, L T', 'Gounder, K', 'Goussiou, A', 'Graf, N', 'Grannis, P D', 'Green, D R', 'Greenlee, H', 'Grim, G P', 'Grinstein, S', 'Grossman, N L', 'Grudberg, P M', 'Grünendahl, S', 'Guglielmo, G', 'Guida, J A', 'Guida, J M', 'Sen-Gupta, A', 'Gurzhev, S N', 'Gutíerrez, P', 'Gutnikov, Yu E', 'Hadley, N J', 'Haggerty, H', 'Hagopian, S', 'Hagopian, V', 'Hahn, K S', 'Hall, R E', 'Hanlet, P', 'Hansen, S', 'Hauptman, J M', 'Hedin, D', 'Heinson, A P', 'Heintz, U', 'Hernández-Montoya, R', 'Heuring, T C', 'Hirosky, R', 'Hobbs, J D', 'Hoeneisen, B', 'Hoftun, J S', 'Hsieh, F', 'Ting Hu Tong Hu', 'Hühn, T', 'Ito, A S', 'James, E', 'Jaques, J', 'Jerger, S A', 'Jesik, R', 'Jiang, J Z Y', 'Joffe-Minor, T M', 'Johns, K', 'Johnson, M', 'Jonckheere, A M', 'Jones, M', 'Jöstlein, H', 'Jun, S Y', 'Jung, C K', 'Kahn, S', 'Kalbfleisch, G R', 'Kang, J S', 'Karmanov, D E', 'Karmgard, D J', 'Kehoe, R', 'Kelly, M L', 'Kim, C L', 'Kim, S K', 'Klatchko, A', 'Klima, B', 'Klopfenstein, C', 'Klioukhine, V I', 'Kochetkov, V I', 'Kohli, J M', 'Koltick, D S', 'Kostritskii, A V', 'Kotcher, J', 'Kotwal, A V', 'Kourlas, J', 'Kozelov, A V', 'Kozlovskii, E A', 'Krane, J', 'Krishnaswamy, M R', 'Krzywdzinski, S', 'Kunori, S', 'Lami, S', 'Lander, R', 'Landry, F J', 'Landsberg, G L', 'Lauer, B M', 'Leflat, A', 'Li, H', 'Li, J', 'Li-Demarteau, Q Z', 'Lima, J G R', 'Lincoln, D', 'Linn, S L', 'Linnemann, J', 'Lipton, R', 'Liu, Y C', 'Lobkowicz, F', 'Loken, S C', 'Lökös, S', 'Lueking, L H', 'Lyon, A L', 'Maciel, A K A', 'Madaras, R J', 'Madden, R', 'Magana-Mendoza, L', 'Manankov, V', 'Mani, S', 'Mao, H S', 'Markeloff, R', 'Marshall, T', 'Martin, M I', 'Mauritz, K M', 'May, B', 'Mayorov, A A', 'McCarthy, R', 'McDonald, J', 'McKibben, T', 'McKinley, J', 'McMahon, T', 'Melanson, H L', 'Merkin, M', 'Merritt, K W', 'Miettinen, H', 'Mincer, A', 'Mishra, C S', 'Mokhov, N V', 'Mondal, N K', 'Montgomery, H E', 'Mooney, P', 'Da Motta, H', 'Murphy, C', 'Nang, F', 'Narain, M', 'Narasimham, V S', 'Narayanan, A', 'Neal, H A', 'Negret, J P', 'Némethy, P', 'Norman, D', 'Oesch, L H', 'Oguri, V', 'Oliveira, E', 'Oltman, E', 'Oshima, N', 'Owen, D', 'Padley, P', 'Para, A', 'Park, Y M', 'Partridge, R', 'Parua, N', 'Paterno, M', 'Pawlik, B', 'Perkins, J', 'Peters, M', 'Piegaia, R', 'Piekarz, H', 'Pishchalnikov, Yu', 'Podstavkov, V M', 'Pope, B G', 'Prosper, H B', 'Protopopescu, Serban D', 'Qian, J', 'Quintas, P Z', 'Raja, R', 'Rajagopalan, S', 'Ramírez, O', 'Rasmussen, L', 'Reucroft, S', 'Rijssenbeek, M', 'Rockwell, T', 'Roco, M T', 'Roe, N A', 'Rubinov, P M', 'Ruchti, R C', 'Rutherfoord, J P', 'Sánchez-Hernández, A', 'Santoro, A F S', 'Sawyer, L', 'Schamberger, R D', 'Schellman, H', 'Scully, J R', 'Shabalina, E', 'Shaffer, C', 'Shankar, H C', 'Shivpuri, R K', 'Shupe, M', 'Singh, H', 'Singh, J B', 'Sirotenko, V', 'Smart, W', 'Smith, E', 'Smith, R P', 'Snihur, R', 'Snow, G A', 'Snow, J', 'Snyder, S', 'Solomon, J', 'Sood, P M', 'Sosebee, M', 'Sotnikova, N', 'Souza, M', 'Spadafora, A L', 'Steinbruck, G', 'Stephens, R W', 'Stevenson, M L', 'Stewart, D', 'Stichelbaut, F', 'Stoyanova, D A', 'Stoker, D', 'Strauss, M', 'Streets, K', 'Strovink, M', 'Sznajder, A', 'Tamburello, P D', 'Tarazi, J', 'Tartaglia, M', 'Thomas, T L T', 'Thompson, J', 'Trippe, T G', 'Tuts, P M', 'Varelas, N', 'Varnes, E W', 'Vititoe, D', 'Volkov, A A', 'Vorobev, A P', 'Wahl, H D', 'Wang, G', 'Warchol, J', 'Watts, G', 'Wayne, M', 'Weerts, H', 'White, A', 'White, J T', 'Wightman, J A', 'Willis, S', 'Wimpenny, S J', 'Wirjawan, J V D', 'Womersley, J', 'Won, E', 'Wood, D R', 'Xu, H', 'Yamada, R', 'Yamin, P', 'Yang, J', 'Yasuda, T', 'Yepes, P', 'Yoshikawa, C', 'Youssef, S', 'Yu, J', 'Yu, Y', 'Zhu, Z H', 'Zieminska, D', 'Zieminski, A', 'Zverev, E G', 'Zylberstejn, A']",['Direct Measurement of the Top Quark Mass at D0'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'mass, truth', 'quark, decay', 'final state, ((n)jet lepton)', 'final state, dilepton', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'tables', 'truth --> W beauty', 'W --> quark antiquark', 'W --> lepton neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801025'],"['We determine the top quark mass m_t using t-tbar pairs produced in the D0 detector by \\sqrt{s} = 1.8 TeV p-pbar collisions in a 125 pb^-1 exposure at the Fermilab Tevatron. We make a two constraint fit to m_t in t-tbar -> b W^+bbar W^- final states with one W boson decaying to q-qbar and the other to e-nu or mu-nu. Likelihood fits to the data yield m_t(l+jets) = 173.3 +- 5.6 (stat) +- 5.5 (syst) GeV/c^2. When this result is combined with an analysis of events in which both W bosons decay into leptons, we obtain m_t = 172.1 +- 5.2 (stat) +- 4.9 (syst) GeV/c^2. An alternate analysis, using three constraint fits to fixed top quark masses, gives m_t(l+jets) = 176.0 +- 7.9 (stat) +- 4.8 (syst) GeV/C^2, consistent with the above result. Studies of kinematic distributions of the top quark candidates are also presented.']",['1998-01-28']
1917,['eng'],"['Diwan, M V']",['Search for T-violation in $K_{\\mu 3}$ decay'],['Particle Physics - Experimental Results'],"['talk, Tsukuba 1997/10/31', 'K+, leptonic decay', 'K+, radiative decay', 'K+, separated beam', 'time reversal, violation', 'muon+, polarization', 'astrophysics', 'baryon, asymmetry', 'proposed experiment, Brookhaven PS', 'K+ --> pi0 muon+ neutrino', 'K+ --> muon+ neutrino photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801023'],"['We have designed a new experiment (E923) at the BNL-AGS to search for the T-violating polarization of the muon normal to the decay plane of the KMU3 decay. The experiment aims to search for T-violation beyond the Standard Model; such a search is motivated by the need for a stronger CP violation source to account for the baryon asymmetry of the Universe. The experiment will be performed with in-flight decays from an intense (2.10e7 K/sec) 2 GeV/c separated K+ beam in an existing beam-line at the AGS. We expect to analyze more than 10e9 events to obtain the sensitivity of (delta P_t = +-0.00013) at 1 sigma, corresponding to the sensitivity of +-0.0007 to Im(xi), an improvement by 40 over the present limit on the same measurement. This paper describes the motivation for this experiment as well as other measurements of the same type. The experimental technique and the sensitivity is also described.']",['1998-01-27']
1918,['eng'],"['Paulini, M']",['Heavy Quarks at the Tevatron'],['Particle Physics - Experimental Results'],"['review, Rostock 1997/09/20', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, beauty', 'quark, pair production', 'quark, decay', 'final state, dilepton', 'final state, ((n)jet lepton)', 'final state, ((n)jet)', 'mass, truth', 'channel cross section', 'B0 anti-B0, interference', 'B0, mass difference', 'B, lifetime', 'B/s0, lifetime', 'B0, semileptonic decay', 'correlation, (charmed meson lepton)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802018'],"['We review the status of heavy quark physics at the Fermilab Tevatron collider by summarizing recent top quark and B physics results from CDF and DO. In particular, we discuss the measurement of the top quark mass and top production cross section as well as B meson lifetimes and time dependent B0 B0= mixing results.']",['1998-02-24']
1919,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Behnke, T', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'de Roeck, A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Estabrooks, P G', 'Etzion, E', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kowalewski, R V', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Lawson, I', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'List, B', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mihara, S', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Sachs, K', 'Saeki, T', 'Sahr, O', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Ueda, I', 'Utzat, P', 'Van Kooten, R', 'Vannerem, P', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Investigation of CP violation in $B^{0} \\to J/\\psi K_{s}^{0}$ decays at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'quark, beauty', 'quark, pair production', 'B0, hadronic decay', 'particle identification, flavor', 'mass spectrum, (J/psi(3100) K0(S))', 'violation, CP', 'Kobayashi-Maskawa angle', 'J/psi(3100), leptonic decay', 'K0(S), hadronic decay', 'charge correlation, (jet lepton)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'B0 --> J/psi(3100) K0(S)', 'anti-B0 --> J/psi(3100) K0(S)', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=EP-98-001', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801022']","['An investigation of CP violation was performed using a total of 24 candidates for B^0 -> J/psi K^0_S decay, with a purity of about 60%. These events were selected from 4.4 million hadronic Z^0 decays recorded by the OPAL detector at LEP. An analysis procedure, involving techniques to reconstruct the proper decay times and tag the produced b-flavours, B^0 or B^0(bar), has been developed to allow a first direct study of the time dependent CP asymmetry that, in the Standard Model, is sin(2beta). The result is sin(2beta) = 3.2_{-2.0}^{+1.8} +/- 0.5, where the first error is statistical and the second systematic. This result is used to determine probabilities for different values of sin(2beta) in the physical region from -1 to +1.']",['1998-01-26']
1920,['eng'],"['Avati, V', 'Eggert, Karsten', 'Taylor, C']",['FELIX'],['Detectors and Experimental Techniques'],"['talk, Frascati 1997/09/08', 'p p, colliding beam detector', 'colliding beam detector, proposed', 'p p, interaction', 'momentum spectrum, parton', 'small-x', 'jet, hadroproduction', 'multiplicity, minijet', 'diffraction', 'impact parameter, high', 'vacuum state', 'symmetry, chiral', 'scattering, heavy ion', 'transverse energy', 'exchange, two-photon', 'bending magnet, superconducting', 'semiconductor detector, pixel', 'drift chamber, time projection', 'counters and detectors, gas', 'calorimeter', 'trigger', 'data acquisition', 'magnetic detector, FELIX', 'proposed experiment, CERN LHC Coll', '14000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801021'],"['The FELIX collaboration has proposed the construction of a full acceptance detector for the LHC, to be located at Intersection Region 4, and to be commissioned concurrently with the LHC. The primary mission of FELIX is QCD: to provide comprehensive and definitive observations of a very broad range of strong-interaction processes. This paper reviews the detector concept and performance characteristics, the physics menu, and plans for integration of FELIX into the collider lattice and physical environment. The current status of the FELIX Letter of Intent is discussed.']",['1998-01-26']
1921,['eng'],"['Convery, M E']",['A Disoriented Chiral Condensate Search at the Fermilab Tevatron'],['Particle Physics - Experimental Results'],"['thesis', 'anti-p p, colliding beams', 'quantum chromodynamics, vacuum state', 'condensation, chiral', 'cosmic radiation, centauro', 'pi, hadroproduction', 'charged particle, multiplicity', 'photon, multiplicity', 'rapidity dependence', 'proportional chamber', 'calorimeter, electromagnetic', 'track data analysis', 'numerical calculations, Monte Carlo', 'experimental results, Batavia TEVATRON Coll', 'bibliography', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801020'],"[""MiniMax (Fermilab T-864) was a small test/experiment at the Tevatron designed to search for disoriented chiral condensates (DCC) in the forward direction. The MiniMax detector at the C0 collision region of the Tevatron was a telescope of 24 multi-wire proportional chambers (MWPC's) with a lead converter behind the eighth MWPC, allowing the detection of charged particles and photon conversions in an acceptance approximately a circle of radius 0.6 in pseudorapidity-azimuthal-angle space, centered on a pseudorapidity of about 4. The use of standard Monte Carlo simulations (PYTHIA, GEANT) is described, along with the simulation created by the MiniMax Collaboration to generate DCC domains. A description of the data analysis software is given, including detailed studies of its performance on data from the simulations. A set of robust observables is derived. These are insensitive to many efficiencies and to the details of the modeling of the parent pion production mechanisms, yet have distinguishable values for DCC and generic charged-neutral distributions. Simulations show that the robust observables are insensitive to detector efficiencies and to systematic errors in the data analysis software. The resulting values for robust observables for approximately 1.5 million events are shown to be consistent with production by only generic mechanisms. Results from samples of diffractive-tagged events and of high-multiplicity events also show no evidence for DCC.""]",['1998-01-23']
1922,['eng'],"['Abe, F', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amadon, A', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Aota, S', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bagdasarov, S L', 'Bailey, M W', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Baumann, T', 'Bedeschi, F', 'Behrends, S', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bettelli, S', 'Bevensee, B E', 'Bhatti, A A', 'Biery, K', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Blusk, S R', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Breccia, L', 'Bromberg, C', 'Bruner, N L', 'Brunetti, R', 'Buckley-Geer, E', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon, A', 'Wagner', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chang, P S', 'Chang, P T', 'Chao, H Y', 'Chapman, J', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chiou, C N', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Clark, A G', 'Cobal, M', 'Cocca, E', 'Contreras, M', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Costanzo, D', 'Couyoumtzelis, C', 'Cronin, D', 'Hennessy', 'Culbertson, R J', 'Dagenhart, D', 'Daniels, T', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Ely, R P', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Feng, Z', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Frisch, H', 'Fukui, Y', 'Gadomski, S', 'Galeotti, S', 'Gallinaro, M', 'Ganel, O', 'García-Sciveres, M', 'Garfinkel, A F', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giokaris, N D', 'Giromini, P', 'Giusti, G', 'Gold, M', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Groer, L S', 'Grosso-Pilcher, C', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hamilton, R', 'Handa, T', 'Handler, R', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hauser, J', 'Hayashi, E', 'Heinrich, J', 'Hao, W', 'Hinrichsen, B', 'Hoffman, K D', 'Hohlmann, M', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Huang, Z', 'Huffman, B T', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incagli, M', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Joshi, U', 'Kajfasz, E', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K M', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kennedy, R D', 'Kephart, R D', 'Kestenbaum, D S', 'Khazins, D M', 'Kikuchi, T', 'Kim, B J', 'Kim, H S', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Knoblauch, D', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korytov, A V', 'Kovacs, E', 'Kowald, W', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kuns, E W', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Nakano, I', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Lanzoni, M', 'Latino, G', 'LeCompte, T J', 'Leone, S', 'Lewis, J D', 'Limon, P', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Long, O', 'Loomis, C', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lys, J', 'Maeshima, K', 'Maksimovic, P', 'Mangano, Michelangelo L', 'Mariotti, M', 'Marriner, J P', 'Martin, A', 'Matthews, J A J', 'Mazzanti, P', 'McIntyre, P', 'Mélèse, P', 'Menguzzato, M', 'Menzione, A', 'Meschi, E', 'Metzler, S', 'Miao, C', 'Miao, T', 'Michail, G', 'Miller, R', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Miyashita, S', 'Moggi, N', 'Moore, E', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Murat, P', 'Murgia, S', 'Musy, M', 'Nakada, H', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman, C', 'Holmes, A J T', 'Ngan, C Y P', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okabe, M', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Parashar, N', 'Parri, A', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Perazzo, A', 'Pescara, L', 'Peters, M D', 'Phillips, T J', 'Piacentino, G', 'Pillai, M', 'Pitts, K T', 'Plunkett, R K', 'Pondrom, L', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Reher, D', 'Reischl, M', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Saab, T', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shaw, N M', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Ströhmer, R', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, J', 'Suzuki, T', 'Takahashi, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tanaka, M', 'Tannenbaum, B', 'Tartarelli, F', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Teramoto, Y', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thomas, T L', 'Thurman-Keup, R M', 'Keup, R M', 'Timko, M', 'Tipton, P', 'Titov, A', 'Tkaczyk, S M', 'Toback, D', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Truitt, S', 'Tseng, J', 'Turini, N', 'Uchida, T', 'Ukegawa, F', 'Valls, J', 'van den Brink, S C', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Warburton, A', 'Watanabe, T', 'Watts, T', 'Webb, R', 'Wei, C', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Wilkinson, R P', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolinski, D', 'Wolinski, J', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yasuoka, K', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Searches for New Physics in Diphoton Events in Proton Antiproton Collisions at $\\sqrt{s}=1.8$ TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'supersymmetry', 'supergravity', 'photon, pair production', 'transverse energy, missing-energy', 'jet, associated production', 'lepton, associated production', 'photon, associated production', 'quark, beauty', 'sparticle, pair production', 'sparticle, decay', 'gravitino', 'neutralino', 'electroweak interaction, validity test', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801019'],"['We have searched for anomalous production of missing E$_{\\rm T}$ ($\\mett$), jets, leptons ($e, \\mu, \\tau$), $b$-quarks, or additional photons in events containing two isolated, central']",['1998-01-21']
1923,['eng'],"['Soffer, A']",['Improving Measurements of the CKM Phase $\\gamma$ Using Charm Factory Results'],['Particle Physics - Experimental Results'],"['B+, hadronic decay', 'B+, branching ratio', 'Kobayashi-Maskawa angle, unitarity', 'measurement, efficiency', 'violation, CP', 'invariance, CP', 'interference, decay modes', 'width, asymmetry', 'D0, hadronic decay', 'anti-D0, hadronic decay', 'electron positron, annihilation', 'psi(3770), electroproduction', 'D0, pair production', 'experimental methods, proposed', 'B+ --> D0 K+', 'B+ --> anti-D0 K+', 'D0 --> K- pi+', 'anti-D0 --> K- pi+']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801018'],['Several authors have proposed methods to measure the phase $\\gamma$ of the Cabibbo-Kobayashi-Maskawa (CKM) unitarity triangle using decays of the type $B\\to DK$. We show how to remove uncertainties from these measurements and increase their sensitivity by measuring CP-conserving phases at a charm factory.'],['1998-01-21']
1924,['eng'],"['Kettell, S H']",['Rare and Forbidden Kaon Decays at the AGS'],['Particle Physics - Experimental Results'],"['review, Stanford 1997/08/04', 'K, rare decay', 'K, branching ratio', 'counters and detectors', 'experimental results', 'Brookhaven PS', 'tables', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801016'],"['An overview of the Rare Kaon Decay program at the AGS is presented, with particular emphasis on the three major experiments currently running and analyzing data. A brief review of earlier kaon decay experiments and of recent improvements in AGS performance is provided. This review concludes with a discussion of proposed and developing experiments planned to run in the year 2000 and beyond (AGS2000).']",['1998-01-19']
1925,['eng'],"['Devenish, R C E']",['PL3 Structure Functions'],['Particle Physics - Experimental Results'],"['review, Jerusalem 1997/08/19', 'lepton nucleon, deep inelastic scattering', 'nucleon, structure function', 'polarization, dependence', 'structure function, longitudinal', 'structure function, charm', 'photon, structure function', 'nucleon, spin', 'momentum spectrum, parton', 'hadron, electroproduction', 'hadron, photoproduction', 'total cross section', 'sum rule', 'experimental results', 'DESY HERA Stor', 'CERN SPS', 'SLAC Lab']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801013'],['Recent measurements of unpolarised and polarised nucleon structure functions and F_2(gamma) are reviewed. The implications for QCD and the gluon momentum distribution are discussed. The status of the understanding of the total virtual-photon proton total cross-section in the transition region between real photoproduction and deep-inelastic scattering is summarised briefly.'],['1998-01-15']
1926,['eng'],"['Wegener, D']",['b-Quark Physics at DORIS'],['Particle Physics - Experimental Results'],"['talk, Chicago 1997/06/29', 'history', 'electron positron, colliding beams', 'electron positron, annihilation', 'upsilon mesons, electroproduction', 'upsilon mesons, hadronic decay', 'final state, (3gluon)', 'B, pair production', 'B0 anti-B0, interference', 'B, decay modes', 'counters and detectors', 'DESY DORIS Stor', 'approx. 10 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802001'],['b-Quark Physics at DORIS'],['1998-02-03']
1927,['eng'],"['Behrens, B H']","[""Two-Body B Meson Decays to $\\eta$ and $\\eta^{'}$; 1$, Observation of $B\\to \\eta${'}K$""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, decay modes', 'B, branching ratio', 'final state, (2meson)', 'eta(958)', 'eta', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> eta(958) K', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801012'],"[""In a sample of 6.6 million produced B mesons we have observed decays B -> eta' K, with branching fractions BR(B+ -> eta' K+ = 6.5 +1.5 -1.4 +- 0.9) x $10^{-5}$ and BR(B0 -> eta' K0 = 4.7 +2.7 -2.0 +- 0.9) x $10^{-5}$. We have searched with comparable sensitivity for 17 related decays to final states containing an eta or eta' meson accompanied by a single particle or low-lying resonance. Our upper limits for these constrain theoretical interpretations of the B -> eta' K signal.""]",['1998-01-14']
1928,['eng'],"['Moinester, M A', 'Steiner, V']",['Primakoff Physics for CERN COMPASS Hadron Beam'],['Particle Physics - Experimental Results'],"['talk, Prague 1997/08', 'hadron hadron, interaction', 'hadron nucleus, interaction', 'lead', 'photon hadron, interaction', 'Primakoff effect', 'pi, polarizability', 'K, polarizability', 'p, polarizability', 'meson, hybrid', 'glueball', 'perturbation theory, chiral', 'anomaly, axial', 'angular distribution', 'meson, excited state', 'meson, transition', 'magnetic spectrometer, proposed', 'calorimeter', 'trigger', 'numerical calculations, Monte Carlo', 'proposed experiment, CERN SPS', 'approx. 300 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801011'],"['We describe a hadron physics program attainable with a partially instrumented CERN COMPASS spectrometer, involving tracking detectors and moderate-size ECAL2/HCAL2 calorimeters. COMPASS can realize a state-of-the-art hadron beam physics program based on hadron polarizability, hybrid mesons, chiral anomaly, and meson radiative transition studies. We review here the physics motivation for this hadron beam program. We describe the beam, detector, trigger requirements, and hardware/software requirements for this program. The triggers for all this physics can be implemented for simultaneous data taking. The program is based on using a hadron beam (positive/negative pion, kaon, proton) in COMPASS.']",['1998-01-14']
1929,['eng'],"['Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Schaffner, S F', 'Ugolini, D W', 'Wang, R', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Shelkov, V', 'Staeck, J', 'Stroynowski, R', 'Volobuev, I', 'Ye, J', 'Artuso, M', 'Efimov, A', 'Frasconi, F', 'Gao, M', 'Goldberg, M', 'He, D', 'Kopp, S E', 'Moneti, G C', 'Mountain, R', 'Mukhin, Y', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Xing, X', 'Bartelt, J', 'Csorna, S E', 'Jain, V', 'Marka, S', 'Freyberger, A P', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Barish, B C', 'Chadha, M', 'Chan, S', 'Eigen, G', 'Miller, J S', ""O'Grady, C"", 'Schmidtler, M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Asner, D M', 'Bliss, D W', 'Brower, W S', 'Masek, G E', 'Paar, H P', 'Sharma, V', 'Gronberg, J B', 'Kutschke, R', 'Lange, D J', 'Menary, S R', 'Morrison, R J', 'Nelson, H N', 'Nelson, T K', 'Qiao, C', 'Richman, J D', 'Roberts, D', 'Ryd, A', 'Witherell, M S', 'Balest, R', 'Behrens, B H', 'Cho, K', 'Ford, W T', 'Park, H', 'Rankin, P', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Bloom, K', 'Cassel, David G', 'Cho, H A', 'Coffman, D M', 'Crowcroft, D S', 'Dickson, M', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Elia, R', 'Foland, A D', 'Gaidarev, P', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Kandaswamy, J', 'Katayama, N', 'Kim, P C', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Ludwig, G S', 'Masui, J', 'Mevissen, J', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Ogg, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Soffer, A', 'Ward, C', 'Athanas, M', 'Avery, P', 'Jones, C D', 'Lohner, M', 'Prescott, C', 'Yang, S', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Briere, R A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Yamamoto, H', 'Browder, T E', 'Li, F', 'Li, Y', 'Rodríguez, J L', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Selen, M', 'Thaler, J J', 'Edwards, K W', 'Bellerive, A', 'Janicek, R', 'MacFarlane, D B', 'McLean, K W', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Coppage, D', 'Darling, C L', 'Davis, R', 'Hancock, N', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Anderson, S', 'Kubota, Y', 'Lattery, M', ""O'Neill, J J"", 'Patton, S', 'Poling, R A', 'Riehle, T', 'Savinov, V', 'Smith, A', 'Alam, M S', 'Athar, S B', 'Ling, Z', 'Mahmood, A H', 'Severini, H', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Blinov, S', 'Duboscq, J E', 'Fisher, K D', 'Fujino, D', 'Fulton, R', 'Gan, K K', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lee, J', 'Spencer, M B', 'Sung, M', 'Undrus, A E', 'Wanke, R', 'Wolf, A', 'Zoeller, M M', 'Nemati, B', 'Richichi, S J', 'Ross, W R', 'Skubic, P L', 'Wood, M', 'Bishai, M', 'Fast, J', 'Gerndt, E', 'Hinson, J W', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Yurko, M', 'Gibbons, L K', 'Johnson, S D', 'Kwon, Y', 'Roberts, S', 'Thorndike, E H']","[""Measurement of the Branching Ratios for the Decays of $D_{s}^{+}\\to \\eta\\pi^{+}, \\eta^{'}\\pi^{+}, \\eta\\rho^{+}$, and $\\eta ^{'}\\rho^{+}$""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D/s+, electroproduction', 'D/s+, hadronic decay', 'meson, pair production', 'eta', 'eta(958)', 'pi+', 'rho(770)+', 'Phi(1020)', 'D/s+, semileptonic decay', 'factorization', 'D/s+, branching ratio', 'D+, hadronic decay', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801010'],"[""Using a data sample with integrated luminosity of about 3.9 fb^{-1} collected in e+ e- annihilation with the CLEO-II detector at the Cornell Electron Storage Ring, we have measured the branching ratios for the decay modes Ds -> (eta, eta') pi and Ds -> (eta, eta') rho relative to Ds -> phi pi. These decay modes are among the most common hadronic decays of the Ds's and can be related by factorization to the semileptonic decays Ds -> (eta,eta') l nu. The results obtained are compared with previous CLEO results and with the branching ratios measured for the related semileptonic decays. We also report results on the Cabibbo-suppressed decays of the D+ to the same final states.""]",['1998-01-13']
1930,['eng'],"['Halzen, Francis']",['Large Natural Cherenkov Detectors'],['Detectors and Experimental Techniques'],"['review, Gran Sasso 1997/09/07', 'Cherenkov counter, water', 'solids, water', 'neutrino, cosmic radiation', 'muon, cosmic radiation', 'deep underground detector, Baikal', 'deep underground detector, NESTOR', 'deep underground detector, AMANDA']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801009'],"['In this review we first address two questions: 1. Why do we need kilometer-scale muon and neutrino detectors? 2. What do we learn from the operating Baikal and AMANDA detectors about the construction of kilometer-scale detectors? I will subsequently discuss the challenges for building the next-generation detectors. The main message is that these are different, in fact less ominous, than for commissioning the present, relatively small, detectors which must reconstruct events far outside their instrumented volume in order to achieve large effective telescope area.']",['1998-01-09']
1931,['eng'],"['Moinester, M A', 'Steiner, V']",['Pion and Kaon Polarizabilities and Radiative Transitions'],['Particle Physics - Experimental Results'],"['talk, Mainz 1997/09/01', 'photon meson, Compton scattering', 'pi, polarizability', 'K, polarizability', 'Primakoff effect', 'meson, photoproduction', 'symmetry, chiral', 'anomaly, chiral', 'meson resonance, photoproduction', 'effective Lagrangian, chiral', 'electron pi, interaction', 'hadron, beam', 'magnetic spectrometer', 'momentum resolution', 'calorimeter', 'trigger', 'numerical calculations, Monte Carlo', 'proposed experiment, CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801008'],"[""CERN COMPASS plans measurements of gamma-pi and gamma-K interactions using 50-280 GeV pion (kaon) beams and a virtual photon target. Pion (kaon) polarizabilities and radiative transitions will be measured via Primakoff effect reactions such as pi+gamma->pi'+gamma and pi+gamma->meson. The former can test a precise prediction of chiral symmetry; the latter for pi+gamma->a1(1260) is important for understanding the polarizability. The radiative transition of a pion to a low mass two-pion system, pi+gamma->pi+pi0, can also be studied to measure the chiral anomaly amplitude F(3pi) (characterizing gamma->3pi), arising from the effective Chiral Lagrangian. We review here the motivation for the above physics program. We describe the beam, target, detector, and trigger requirements for these experiments. We also describe FNAL SELEX attempts to study related physics via the interaction of 600 GeV pions with target electrons. Data analysis in progress aims to identify the reactions pi+e->pi'+e'+pi0 related to the chiral anomaly, and pi+e->pi'+e'+gamma related to pion polarizabilities.""]",['1998-01-09']
1932,['eng'],"['Armbruster, B', 'Blair, I M', 'Bodmann, B A', 'Booth, N E', 'Drexlin, G', 'Eberhard, V', 'Edgington, J A', 'Eichner, C', 'Eitel, K', 'Finckh, E', 'Gemmeke, H', 'Hössel, J G', 'Jannakos, T', 'Jünger, P', 'Kleifges, M', 'Kleinfeller, J', 'Kretschmer, W', 'Maschuw, R', 'Oehler, C', 'Plischke, P', 'Rapp, J', 'Ruf, C', 'Steidl, M', 'Stumm, O', 'Wolf, J', 'Zeitnitz, B']",['KARMEN Limits on $\\nu_{e} \\to \\nu_{\\tau}$ Oscillations in $2-\\nu$ and $3-\\nu$ Mixing Schemes'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'neutrino, interference', 'muon+, leptonic decay', 'at rest', 'neutrino/e, particle source', 'neutrino/mu', 'neutrino/tau', 'neutrino nucleus, nuclear reaction', 'carbon', 'charged current', 'neutrino, mass difference', 'neutrino, mixing angle', 'scintillation counter, liquid', 'calorimeter, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801007'],"[""The 56 tonne high resolution liquid scintillation calorimeter KARMEN at the beam stop neutrino source ISIS has been used to search for neutrino oscillations in the disappearance channel nu_e->x. The nu_e emitted in mu+ decay at rest are detected with spectroscopic quality via the exclusive charged current reaction 12-C(nu_e,e-)12-N_g.s. almost free of background. Analysis of the spectral shape of e- from the nu_e induced reaction as well as a measurement of the absolute nu_e flux allow to investigate oscillations of the type nu_e->nu_tau and nu_e->nu_mu . The flux independent ratio R(CC/NC) of charged current events 12-C(nu_e,e-)12-N_g.s. to neutral current events 12-C(nu,nu')12-C* provides additional information in the oscillation channel nu_e->x . All three analysis methods show no evidence for oscillations. For the nu_e->nu_tau channel 90%CL limits of sin^2(2t)<0.338 for dm^2>100eV^2 and dm^2<0.77eV^2 for maximal mixing in a simple 2 flavor oscillation formalism are derived. A complete 3 flavor analysis of the experimental data from five years of measurement with respect to nu_e<->nu_tau and nu_e<->nu_mu mixing is presented.""]",['1998-01-09']
1933,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the one-prong hadronic $\\tau$ branching ratios at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, pair production', 'tau-, semileptonic decay', 'tau-, branching ratio', 'final state, (1charged particle)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'tau- --> hadron- neutrino/tau', 'tau- --> hadron- (n)pi0 neutrino/tau', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801029', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-152']","['The branching ratios of the \\tau^- -> h^- \\nu_\\tau, \\tau^- -> h^- \\pi^0 1991-1995 data recorded with the OPAL detector at LEP. These branching ratios are measured simultaneously using three selection criteria and are found to be BR(\\tau^- -> h^- \\nu_\\tau) = (11.98 +/- 0.13 +/- 0.16)% BR(\\tau^- -> h^- \\pi^0 \\nu_\\tau) = (25.89 +/- 0.17 +/- 0.29)% BR(\\tau^- -> h^- >=2 \\pi^0 \\nu_\\tau) = ( 9.91 +/- 0.31 +/- 0.27)% where the first error is statistical and the second is systematic.']",['1998-02-02']
1934,['eng'],"['Bassler, U', 'Bernardi, G']",['Structure Function Measurements and Kinematic Reconstruction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'differential cross section', 'p, structure function', 'kinematics', 'small-x', 'data analysis method', 'rescaling', 'numerical calculations', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801017'],"['The procedure used for structure function measurements at HERA is briefly described and related to the properties of kinematic reconstruction. The reconstruction methods of the inclusive deep inelastic scattering variables are reviewed and their sensitivity to the energy and angle miscalibrations are discussed in detail. New prescriptions are introduced and related to the standard methods in order to optimize the F_2 structure function measurement over the widest kinematic range, both in the low x, low Q^2 and in the high x, high Q^2 regions. The prospects for the future high Q^2 studies are briefly discussed.']",['1998-01-20']
1935,['eng'],"['Spanier, S M']",['Crystal Barrel Results on Two-Body Decays of the Scalar Glueball'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'anti-p p, annihilation', 'at rest', 'scalar meson, hadroproduction', 'glueball, scalar', 'partial wave analysis', 'f0(1500), hadronic decay', 'four-pi-detector, experimental results', 'CERN LEAR', 'anti-p p --> p K0(L) K (n) pi', 'anti-p p --> 2K0(L) pi0', '0 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801006'],['The Crystal Barrel Collaboration observes scalar meson resonances in $\\bar p p$ annihilation. Based on the measurements and partial wave analyses these are candidates for the $^3$P$_0$ groundstate nonet. The supernummerary $f_0(1500)$ resonance is identified as a scalar groundstate glueball. Important information for its characterization comes from the decay pattern into pseudoscalar and scalar mesons. Data on kaonic decays in the mass region up to 1700 MeV are now avaible at Crystal Barrel. New analysis results are presented.'],['1998-01-08']
1936,['eng'],"['Raja, R', 'Tollestrup, A V']",['Calibrating the energy of a 50 X 50 GeV muon collider using spin precession'],['Particle Physics - Experimental Results'],"['muon+ muon-, storage ring', 'storage ring, proposed', 'energy, calibration', 'muon, leptonic decay', 'electron, energy loss', 'muon, polarization', 'muon, magnetic moment', 'magnetic field', 'electric field', 'numerical calculations', '100 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801004'],"['The neutral Higgs boson is expected to have a mass in the region 90-150 GeV in various schemes within the Minimal Supersymmetric extension to the Standard Model. A first generation Muon Collider is uniquely suited to investigate the mass, width and decay modes of the Higgs boson, since the coupling of the Higgs to muons is expected to be strong enough for it to be produced in the s channel mode in the muon collider. Due to the narrow width of the Higgs, it is necessary to measure and control the energy of the individual muon bunches to a precision of a few parts in a million. We investigate the feasibility of determining the energy scale of a muon collider ring with circulating muon beams of 50 GeV energy by measuring the turn by turn variation of the energy deposited by electrons produced by the decay of the muons. This variation is caused by the existence of an average initial polarization of the muon beam and a non-zero value of g-2 for the muon. We demonstrate that it is feasible to determine the energy scale of the machine with this method to a few parts per million using data collected during 1000 turns.']",['1998-01-06']
1937,['eng'],"['Barberis, D', 'Beusch, Werner', 'Binon, Freddy G', 'Blick, A M', 'Close, Francis Edwin', 'Danielsen, K M', 'Dolgopolov, A V', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Inyakin, A V', 'Ishida, T', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinashi, T', 'Kinson, J B', 'Kirk, A', 'Klempt, W', 'Kolosov, V', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Maljukov, S', 'Martinengo, P', 'Minashvili, I A', 'Myklebost, K', 'Nakagawa, T', 'Norman, K L', 'Olsen, J M', 'Peigneux, J P', 'Polovnikov, S A', 'Polyakov, V A', 'Prokoshkin, Yu', 'Romanovsky, V I', 'Rotscheidt, Herbert', 'Rumyantsev, V', 'Rusakovitch, N', 'Samoylenko, V D', 'Semenov, A A', 'Sené, M', 'Sené, R', 'Shagin, P M', 'Shimizu, H', 'Singovsky, A V', 'Sobol, A E', 'Soloviev, A S', 'Stassinaki, M', 'Stroot, J P', 'Sugonyaev, V P', 'Takamatsu, K', 'Tchlatchidze, G', 'Tsuru, T', 'Vasileiadis, G', 'Venables, M', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the centrally produced $\\pi^{+}\\pi^{-} \\pi^{0}$ channel in pp interactions at $450 GeV/c$'],['Particle Physics - Experimental Results'],"['p p, exclusive reaction', 'pi, multiple production', 'mass spectrum, (pi+ pi- pi0)', 'meson resonance, hadroproduction', 'glueball, search for', 'transverse momentum, dependence', 'Dalitz plot', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p pi+ pi- pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801003'],"['The reaction pp -> pf (pi+pi-pi0) ps has been studied at 450 GeV/c in an experiment designed to search for gluonic states. A spin analysis has been performed and the dPT filter applied. The analysis confirms the previous observation that all undisputed qqbar states are suppressed at small dPT. In addition, a clear difference is observed in the production mechanism for the eta and omega.']",['1998-01-06']
1938,['eng'],"['Willocq, S']",['Electroweak and Heavy Flavor Physics at SLD'],['Particle Physics - Experimental Results'],"['talk, Batavia 1997/11/06', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'polarization, asymmetry', 'Z0, hadronic decay', 'Weinberg angle', 'quark, beauty', 'quark, charm', 'quark, pair production', 'Z0, branching ratio', 'B+, lifetime', 'B0, lifetime', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'time dependence', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802005'],"['We review recent electroweak and B physics results obtained in polarized e+e- interactions at the SLC by the SLD experiment. Unique and precise measurements of the electroweak parameters Ae, Ab, Ac, Rb and Rc provide powerful constraints on the Standard Model. The excellent 3-D vertexing capabilities of SLD are further exploited to extract precise B+ and B0 lifetimes, as well as measurements of the time evolution of B0-B0-bar mixing.']",['1998-02-03']
1939,['eng'],"['Etzion, E']",['Measurements of Hadronic Asymmetries in $e^{+}e^{-}$ Collisions'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, charm', 'quark, beauty', 'angular distribution, asymmetry', 'polarization, asymmetry', 'jet, charge', 'charge, asymmetry', 'Weinberg angle', 'experimental results', 'SLAC SLC Linac', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801002'],"['High precision experimental new electroweak results measured at the four LEP experiments and the SLD collaboration are discussed. Heavy quark (b b-bar and c c-bar) forward-backward asymmetries measured at LEP are presented along with polarized forward-backward and left-right asymmetries measured at SLD. The results are compared, and the combined averages are used to evaluate the Standard Model parameters.']",['1998-01-02']
1940,['eng'],"['Hoffman, K']",['Searches for heavy exotic states at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'Higgs particle', 'charged particle, massive', 'Higgs particle, hadroproduction', 'W, associated production', 'Higgs particle, hadronic decay', 'lepton, transverse momentum', 'transverse energy, missing-energy', 'jet, multiplicity', 'mass spectrum, (2jet)', 'resonance, search for', 'mass spectrum, dilepton', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> Higgs particle W anything', 'Higgs particle --> 2beauty', ""anti-p p --> Z' anything"", ""Z' --> lepton+ lepton-"", '1800 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712032', 'http://www-lib.fnal.gov/archive/1997/conf/Conf-97-430-E.html']","['We present the results of searches for Standard Model Higgs, charged stable massive particles, dijet mass resonances, and heavy neutral gauge bosons in Tevatron ppbar collisions at sqrt s = 1.8 TeV using the CDF and D0 detectors.']",['1997-12-30']
1941,['eng'],"['Daoudi, M', 'Beneke, M', 'Buchalla, G', 'Dunietz, I', 'Jackson, D J', 'Kaganand, J', 'Rathsman, A']",['Search for CP violation and $b \\to sg$ in inclusive B decays'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'electron positron, colliding beams', 'electron positron, annihilation', 'B0, pair production', 'B0, decay modes', 'asymmetry', 'violation, CP', 'track data analysis, vertex', 'decay, path length', 'quark, beauty', 'quark, decay', 'K+, transverse momentum', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'beauty --> strangeness gluon', '91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712031'],['We present preliminary results on two analyses performed by the SLD Collaboration using inclusive B decays: a search for CP violation and a search for the b --> sg transition.'],['1997-12-24']
1942,['eng'],"['Foster, B']",['Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron p, colliding beams', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'scaling, violation', 'p, structure function', 'gluon, momentum spectrum', 'diffraction, structure function', 'model, pomeron', 'momentum transfer, high', 'structure function, longitudinal', 'structure function, charm', 'jet, multiplicity', 'vector meson, photoproduction', 'J/psi(3100)', 'production, charm', 'production, small-angle', 'neutral current', 'charged current', 'strong interaction, coupling constant', 'differential cross section', 'cross section, energy dependence', 'cross section, momentum transfer', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'DESY HERA Stor', 'bibliography', '((5)) ((6))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712030'],['Results from the H1 and ZEUS experiments at HERA on deep inelastic scattering are reviewed. The data lead to a consistent picture of a steep rise in the F_2 structure function and in the gluon density within the proton. Important new information on the partonic structure of diffraction is emerging from H1 and ZEUS. The space-like region in which the weak and electromagnetic interactions become of equal strength is being explored for the first time. A possible excess of events at high x and Q^2 compared to the expectations of the Standard Model has been observed in both experiments.'],['1997-12-24']
1943,['eng'],"['Abbott, B', 'Abolins, M', 'Acharya, B S']",['A Measurement of the W Boson Mass'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'W, mass', 'mass spectrum, transverse', 'electron, transverse momentum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'W --> electron neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712029'],"['We present a measurement of the W boson mass using data collected by the D0 experiment at the Fermilab Tevatron during 1994--1995. We identify W bosons by their decays to $e\\nu$ final states. We extract the W mass, M(W), by fitting the transverse mass and transverse electron momentum spectra from a sample of 28,323 W to $e\\nu$ decay candidates. We use a sample of 3,563 dielectron events, mostly due to Z to ee decays, to constrain our model of the detector response. From the transverse mass fit we measure M(W) = $80.44\\pm0.10(stat)\\pm0.07(syst)$ GeV. Combining this with our previously published result from data taken in 1992--1993, we obtain M(W) $= 80.43\\pm0.11$ GeV.']",['1997-12-23']
1944,['eng'],"['Abbott, B', 'Abolins, M', 'Acharya, B S']",['A measurement of the W boson mass at the Fermilab p$\\bar p$ collider'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'W, mass', 'mass spectrum, transverse', 'transverse momentum, spectra', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712028'],"['We report a measurement of the W boson mass based on an integrated luminosity of 82 pb$^{-1}$ from \\ppbar collisions at $\\sqrt{s}=1.8$ TeV recorded in 1994--1995 by the \\Dzero detector at the Fermilab Tevatron. We identify W bosons by their decays to $e\\nu$ and extract the mass by fitting the transverse mass spectrum from 28,323 W boson candidates. A sample of 3,563 dielectron events, mostly due to Z to ee decays, constrains models of W boson production and the detector. We measure $\\mw=80.44\\pm0.10(stat)\\pm0.07(syst)$~GeV. By combining this measurement with our result from the 1992--1993 data set, we obtain $\\mw=80.43\\pm0.11$ GeV.']",['1997-12-23']
1945,['eng'],"['Doyle, A T']",['Diffraction'],['Particle Physics - Experimental Results'],"['review, Stanford 1997/08/04', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'anti-p p, colliding beams', 'anti-p p, interaction', 'diffraction, structure function', 'Regge poles', 'exchange, pomeron', 'color, singlet', 'quantum chromodynamics', 'vector meson, photoproduction', 'jet, photoproduction', 'photon, dissociation', 'hadron, multiple production', 'event shape analysis', 'W, associated production', 'jet, hadroproduction', 'final state, (2jet)', 'channel cross section, energy dependence', 'momentum transfer, dependence', 'experimental results', 'DESY HERA Stor', 'Batavia TEVATRON Coll', '((6)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712027'],"['Measurements of diffractive phenomena observed at HERA and the Tevatron are reviewed. A short introduction to the theoretical background is presented where colour singlet exchange reactions are discussed and the diffractive contribution and its interpretation via pomeron exchange outlined. The review focuses on the current experimental directions at HERA and discusses exclusive production of vector mesons, the dissociation of real photons and the deep inelastic structure of diffraction. Complementary information obtained from hadronic final states and jet structures is also discussed. The experimental signatures for diffractive jet and $W^\\pm$ production observed at the Tevatron are described and the rates compared with those from the HERA experiments.']",['1997-12-23']
1946,['eng'],"['Bianco, S']","['DEAR, FINUDA, KLOE']",['Particle Physics - Experimental Results'],"['talk, Merida 1996/10/30', 'electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), hadronic decay', 'K, pair production', 'K, decay modes', 'violation, CP', 'K- nucleus, nuclear reaction', 'hyperfragment, hadroproduction', 'K-, mesic atom', 'energy levels, mesic atom', 'K nucleon, scattering length', 'magnetic detector, KLOE', 'magnetic spectrometer, FINUDA', 'proposed experiment, Frascati Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712026'],"['Physics at DAFNE, the new Frascati e+e- machine, is reviewed, as well as the esperiments: DEAR - search for KN exotic atoms, FINUDA - spectroscopy and decays of hypernuclei, and KLOE - a multipurpose detector designed for measuring direct CP violation in the K system.']",['1997-12-19']
1947,['eng'],"['Suleimanov, M K', 'Abdinov, O B', 'Anoshin, A I', 'Bagirov, A M', 'Bogdanowicz, J', 'Kuznetsov, A A']",['Single-particle correlations in events with the total disintegration of nuclei'],['Particle Physics - Experimental Results'],"['pi- nucleus, nuclear reaction', 'p nucleus, nuclear reaction', 'nucleus nucleus, nuclear reaction', 'deuteron', 'carbon', 'multiple production', 'correlation function, one-particle', 'transverse momentum', 'momentum transfer, dependence', 'dependence, mass number', 'bubble chamber(heavy liquid), experimental results', 'Dubna PS', 'Serpukhov PS', '40 GeV/c (pi-), 4.2 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712025'],"['New experimental data on the behaviour of the single-particle two-dimensional correlation functions R versus Q (Q is the number of nucleons emitted from nuc- lei) and Ap (Ap is the mass of projectile nuclei) are presented in this paper. The interactions of protons, d, 4He and 12C nuclei with carbon nuclei (at a momentum of 4.2 A GeV/c) are considered.The values of R are obtained separately for pi minus mesons and protons.In so doing,the values of R are normalized so that -1=<R=<1.The value of R=0 corresponds to the case of the absence of corre- lations.It has been found that the Q- and Ap-dependence of R takes place only for weak correlations (R< 0.3).In the main (90 %),these correlations are con- nected with the variable pt and have a nonlinear character, that is the regi- ons with different characters of the Q-dependence of R are separated: there is a change of regimes in the Q-dependences of R.The correlations weaken with increasing Ap, and the variable R gets the least values of all the considered ones in 12CC interactions.Simultaneously with weakening the correlations in the region of large Q, the character of the Q-dependence of R changes.']",['1997-12-19']
1948,['eng'],"['Frlez, E', 'Pocanic, D', 'Assamagan, K A', 'Chen, J P', 'Keeter, K J', 'Marshall, R M', 'Minehart, R C', 'Smith, L C', 'Dodge, G E', 'Hanna, S S', 'King, B H', 'Knudson, J N']",['Differential cross sections for pion charge exchange on the proton at 27.5 MeV'],['Particle Physics - Experimental Results'],"['pi- p, charge exchange', 'differential cross section, angular dependence', 'partial wave analysis', 'magnetic spectrometer, experimental results', 'LAMPF Linac', 'pi- p --> n pi0', '0.0027 GeV-kin']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712024'],['We have measured pion single charge exchange differential cross sections on the proton at 27.5 MeV incident $\\pi^-$ kinetic energy in the center of momentum angular range between $0^\\circ$ and $55^\\circ$. The extracted cross sections are compared with predictions of the standard pion-nucleon partial wave analysis and found to be in excellent agreement.'],['1997-12-19']
1949,['eng'],"['Artuso, M', 'Azfar, F', 'Efimov, A', 'Goldberg, M', 'He, D', 'Kopp, S E', 'Moneti, G C', 'Mountain, R', 'Schuh, S', 'Skwarnicki, T', 'Stone, S', 'Viehhauser, G', 'Xing, X', 'Bartelt, J', 'Csorna, S E', 'Jain, V', 'McLean, K W', 'Marka, S', 'Godang, R', 'Kinoshita, K', 'Lai, I C', 'Pomianowski, P A', 'Schrenk, S', 'Bonvicini, G', 'Cinabro, D', 'Greene, R', 'Perera, L P', 'Zhou, G J', 'Chadha, M', 'Chan, S', 'Eigen, G', 'Miller, J S', ""O'Grady, C"", 'Schmidtler, M', 'Urheim, J', 'Weinstein, A J', 'Würthwein, F', 'Bliss, D W', 'Masek, G E', 'Paar, H P', 'Prell, S', 'Sharma, V', 'Asner, D M', 'Gronberg, J B', 'Hill, T S', 'Lange, D J', 'Morrison, R J', 'Nelson, H N', 'Nelson, T K', 'Roberts, D', 'Ryd, A', 'Balest, R', 'Behrens, B H', 'Ford, W T', 'Park, H', 'Roy, J D', 'Smith, J G', 'Alexander, J P', 'Baker, R', 'Bebek, C', 'Berger, B E', 'Berkelman, K', 'Bloom, K', 'Boisvert, V', 'Cassel, David G', 'Crowcroft, D S', 'Dickson, M', 'Von Dombrowski, S', 'Drell, P S', 'Ecklund, K M', 'Ehrlich, R', 'Foland, A D', 'Gaidarev, P', 'Gibbons, L K', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Hopman, P I', 'Kandaswamy, J', 'Kim, P C', 'Kreinick, D L', 'Lee, T', 'Liu, Y', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Ogg, M', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Soffer, A', 'Valant-Spaight, B L', 'Ward, C', 'Athanas, M', 'Avery, P', 'Jones, C D', 'Lohner, M', 'Patton, S', 'Prescott, C', 'Yelton, J', 'Zheng, J', 'Brandenburg, G', 'Briere, R A', 'Ershov, A', 'Gao, Y S', 'Kim, D Y J', 'Wilson, R', 'Yamamoto, H', 'Browder, T E', 'Li, Y', 'Rodríguez, J L', 'Bergfeld, T', 'Eisenstein, B I', 'Ernst, J', 'Gladding, G E', 'Gollin, G D', 'Hans, R M', 'Johnson, E', 'Karliner, I', 'Marsh, M A', 'Palmer, M', 'Selen, M', 'Thaler, J J', 'Edwards, K W', 'Bellerive, A', 'Janicek, R', 'MacFarlane, D B', 'Patel, P M', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Coppage, D', 'Darling, C L', 'Davis, R', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Zhou, L', 'Anderson, S', 'Kubota, Y', 'Lee, S J', ""O'Neill, J J"", 'Poling, R A', 'Riehle, T', 'Smith, A', 'Alam, M S', 'Athar, S B', 'Ling, Z', 'Mahmood, A H', 'Timm, S', 'Wappler, F', 'Anastassov, A', 'Duboscq, J E', 'Fujino, D', 'Gan, K K', 'Hart, T', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lee, J', 'Spencer, M B', 'Sung, M', 'Undrus, A E', 'Wanke, R', 'Wolf, A', 'Zoeller, M M', 'Nemati, B', 'Richichi, S J', 'Ross, W R', 'Severini, H', 'Skubic, P L', 'Bishai, M', 'Fast, J', 'Hinson, J W', 'Menon, N', 'Miller, D H', 'Shibata, E I', 'Shipsey, I P J', 'Yurko, M', 'Glenn, S', 'Johnson, S D', 'Kwon, Y', 'Roberts, S', 'Thorndike, E H', 'Jessop, C P', 'Lingel, K', 'Marsiske, H', 'Perl, Martin Lewis', 'Savinov, V', 'Ugolini, D W', 'Wang, R', 'Zhou, X', 'Coan, T E', 'Fadeev, V', 'Korolkov, I Ya', 'Maravin, Y', 'Narsky, I', 'Shelkov, V', 'Staeck, J', 'Stroynowski, R', 'Volobuev, I', 'Ye, J']",['Measurement of $Br(D^{0}\\to K^{-}\\pi^{+})$ using Partial Reconstruction of $\\overline{B}\\to D^{*+}X l^{-}\\overline{\\nu}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, cascade decay', 'D0, hadronic decay', 'D, branching ratio', 'final state, (pi+ lepton-)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'anti-B --> D*(2010) lepton- antineutrino anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712023'],"['We present a measurement of the absolute branching fraction for $D^0 -> K^- pi^+$ using the reconstruction of the decay chain $Bbar -> D^{*+} X l^- nubar $, $D^{*+} -> D^0 pi^+$ where only the lepton and the low-momentum pion from the $D^{*+}$ are detected. With data collected by the CLEO II detector at the Cornell Electron Storage Ring, we have determined $Br(D^0 -> K^- pi^+)= [3.81 +- 0.15(stat.) +- 0.16(syst.)]%$.']",['1998-01-05']
1950,['eng'],"['Carena, M S', 'Culbertson, R J', 'Eno, S', 'Frisch, H J', 'Mrenna, S']",['The Search for Supersymmetry at the Tevatron Collider'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'supersymmetry, symmetry breaking', 'sparticle, search for', 'Higgs particle, search for', 'Higgs particle, multiplet', 'doublet, 2', 'sparticle, mass spectrum', 'supergravity', 'R parity, violation', 'sparticle, pair production', 'sparticle, decay modes', 'final state, (3lepton)', 'final state, ((n)jet missing-energy)', 'final state, (dilepton missing-energy)', 'final state, (2photon missing-energy)', 'transverse energy, missing-energy', 'quark, truth', 'quark, pair production', 'quark, decay', 'LSP', 'jet, multiplicity', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712022'],"['We review the status of searches for Supersymmetry at the Tevatron Collider. After discussing the theoretical aspects relevant to the production and decay of supersymmetric particles at the Tevatron, we present the current results for Runs Ia and Ib as of the summer of 1997. To appear in the book ""Perspectives in Supersymmetry"", edited by G.L. Kane, World Scientific.']",['1998-01-05']
1951,['eng'],"['Kaplan, D M']",['Remarks on Muon $g-2$ Experiments and Possible CP Violation in $\\pi\\to\\mu\\to e$ Decay'],['Particle Physics - Experimental Results'],"['muon, leptonic decay', 'muon, magnetic moment', 'violation, CP', 'pi+, leptonic decay', 'pi-, leptonic decay', 'muon, polarization', 'polarization, asymmetry', 'magnetic field', 'electron, yield', 'time dependence', 'interpretation of experiments', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712021'],['The first experimental limit on CP violation in pi -> mu -> e decay is extracted from published results of the CERN g-2 experiment.'],['1997-12-17']
1952,['eng'],"['Breitweg, J']",['Measurement of the t Distribution in Diffractive Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'photon p, interaction', 'diffraction', 'hadron, photoproduction', 'photon, dissociation', 'momentum transfer, spectra', 'slope', 'transverse momentum, spectra', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'photon p --> p (n)hadron', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712019'],"['Photon diffractive dissociation, $\\gamma p \\to Xp$, has been studied at HERA with the ZEUS detector using $ep$ interactions where the virtuality $Q^2$ of the exchanged photon is smaller than 0.02 GeV$^2$. The squared four-momentum $t$ exchanged at the proton vertex was determined in the range $0.073<|t|<0.40$ GeV$^2$ by measuring the scattered proton in the ZEUS Leading Proton Spectrometer. In the photon-proton centre-of-mass energy interval $176<W<225$ GeV and for masses of the dissociated photon system $4<M_X<32$ GeV, the $t$ distribution has an exponential shape, $dN/d|t| \\propto \\exp{(-b|t|)}$, with a slope parameter $b=6.8 \\pm 0.9$~(stat.)~$ ^{+1.2}_{-1.1}$~(syst.)~GeV$^{-2}$.']",['1997-12-16']
1953,['eng'],"['Breitweg, J']",['Elastic and Proton-Dissociative $\\rho^0$ Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'rho(770)0, photoproduction', 'rho(770)0, hadronic decay', 'mass spectrum, (pi+ pi-)', 'channel cross section, energy dependence', 'differential cross section, momentum transfer', 'spin, density matrix', 'angular distribution', 'exchange, pomeron', 'p, dissociation', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712020'],"['Elastic and proton-dissociative rho0 photoproduction (gamma p-->rho0 p,gamma p -->rho0 N,with rho0-->pi+pi-) has been studied in ep interactions at HERA for gamma-p centre-of-mass energies in the range 50<W<100 GeV and for |t|<0.5 GeV2; the results on the p-dissociative reaction are presented for masses of the dissociated proton system in the range MN^2<0.1W^2.For the elastic process,the pi+pi- invariant mass spectrum has been investigated as a function of t. As in fixed target experiments, the rho0 resonance shape is asymmetric;this asymmetry decreases with increasing |t|.The cross section has been studied as a function of W; a fit to the resonant part with the form W^a gives a=0.16\\pm0.06(stat.) +0.11-0.15(syst.). The resonant part of the gamma p-->pi+pi- p cross section is 11.2\\pm 0.1(stat.)+1.1-1.2 (syst.) mub at <W>=71.7 GeV. The t dependence of the cross section can be described by a function of the type Ae^(-b|t|+ct^2) with b=10.9\\pm0.3(stat.)+1.0-0.5(syst.)GeV-2 and c=2.7\\pm0.9(stat.)+1.9-1.7(syst.) GeV-4. The t dependence has also been studied as a function of W and a value of the slope of the pomeron trajectory 0.23\\pm0.15(stat.)+0.10-0.07(syst.)GeV-2 has been deduced. The rho spin density matrix elements r^04_00,r^04_1-1 and Re[r^04_10] have been measured and found to be consistent with expectations based on SCHC. For p-dissociative pi+pi- photoproduction in the rho0 mass range, the distributions of the two-pion invariant mass, W and the polar and azimuthal angles of the pions in the helicity frame are the same within errors as those for the elastic process. The t distribution has been fitted to an exponential function with a slope parameter 5.8\\pm0.3(stat.)\\pm0.5(syst.)GeV-2. The ratio of the elastic to p-dissociative rho0 photoproduction cross section is 2.0\\pm0.2(stat.)\\pm0.7(syst.).']",['1997-12-17']
1954,['eng'],"['Schwiening, J']","['DIRC, a New Type of Particle Identification System for BaBar']",['Detectors and Experimental Techniques'],"['talk, Santa Monica 1997/10/13', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'optics, reflection', 'glass', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712018'],"['The DIRC, a new type of Cherenkov imaging device, has been selected as the primary particle identification system for the BaBar detector at the asymmetric B-factory, PEP-II. It is based on total internal reflection and uses long, rectangular bars made from synthetic fused silica as Cherenkov radiators and light guides. In this paper, the principles of the DIRC ring imaging Cherenkov technique are explained and results from the prototype program are presented. The studies of the optical properties and radiation hardness of the quartz radiators are described, followed by a discussion of the detector design.']",['1997-12-15']
1955,['eng'],"['Chèze, J B', 'Erhan, S', 'Kuzucu-Polatoz, A', 'Medinnis, M', 'Ozdes, N', 'Schlein, Peter E', 'Zeyrek, M T', 'Zsembery, J', 'Zweizig, J G']",['Measurements of Inclusive $\\overline{\\Lambda}$ Production with Large $x_f$ at the $Sp\\overline{p}S$-Collider'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Antilambda, hadroproduction', 'production, small-angle', 'Antilambda, hadronic decay', 'differential cross section, dependence', 'transverse momentum, dependence', 'Antilambda, polarization', 'magnetic spectrometer, experimental results', 'CERN SPS', 'anti-p p --> Antilambda anything', '630 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712017'],"['We report results of inclusive measurements of anti-Lambda, produced in the forward direction at the SPS with sqrt(s) = 630 GeV, using the UA8 small angle Roman Pot spectrometers. These measurements cover the range in Feynman-x_f and transverse momentum, 0.6 < x_f < 1.0 and 0.4 < p_t < 0.7 GeV, respectively. Within a systematic uncertainty of +-20% on the absolute cross section measurements, the results are indistinguishable from those made by some of us in two earlier experiments at the CERN Intersecting Storage Rings, with energies, sqrt(s) = 53 and 62 GeV. In the x_f-range, 0.6-0.9, the absolute cross sections are lower by a factor of 2 to 3 than the predictions of the Lund model as embodied in the PYTHIA 5.6 and JETSET 7.3 Monte Carlo programs, indicating inadequacies in knowledge of the baryon fragmentation function. For the largest x_f-range, 0.9-1.0, the measurements agree with the Monte Carlo predictions. We have measured the average anti-Lambda polarization for our events and find (6 +- 12%), consistent with previous measurements at the ISR in the present region of x_f - p_t.']",['1997-12-15']
1956,['eng'],"['Taylor, L']",['Properties of the W boson'],['Particle Physics - Experimental Results'],"['review, Bristol 1997/06/25', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, hadroproduction', 'W, electroproduction', 'W, pair production', 'W, leptonic decay', 'W, hadronic decay', 'W, branching ratio', 'W, width', 'coupling, (Z0 2W)', 'coupling, (2W photon)', 'W, mass', 'mass spectrum', 'experimental results', 'Batavia TEVATRON Coll', 'CERN LEP Stor', '((5)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712016'],['The properties of the W boson are reviewed. Particular emphasis is placed on recent measurements from the LEP2 and Tevatron experiments.'],['1997-12-15']
1957,['eng'],"['Swain, J D', 'Taylor, L']",['Numerical Construction of Likelihood Distributions and the Propagation of Errors'],['Detectors and Experimental Techniques'],"['statistical analysis, error', 'numerical methods', 'W, mass', 'mass spectrum, transverse', 'neutrino/tau, mass', 'mixing angle, (neutrino/tau neutrino/L)', 'tau, decay modes', 'tau, branching ratio', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712015'],"['The standard method for the propagation of errors, based on a Taylor series expansion, is approximate and frequently inadequate for realistic problems. A simple and generic technique is described in which the likelihood is constructed numerically, thereby greatly facilitating the propagation of errors.']",['1997-12-15']
1958,['eng'],"['Chadha, M']",['Improved Measurement of the Pseudoscalar Decay Constant $f_{D_{s}}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'quark, charm', 'quark, pair production', 'yield, (D/s*(2110) D/s+)', 'D/s+, hadronic decay', 'D/s+, leptonic decay', 'D/s+, branching ratio', 'D/s, decay constant', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D/s+ --> Phi(1020) pi+', 'D/s+ --> muon+ neutrino', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712014'],"['We present a new determination of the Ds decay constant, f_{Ds} using 5 million continuum charm events obtained with the CLEO II detector. Our value is derived from our new measured ratio of widths for Ds -> mu nu/Ds -> phi pi of 0.173+/- 0.021 +/- 0.031. Taking the branching ratio for Ds -> phi pi as (3.6 +/- 0.9)% from the PDG, we extract f_{Ds} = (280 +/- 17 +/- 25 +/- 34){MeV}. We compare this result with various model calculations.']",['1997-12-12']
1959,['eng'],"['Barate, R', 'Buskulic, D', 'Décamp, D', 'Ghez, Philippe', 'Goy, C', 'Lees, J P', 'Lucotte, A', 'Minard, M N', 'Nief, J Y', 'Pietrzyk, B', 'Boix, G', 'Casado, M P', 'Chmeissani, M', 'Crespo, J M', 'Delfino, M C', 'Fernández, E', 'Fernández-Bosman, M', 'Garrido, L', 'Graugès, E', 'Juste, A', 'Martínez, M', 'Merino, G', 'Miquel, R', 'Mir, L M', 'Morawitz, P', 'Park, I C', 'Pascual, A', 'Perlas, J A', 'Riu, I', 'Sánchez, F', 'Colaleo, A', 'Creanza, D', 'De Palma, M', 'Gelao, G', 'Iaselli, Giuseppe', 'Maggi, G', 'Maggi, M', 'Marinelli, N', 'Nuzzo, S', 'Ranieri, A', 'Raso, G', 'Ruggieri, F', 'Selvaggi, G', 'Silvestris, L', 'Tempesta, P', 'Tricomi, A', 'Zito, G', 'Huang, X', 'Lin, J', 'Ouyang, Q', 'Wang, T', 'Xie, Y', 'Xu, R', 'Xue, S', 'Zhang, J', 'Zhang, L', 'Zhao, W', 'Abbaneo, D', 'Alemany, R', 'Becker, U', 'Bright-Thomas, P G', 'Casper, David William', 'Cattaneo, M', 'Cerutti, F', 'Ciulli, V', 'Dissertori, G', 'Drevermann, H', 'Forty, Roger W', 'Frank, M', 'Gianotti, F', 'Hagelberg, R', 'Hansen, J B', 'Harvey, J', 'Janot, P', 'Jost, B', 'Lehraus, Ivan', 'Mato, P', 'Minten, A', 'Moneta, L', 'Pacheco, A', 'Pusztaszeri, J F', 'Ranjard, F', 'Rolandi, Luigi', 'Rousseau, D', 'Schlatter, D', 'Schmitt, M', 'Schneider, O', 'Tejessy, W', 'Teubert, F', 'Tomalin, I R', 'Vreeswijk, M', 'Wachsmuth, Horst Werner', 'Wagner, A', 'Ajaltouni, Ziad J', 'Badaud, F', 'Chazelle, G', 'Deschamps, O', 'Falvard, A', 'Ferdi, C', 'Gay, P', 'Guicheney, C', 'Henrard, P', 'Jousset, J', 'Michel, B', 'Monteil, S', 'Montret, J C', 'Pallin, D', 'Perret, P', 'Podlyski, F', 'Proriol, J', 'Rosnet, P', 'Fearnley, Tom', 'Hansen, J D', 'Hansen, J R', 'Hansen, P H', 'Nilsson, B S', 'Rensch, B', 'Wäänänen, A', 'Daskalakis, G', 'Kyriakis, A', 'Markou, C', 'Simopoulou, Errietta', 'Vayaki, Anna', 'Blondel, Alain', 'Brient, J C', 'Machefert, F P', 'Rougé, A', 'Rumpf, M', 'Valassi, A', 'Videau, H L', 'Boccali, T', 'Focardi, E', 'Parrini, G', 'Zachariadou, K', 'Cavanaugh, R J', 'Corden, M', 'Georgiopoulos, C H', 'Hühn, T', 'Jaffe, D E', 'Antonelli, A', 'Bencivenni, G', 'Bologna, G', 'Bossi, F', 'Campana, P', 'Capon, G', 'Chiarella, V', 'Felici, G', 'Laurelli, P', 'Mannocchi, G', 'Murtas, F', 'Murtas, G P', 'Passalacqua, L', 'Pepé-Altarelli, M', 'Curtis, L', 'Dorris, S J', 'Halley, A W', 'Lynch, J G', 'Negus, P', ""O'Shea, V"", 'Raine, C', 'Scarr, J M', 'Smith, K', 'Teixeira-Dias, P', 'Thompson, A S', 'Thomson, E', 'Thomson, F', 'Buchmüller, O L', 'Dhamotharan, S', 'Geweniger, C', 'Graefe, G', 'Hanke, P', 'Hansper, G', 'Hepp, V', 'Kluge, E E', 'Putzer, A', 'Sommer, J', 'Tittel, K', 'Werner, S', 'Wunsch, M', 'Beuselinck, R', 'Binnie, David M', 'Cameron, W', 'Dornan, Peter J', 'Girone, M', 'Goodsir, S M', 'Martin, E B', 'Moutoussi, A', 'Nash, J', 'Sedgbeer, J K', 'Spagnolo, P', 'Williams, M D', 'Ghete, V M', 'Girtler, P', 'Kneringer, E', 'Kuhn, D', 'Rudolph, G', 'Betteridge, A P', 'Bowdery, C K', 'Buck, P G', 'Colrain, P', 'Crawford, G', 'Finch, A J', 'Foster, F', 'Hughes, G', 'Jones, R W L', 'Whelan, E P', 'Williams, M I', 'Giehl, I', 'Hoffmann, C', 'Jakobs, K', 'Kleinknecht, K', 'Quast, G', 'Renk, B', 'Rohne, E', 'Sander, H G', 'Van Gemmeren, P', 'Zeitnitz, C', 'Aubert, Jean-Jacques', 'Benchouk, C', 'Bonissent, A', 'Bujosa, G', 'Carr, J', 'Coyle, P', 'Diaconu, C A', 'Ealet, A', 'Fouchez, D', 'Leroy, O', 'Motsch, F', 'Payre, P', 'Talby, M', 'Sadouki, A', 'Thulasidas, M', 'Tilquin, A', 'Trabelsi, K', 'Aleppo, M', 'Antonelli, M', 'Ragusa, F', 'Berlich, R', 'Blum, Walter', 'Büscher, V', 'Dietl, H', 'Ganis, G', 'Gotzhein, C', 'Kroha, H', 'Lütjens, G', 'Lutz, G', 'Mannert, C', 'Männer, W', 'Moser, H G', 'Richter, R H', 'Rosado-Schlosser, A', 'Schael, S', 'Settles, Ronald', 'Seywerd, H C J', 'Stenzel, H', 'Wiedenmann, W', 'Wolf, G', 'Boucrot, J', 'Callot, O', 'Chen, S', 'Davier, M', 'Duflot, L', 'Grivaz, J F', 'Heusse, P', 'Höcker, A', 'Jacholkowska, A', 'Kado, M', 'Kim, D W', 'Le Diberder, F', 'Lefrançois, J', 'Lutz, A M', 'Schune, M H', 'Serin, L', 'Tournefier, E', 'Veillet, J J', 'Videau, I', 'Zerwas, D', 'Azzurri, P', 'Bagliesi, G', 'Bettarini, S', 'Bozzi, C', 'Calderini, G', ""Dell'Orso, R"", 'Fantechi, R', 'Ferrante, I', 'Giassi, A', 'Gregorio, A', 'Ligabue, F', 'Lusiani, A', 'Marrocchesi, P S', 'Messineo, A', 'Palla, Fabrizio', 'Rizzo, G', 'Sanguinetti, G', 'Sciabà, A', 'Sguazzoni, G', 'Steinberger, Jack', 'Tenchini, Roberto', 'Vannini, C', 'Venturi, A', 'Verdini, P G', 'Blair, G A', 'Bryant, L M', 'Chambers, J T', 'Coles, J', 'Green, M G', 'Medcalf, T', 'Perrodo, P', 'Strong, J A', 'Von Wimmersperg-Töller, J H', 'Botterill, D R', 'Clifft, R W', 'Edgecock, T R', 'Haywood, S', 'Maley, P', 'Norton, P R', 'Thompson, J C', 'Wright, A E', 'Bloch-Devaux, B', 'Colas, P', 'Fabbro, B', 'Faïf, G', 'Lançon, E', 'Lemaire, M C', 'Locci, E', 'Pérez, P', 'Przysiezniak, H', 'Rander, J', 'Renardy, J F', 'Rosowsky, A', 'Roussarie, A', 'Trabelsi, A', 'Vallage, B', 'Black, S N', 'Dann, J H', 'Kim, H Y', 'Konstantinidis, N P', 'Litke, A M', 'McNeil, M A', 'Taylor, G', 'Booth, C N', 'Brew, C A J', 'Cartwright, S L', 'Combley, F', 'Kelly, M S', 'Lehto, M H', 'Reeve, J', 'Thompson, L F', 'Affholderbach, K', 'Böhrer, A', 'Brandt, S', 'Cowan, G D', 'Foss, J', 'Grupen, Claus', 'Smolik, L', 'Stephan, F', 'Apollonio, M', 'Bosisio, L', 'Della Marina, R', 'Giannini, G', 'Gobbo, B', 'Musolino, G', 'Pütz, J', 'Rothberg, J E', 'Wasserbaech, S R', 'Williams, R W', 'Armstrong, S R', 'Charles, E', 'Elmer, P', 'Ferguson, D P S', 'Gao, Y', 'González, S', 'Greening, T C', 'Hayes, O J', 'Hu, H', 'Jin, S', 'McNamara, P A', 'Nachtman, J M', 'Nielsen, J', 'Orejudos, W', 'Pan, Y B', 'Saadi, Y', 'Scott, I J', 'Walsh, J', 'Wu Sau Lan', 'Wu, X', 'Yamartino, J M', 'Zobernig, G']",['Search for supersymmetry with a dominant R-parity violating $LL\\overline{E}$ coupling in $e^+ e^-$ collisions at centre-of-mass energies of 130 GeV to 172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'supersymmetry, search for', 'sparticle, pair production', 'R parity, violation', 'sparticle, decay modes', 'sparticle, mass', 'lower limit', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '130-172 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712013', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-151']","['A search for pair-production of supersymmetric particles under the assumption that R-parity is violated via a dominant LLE coupling has been performed using the data collected by ALEPH at centre-of-mass energies of 130-172 GeV. The observed candidate events in the data are in agreement with the Standard Model expectation. This is translated into lower limits on the mass of charginos, neutralinos, sleptons, sneutrinos and squarks. For instance, charginos with masses less than 73 GeV and neutralinos with masses less than 23 GeV are excluded at 95% confidence level for any generation structure of the LLE coupling, and for neutralino, slepton or sneutrino LSPs.']",['1997-12-15']
1960,['eng'],"['Nisius, R']",['The photon structure function measurements from LEP'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'photon, structure function', 'muon, pair production', 'quark, pair production', 'momentum transfer, dependence', 'x-dependence', 'experimental results', 'CERN LEP Stor', '((3)) ((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712012'],['The present knowledge of the structure of the photon based on measurements of photon structure functions is discussed. This review covers QED structure functions and the hadronic structure function F_2^gamma.'],['1997-12-15']
1961,['eng'],"['Bugg, D V', 'Sarantsev, A V']",['Comment on the review paper of Amsler'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'meson, hadron spectroscopy', 'scalar meson', 'glueball, scalar', 'tensor meson', 'interpretation of experiments, CERN LEAR']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712007'],['We present a dissenting view of some aspects of the work of the Crystal Barrel collaboration.'],['1997-12-08']
1962,['eng'],"['Eichler, R']",['Soft and Diffractive Phenomena'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'positron p, colliding beams', 'anti-p p, colliding beams', 'photon p, interaction', 'photon photon, interaction', 'diffraction', 'hard scattering', 'charged particle, multiplicity', 'jet, electroproduction', 'jet, hadroproduction', 'quark, jet', 'gluon, jet', 'quark, fragmentation', 'spin, effect', 'effect, leading particle', 'cross section, energy dependence', 'structure function', 'experimental results', 'DESY HERA Stor', 'Batavia TEVATRON Coll', '((6)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712011'],['Recent results on hard diffraction at HERA and the Tevatron are presented. Charged particle multiplicities in diffraction and differences in multiplicity in quark and gluon jets measured at LEP are discussed. Spin effects in the fragmentation of leading quarks show some interesting features.'],['1997-12-15']
1963,['eng'],"['Bliss, D W']",['New Limits for Neutrinoless $\\tau$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, rare decay', 'tau, semileptonic decay', 'tau, leptonic decay', 'final state, (0neutrino)', 'tau, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712010'],['Neutrinoless 3-prong tau lepton decays into a charged lepton and either two charged particles or one neutral meson have been searched for using 4.79 fb^{-1} of data collected with the CLEO II detector at CESR. This analysis represents an update of a previous study and the addition of six decay channels. In all channels the numbers of events found are compatible with background estimates and branching fraction upper limits are set for 28 different decay modes. These limits are either more stringent than those set previously or represent the first attempt to find these decays.'],['1997-12-09']
1964,['eng'],"['Alde, D', 'Binon, Freddy G', 'Boutemeur, M', 'Bricman, C', 'Donskov, S V', 'Gouanère, M', 'Inyakin, A V', 'Inaba, S', 'Kachanov, V A', 'Khaustov, G V', 'Knapp, E A', 'Kondashov, A A', 'Lednev, A A', 'Lishin, V A', 'Peigneux, J P', 'Poulet, M', 'Prokoshkin, Yu', 'Sadovsky, S A', 'Samoylenko, V D', 'Shagin, P M', 'Singovsky, A V', 'Sobol, A E', 'Stroot, J P', 'Sugonyaev, V P', 'Takamatsu, K', 'Tsuru, T']",['Study of the $\\eta\\pi^0$ system in the mass range up to 1200 MeV'],['Particle Physics - Experimental Results'],"['talk, Upton 1997/08/25', 'pi- p, exclusive reaction', 'pi0, hadroproduction', 'eta, hadroproduction', 'mass spectrum, (eta pi0)', 'partial wave analysis', 'momentum transfer, spectra', 'a0(980), mass', 'a0(980), width', 'vector meson, exchange', 'spectrometer, GAMS', 'experimental results', 'Serpukhov PS', 'pi- p --> n eta pi0', 'pi- p --> a0(980) n', '38 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712009'],['The reaction $\\pi^-p \\to \\eta\\pi^o n$ has been studied with GAMS-2000 spectrometer in the secondary 38 GeV/c $\\pi^-$-beam of the IHEP U-70 accelerator. Partial wave analysis of the reaction has been performed in the peak in S-wave. The $t$-dependence of $a_0(980)$ production cross section has been studied. Dominant production of the $a_0(980)$ at a small transfer momentum $t$ confirms the hypothesis of Achasov and Shestakov about significant contribution of the $\\rho_2$ exchange ($I^GJ^{PC}=1^+2^{--}$) in the mechanism of $a_0(980)$ meson production in $t$-channel of the reaction.'],['1997-12-09']
1965,['eng'],"['Bonvicini, G']",['Study of semileptonic decays of B mesons to charmed baryons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'B, hadronic decay', 'Lambda/c+, production', 'anti-p, associated production', 'electron, energy', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B- --> Lambda/c+ anti-p electron antineutrino/e', 'anti-B --> Lambda/c+ anti-p anything', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712008'],"['Using data collected by the CLEO II detector at the center-of-mass energy on or near the Upsilon(4S) resonance, we have determined the 90% confidence level upper limit B(Bbar --> Lambda_c^+ e- X)/B(Bbar --> Lambda_c^+ X, Lambdabar_c^- X) < 0.05 for electrons with momentum above 0.6 GeV/c. We have also derived the ratio B(B^- --> Lambda_c^+ pbar e- nubar_e)/B(Bbar --> Lambda_c^+ pbar X) < 0.04 at the 90% confidence level and measured the ratio B(Bbar --> Lambda_c^+ pbar X)/B(Bbar --> Lambda_c^+ X, Lambdabar_c^- X) = 0.57 +- 0.05 +- 0.05.']",['1997-12-08']
1966,['eng'],"['Maggiora, A']",['The DISTO Data Acquisition System at SATURNE'],['Detectors and Experimental Techniques'],"['talk, Albuquerque 1997/11/09', 'p p, interaction', 'p, polarized beam', 'magnetic spectrometer', 'scintillation counter, fibre', 'proportional chamber, wire', 'data acquisition', 'signal processing', 'microprocessor, multiprocessor', 'programming', 'data management', 'Saclay PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712006'],"['The DISTO collaboration has built a large-acceptance magnetic spectrometer designed to provide broad kinematic coverage of multi-particle final states produced in $pp$ scattering. The spectrometer has been installed in the polarized proton beam of the Saturne accelerator in Saclay to study polarization observables in the $\\vec{p} p \\to p K^{+} \\vec{Y}$ ($Y = \\Lambda, and $\\rho$) in $pp$ collisions. The data acquisition system is based on a VME 68030 CPU running the OS/9 operating system, housed in a single VME crate together with the CAMAC interface, the triple port ECL memories, and four RISC R3000 CPU. The digitization of signals from the detectors is made by PCOS III and FERA front-end electronics. Data of several events belonging to a single Saturne extraction are stored in VME triple-port ECL memories using a hardwired fast sequencer. The buffer, optionally filtered by the RISC R3000 CPU, is recorded on a DLT cassette by DAQ CPU using the on-board SCSI interface during the acceleration cycle. Two UNIX workstations are connected to the VME CPUs through a fast parallel bus and the Local Area Network. They analyze a subset of events for on-line monitoring. The data acquisition system is able to read and record 3500 ev/burst in the present configuration with a dead time of 15%.']",['1997-12-08']
1967,['eng'],"['Maggiora, A']",['The DISTO First Level Trigger at SATURNE'],['Detectors and Experimental Techniques'],"['talk, Albuquerque 1997/11/09', 'p p, interaction', 'p, polarized beam', 'magnetic spectrometer', 'scintillation counter, fibre', 'scintillation counter, hodoscope', 'proportional chamber, wire', 'trigger', 'signal processing', 'programming', 'Saclay PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712005'],"['The DISTO collaboration has built a large-acceptance magnetic spectrometer designed to provide broad kinematic coverage of multi-particle final states produced in $pp$ scattering. The spectrometer has been installed in the polarized proton beam of the Saturne accelerator in Saclay to study polarization observables in the $\\vec{p} p \\to p K^{+} \\vec{Y}$ ($Y = \\Lambda, and $\\rho$) in $pp$ collisions. The common signature of such events is the multiplicity of four charged particles in the final state. A flexible 1st level trigger which uses topological information from fast detectors (scintillating fibers and hodoscope) has been built. It is completely software programmable through a menu-driven user interface and allows switching between production and monitor triggers on successive beam spills.']",['1997-12-08']
1968,['eng'],"['Kittel, E Wolfram', 'Chekanov, S V', 'Mangeol, D J', 'Metzger, W J']","['Multiplicities, fluctuations and QCD']",['Particle Physics - Experimental Results'],"['talk, Frascati 1997/09/08', 'electron positron, annihilation', 'Z0, electroproduction', 'hadron, multiple production', 'charged particle, multiplicity', 'multiplicity, moment', 'multiplicity, fluctuation', 'quantum chromodynamics, perturbation theory', 'correlation, higher-order', 'jet, multiplicity', 'numerical calculations, Monte Carlo', 'interpretation of experiments, L3', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712003'],"['Multiplicity fluctuations are studied both globaly (in terms of high-order moments) and locally (in terms of small phase-space intervals). The ratio of cumulant factorial to factorial moments of the charged-particle multiplicity distribution shows a quasi-oscillatory behaviour similar to that predicted by the NNLLA of perturbative QCD. However, an analysis of the sub-jet multiplicity distribution at perturbative scales shows that these oscillations cannot be related to the NNLLA prediction. We investigate how it is possible to reproduce the oscillations within the framework of Monte-Carlo models. Furthermore, local multiplicity fluctuations in angular phase-space intervals are compared with Monte-Carlo models and with first-order QCD predictions. While JETSET reproduces the experimental data very well, the predictions of the Double Leading Log Approximations and estimates obtained in Modified Leading Log Approximations deviate significantly from the data.']",['1997-12-04']
1969,['eng'],"['Chekanov, S V', 'Kittel, E Wolfram', 'Metzger, W J']",['Local properties of local multiplicity distributions in hadronic Z decay'],['Particle Physics - Experimental Results'],"['talk, Frascati 1997/09/08', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'hadron, multiple production', 'multiplicity, spectra', 'parametrization', 'multiplicity, fluctuation', 'event shape analysis', 'momentum, difference', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', '91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712002'],"['Preliminary results on local multiplicity fluctuations in hadronic Z decays are presented. The data were obtained using the L3 detector at LEP. It is investigated to what extent Monte-Carlo models, which are tuned to reproduce global event-shape variables and single-particle inclusive distributions, can describe the local fluctuations measured by means of bunching parameters.']",['1997-12-03']
1970,['eng'],"['Schwiening, J']","['DIRC, the Internally Reflecting Ring Imaging Cherenkov Detector for BaBar']",['Detectors and Experimental Techniques'],"['talk, Albuquerque 1997/11/09', 'particle identification, (K pi)', 'Cherenkov counter, ring imaging', 'optics, reflection', 'glass', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712001'],"['The DIRC is a new type of Cherenkov imaging device that will be used for the first time in the BaBar detector at the asymmetric B-factory, PEP-II. It is based on total internal reflection and uses long, rectangular bars made from synthetic fused silica as Cherenkov radiator and light guide. The principles of the DIRC ring imaging Cherenkov technique are explained and results from the prototype program are presented. Its choice for the BaBar detector particle identification system is motivated, followed by a discussion of the quartz radiator properties and the detector design.']",['1997-12-02']
1971,['eng'],"['Glasman, C']",['Jet Production at HERA'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'positron p, colliding beams', 'exchange, one-photon', 'photon p, interaction', 'jet, photoproduction', 'photon, structure function', 'momentum spectrum, parton', 'differential cross section, transverse energy', 'rapidity dependence', 'mass, (2jet)', 'angular dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711025'],['Studies on the structure of the photon are presented by means of the extraction of a leading order effective parton distribution in the photon and measurements of inclusive jet differential cross sections in photoproduction. Measurements of the internal structure of jets have been performed and are also presented as a function of the transverse energy and pseudorapidity of the jets. Dijet cross sections have been measured as a function of the dijet mass and centre-of-mass scattering angle.'],['2000-09-06']
1972,['eng'],"['Appelshäuser, H', 'Bächler, J', 'Bailey, S J', 'Barnby, L S', 'Bartke, J', 'Barton, R A', 'Bialkowska, H', 'Billmeier, A', 'Blyth, C O', 'Bock, R', 'Bormann, C', 'Brady, F P', 'Brockmann, R', 'Brun, R', 'Buncic, P', 'Caines, H L', 'Cebra, D', 'Cooper, G E', 'Cramer, J G', 'Csató, P', 'Dunn, J', 'Eckardt, V', 'Eckhardt, F', 'Ferguson, M I', 'Ferenc, D', 'Fischer, H G', 'Flierl, D', 'Fodor, Zoltán', 'Foka, P Y', 'Freund, P', 'Friese, V', 'Fuchs, M', 'Gabler, F', 'Gál, J', 'Gazdzicki, M', 'Gladysz-Dziadus, E', 'Grebieszkow, J', 'Günther, J', 'Harris, J W', 'Hegyi, S', 'Henkel, T', 'Hill, L A', 'Huang, I', 'Hümmler, H', 'Igo, G', 'Irmscher, D', 'Jacobs, P', 'Jones, P G', 'Kadija, K', 'Kolesnikov, V I', 'Kowalski, M', 'Lasiuk, B', 'Lévai, P', 'Malakhov, A I', 'Margetis, S', 'Markert, C', 'Melkumov, G L', 'Mock, A', 'Molnár, J', 'Nelson, J M', 'Oldenburg, M D', 'Odyniec, G J', 'Pálla, G', 'Panagiotou, A D', 'Petridis, A', 'Piper, A', 'Porter, R J', 'Poskanzer, A M', 'Poziombka, S', 'Prindle, D J', 'Pühlhofer, F', 'Rauch, W', 'Reid, J G', 'Renfordt, R E', 'Retyk, W', 'Ritter, H G', 'Röhrich, D', 'Roland, C', 'Roland, G', 'Rudolph, H', 'Rybicki, A', 'Sandoval, A', 'Sann, H', 'Semenov, A Yu', 'Schäfer, E', 'Schmischke, D', 'Schmitz, N', 'Schönfelder, S', 'Seyboth, P', 'Seyerlein, J', 'Sikler, F', 'Skrzypczak, E', 'Squier, G T A', 'Stock, Reinhard', 'Ströbele, H', 'Struck, C', 'Szentpétery, I', 'Sziklai, J', 'Toy, M', 'Trainor, T A', 'Trentalange, S', 'Ullrich, T S', 'Vassiliou, M', 'Vesztergombi, György', 'Vranic, D', 'Wang, F', 'Weerasundara, D D', 'Wenig, S', 'Whitten, C', 'Wienold, T', 'Wood, L', 'Yates, T A', 'Xu, N', 'Zimányi, J', 'Zhu, X Z', 'Zybert, R']",['Hadronic Expansion Dynamics in Central Pb+Pb Collisions at 158 GeV per Nucleon'],['Particle Physics - Experimental Results'],"['nucleus nucleus, nuclear reaction', 'scattering, heavy ion', 'lead', 'hadron, multiple production', 'deuteron, hadroproduction', 'correlation function, (2negative particle)', 'correlation function, (pi+ pi-)', 'mass spectrum, transverse', 'boson, statistics', 'correction, Coulomb', 'nuclear reaction, space-time', 'hadron, particle source', 'temperature', 'velocity', 'magnetic spectrometer, experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711024'],"['Two-particle correlation functions of negative hadrons over wide phase space, and transverse mass spectra of negative hadrons and deuterons near mid-rapidity have been measured in central Pb+Pb collisions at 158 GeV per nucleon by the NA49 experiment at the CERN SPS. A novel Coulomb correction procedure for the negative two-particle correlations is employed making use of the measured oppositely charged particle correlation. Within an expanding source scenario these results are used to extract the dynamic characteristics of the hadronic source, resolving the ambiguities between the temperature and transverse expansion velocity of the source, that are unavoidable when single and two particle spectra are analysed separately. The source shape, the total duration of the source expansion, the duration of particle emission, the freeze-out temperature and the longitudinal and transverse expansion velocities are deduced.']",['2000-09-06']
1973,['eng'],"['Achasov, M N', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Dimova, T V', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Koop, I A', 'Korol, A A', 'Koshuba, S V', 'Pakhtusova, E V', 'Salnikov, A A', 'Serednyakov, S I', 'Shary, V V', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V']",['Evidence of $\\phi \\to \\pi^0 \\pi^0 \\gamma$ and $\\phi \\to \\pi^0 \\eta \\gamma$ decays in SND experiment at VEPP-2M'],['Particle Physics - Experimental Results'],"['talk, Upton 1997/08/25', 'electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'Phi(1020), branching ratio', 'mass spectrum, (2pi0)', 'mass spectrum, (eta pi0)', 'four-pi-detector, SND', 'experimental results', 'Novosibirsk Stor2', 'electron positron --> Phi(1020)', 'Phi(1020) --> 2pi0 photon', 'Phi(1020) --> eta pi0 photon', '10.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711023'],"['Preliminary results on the study of e+e- --> phi(1020) --> pi0 pi0 gamma, eta pi0 gamma processes from SND experiment at VEPP-2M collider in Novosibirsk are presented. Branching ratios of rare radiative phi --> pi0 pi0 gamma and phi --> pi0 eta gamma decays are measured: B(phi --> pi0 pi0 gamma ) = (1.1 +- 0.2) * 10^-4 (invariant mass (pi0 pi0) < 800 MeV), B(phi --> eta pi0 gamma ) = (1.3 +- 0.5) * 10^-4.']",['1997-12-01']
1974,['eng'],"['Nystrand, J', 'Klein, S']",['Two-Photon Physics at RHIC'],['Particle Physics - Experimental Results'],"['talk, Upton 1997/08/25', 'scattering, heavy ion', 'exchange, two-photon', 'photon photon, interaction', 'muon, pair production', 'meson, photoproduction', 'meson, pair production', 'meson, hadronic decay', 'numerical calculations, Monte Carlo', 'magnetic detector, STAR', 'proposed experiment, Brookhaven RHIC Coll', '200 GeV-cms/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711021'],"['This presentation will show the feasibility of studying two-photon interactions in the STAR experiment at RHIC. Signals, detection efficiencies, backgrounds, triggering and analysis techniques will be discussed.']",['1997-11-27']
1975,['eng'],"['Drell, P']",['Heavy Quark Decays'],['Particle Physics - Experimental Results'],"['review, Hamburg 1997/07/28', 'quark, heavy', 'quark, decay modes', 'B, semileptonic decay', 'B, hadronic decay', 'B, radiative decay', 'Kobayashi-Maskawa angle', 'final state, (0charmed particle)', 'B, branching ratio', 'HQET model', 'tree approximation', 'D, semileptonic decay', 'D, hadronic decay', 'D, branching ratio', 'neutral current, flavor changing', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711020'],"['Recent results in the decays of the heavy quarks, bottom and charm, are reviewed.']",['1997-11-27']
1976,['eng'],"['Ward, J J']",['The Hadronic Final States in Deep Inelastic $e\\gamma$ Scattering at a Future $e^{+}e^-$ Linear Collider'],['Particle Physics - Experimental Results'],"['electron positron, linear collider', 'photon electron, deep inelastic scattering', 'photon photon, interaction', 'hadron, photoproduction', 'photon, structure function', 'energy flow, rapidity dependence', 'numerical calculations, Monte Carlo', '91.2, 350.0 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711019'],"['Energy flow distributions from tagged $\\gamma\\gamma$ events generated with HERWIG are presented for $E_{beam} = 45.6$ GeV (LEP1) and $E_{beam} = 175$ GeV (top-quark threshold at a future e^+e^- Linear Collider). They have very similar shapes regardless of the beam energy. Using the present knowledge of the LEP $F_2^{\\gamma}$ analyses, it is forseen that the understanding of the hadronic response of the forward region of the LC detector is vital to the development of the final state models in $\\gamma\\gamma$ Monte Carlos. Such models are relied upon to extract $F_2^{\\gamma}$ from the data, and hence understanding the forward region well may be crucial in the determination of whether or not a low-$x$ rise exists in the photon structure function.']",['1997-11-27']
1977,['eng'],"['Breitweg, J']",['Charged particles and neutral kaons in photoproduced jets at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'jet, photoproduction', 'K0, associated production', 'charged particle, associated production', 'fragmentation function', 'K0(S), hadronic decay', 'mass spectrum, (pi+ pi-)', 'transverse momentum, spectra', 'rapidity spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711018'],"['Charged particles ($h^\\pm$) and \\kz mesons have been studied in photoproduced events containing at least one jet of $E_T > 8$ GeV in a pseudorapidity interval (--0.5, 0.5) in the ZEUS laboratory frame. Distributions are presented in terms of transverse momentum, pseudorapidity and distance of the particle from the axis of a jet. The properties of \\hpm within the jet are described well using the standard settings of PYTHIA, but the use of the multiparton interaction option improves the description outside the jets. A reasonable overall description of the \\kz behaviour is possible with PYTHIA using a reduced value of the strangeness suppression parameter. The numbers of $h^\\pm$ and \\kz within a jet as defined above are measured to be $3.25\\pm0.02\\pm0.28$ and $0.431\\pm0.013\\pm0.088$ respectively. Fragmentation functions are presented for $h^\\pm$ and \\kz in photoproduced jets; agreement is found with calculations of Binnewies et al. and, at higher momenta, with $p\\bar p$ scattering and with standard PYTHIA. Fragmentation functions in direct photoproduced events are extracted, and at higher momenta give good agreement with data from related processes in $e^+e^-$ annihilation and deep inelastic $ep$ scattering.']",['1997-11-26']
1978,['eng'],"['Apanasevich, L']",['Evidence for Parton $K_T$ Effects in High -$p_T$ Particle Production'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'pi- nucleus, inclusive reaction', 'beryllium', 'pi0, hadroproduction', 'photon, direct production', 'quantum chromodynamics, perturbation theory', 'transverse momentum, high', 'transverse momentum, parton', 'transverse momentum, spectra', 'angular distribution', 'experimental results', 'Batavia TEVATRON PS', 'hadron beryllium --> pi0 anything', 'hadron beryllium --> photon anything', '515 GeV/c (pi-), 530, 800 GeV/c (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711017'],['Inclusive pizero and direct-photon cross sections in the kinematic range 3.5 < pT < 12 GeV/c with central rapidities are presented for 530 and 800 GeV/c proton beams and a 515 GeV/c pi- beam incident on beryllium targets. Current Next-to-Leading-Order perturbative QCD calculations fail to adequately describe the data for conventional choices of scales. Kinematic distributions from these hard scattering events provide evidence that the interacting partons carry significant initial-state parton transverse momentum (kT). Incorporating these kT effects phenomenologically greatly improves the agreement between calculations and the measured cross sections.'],['1997-11-25']
1979,['eng'],"['Chumney, P']",['Results on $\\Lambda^0$ Production at HERMES'],['Particle Physics - Experimental Results'],"['talk, Zeuthen 1997/09/01', 'positron nucleon, deep inelastic scattering', 'hyperon, electroproduction', 'hyperon, hadronic decay', 'Lambda, polarization', 'mass spectrum, (p pi)', 'nucleon, polarized target', 'polarization, transverse', 'semiconductor detector, proposed', 'magnetic detector, HERMES', 'experimental results', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711016'],"[""The production of Lambda^0's at the HERMES experiment is presented. Prospects for the future of Lambda measurements at HERMES are discussed.""]",['1997-11-24']
1980,['eng'],"['Fanourakis, G K', 'Fassouliotis, D', 'Tzamarias, S']",['Accurate Estimation of the Trilinear Gauge Couplings Using Optimal Observables Including Detector Effects'],['Detectors and Experimental Techniques'],"['electron positron, annihilation', 'final state, (4fermion)', 'coupling, (3gauge boson)', 'W, pair production', 'W, hadronic decay', 'W, leptonic decay', 'data analysis method', 'counters and detectors, effect', 'statistical analysis', 'numerical calculations, Monte Carlo', 'electron positron --> quark antiquark lepton neutrino', '172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711015'],"['This paper describes the definition of maximum likelihood equivalent estimators of the Trilinear Gauge Couplings which include detector effects. The asymptotic properties of these estimators as well as their unbiasedness and efficiency when dealing with finite statistical samples are demonstrated by Monte Carlo experimentation, using simulated events corresponding to the production of q qbar lepton neutrino in e+ e- collisions at 172 GeV. Emphasis is given to the determination of the expected efficiencies in extracting the aWphi, aW and aBphi couplings from LEPII data, which in this particular case found to be close to the maximum possible.']",['1997-11-21']
1981,['eng'],"['Fanourakis, G K', 'Fassouliotis, D', 'Tzamarias, S']",['A Method to include Detector Effects in Estimators sensitive to the Trilinear Gauge Couplings'],['Detectors and Experimental Techniques'],"['data analysis method, proposed', 'counters and detectors, effect', 'electron positron, annihilation', 'final state, (4fermion)', 'coupling, (3gauge boson)', 'cross section', 'angular distribution', 'efficiency', 'statistical analysis', 'coupling, dependence', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711014'],"['This paper describes the use of weighted Monte Carlo events to accurately approximate integrals of functions of the experimentally measured kinematical vectors and their dependence on physical parameters. This technique is demonstrated in estimating the evolution of cross sections, efficiencies, measured kinematical distributions and mean values as functions of the Trilinear Gauge Couplings.']",['1997-11-21']
1982,['eng'],"['Ohshima, T', 'Suito, S', 'Sugiyama, A', 'Suzuki, S', 'Haba, N']",['Examination of T/CP Invariance in the $e ^{+}e^{-} \\to \\tau^{+} \\tau^{-}$ Reaction'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'tau, pair production', 'tau, leptonic decay', 'time reversal, invariance', 'invariance, CP', 'validity test', 'momentum, correlation', 'asymmetry', 'efficiency', 'numerical calculations', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711013'],"['We propose a method to examine the T/CP invariance of the heaviest lepton, tau, by means of a triple-momentum correlation for the reaction e^+e^- -->tau^+tau^-, tau --> e/mu nu nubar during the course of the B-Factory experimental program. An unprecedented high sensitivity could be obtained without requiring a high integrated luminosity.']",['1997-11-21']
1983,['eng'],"['Adloff, C']",['Photo-production of $\\psi(2S)$ Mesons at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inclusive reaction', 'psi(3685), photoproduction', 'psi(3685), leptonic decay', 'psi(3685), hadronic decay', 'J/psi(3100), photoproduction', 'channel cross section, ratio', 'color, dipole', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> psi(3685) positron anything', 'positron p --> J/psi(3100) positron anything', 'psi mesons --> lepton+ lepton-', 'psi(3685) --> J/psi(3100) pi+ pi-', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711012'],"[""Quasi-elastic (z >0.95) photo-production of psi' mesons has been observed at HERA for photon-proton centre-of-mass energies in the range 40 to 160 GeV. The psi' mesons were identified through their decays to l+l- and to J/psi pi+ pi-, where the J/psi subsequently decays to l+l-, the lepton l being either a muon or an electron. The cross-section for quasi-elastic photoproduction was measured to be [18.0 +- 2.8 (stat) +- 3.0(syst)] nb at a photon-proton centre-of-mass energy of 80 GeV. The ratio of the psi' to J/psi quasi-elastic cross-sections is 0.150 +- 0.027 (stat) +- 0.022 (syst).""]",['1997-11-20']
1984,['eng'],"['Bartelt, J']",['Observation of the Radiative Decay $D^{*+}\\to D^{+}\\gamma$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D*(2010), electroproduction', 'D*(2010), radiative decay', 'D*(2010), branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> D*(2010) anything', 'D*(2010) --> D+ photon', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711011'],"['We have observed a signal for the decay D*+ -> D+ gamma at a significance of 4 standard deviations. From the measured branching ratio B(D*+ -> D+ gamma)/B(D*+ -> D+ pi0)=0.055 +- 0.014 +- 0.010 we find B(D*+ -> D+ gamma)= 0.017 +- 0.004 +- 0.003, where the first uncertainty is statistical and the second is systematic. We also report the highest precision measurements of the remaining D*+ branching fractions.']",['1997-11-20']
1985,['eng'],"['Godang, R']",['Observation of exclusive two-body B decays to kaons and pions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'meson, pair production', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> K+ pi-', 'B+ --> K0 pi+', 'B+ --> pi+ pi0', 'B+ --> K+ pi0', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711010'],"['We have studied two-body charmless hadronic decays of B mesons into the final states $\\pi\\pi$, $K \\pi$, and $KK$. Using 3.3 million $B\\bar{B}$ pairs collected with the CLEO-II detector, we have made the first observation of the decays $B^0\\to K^+\\pi^-$, $B^+\\to K^0\\pi^+$, and the sum of $B^+ \\to states is always implied). We place upper limits on branching fractions for the remaining decay modes.']",['1997-11-19']
1986,['eng'],"['Agababian, N M']",['Estimation of hydrodynamical model parameters from the invariant spectrum and the Bose-Einstein correlations of $\\pi$-mesons produced in ($\\pi^{+}/K^{+})p$ interactions at 250 GeV/c'],['Particle Physics - Experimental Results'],"['pi+ p, interaction', 'K+ p, interaction', 'pi-, hadroproduction', 'pi-, multiple production', 'correlation, two-pion', 'boson, statistics', 'model, hydrodynamical', 'pi, particle source', 'rapidity spectrum', 'mass spectrum, transverse', 'magnetic spectrometer, experimental results', 'CERN SPS', '250 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711009'],"['The invariant spectra of pi- mesons produced in (pi+/K+)p interactions at 250 GeV/c are analysed in the framework of the hydrodynamical model of three-dimensionally expanding cylindrically symmetric finite systems. A satisfactory description of experimental data is achieved. The data favour the pattern according to which the hadron matter undergoes predominantly longitudinal expansion and non-relativistic transverse expansion with mean transverse velocity <u_t> = 0.20(7), and is characterized by a large temperature inhomogeneity in the transverse direction: the extracted freeze-out temperature at the center of the tube and at the transverse rms radius are 140(3) MeV and 82(7) MeV, respectively. The width of the (longitudinal) space-time rapidity distribution of the pion source is found to be Delta eta = 1.36(2). Combining this estimate with results of the Bose-Einstein correlation analysis in the same experiment, one extracts a mean freeze-out time of the source of <tau_f> = 1.4(1) fm/c and its transverse geometrical rms radius, R_G (rms)=1.2(2) fm.']",['1997-11-19']
1987,['eng'],"['Buzzo, A', 'Debevec, P T', 'Drijard, Daniel', 'Eisenstein, R A', 'Evangelista, C', 'Eyrich, W', 'Fischer, H', 'Franz, J', 'Geyer, R', 'Hamann, N H', 'Harris, P G', 'Hertzog, D W', 'Hughes, S A', 'Johansson, T', 'Jones, R T', 'Kilian, K', 'Kirsebom, K', 'Korsmo, H', 'Lo Vetere, M', 'Macri, M', 'Marinelli, M', 'Moosburger, M', 'Mouëllic, B', 'Oelert, Walter', 'Ohlsson, S', 'Palano, A', 'Passaggio, S', 'Perreau, J M', 'Pia, M G', 'Pomp, S', 'Price, M', 'Reimer, P E', 'Ritter, J B', 'Robutti, E', 'Röhrich, K', 'Rook, M', 'Rössle, E', 'Santroni, A', 'Schmitt, H', 'Sefzick, T', 'Steinkamp, O', 'Stinzing, F', 'Stugu, B', 'Wirth, H']",['Search for narrow $p\\overline p$ resonances in the reaction $p\\overline p\\top\\overline p \\pi^{+}\\pi^-$'],['Particle Physics - Experimental Results'],"['anti-p p, inelastic scattering', 'pi, pair production', 'mass spectrum, (p anti-p)', 'search for, narrow resonance', 'narrow resonance, (2020)', 'production, upper limit', 'channel cross section, momentum dependence', 'experimental results', 'CERN LEAR']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801015'],"['The reaction pbar p -> pbar p pi+ pi- has been studied with high statistics at CERN-LEAR with incident pbar momenta from 1.65 to 2.0 GeV/c by the JETSET (PS202) experiment. The aim of this paper is to search for narrow resonances decaying to pbar p. No evidence for such structures is found. In particular, an upper limit for the production of a 2.02 GeV state with a width of Gamma = 20 MeV, having been seen in other hadroproduction experiments, is established. Our results restrict the cross section for such a peak to be below 200 nb at the 95% confidence level.']",['1998-01-19']
1988,['eng'],"['Adeva, B', 'Akdogan, T', 'Arik, E', 'Arvidson, A', 'Badelek, B', 'Bardin, G', 'Baum, G', 'Berglund, P', 'Betev, L', 'Birsa, R', 'De Botton, N R', 'Bradamante, Franco', 'Bravar, A', 'Bressan, A', 'Bültmann, S', 'Burtin, E', 'Crabb, D', 'Cranshaw, J', 'Çuhadar-Dönszelmann, T', 'Dalla Torre, S', 'Van Dantzig, R', 'Derro, B R', 'Deshpande, A A', 'Dhawan, S K', 'Dulya, C M', 'Eichblatt, S', 'Fasching, D', 'Feinstein, F', 'Fernández, C', 'Forthmann, S', 'Frois, Bernard', 'Gallas, A', 'Garzón, J A', 'Gilly, H', 'Giorgi, M A', 'von Goeler, E', 'Görtz, S', 'Gracia, G', 'De Groot, N', 'Grosse-Perdekamp, M', 'Haft, K', 'Von Harrach, D', 'Hasegawa, T', 'Hautle, P', 'Hayashi, N', 'Heusch, C A', 'Horikawa, N', 'Hughes, V W', 'Igo, G', 'Ishimoto, S', 'Iwata, S', 'Kabuss, E M', 'Kageya, T', 'Karev, A G', 'Kessler, H J', 'Ketel, T J', 'Kiryluk, J', 'Kiselev, Yu F', 'Krämer, D', 'Krivokhizhin, V G', 'Kröger, W', 'Kukhtin, V V', 'Kurek, K', 'Kyynäräinen, J', 'Lamanna, M', 'Landgraf, U', 'Le Goff, J M', 'Lehar, F', 'de Lesquen, A', 'Lichtenstadt, J', 'Litmaath, M', 'Magnon, A', 'Mallot, G K', 'Marie, F', 'Martin, A', 'Martino, J', 'Matsuda, T', 'Mayes, B', 'McCarthy, J S', 'Medved, K S', 'Meyer, W T', 'Van Middelkoop, G', 'Miller, D', 'Miyachi, Y', 'Mori, K', 'Moromisato, J H', 'Nassalski, J P', 'Naumann, L', 'Niinikoski, T O', 'Oberski, J', 'Ogawa, A', 'Ozben, C', 'Pereira, H', 'Perrot-Kunne, F', 'Peshekhonov, D V', 'Pinsky, L', 'Platchkov, S K', 'Pló, M', 'Pose, D', 'Postma, H', 'Pretz, J', 'Puntaferro, R', 'Rädel, G', 'Rijllart, A', 'Reicherz, G', 'Roberts, J', 'Rodríguez, M', 'Rondio, E', 'Roscherr, B', 'Sabo, I', 'Saborido, J', 'Sandacz, A', 'Savin, I A', 'Schiavon, R P', 'Schiller, A', 'Sichtermann, E P', 'Simeoni, F', 'Smirnov, G I', 'Staude, A', 'Steinmetz, A', 'Stiegler, U', 'Stuhrmann, H B', 'Szleper, M', 'Tessarotto, F', 'Thers, D', 'Tlaczala, W', 'Tripet, A', 'Ünel, G', 'Velasco, M', 'Vogt, J', 'Voss, R', 'Whitten, C', 'Windmolders, R', 'Willumeit, R', 'Wislicki, W', 'Witzmann, A', 'Ylöstalo, J', 'Zanetti, A M', 'Zaremba, K', 'Zhao, J']",['Polarised quark distributions in the nucleon from semi-inclusive spin asymmetries'],['Particle Physics - Experimental Results'],"['muon p, deep inelastic scattering', 'muon deuteron, deep inelastic scattering', 'muon, polarized beam', 'nucleon, polarized target', 'polarization, asymmetry', 'nucleon, structure function', 'structure function, spin', 'structure function, moment', 'quark, momentum spectrum', 'quark, polarization', 'quark, valence', 'quark, sea', 'magnetic spectrometer, experimental results', 'CERN SPS', '190 GeV']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-147', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711008']","['We present a measurement of semi-inclusive spin asymmetries for positively and negatively charged hadrons from deep inelastic scattering of polarised muons on polarised protons and deuterons in the range $0.003<x<0.7$ and $Q^2>$1~GeV$^2$. Compared to our previous publication on this subject, with the new data the statistical errors have been reduced by nearly a factor of two. From these asymmetries and our inclusive spin asymmetries we determine the polarised quark distributions of valence quarks and non-strange sea quarks at $Q^2$=10~GeV$^2$. The polarised $u$ valence quark distribution, $\\Delta u_v(x)$, is positive and the polarisation increases with $x$. The polarised $d$ valence quark distribution, $\\Delta d_v(x)$, is negative and the non-strange sea distribution, $\\Delta \\bar q(x)$, is consistent with zero over the measured range of $x$. We find for the first moments $\\int_0^1 \\Delta u_v(x) {\\rm d}x = 0.77 \\pm 0.10 \\pm 0.08$, $\\int_0^1 \\Delta d_v(x) {\\rm d}x = -0.52 \\pm 0.14 \\pm 0.09$ and $\\int_0^1 \\Delta \\bar q(x) {\\rm d}x= 0.01 \\pm 0.04 \\pm 0.03$, where we assumed $\\Delta \\bar u(x) = \\Delta \\bar d(x)$. We also determine for the first time the second moments of the valence distributions $\\int_0^1 x \\Delta q_v(x) {\\rm d}x$.']",['1997-12-11']
1989,['eng'],"['Akhmetshin, R R']",['Search for rare $\\phi$ decays in $\\pi^{+} \\pi^{-} \\gamma$ final state'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'Phi(1020), radiative decay', 'f0(975)', 'rho(770)', 'eta, hadronic decay', 'parity, violation', 'violation, CP', 'Phi(1020), branching ratio', 'eta, branching ratio', 'upper limit', 'photon, energy spectrum', 'channel cross section, energy dependence', 'magnetic detector, experimental results', 'Novosibirsk Stor2', 'electron positron --> pi+ pi- photon', 'electron positron --> muon+ muon- photon', 'Phi(1020) --> f0(975) photon', 'Phi(1020) --> rho(770) photon', 'Phi(1020) --> muon+ muon- photon', 'approx. 10 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711007'],"['A search for phi radiative decays has been performed using a data sample of about 2.0 million phi decays collected by the CMD-2 detector at VEPP-2M collider in Novosibirsk. From the selected e+ e- -> pi+ pi- gamma events the following results were obtained: B(phi -> f0(980) gamma) < 1x10-4 for destructive and B(phi -> f0(980) gamma) < 7x10-4 for constructive interference with the Bremsstrahlung process respectively, B(phi -> gamma -> pi+ pi- gamma) < 3x10-5 for E of gamma > 20 MeV, B(phi -> rho gamma) < 7x10-4. From the selected e+ e- -> mu+ mu- gamma events B(phi -> mu+ mu- gamma) = (2.3+-1.0)x10-5 has been obtained for E of gamma> 20 MeV. The upper limit on the P,CP-violating decay eta -> pi+ pi- has also been placed: B(eta -> pi+ pi-) < 9x10-4 . All upper limits are at 90 % C.L.']",['1997-11-17']
1990,['eng'],"['Adloff, C']",['Thrust Jet Analysis of Deep-Inelastic Large-Rapidity-Gap Events'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'rapidity, gap', 'photon, dissociation', 'event shape analysis, thrust', 'jet, alignment', 'mass, hadronic', 'transverse momentum, spectra', 'color, exchange', 'photon, resolved', 'vector dominance', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711006'],"['A thrust analysis of Large-Rapidity-Gap events in deep-inelastic ep collisions is presented, using data taken with the H1 detector at HERA in 1994. The average thrust of the final states X, which emerge from the dissociation of virtual photons in the range 10 < Q2 < 100 GeV2, grows with hadronic mass M_X and implies a dominant 2-jet topology. Thrust is found to decrease with growing Pt, the thrust jet momentum transverse to the photon-proton collision axis. Distributions of Pt2 are consistent with being independent of MX. They show a strong alignment of the thrust axis with the photon-proton collision axis, and have a large high-Pt tail. The correlation of thrust with MX is similar to that in e+e- annihilation at sqrt(see)=MX, but with lower values of thrust in the ep data. The data cannot be described by interpreting the dissociated system X as a qqbar state but inclusion of a substantial fraction of qqbarg parton configurations leads naturally to the observed properties. The soft colour exchange interaction model does not describe the data.']",['1997-11-14']
1991,['eng'],"['Söldner-Rembold, S']",['The Structure of the Photon'],['Particle Physics - Experimental Results'],"['review, Hamburg 1997/07/28', 'photon, structure function', 'parametrization', 'electron positron, inelastic scattering', 'photon electron, interaction', 'photon photon, interaction', 'photon p, interaction', 'jet, photoproduction', 'event shape analysis', 'energy flow, hadronic', 'photon, direct production', 'cross section', 'angular correlation', 'momentum spectrum, parton', 'D*(2010), photoproduction', 'D*(2010), hadronic decay', 'quark, charm', 'quark, pair production', 'photon, fragmentation function', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711005'],['The structure of the photon is studied in high energy photon-proton interactions at HERA and photon-photon interactions at LEP. The status of these measurements is reviewed.'],['1997-11-14']
1992,['eng'],"['Aitala, E M']","['Branching Fractions for $D_{0}\\to K^{+}K ^{-}$ and $D_{0}\\to \\pi^{+}\\pi^{-}$, and a Search for CP Violation in $D_0$ Decays']",['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'D*(2010), hadroproduction', 'D0, hadroproduction', 'charmed meson, hadronic decay', 'D0, branching ratio', 'meson, pair production', 'mass spectrum, (2meson)', 'violation, CP', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> charmed meson anything', 'D*(2010) --> D0 pi+', 'D0 --> K- pi+', 'D0 --> K+ K-', 'D0 --> pi+ pi-', '500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711003'],"['Using the large hadroproduced charm sample collected in experiment E791 at Fermilab, we have measured ratios of branching fractions for the two-body singly-Cabibbo-suppressed charged decays of the D0: (D0 -> KK)/(D0 -> Kpi) = 0.109 +- 0.003 +- 0.003, (D0 -> pipi)/(D0 -> Kpi) = 0.040 +- 0.002 +- 0.003, and (D0 -> KK)/(D0 -> pipi) = 2.75 +- 0.15 +- 0.16. We have looked for differences in the decay rates of D0 and D0bar to the CP eigenstates K+K- and pi+pi-, and have measured the CP asymmetry parameters A_CP(K+K-) = -0.010 +- 0.049 +- 0.012 and A_CP(pi+pi-) = -0.049 +- 0.078 +- 0.030, both consistent with zero.']",['1997-11-11']
1993,['eng'],"['Abe, F']",['Observation of Hadronic W Decays in $t-\\overline{t}$ Events with the Collider Detector at Fermilab'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, ((n)jet lepton)', 'W, leptonic decay', 'W, hadronic decay', 'mass spectrum, (2jet)', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711004'],['We observe hadronic W decays in t-tbar -> W (-> l nu) + >= 4 jet events using a 109 pb-1 data sample of p-pbar collisions at sqrt{s} = 1.8 TeV collected with the Collider Detector at Fermilab (CDF). A peak in the dijet invariant mass distribution is obtained that is consistent with W decay and inconsistent with the background prediction by 3.3 standard deviations. From this peak we measure the W mass to be 77.2 +- 4.6 (stat+syst) GeV/c^2. This result demonstrates the presence of two W bosons in t-tbar candidates in the W (-> l nu) + >= 4 jet channel.'],['1997-11-12']
1994,['eng'],"['Ben-David, R']",['Status of the KTeV Experiment at Fermilab'],['Particle Physics - Experimental Results'],"['talk, Capri 1997/06/22', 'K0, rare decay', 'K0, hadronic decay', 'K0(L)', 'K0(S)', 'violation, CP', 'K0, branching ratio', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'K0 --> pi0 lepton+ lepton-', 'K0 --> pi0 neutrino antineutrino', 'K0 --> pi+ pi-', 'K0 --> 2pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801005'],['The KTeV experiment is a fixed target experiment at Fermilab. Its primary goal is the search for direct CP violation in the decay of neutral kaons. Its current status and some preliminary results will be discussed.'],['1998-01-08']
1995,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for the $B_c$ meson in hadronic $Z^0$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'search for, B/c', 'B/c, hadronic decay', 'B/c, semileptonic decay', 'mass, B/c', 'branching ratio, upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'B/c --> J/psi(3100) lepton neutrino', 'B/c --> J/psi(3100) a1(1260)', 'B/c --> J/psi(3100) pi+', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801026', 'http://www.cern.ch/Opal/pubs/paper/index.html']","['A search for decays of the B_c meson was performed using data collected from 1990-1995 with the OPAL detector on or near the Z peak at LEP. The decay channels B_c^+ -> J/psi pi^+, B_c^+ -> J/psi a_1^+ and B_c^+ -> J/psi ell^+ nu were investigated, where ell denotes an electron or a muon. Two candidates are observed in the mode B_c^+ -> J/psi pi^+, with an estimated background of (0.63 +/- 0.20) events. The weighted mean of the masses of the two candidates is (6.32 +/- 0.06) GeV/c^2, which is consistent with the predicted mass of the B_c meson. One candidate event is observed in the mode B_c^+ -> J/psi ell^+ nu with an estimated background of (0.82 +/- 0.19) events. No candidate events are observed in the B_c^+ -> J/psi a_1^+ decay mode, with an estimated background of (1.10 +/- 0.22) events. Upper bounds at the 90% confidence level are set on the production rates for these processes.']",['1997-11-13']
1996,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Ashby, S F', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Betts, S', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Couyoumtzelis, C', 'Coxe, R L', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanfani, A', 'Fanti, M', 'Faust, A A', 'Feld, L', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Höcker, A', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Kanzaki, J I', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Liu, D', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markopoulos, C', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rembser, C', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sang, W M', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Ströhmer, R', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Torrence, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for anomalous production of photonic events with missing energy in $e^+ e^-$ collisions at $\\sqrt{s}$ = 130-172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'photon, electroproduction', 'photon, pair production', 'transverse energy, missing-energy', 'event shape analysis, planarity', 'neutrino, pair production', 'electroweak interaction, validity test', 'new particle, search for', 'neutrino, excited state', 'neutralino', 'channel cross section, branching ratio', 'magnetic detector, OPAL', 'experimental results', 'CERN SPS Coll', '130-172 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801024', 'http://www.cern.ch/Opal/pubs/paper/index.html']","['Photonic events with large missing energy have been observed in e+e- collisions at centre-of-mass energies of 130, 136, 161 and 172 GeV using the OPAL detector at LEP. Results are presented based on search topologies designed to select events with a single photon and missing transverse energy or events with a pair of acoplanar photons. In both search topologies, cross-section measurements are performed within the kinematic acceptance of the selection. These results are compared with the expectations from the Standard Model processes e+e- -> nu nu(bar) gamma (gamma) (single-photon) and e+e- -> \\nu new physics contributions to these final states. Upper limits on sigma(e+e- -> XY)*Br(X -> Y gamma) and sigma(e+e- -> XX)*Br**2(X -> Y gamma) are derived for the case of stable and invisible Y. These limits apply to single and pair production of excited neutrinos (X = \\nu^*, Y = \\nu), to neutralino production (X = \\chi^0_2, Y = \\chi^0_1), and to supersymmetric models in which X = results of the acoplanar-photons search are used to provide model-dependent lower limits on the mass of the lightest neutralino.']",['1997-11-13']
1997,['eng'],"['Apollonio, M']",['Initial Results from the CHOOZ Long Baseline Reactor Neutrino Oscillation Experiment'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'upper limit', 'fission, particle source', 'antineutrino/e, particle identification', 'neutrino, mass difference', 'neutrino, mixing angle', 'scintillation counter, liquid', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711002'],"['Initial results are presented from CHOOZ, a long-baseline reactor-neutrino vacuum-oscillation experiment. Electron antineutrinos were detected by a liquid scintillation calorimeter located at a distance of about 1 km. The detector was constructed in a tunnel protected from cosmic rays by a 300 MWE rock overburden. This massive shielding strongly reduced potentially troublesome backgrounds due to cosmic-ray muons, leading to a background rate of about one event per day, more than an order of magnitude smaller than the observed neutrino signal. From the statistical agreement between detected and expected neutrino event rates, we find (at 90% confidence level) no evidence for neutrino oscillations in the electron antineutrino disappearance mode for the parameter region given approximately by deltam**2 > 0.9 10**(-3) eV**2 for maximum mixing and (sin(2 theta)**2) > 0.18 for large deltam**2.']",['1997-11-06']
1998,['eng'],"['Alber, T']","['Charged Particle Production in Proton-, Deuteron-, Oxygen- and Sulphur-Nucleus Collisions at 200 GeV per Nucleon']",['Particle Physics - Experimental Results'],"['p nucleus, nuclear reaction', 'nucleus nucleus, nuclear reaction', 'deuteron', 'sulfur', 'gold', 'scattering, heavy ion', 'charged particle, multiple production', 'p, multiplicity', 'negative particle, multiplicity', 'transverse momentum, spectra', 'rapidity spectrum', 'dependence, mass number', 'nuclear reaction, temperature', 'experimental results', 'CERN SPS', '200 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711001'],"[""The transverse momentum and rapidity distributions of net protons and negatively charged hadrons have been measured for minimum bias proton-nucleus and deuteron-gold interactions, as well as central oxygen-gold and sulphur-nucleus collisions at 200 GeV per nucleon. The rapidity density of net protons at midrapidity in central nucleus-nucleus collisions increases both with target mass for sulphur projectiles and with the projectile mass for a gold target. The shape of the rapidity distributions of net protons forward of midrapidity for d+Au and central S+Au collisions is similar. The average rapidity loss is larger than 2 units of rapidity for reactions with the gold target. The transverse momentum spectra of net protons for all reactions can be described by a thermal distribution with `temperatures' between 145 +- 11 MeV (p+S interactions) and 244 +- 43 MeV (central S+Au collisions). The multiplicity of negatively charged hadrons increases with the mass of the colliding system. The shape of the transverse momentum spectra of negatively charged hadrons changes from minimum bias p+p and p+S interactions to p+Au and central nucleus-nucleus collisions. The mean transverse momentum is almost constant in the vicinity of midrapidity and shows little variation with the target and projectile masses. The average number of produced negatively charged hadrons per participant baryon increases slightly from p+p, p+A to central S+S,Ag collisions.""]",['1997-11-04']
1999,['eng'],"['Solano, J M', 'Magnin, J', 'Simão, F R A']",['Hyperon production asymmetries in 500 GeV/c pion nucleus interactions'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 1997/08/27', 'pi nucleus, inclusive reaction', 'hyperon, hadroproduction', 'hyperon, hadronic decay', 'yield, (hyperon antihyperon)', 'asymmetry', 'Lambda', 'Xi-', 'Omega-', 'transverse momentum, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710033'],"[""We present a preliminary study from Fermilab experiment E791 of Lambda^0 / Lambda^0 bar, Xi^- / Xi^+ and Omega^- /Omega^+ production asymmetries from pi^- nucleus interactions at 500 Gev/c. The production asymmetries for these particles are studied as a function of x_F and pt^2. We observed an asymmetry in the target fragmentation region for Lambda^0's larger than that for Xi's, suggesting diquark effects. The asymmetry for Omega's is significatively smaller than for the other two hyperons consistent with the fact that Omega's do not share valence quarks with either the pion or the target particle. In the beam fragmentation region, the asymmetry tends to 0.1 for both Lambda^0's and Xi's. The asymmetries vs pt^2 are approximately constant for the three strange baryons under study.""]",['1997-11-03']
2000,['eng'],"['Abbott, B']",['Search for First Generation Scalar Leptoquark Pairs in $p\\overline{p}$ Collisions a $\\sqrt{s}$=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, leptoquark', 'scalar particle, leptoquark', 'leptoquark, pair production', 'decay, leptoquark', 'mass, leptoquark', 'lower limit', 'channel cross section, upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> (n)jet electron neutrino anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710032'],"['We have searched for first generation scalar leptoquark (LQ) pairs in the enu+jets channel using ppbar collider data (integrated luminosity= 115 pb^-1) collected by the DZero experiment at the Fermilab Tevatron during 1992-96. The analysis yields no candidate events. We combine the results with those from the ee+jets and nunu+jets channels to obtain 95% confidence level (CL) upper limits on the LQ pair production cross section as a function of mass and of beta, the branching fraction to a charged lepton. Comparing with the next-to-leading order theory, we set 95% CL lower limits on the LQ mass of 225, 204, and 79 GeV/c^2 for beta=1, 1/2, and 0, respectively.']",['1997-11-03']
2001,['eng'],"['Abbott, B']",['$Z\\gamma$ Production in $p\\bar{p}$ Collisions at $\\sqrt{s}$=1.8 TeV and Limits on Anomalous $ZZ\\gamma$ and $Z\\gamma\\gamma$ Couplings'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Z0, hadroproduction', 'Z0, leptonic decay', 'photon, associated production', 'coupling, (2Z0 photon)', 'coupling, (Z0 2photon)', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710031'],"['We present a study of Z +gamma + X production in p-bar p collisions at sqrt{S}=1.8 TeV from 97 (87) pb^{-1} of data collected in the eegamma (mumugamma) decay channel with the D0 detector at Fermilab. The event yield and kinematic characteristics are consistent with the Standard Model predictions. We obtain limits on anomalous ZZgamma and Zgammagamma couplings for form factor scales Lambda = 500 GeV and Lambda = 750 GeV. Combining this analysis with our previous results yields 95% CL limits |h{Z}_{30}| < 0.36, |h{Z}_{40}| < 0.05, |h{gamma}_{30}| < 0.37, and |h{gamma}_{40}| < 0.05 for a form factor scale Lambda=750 GeV.']",['1997-10-30']
2002,['eng'],"['Bethke, Siegfried']",['QCD Tests at $e^{+}e^{-}$ Colliders'],['Particle Physics - Experimental Results'],"['review, Montpellier 1997/07/03', 'electron positron, colliding beams', 'electron positron, annihilation', 'quantum chromodynamics, validity test', 'jet, electroproduction', 'hadron, multiple production', 'jet, multiplicity', 'Z0, electroproduction', 'Z0, hadronic decay', 'event shape analysis', 'strong interaction, coupling constant', 'experimental results', 'bibliography', '((2)) ((3)) ((4)) ((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710030'],"[""A short review of the history and a 'slide-show' of QCD tests in $e^+e^-$ annihilation is given. The world summary of measurements of $\\alpha_s$ is updated.""]",['1997-10-30']
2003,['eng'],"['De Angelis, A']",['Interconnections effects in multiparticle production from W W events at LEP'],['Particle Physics - Experimental Results'],"['talk, Frascati 1997/09/08', 'electron positron, colliding beams', 'electron positron, annihilation', 'W, pair production', 'W, decay modes', 'final state, (4jet)', 'final state, (2jet lepton neutrino)', 'hadron, multiple production', 'color, interference', 'gluon, exchange', 'correlation, two-pion', 'boson, statistics', 'W, mass', 'event shape analysis', 'charged particle, multiplicity', 'experimental results', 'CERN LEP Stor', '172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9805005'],"['Interactions between the products of the hadronic decays of different Ws in WW pair events can occur at several stages: from the colour rearrangement between the quarks coming from the primary branching, to the gluon exchange during the parton cascade, to the mixing of identical pions due to Bose-Einstein correlations. Besides the intrinsic interest of their study related to the understanding of the multiparticle production mechanisms, these phenomena can affect the ultimate accuracy in the W mass measurement by LEP 2. The status of the experimental analysis on interconnection effects between W pairs hadronically decaying is reviewed in this paper.']",['1997-10-09']
2004,['eng'],"['Brower, W S', 'Paar, H P']",['A new method for selecting exclusive semileptonic charmless B-decays at e+e- colliders at the gamma(4S)'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'final state, (0charmed particle)', 'D*(2010)', 'data analysis method', 'energy, correlation', 'numerical calculations, Monte Carlo', 'magnetic detector, CLEO', 'Cornell CESR Stor', 'B --> pi lepton neutrino', 'anti-B --> D*(2010) lepton- antineutrino', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710029'],"[""We introduce a new method for selecting exclusive semileptonic charmless B-decays in the presence of a large background. The method can be applied to charged and neutral B-mesons decaying into any exclusive neutral or charged hadronic final state. The method is designed for high luminosity $\\eplemi$ colliders operating at the $\\Upsilon(4S)$. It employs an improved partial reconstruction technique for $\\Dstar-mesons$ and a novel 0-C event fit to both B-meson's decay products resulting in the kinematics of all particles (including neutrinos) in the event. The charged lepton energies are accessible from $1.0 \\GeV$ to the kinematic limit.""]",['1997-10-28']
2005,['eng'],"['Coan, T E']",['Flavor-Specific Inclusive B Decays to Charm'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B, semileptonic decay', 'quark, beauty', 'quark, branching ratio', 'angular distribution', 'D, momentum spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D anything', 'B --> anti-D anything', 'B --> anti-D lepton anything', 'beauty --> 2charm strangeness', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710028'],"[""We have measured the branching fractions for B -> D_bar X, B -> D X, and B -> D_bar X \\ell^+ \\nu, where ``B'' is an average over B^0 and B^+, ``D'' is a sum over D^0 and D^+, and``D_bar'' is a sum over D^0_bar and D^-. From these results and some previously measured branching fractions, we obtain Br(b -> c c_bar s) = (21.9 $\\pm$ 3.7)%, Br(b -> s g) < 6.8% @ 90% c.l, and Br(D^0 -> K^- problem'' (measured branching fraction being below theoretical expectations) are discussed. The increase in the value of Br(b -> c c_bar s) due to $B -> D X$ eliminates 40% of the discrepancy.""]",['1997-10-27']
2006,['eng'],"['Breitweg, J']",['Event Shape Analysis of Deep Inelastic Scattering Events with a Large Rapidity Gap at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'rapidity, gap', 'event shape analysis', 'mass, dependence', 'exchange, pomeron', 'diffraction', 'structure function, pomeron', 'gluon, momentum spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710027'],"['A global event shape analysis of the multihadronic final states observed in neutral current deep inelastic scattering events with a large rapidity gap with respect to the proton direction is presented. The analysis is performed in the range $5 \\leq Q^2 \\leq 185\\gev^2$ and $160 \\leq W \\leq 250\\gev$, where $Q^2$ is the virtuality of the photon and $W$ is the virtual-photon proton centre of mass energy. Particular emphasis is placed on the dependence of the shape variables, measured in the $\\gamma^*-$pomeron rest frame, on the mass of the hadronic final state, $M_X$. With increasing $M_X$ the multihadronic final state becomes more collimated and planar. The experimental results are compared with several models which attempt to describe diffractive events. The broadening effects exhibited by the data require in these models a significant gluon component of the pomeron.']",['1997-10-24']
2007,['eng'],"['Patt, J']",['Results from $\\gamma-\\gamma$ Collisions in OPAL'],['Particle Physics - Experimental Results'],"['talk, Upton 1997/08/25', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'jet, photoproduction', 'hadron, multiple production', 'photon, resolved', 'quantum chromodynamics, perturbation theory', 'differential cross section, transverse momentum', 'differential cross section, rapidity dependence', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710025'],['The production of charged hadrons and jets is measured in collisions of quasi-real photons. The data were taken with the OPAL detector at LEP at e+e- centre-of-mass energies of 161 and 172 GeV. The measured cross-sections are compared to perturbative next-to-leading order QCD calculations. The separation of the direct and the resolved component of the photon is demonstrated.'],['1997-10-24']
2008,['eng'],"['Adamovich, M I', 'Alexandrov, Yu A', 'Barberis, D', 'Beck, M', 'Bérat, C', 'Beusch, Werner', 'Boss, M', 'Brons, S', 'Brückner, W', 'Buénerd, M', 'Busch, C', 'Büscher, C', 'Charignon, F', 'Chauvin, J', 'Chudakov, E A', 'Dersch, U', 'Dropmann, F', 'Engelfried, J', 'Faller, F', 'Fournier, A', 'Gerassimov, S G', 'Godbersen, M', 'Grafström, P', 'Haller, T', 'Heidrich, M', 'Hubbard, E', 'Hurst, R B', 'Königsmann, Kay C', 'Konorov, I', 'Keller, N', 'Martens, K', 'Martin, P', 'Masciocchi, S', 'Michaels, R', 'Müller, U', 'Neeb, H', 'Newbold, D', 'Newsom, C R', 'Paul, S', 'Pochodzalla, J', 'Potashnikova, I K', 'Povh, B', 'Ren, Z', 'Rey-Campagnolle, M', 'Rosner, G', 'Rossi, L', 'Rudolph, H', 'Scheel, C V', 'Schmitt, L', 'Siebert, Hans-Wolfgang', 'Simon, A', 'Smith, V J', 'Thilmann, O', 'Trombini, A', 'Vesin, E', 'Volkemer, B', 'Vorwalter, K', 'Walcher, T', 'Wälder, G', 'Werding, R', 'Wittmann, E', 'Zavertyaev, M V']",['First observation of the $\\Xi^{-} \\pi^{+}$ decay mode of the $\\Xi^{0}(1690)$ hyperon'],['Particle Physics - Experimental Results'],"['Sigma nucleus, inclusive reaction', 'carbon', 'copper', 'Xi(1690), hadroproduction', 'Xi(1690), hadronic decay', 'Xi(1690), mass', 'Xi(1690), width', 'channel cross section, branching ratio', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'Sigma- nucleus --> Xi(1690) anything', 'Xi(1690) --> Xi- pi+', '345 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710024'],"['We report the first observation of the Xi- pi+ decay mode of the Xi0(1690), confirming the existence of this resonance. The Xi0(1690) were produced by Sigma- of 345 Gev/c mean momentum in copper and carbon targets. The mass and width are close to those observed earlier for the Xi-(1690) in the Lambda K- decay channel. The product of inclusive production cross section and branching ratio is given relative to that of the Xi0(1530).']",['1997-10-24']
2009,['eng'],"['Bishai, M']",['Search for the decay $B\\to D_{s1}^{+}(2536)X$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'D/s1(2536), decay constant', 'B, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D/s1(2536) anything', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710023'],"['Using data recorded by the CLEO II detector at CESR, we have searched for the decay B -> Ds1+(2536) X, where Ds1+ is the narrow P-wave D_s^+ meson with J^P=1^+. The upper limit to the inclusive branching fraction is measured to be Br(B -> Ds1+ X) < 0.95% at the 90% confidence level. This limit is small compared with the total expected B -> Dbar(*)D(*)KX rate. Assuming factorization, the Ds1+ decay constant is constrained to be f_Ds1 < 114 MeV at the 90% confidence level, which is at least 2.5 times smaller than that of Ds+.']",['1997-10-24']
2010,['eng'],"['Sopczak, André']",['Charged Higgs Boson Detector Aspects'],['Detectors and Experimental Techniques'],"['talk, Frascati 1996/02/05', 'talk, Hamburg 1996/11/20', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, pair production', 'Higgs particle, hadronic decay', 'Higgs particle, charged particle', 'calorimeter, hadronic', 'resolution', 'particle identification, efficiency', 'numerical calculations', 'electron positron --> 2Higgs particle anything', 'Higgs particle --> charm strangeness']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710022'],['The discovery potential for charged Higgs bosons has been studied including background simulations for sqrts = 500 GeV and a luminosity of 10 fb-1 depending on the hadronic calorimeter resolution of a LC500 detector. The hadronic decay channel H+H- --> cscs is in particular suited for this study due to a large sensitivity dependence on the hadron calorimeter performance. For this study a hadronic energy resolution as achieved at LEP experiments is sufficient to reach a very good sensitivity. A calorimeter with weaker energy resolution would reduce the sensitivity by a factor of two.'],['1997-10-24']
2011,['eng'],"['Brook, N H']","['CP Violation and Future ""B-Factories""']",['Particle Physics - Experimental Results'],"['lectures, Gomel 1997/08/08', 'B, hadronic decay', 'violation, CP', 'time dependence', 'Feynman graph, penguin', 'B, particle source', 'electron positron, annihilation', 'anti-p p, annihilation', 'p p, interaction', 'electron p, deep inelastic scattering', 'B, particle identification', 'counters and detectors', 'proposed experiment', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710021'],['This lecture contains a brief introduction to CP violation in the B system before discussing future experimental programmes and their CP reach in the B system.'],['1997-10-24']
2012,['eng'],"['Brook, N H']",['Hadronic Final States in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['talk, Gomel 1997/08/08', 'positron p, deep inelastic scattering', 'model, parton', 'quantum chromodynamics, perturbation theory', 'jet, electroproduction', 'hadron, multiple production', 'event shape analysis', 'fragmentation function', 'Lipatov equation', 'Altarelli-Parisi equation', 'strong interaction, coupling constant', 'momentum transfer, dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710020'],"['This lecture contains a brief introduction to HERA and deep inelastic scattering (DIS), before going on to highlight some of the measurements of the hadronic final state in DIS performed by the H1 and ZEUS collaborations.']",['1997-10-24']
2013,['eng'],"['Klima, B']",['Searches for First Generation Leptoquark Pair Production in $p \\overline{p}$ Collisions at D0$^{1}$'],['Particle Physics - Experimental Results'],"['talk, Jerusalem 1997/08/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, leptoquark', 'leptoquark, pair production', 'decay, leptoquark', 'channel cross section, branching ratio', 'mass, dependence', 'mass, leptoquark', 'lower limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> (n)jet positron electron anything', 'anti-p p --> (n)jet electron neutrino anything', 'anti-p p --> (n)jet 2neutrino anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710019'],"['We have searched for the pair production of first generation scalar leptoquarks using the full data set (123 pb**-1) collected with the D0 detector at the Fermilab Tevatron during 1992-1996. We observe no candidates, consistent with the expected background. We combine these new results from the ee + jets and enu + jets channels with the published nunu + jets result to obtain a 95% CL upper limits on the LQ pair production cross section as a function of mass and beta, the branching ratio to a charged lepton and a quark. Comparing to the NLO theory predictions, we set 95% CL lower limits on the LQ mass of 225, 204, and 79 GeV/c**2 for beta=1, 1/2, and 0, respectively. The results of this analysis rule out an interpretation of the excess of high Q**2 events at HERA as leptoquarks with LQ mass below 200 GeV/c**2 for values of beta > 0.4.']",['1997-10-23']
2014,['eng'],"['Breitweg, J']",['Dijet Cross Sections in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'photon p, interaction', 'jet, photoproduction', 'final state, (2jet)', 'hadron, multiple production', 'jet, particle identification', 'cross section, rapidity dependence', 'transverse energy, dependence', 'quantum chromodynamics, perturbation theory', 'photon, resolved', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'tables', 'positron p --> 2jet positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710018'],"['Dijet cross sections are presented using photoproduction data obtained with the ZEUS detector during 1994. These measurements represent an extension of previous results, as the higher statistics allow cross sections to be measured at higher jet transverse energy (ETJ). Jets are identified in the hadronic final state using three different algorithms, and the cross sections compared to complete next-to-leading order QCD calculations. Agreement with these calculations is seen for the pseudorapidity dependence of the direct photon events with ETJ > 6 GeV and of the resolved photon events with ETJ > 11 GeV. Calculated cross sections for resolved photon processes with 6 GeV < ETJ < 11 GeV lie below the data.']",['1997-10-23']
2015,['eng'],"['Achasov, M N', 'Bek, M G', 'Beloborodov, K I', 'Berdyugin, A V', 'Bozhenok, A V', 'Bukin, A D', 'Bukin, D A', 'Burdin, S V', 'Danilov, V V', 'Dimova, T V', 'Dolinski, S I', 'Druzhinin, V P', 'Dubrovin, M S', 'Gaponenko, I A', 'Golubev, V B', 'Ivanchenko, V N', 'Ivanov, P I', 'Koop, I A', 'Korol, A A', 'Korostelev, M S', 'Koshuba, S V', 'Lysenko, A P', 'Mamutkin, A A', 'Nesterenko, I N', 'Pakhtusova, E V', 'Perevedentsev, E A', 'Polunin, A A', 'Pozdeev, E G', 'Ptitsyn, V I', 'Pyata, E E', 'Salnikov, A A', 'Savchkov, A V', 'Shary, V V', 'Serednyakov, S I', 'Shatunov, Yu M', 'Sidorov, V A', 'Silagadze, Z K', 'Skrinsky, A N', 'Usov, Yu V', 'Valishev, A A', 'Varganov, A V', 'Vasilev, A', 'Velikzhanin, Yu S']",['First Physical Results from SND Detector at VEPP-2M'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron positron, inelastic scattering', 'meson, electroproduction', 'meson, multiple production', 'pi', 'K', 'omega(783)', 'Phi(1020), hadronic decay', 'Phi(1020), branching ratio', 'vector meson, radiative decay', 'muon, pair production', 'eta, rare decay', 'photon, multiple production', 'electron p, exclusive reaction', 'Delta(1232), electroproduction', 'mass spectrum', 'angular distribution', 'photon, energy spectrum', 'four-pi-detector, SND', 'Novosibirsk Stor2', '((1))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710017'],"[""The paper describes experiments with the SND detector at VEPP-2M collider, carried out during the period from October 1995 until June 1997. The total integrated luminosity of 6.4 pb^{-1} was collected in the energy range 2E=0.4-1.4 GeV (MHAD97 experiment), corresponding to 4*10^5 mu^+ mu^- pairs produced. Preliminary results of the 1996 phi-meson experiment (FI96) are presented. The total number of phi-mesons produced is 4*10^6. New data on rare decays of phi and eta (550) mesons, in particular B(phi -> eta gamma) = (1.30+-0.06+-0.07)%, B(phi -> pi^0 pi^0 gamma) = (1.1+-0.2)*10^{-4}, (M_{pi^0 pi^0} > 800 MeV), B(phi -> f^0 gamma) = (4.7+-1.0)*10^{-4}, B(phi -> eta pi^0 gamma) = (1.3+-0.5)*10^{-4}, B(phi -> eta' gamma) < 1.7*10^{-4}, B(phi -> 2 pi^0 ) < 6*10^{-4} were obtained.""]",['1997-10-22']
2016,['eng'],"['Abe, F', 'Abe, F', 'Akimoto, H', 'Akopian, A M', 'Albrow, Michael G', 'Amadon, A', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Aota, S', 'Apollinari, G', 'Arisawa, T', 'Asakawa, T', 'Ashmanskas, W J', 'Atac, Muzaffer', 'Azzi-Bacchetta, P', 'Bacchetta, N', 'Bagdasarov, S L', 'Bailey, M W', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Barone, M', 'Bauer, G', 'Baumann, T', 'Bedeschi, F', 'Behrends, S', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Bensinger, J', 'Beretvas, A', 'Berge, J P', 'Berryhill, J', 'Bertolucci, S', 'Bettelli, S', 'Bevensee, B E', 'Bhatti, A A', 'Biery, K', 'Bigongiari, C', 'Binkley, M', 'Bisello, D', 'Blair, R E', 'Blocker, C A', 'Blusk, S R', 'Bodek, Arie', 'Bokhari, W', 'Bölla, G', 'Bonushkin, Yu', 'Bortoletto, D', 'Boudreau, J', 'Breccia, L', 'Bromberg, C', 'Bruner, N L', 'Brunetti, R', 'Buckley-Geer, E', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlsmith, D', 'Cassada, J A', 'Castro, A', 'Cauz, D', 'Cerri, A', 'Chang, P S', 'Chang, P T', 'Chao, H Y', 'Chapman, J', 'Cheng, M T', 'Chertok, M', 'Chiarelli, G', 'Chiou, C N', 'Chlebana, F S', 'Christofek, L S', 'Chu, M L', 'Cihangir, S', 'Clark, A G', 'Cobal, M', 'Cocca, E', 'Contreras, M', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Costanzo, D', 'Couyoumtzelis, C', 'Cronin-Hennessy, D', 'Culbertson, R J', 'Dagenhart, D', 'Daniels, T', 'De Jongh, F', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demina, R', 'Demortier, L', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dittmann, J R', 'Donati, S', 'Done, J', 'Dorigo, T', 'Eddy, N', 'Einsweiler, Kevin F', 'Elias, J E', 'Ely, R P', 'Engels, E', 'Erdmann, W', 'Errede, D', 'Errede, S', 'Fan, Q', 'Feild, R G', 'Feng, Z', 'Ferretti, C', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Freeman, J', 'Friedman, J', 'Frisch, H', 'Fukui, Y', 'Gadomski, S', 'Galeotti, S', 'Gallinaro, M', 'Ganel, O', 'García-Sciveres, M', 'Garfinkel, A F', 'Gay, C', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giokaris, N D', 'Giromini, P', 'Giusti, G', 'Gold, M', 'Gordon, A', 'Goshaw, A T', 'Gotra, Yu', 'Goulianos, K', 'Grassmann, H', 'Groer, L S', 'Grosso-Pilcher, C', 'Guillian, G', 'Guimarães da Costa, J', 'Guo, R S', 'Haber, C', 'Hafen, E S', 'Hahn, S R', 'Hamilton, R', 'Handa, T', 'Handler, R', 'Happacher, F', 'Hara, K', 'Hardman, A D', 'Harris, R M', 'Hartmann, F', 'Hauser, J', 'Hayashi, E', 'Heinrich, J', 'Hao, W', 'Hinrichsen, B', 'Hoffman, K D', 'Hohlmann, M', 'Holck, C', 'Hollebeek, R J', 'Holloway, L', 'Huang, Z', 'Huffman, B T', 'Hughes, R', 'Huston, J', 'Huth, J E', 'Ikeda, H', 'Incagli, M', 'Incandela, J R', 'Introzzi, G', 'Iwai, J', 'Iwata, Y', 'James, E', 'Jensen, H', 'Joshi, U', 'Kajfasz, E', 'Kambara, H', 'Kamon, T', 'Kaneko, T', 'Karr, K', 'Kasha, H', 'Kato, Y', 'Keaffaber, T A', 'Kelley, K F', 'Kennedy, R D', 'Kephart, R D', 'Kestenbaum, D S', 'Khazins, D M', 'Kikuchi, T', 'Kim, B J', 'Kim, H S', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Klimenko, S', 'Knoblauch, D', 'Koehn, P', 'Köngeter, A', 'Kondo, K', 'Konigsberg, J', 'Kordas, K', 'Korytov, A V', 'Kovacs, E', 'Kowald, W', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kuns, E W', 'Kurino, K', 'Kuwabara, T', 'Laasanen, A T', 'Nakano, I', 'Lami, S', 'Lammel, S', 'Lamoureux, J I', 'Lancaster, M', 'Lanzoni, M', 'Latino, G', 'LeCompte, T J', 'Leone, S', 'Lewis, J D', 'Limon, P', 'Lindgren, M', 'Liss, T M', 'Liu, J B', 'Liu, Y C', 'Lockyer, N', 'Long, O', 'Loomis, C', 'Loreti, M', 'Lucchesi, D', 'Lukens, P', 'Lusin, S', 'Lys, J', 'Maeshima, K', 'Maksimovic, P', 'Mangano, Michelangelo L', 'Mariotti, M', 'Marriner, J P', 'Martin, A', 'Matthews, J A J', 'Mazzanti, P', 'McIntyre, P', 'Mélèse, P', 'Menguzzato, M', 'Menzione, A', 'Meschi, E', 'Metzler, S', 'Miao, C', 'Miao, T', 'Michail, G', 'Miller, R', 'Minato, H', 'Miscetti, S', 'Mishina, M', 'Miyashita, S', 'Moggi, N', 'Moore, E', 'Morita, Y', 'Mukherjee, A', 'Müller, T', 'Murat, P', 'Murgia, S', 'Nakada, H', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Ngan, C Y P', 'Nodulman, L', 'Nomerotski, A', 'Oh, S H', 'Ohmoto, T', 'Ohsugi, T', 'Oishi, R', 'Okabe, M', 'Okusawa, T', 'Olsen, J', 'Pagliarone, C', 'Paoletti, R', 'Papadimitriou, V', 'Pappas, S P', 'Parashar, N', 'Parri, A', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Perazzo, A', 'Pescara, L', 'Peters, M D', 'Phillips, T J', 'Piacentino, G', 'Pillai, M', 'Pitts, K T', 'Plunkett, R K', 'Pondrom, L', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Reher, D', 'Reischl, M', 'Ribon, A', 'Rimondi, F', 'Ristori, L', 'Robertson, W J', 'Rodrigo, T', 'Rolli, S', 'Rosenson, L', 'Roser, R M', 'Saab, T', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Santi, L', 'Sato, H', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Scott, A', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Semeria, F', 'Shah, T', 'Shapiro, M D', 'Shaw, N M', 'Shepard, P F', 'Shibayama, T', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Sliwa, K', 'Smith, C', 'Snider, F D', 'Spalding, J', 'Speer, T', 'Sphicas, P', 'Spinella, F', 'Spiropulu, M', 'Spiegel, L', 'Stanco, L', 'Steele, J', 'Stefanini, A', 'Ströhmer, R', 'Strologas, J', 'Strumia, F', 'Stuart, D', 'Sumorok, K', 'Suzuki, J', 'Suzuki, T', 'Takahashi, T', 'Takano, T', 'Takashima, R', 'Takikawa, K', 'Tanaka, M', 'Tannenbaum, B', 'Tartarelli, F', 'Taylor, W', 'Tecchio, M', 'Teng, P K', 'Teramoto, Y', 'Terashi, K', 'Tether, S', 'Theriot, D', 'Thomas, T L', 'Thurman-Keup, R M', 'Timko, M', 'Tipton, P', 'Titov, A', 'Tkaczyk, S M', 'Toback, D', 'Tollefson, K', 'Tollestrup, A V', 'Toyoda, H', 'Trischuk, W', 'De Trocóniz, J F', 'Truitt, S', 'Tseng, J', 'Turini, N', 'Uchida, T', 'Ukegawa, F', 'Valls, J', 'van den Brink, S C', 'Vejcik, S', 'Velev, G V', 'Vidal, R', 'Vilar, R', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wahl, J', 'Wallace, N B', 'Walsh, A M', 'Wang, C', 'Wang, C H', 'Wang, M J', 'Warburton, A', 'Watanabe, T', 'Watts, T', 'Webb, R', 'Wei, C', 'Wenzel, H', 'Wester, W C', 'Wicklund, A B', 'Wicklund, E', 'Wilkinson, R P', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Winn, D', 'Wolinski, D', 'Wolinski, J', 'Worm, S D', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yasuoka, K', 'Yeh, G P', 'Yeh, P', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yu, I', 'Zanetti, A', 'Zetti, F', 'Zucchelli, S']",['Measurement of the Top Quark Mass and Top-Antitop Production Cross-Section from Dilepton Events at the Collider Detector at Fermilab'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'mass, truth', 'final state, dilepton', 'lepton, transverse momentum', 'jet, transverse energy', 'transverse energy, missing-energy', 'mass spectrum, (beauty lepton)', 'channel cross section', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9802017'],"['We present an analysis of dilepton events originating from top-antitop production in proton-antiproton collisions at sqrt{s}=1.8 TeV at the Fermilab Tevatron Collider. The sample corresponds to an integrated luminosity of 109+-7 pb^{-1}. We observe 9 candidate events, with an estimated background of 2.4+-0.5 events. We determine the mass of the top quark to be M_top = 161+-17(stat.)+-10(syst.) GeV/c^2. In addition we measure a top-antitop production cross section of 8.2+4.4-3.4 pb (where M_top = 175 GeV/c^2 has been assumed for the acceptance estimate).']",['1998-02-19']
2017,['eng'],"['Frey, R E']",['Recent Electroweak Results from SLC/SLD'],['Particle Physics - Experimental Results'],"['talk, Balholm 1997/04/29', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'polarization, asymmetry', 'quark, pair production', 'quark, beauty', 'quark, charm', 'parity, violation', 'Z0, branching ratio', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'track data analysis, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710016'],"['Key electroweak measurements performed by the SLD collaboration at the SLC are described and recent results given. The left-right cross-section asymmetry, $A_{LR}$, has been updated to include the 1996 data. It remains the single most precise measurement of $\\sin^2\\theta_W^{eff}$, and it is compared to the LEP results. The polarized differential cross section for $b$-quarks is measured and is used to perform a unique direct measurement of the parity violation parameter for $b$ quarks, $A_b$. The excellent capability to perform secondary vertexing at SLC with CCD-based vertex detectors is described, including first physics results with the new detector VXD3. The vertexing is used to full advantage to make a highly pure B tag to measure the fraction of hadronic $Z^0$ decays going to $b$ quarks, $R_b$. The vertexing, in combination with electron-beam polarization, is used to measure $B_d^0$ mixing. The prospects for making a $B_s^0$ mixing measurement are excellent given good SLC performance in the upcoming SLC run(s).']",['1997-10-20']
2018,['eng'],"['Aggarwal, M M']",['Search for Disoriented Chiral Condensates in 158 AGeV Pb+Pb Collisions'],['Particle Physics - Experimental Results'],"['nucleus nucleus, nuclear reaction', 'scattering, heavy ion', 'lead', 'condensation, chiral', 'pi, multiple production', 'yield, (pi+ pi- pi0)', 'charged particle, multiplicity', 'photon, multiplicity', 'experimental results', 'CERN SPS', '158 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710015'],"['The restoration of chiral symmetry and its subsequent breaking through a phase transition has been predicted to create regions of Disoriented Chiral Condensates (DCC). This phenomenon has been predicted to cause anomalous fluctuations in the relative production of charged and neutral pions in high-energy hadronic and nuclear collisions. The WA98 experiment has been used to measure charged and photon multiplicities in the central region of 158 AGeV Pb+Pb collisions at the CERN SPS. In a sample of 212646 events, no clear DCC signal can be distinguished. Using a simple DCC model, we have set a 90% C.L. upper limit on the maximum DCC production allowed by the data.']",['1997-10-20']
2019,['eng'],"['Sefkow, F']",['Heavy Quark and Jet Production by Real and Virtual Photons'],['Particle Physics - Experimental Results'],"['talk, Bristol 1997/06/25', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'J/psi(3100), photoproduction', 'D*(2010), photoproduction', 'angular distribution, (2jet)', 'quantum chromodynamics, perturbation theory', 'event shape analysis', 'photon, resolved', 'photon, structure function', 'cross section, energy dependence', 'differential cross section, momentum transfer', 'fusion, boson gluon', 'differential cross section, rapidity dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710014'],"['Recent results from the H1 and ZEUS collaborations on hard QCD processes in ep interactions are reviewed. The topics cover jet shapes, the structure of real and virtual photons, and the production of J/Psi mesons and open charm.']",['1997-10-20']
2020,['eng'],"['Albrecht, H']","['Determination of the Michel Parameters $\\rho$, $\\xi$, and $\\delta$ in $\\tau$-Lepton Decays with $\\tau \\to \\rho \\nu$ Tags']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, semileptonic decay', 'tau, leptonic decay', 'Michel parameter', 'magnetic detector, ARGUS', 'experimental results', 'DESY HERA Stor', 'electron positron --> tau+ tau-', 'tau --> lepton neutrino/tau neutrino', 'tau --> rho(770) neutrino/tau']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9711022'],"['Using the ARGUS detector at the $e^+ e^-$ storage ring DORIS II, we have measured the Michel parameters $\\rho$, $\\xi$, and $\\xi\\delta$ for center of mass energies in the region of the $\\Upsilon$ resonances. Using 0.04 \\pm 0.08$, $\\xi_{e}= 1.12 \\pm 0.20 \\pm 0.09$, $\\xi\\delta_{e}= 0.57 \\pm 0.14 \\pm 0.07$, $\\rho_{\\mu}= 0.69 \\pm 0.06 \\pm 0.08$, $\\xi_{\\mu}= 1.25 \\pm 0.27 the combined ARGUS results on $\\rho$, $\\xi$, and $\\xi\\delta$ using this work und previous measurements.']",['1997-12-01']
2021,['eng'],"['Gallo, E']",['Diffraction'],['Particle Physics - Experimental Results'],"['review, Hamburg 1997/07/28', 'photon p, interaction', 'hadron p, interaction', 'diffraction, dissociation', 'cross section, factorization', 'vector meson, hadroproduction', 'vector meson, photoproduction', 'Regge poles', 'exchange, pomeron', 'structure function, diffraction', 'jet, hadroproduction', 'final state, (2jet)', 'cross section, energy dependence', 'cross section, slope', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'experimental results', 'DESY HERA Stor', 'Batavia TEVATRON Coll', 'Batavia TEVATRON PS', '((6)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710013'],"['This report summarizes recent results on diffraction obtained at HERA, at the Tevatron and by the fixed target experiment E665. The measurements include vector meson production, inclusive diffraction at HERA and the pomeron structure function as inferred from the HERA and the Tevatron data.']",['1997-10-17']
2022,['eng'],"['Barate, R', 'Buskulic, D', 'Décamp, D', 'Ghez, Philippe', 'Goy, C', 'Lees, J P', 'Lucotte, A', 'Minard, M N', 'Nief, J Y', 'Pietrzyk, B', 'Casado, M P', 'Chmeissani, M', 'Comas, P', 'Crespo, J M', 'Delfino, M C', 'Fernández, E', 'Fernández-Bosman, M', 'Garrido, L', 'Juste, A', 'Martínez, M', 'Merino, G', 'Miquel, R', 'Mir, L M', 'Padilla, C', 'Park, I C', 'Pascual, A', 'Perlas, J A', 'Riu, I', 'Sánchez, F', 'Colaleo, A', 'Creanza, D', 'De Palma, M', 'Gelao, G', 'Iaselli, Giuseppe', 'Maggi, G', 'Maggi, M', 'Marinelli, N', 'Nuzzo, S', 'Ranieri, A', 'Raso, G', 'Ruggieri, F', 'Selvaggi, G', 'Silvestris, L', 'Tempesta, P', 'Tricomi, A', 'Zito, G', 'Huang, X', 'Lin, J', 'Ouyang, Q', 'Wang, T', 'Xie, Y', 'Xu, R', 'Xue, S', 'Zhang, J', 'Zhang, L', 'Zhao, W', 'Abbaneo, D', 'Alemany, R', 'Bazarko, A O', 'Becker, U', 'Bright-Thomas, P G', 'Cattaneo, M', 'Cerutti, F', 'Dissertori, G', 'Drevermann, H', 'Forty, Roger W', 'Frank, M', 'Gianotti, F', 'Hagelberg, R', 'Hansen, J B', 'Harvey, J', 'Janot, P', 'Jost, B', 'Kneringer, E', 'Lehraus, Ivan', 'Mato, P', 'Minten, A', 'Moneta, L', 'Pacheco, A', 'Pusztaszeri, J F', 'Ranjard, F', 'Rizzo, G', 'Rolandi, Luigi', 'Rousseau, D', 'Schlatter, D', 'Schmitt, M', 'Schneider, O', 'Tejessy, W', 'Teubert, F', 'Tomalin, I R', 'Wachsmuth, Horst Werner', 'Wagner, A', 'Ajaltouni, Ziad J', 'Barrès, A', 'Boyer, C', 'Falvard, A', 'Ferdi, C', 'Gay, P', 'Guicheney, C', 'Henrard, P', 'Jousset, J', 'Michel, B', 'Monteil, S', 'Montret, J C', 'Pallin, D', 'Perret, P', 'Podlyski, F', 'Proriol, J', 'Rosnet, P', 'Rossignol, J M', 'Fearnley, Tom', 'Hansen, J D', 'Hansen, J R', 'Hansen, P H', 'Nilsson, B S', 'Rensch, B', 'Wäänänen, A', 'Daskalakis, G', 'Kyriakis, A', 'Markou, C', 'Simopoulou, Errietta', 'Vayaki, Anna', 'Blondel, Alain', 'Brient, J C', 'Machefert, F P', 'Rougé, A', 'Rumpf, M', 'Valassi, A', 'Videau, H L', 'Boccali, T', 'Focardi, E', 'Parrini, G', 'Zachariadou, K', 'Cavanaugh, R J', 'Corden, M', 'Georgiopoulos, C H', 'Hühn, T', 'Jaffe, D E', 'Antonelli, A', 'Bencivenni, G', 'Bologna, G', 'Bossi, F', 'Campana, P', 'Capon, G', 'Casper, David William', 'Chiarella, V', 'Felici, G', 'Laurelli, P', 'Mannocchi, G', 'Murtas, F', 'Murtas, G P', 'Passalacqua, L', 'Pepé-Altarelli, M', 'Curtis, L', 'Dorris, S J', 'Halley, A W', 'Knowles, I G', 'Lynch, J G', ""O'Shea, V"", 'Raine, C', 'Scarr, J M', 'Smith, K', 'Teixeira-Dias, P', 'Thompson, A S', 'Thomson, E', 'Thomson, F', 'Turnbull, R M', 'Buchmüller, O L', 'Dhamotharan, S', 'Geweniger, C', 'Graefe, G', 'Hanke, P', 'Hansper, G', 'Hepp, V', 'Kluge, E E', 'Putzer, A', 'Sommer, J', 'Tittel, K', 'Werner, S', 'Wunsch, M', 'Beuselinck, R', 'Binnie, David M', 'Cameron, W', 'Dornan, Peter J', 'Girone, M', 'Goodsir, S M', 'Martin, E B', 'Morawitz, P', 'Moutoussi, A', 'Nash, J', 'Sedgbeer, J K', 'Spagnolo, P', 'Stacey, A M', 'Williams, M D', 'Ghete, V M', 'Girtler, P', 'Kuhn, D', 'Rudolph, G', 'Betteridge, A P', 'Bowdery, C K', 'Buck, P G', 'Colrain, P', 'Crawford, G', 'Finch, A J', 'Foster, F', 'Hughes, G', 'Jones, R W L', 'Sloan, Terence', 'Whelan, E P', 'Williams, M I', 'Giehl, I', 'Hoffmann, C', 'Jakobs, K', 'Kleinknecht, K', 'Quast, G', 'Renk, B', 'Rohne, E', 'Sander, H G', 'Van Gemmeren, P', 'Zeitnitz, C', 'Aubert, Jean-Jacques', 'Benchouk, C', 'Bonissent, A', 'Bujosa, G', 'Carr, J', 'Coyle, P', 'Diaconu, C A', 'Ealet, A', 'Fouchez, D', 'Konstantinidis, N P', 'Leroy, O', 'Motsch, F', 'Payre, P', 'Talby, M', 'Sadouki, A', 'Thulasidas, M', 'Tilquin, A', 'Trabelsi, K', 'Aleppo, M', 'Antonelli, M', 'Ragusa, F', 'Berlich, R', 'Blum, Walter', 'Büscher, V', 'Dietl, H', 'Ganis, G', 'Gotzhein, C', 'Kroha, H', 'Lütjens, G', 'Lutz, G', 'Männer, W', 'Moser, H G', 'Richter, R H', 'Rosado-Schlosser, A', 'Schael, S', 'Settles, Ronald', 'Seywerd, H C J', 'Saint-Denis, R', 'Stenzel, H', 'Wiedenmann, W', 'Wolf, G', 'Boucrot, J', 'Callot, O', 'Chen, S', 'Davier, M', 'Duflot, L', 'Grivaz, J F', 'Heusse, P', 'Höcker, A', 'Jacholkowska, A', 'Kim, D W', 'Le Diberder, F', 'Lefrançois, J', 'Lutz, A M', 'Marumi, M', 'Schune, M H', 'Serin, L', 'Tournefier, E', 'Veillet, J J', 'Videau, I', 'Zerwas, D', 'Azzurri, P', 'Bagliesi, G', 'Bettarini, S', 'Bozzi, C', 'Calderini, G', 'Ciulli, V', ""Dell'Orso, R"", 'Fantechi, R', 'Ferrante, I', 'Giassi, A', 'Gregorio, A', 'Ligabue, F', 'Lusiani, A', 'Marrocchesi, P S', 'Messineo, A', 'Palla, Fabrizio', 'Sanguinetti, G', 'Sciabà, A', 'Sguazzoni, G', 'Steinberger, Jack', 'Tenchini, Roberto', 'Vannini, C', 'Venturi, A', 'Verdini, P G', 'Blair, G A', 'Bryant, L M', 'Chambers, J T', 'Green, M G', 'Medcalf, T', 'Perrodo, P', 'Strong, J A', 'Von Wimmersperg-Töller, J H', 'Botterill, D R', 'Clifft, R W', 'Edgecock, T R', 'Haywood, S', 'Maley, P', 'Norton, P R', 'Thompson, J C', 'Wright, A E', 'Bloch-Devaux, B', 'Colas, P', 'Fabbro, B', 'Lançon, E', 'Lemaire, M C', 'Locci, E', 'Pérez, P', 'Rander, J', 'Renardy, J F', 'Rosowsky, A', 'Roussarie, A', 'Schwindling, J', 'Trabelsi, A', 'Vallage, B', 'Black, S N', 'Dann, J H', 'Kim, H Y', 'Litke, A M', 'McNeil, M A', 'Taylor, G', 'Booth, C N', 'Brew, C A J', 'Cartwright, S L', 'Combley, F', 'Kelly, M S', 'Lehto, M H', 'Reeve, J', 'Thompson, L F', 'Affholderbach, K', 'Böhrer, A', 'Brandt, S', 'Cowan, G D', 'Foss, J', 'Grupen, Claus', 'Smolik, L', 'Stephan, F', 'Apollonio, M', 'Bosisio, L', 'Della Marina, R', 'Giannini, G', 'Gobbo, B', 'Musolino, G', 'Pütz, J', 'Rothberg, J E', 'Wasserbaech, S R', 'Williams, R W', 'Armstrong, S R', 'Charles, E', 'Elmer, P', 'Ferguson, D P S', 'Gao, Y', 'González, S', 'Greening, T C', 'Hayes, O J', 'Hu, H', 'Jin, S', 'McNamara, P A', 'Nachtman, J M', 'Nielsen, J', 'Orejudos, W', 'Pan, Y B', 'Saadi, Y', 'Scott, I J', 'Walsh, J', 'Wu Sau Lan', 'Wu, X', 'Yamartino, J M', 'Zobernig, G']",['Searches for charginos and neutralinos in $e^+ e^-$ collisions at $\\sqrt{s}$ = 161 and 172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'sparticle, pair production', 'mass, chargino', 'mass, neutralino', 'lower limit', 'effect, slepton', 'supersymmetry', 'sparticle, decay modes', 'cross section, production', 'upper limit', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '161, 170, 172 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&ca', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710012']","['The data recorded by the ALEPH detector at centre-of-mass energies of 161, 170, and 172 GeV are analysed for signals of chargino and neutralino production. No evidence of a signal is found, although candidate events consistent with the expectations from Standard Model processes are observed. Limits at 95% C.L. on the production cross sections are derived and bounds on the parameters of the Minimal Supersymmetric Standard Model are set. The lower limit on the mass of the lightest chargino is 85.5 GeV/c^2 for gaugino-like charginos (mu = -500 GeV/c^2), and 85.0 GeV/c^2 for Higgsino-like charginos (M_2 = 500 GeV/c^2), for heavy sneutrinos (M(snu) > 200 GeV/c^2) and tanb = sqrt(2). The effect of light sleptons on chargino and neutralino limits is investigated. The assumptions of a universal slepton mass and a universal gaugino mass are relaxed, allowing less model-dependent limits to be obtained.']",['1997-10-16']
2023,['eng'],"['Abe, F']",['Measurement of the Top Quark Mass'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, ((n)jet lepton)', 'mass, truth', 'background', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801014'],"['We present a measurement of the top quark mass using a sample of t-tbar decays into an electron or a muon, a neutrino, and four jets. The data were collected in p-pbar collisions at sqrt(s)=1.8 TeV with the Collider Detector at Fermilab and correspond to an integrated luminosity of 109 pb^-1. We measure the top quark mass to be 175.9 +/- 4.8(stat.) +/- 4.9(syst.) GeV/c^2.']",['1998-01-16']
2024,['eng'],"['Abe, F']",['Measurement of the $t\\overline{t}$ Production Cross Section in $p\\overline{p}$ Collisions at $\\sqrt{s}$=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'final state, dilepton', 'final state, ((n)jet lepton)', 'final state, ((n)jet)', 'mass, truth', 'channel cross section', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710008'],"['We present a measurement of the t-tbar cross section in p-pbar collisions at sqrt(s)=1.8 TeV using an integrated luminosity of 109 pb-1 collected with the Collider Detector at Fermilab. The measurement uses t-tbar decays into final states which contain one or two high transverse momentum leptons and multiple jets, and final states which contain only jets. Using acceptances appropriate for a top quark mass of 175 GeV/c^2, we find sigma(t-tbar)=7.6 (+1.8 -1.5) pb .']",['1997-10-13']
2025,['eng'],"['Abbott, B']",['Determination of the Mass of the W Boson Using the D0 Detector at the Tevatron'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'W, mass', 'mass spectrum, transverse', 'mass ratio, (Z0 W)', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710007'],"['A measurement of the mass of the W boson is presented which is based on a sample of 5982 W -> e nu decays observed in p-pbar collisions at sqrt{s} = 1.8 TeV with the D0 detector during the 1992--1993 run. From a fit to the transverse mass spectrum, combined with measurements of the Z boson mass, the W boson mass is measured to be M_W = 80.350+-0.140(stat)+-0.165(sys)+-0.160(scale) GeV/c^2. Detailed discussions of the determination of the absolute energy scale, the measured efficiencies, and all systematic uncertainties are presented.']",['1997-10-10']
2026,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for anomalous production of dilepton events with missing transverse momentum in $e^{+} e^{-}$ collisions at $\\sqrt{s}$ = 161 and 172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'lepton, pair production', 'transverse momentum, missing-energy', 'electroweak interaction, validity test', 'W, pair production', 'W, leptonic decay', 'new particle, search for', 'slepton', 'Higgs particle', 'chargino', 'sparticle, pair production', 'channel cross section, upper limit', 'event shape analysis, planarity', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> lepton+ lepton- missing-energy', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710010'],"['Events containing a pair of charged leptons and significant missing transverse momentum are selected from a data sample corresponding to a total integrated luminosity of 20.6 pb^-1 at centre-of-mass energies of 161 GeV and 172 GeV. The observed number of events, four at 161 GeV and nine at 172 GeV, is consistent with the number expected from Standard Model processes, predominantly arising from W+W- production with each W decaying leptonically. This topology is also an experimental signature for the pair production of new particles that decay to a charged lepton accompanied by one or more invisible particles. Further event selection criteria are described that optimise the sensitivity to particular new physics channels. No evidence for new phenomena is observed and limits on the production of scalar charged lepton pairs and other new particles are presented.']",['1997-10-14']
2027,['eng'],"['Breitweg, J']",['Observation of Scaling Violations in Scaled Momentum Distributions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'charged particle, multiple production', 'scaling, violation', 'momentum spectrum', 'current, fragmentation', 'dependence, momentum transfer', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710011'],"['Charged particle production has been measured in deep inelastic scattering (DIS) events over a large range of $x$ and $Q^2$ using the ZEUS detector. The evolution of the scaled momentum, $x_p$, with $Q^2,$ in the range 10 to 1280 GeV^2, has been investigated in the current fragmentation region of the Breit frame. The results show clear evidence, in a single experiment, for scaling violations in scaled momenta as a function of $Q^2$.']",['1997-10-15']
2028,['eng'],"['Wäckerle, F']",['Total Hadronic Cross-Section for Photon-Photon Interactions at LEP'],['Particle Physics - Experimental Results'],"['talk, Frascati 1997/09/08', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'cross section, hadronic', 'energy dependence', 'hadron, photoproduction', 'hadron, multiple production', 'charged particle, multiplicity', 'photon, flux', 'form factor', 'Regge poles', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> (n)hadron positron electron', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710005'],['The total hadronic cross-section for the interaction of real photons is extracted from a measurement of the cross-section of the process e+e->e+e- + hadrons using a luminosity function for the photon flux and form factors for extrapolating to Q**2=0. The data was taken with the OPAL detector at LEP at e+e- centre-of-mass energies of 161 GeV and 172 GeV. In the energy range 10 < W < 110 GeV the total hadronic photon-photon cross-section is consistent with the Regge behaviour of the total cross-section observed in \\gamma p and hadron-hadron interactions.'],['1997-10-09']
2029,['eng'],"['Brandt, A', 'Chèze, J B', 'Erhan, S', 'Kuzucu-Polatoz, A', 'Lynn, D', 'Medinnis, M', 'Ozdes, N', 'Schlein, Peter E', 'Zeyrek, M T', 'Zsembery, J', 'Zweizig, J G']",['Measurements of Single Diffraction at $\\sqrt{s}$ = 630 GeV'],['Particle Physics - Experimental Results'],"['anti-p p, interaction', 'diffraction', 'Regge poles, multi-Regge', 'exchange, pomeron', 'scattering, pomeron p', 'cross section, mass', 'flux, pomeron', 'energy flow', 'jet', 'differential cross section, momentum transfer', 'magnetic spectrometer, experimental results', 'CERN SPS', 'anti-p p --> p anything', 'anti-p p --> anti-p anything', '630 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710004'],"[""We report measurements of the inclusive differential cross section for the single-diffractive reactions: p + pbar --> p + X and p + pbar --> X + pbar at sqrt(s) = 630 GeV, in the momentum transfer range, t = 0.8--2.0 GeV^2 and final state Feynman-x > 0.90. Based on the assumption of factorization, several new features of the Pomeron Flux Factor are determined from simultaneous fits to our UA8 data and lower energy data from the CHLM collaboration at the CERN-Intersecting Storage Rings. Prominent among these is that the effective Pomeron Regge trajectory requires a term quadratic in t, with coefficient, a'' = 0.079 +- 0.012 GeV^-2. We also show that the data require a Pomeron-proton cross section that first decreases with increasing diffractive mass (corresponding to the PPR term in the triple-Regge expansion) and then increases at larger mass (the PPP term), similar to real particle total cross sections. We measure the product, (K x sigma0) = 0.72 +- 0.10 mb/GeV^2, where K is the normalization constant of the Pomeron Flux Factor in the proton and sigma0 is the scale constant in the Pomeron-proton total cross section. Finally, we report the occurance of ``beam jets'' in the Pomeron direction in the rest frame of the diffractive system.""]",['1997-10-07']
2030,['eng'],"['Glenn, S']",['Search for Inclusive $b\\rightarrow sl^{+}l^{-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'quark, beauty', 'quark, semileptonic decay', 'neutral current, flavor changing', 'lepton, pair production', 'quark, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'beauty --> strangeness lepton+ lepton-', 'beauty --> strangeness muon electron', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710003'],"['We have searched for the effective FCNC decays b->s l+l- using an inclusive method. We set upper limits on the branching ratios B(b->s e+e-) < 5.7 10^{-5}, B(b->s mu+mu-) < 5.8 10^{-5}, and B(b->s e+-mu-+) < 2.2 10^{-5} (at 90 %\\ C.L.). Combining the di-electron and di-muon decay modes we find: B(b->s l+l-) < 4.2 10^{-5} (at 90 % C.L.).']",['1997-10-07']
2031,['eng'],"['Breitweg, J']",['Measurement of Jet Shapes in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'photon p, inclusive reaction', 'jet, photoproduction', 'final state, (2jet)', 'event shape analysis', 'photon, resolved', 'energy flow, hadronic', 'rapidity dependence', 'transverse energy, dependence', 'quark, jet', 'gluon, jet', 'showers, parton', 'multiple scattering, parton', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710002'],"['The shape of jets produced in quasi-real photon-proton collisions at centre-of-mass energies in the range $134-277$ GeV has been measured using the hadronic energy flow. The measurement was done with the ZEUS detector at HERA. Jets are identified using a cone algorithm in the $\\eta - \\phi$ plane with a cone radius of one unit. Measured jet shapes both in inclusive jet and dijet production with transverse energies $E^{jet}_T>14$ GeV are presented. The jet shape broadens as the jet pseudorapidity ($\\eta^{jet}$) increases and narrows as $E^{jet}_T$ increases. In dijet photoproduction, the jet shapes have been measured separately for samples dominated by resolved and by direct processes. Leading-logarithm parton-shower Monte Carlo calculations of resolved and direct processes describe well the measured jet shapes except for the inclusive production of jets with high $\\eta^{jet}$ and low $E^{jet}_T$. The observed broadening of the jet shape as $\\eta^{jet}$ increases is consistent with the predicted increase in the fraction of final state gluon jets.']",['1997-10-07']
2032,['eng'],"['Etzion, E']",['Experimental Studies of Electroweak Physics'],['Particle Physics - Experimental Results'],"['review, Nashville 1997/05/11', 'electron positron, colliding beams', 'electron positron, annihilation', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Z0, electroproduction', 'W, electroproduction', 'fermion, pair production', 'electron, polarized beam', 'angular distribution, asymmetry', 'energy dependence', 'tau, polarization', 'Z0, mass', 'Weinberg angle', 'charge, asymmetry', 'W, mass', 'W, hadroproduction', 'W, pair production', 'coupling, (3gauge boson)', 'CERN LEP Stor', 'SLAC SLC Linac', 'Batavia TEVATRON Coll', '((4)) ((5)) ((7))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9801001'],"['Some experimental new Electroweak physics results measured at the LEP/SLD and the TEVATRON are discussed. The excellent accuracy achieved by the experiments still yield no significant evidence for deviation from the Standard Model predictions, or signal to physics beyond the Standard Model. The Higgs particle still has not been discovered and a low bound is given to its mass.']",['1998-01-02']
2033,['eng'],"['Kühne, R W']",['Tabletop Experiment to Verify Magnetic Monopoles'],['Detectors and Experimental Techniques'],"['search for, magnetic monopole', 'radiation, laser', 'metal, absorption', 'photon, magnetic', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709033'],"['Recently, we suggested a model of magnetic monopoles (hep-ph/9708394). Here we will propose a tabletop experiment to test this model. The verification of the predicted effect would have far-reaching consequences.']",['1997-10-01']
2034,['eng'],"['Kharchilava, A I']",['Searches for SUSY at LHC'],['Detectors and Experimental Techniques'],"['talk, Les Arcs 1997/03/22', 'p p, interaction', 'supersymmetry, search for', 'supergravity', 'R parity, invariance', 'sparticle, pair production', 'sparticle, decay modes', 'sparticle, mass', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709032'],"['One of the main motivations of experiments at the LHC is to search for SUSY particles. The talk is based on recent analyses, performed by CMS Collaboration, within the framework of the Supergravity motivated minimal SUSY extension of the Standard Model. The emphasis is put on leptonic channels. The strategies for obtaining experimental signatures for strongly and weakly interacting sparticles productions, as well as examples of determination of SUSY masses and model parameters are discussed. The domain of parameter space where SUSY can be discovered is investigated. Results show, that if SUSY is of relevance at Electro-Weak scale it could hardly escape detection at LHC.']",['1997-10-01']
2035,['eng'],"['Barate, R', 'Buskulic, D', 'Décamp, D', 'Ghez, Philippe', 'Goy, C', 'Lees, J P', 'Lucotte, A', 'Minard, M N', 'Nief, J Y', 'Pietrzyk, B', 'Casado, M P', 'Chmeissani, M', 'Comas, P', 'Crespo, J M', 'Delfino, M C', 'Fernández, E', 'Fernández-Bosman, M', 'Garrido, L', 'Juste, A', 'Martínez, M', 'Merino, G', 'Miquel, R', 'Mir, L M', 'Padilla, C', 'Park, I C', 'Pascual, A', 'Perlas, J A', 'Riu, I', 'Sánchez, F', 'Colaleo, A', 'Creanza, D', 'De Palma, M', 'Gelao, G', 'Iaselli, Giuseppe', 'Maggi, G', 'Maggi, M', 'Marinelli, N', 'Nuzzo, S', 'Ranieri, A', 'Raso, G', 'Ruggieri, F', 'Selvaggi, G', 'Silvestris, L', 'Tempesta, P', 'Tricomi, A', 'Zito, G', 'Huang, X', 'Lin, J', 'Ouyang, Q', 'Wang, T', 'Xie, Y', 'Xu, R', 'Xue, S', 'Zhang, J', 'Zhang, L', 'Zhao, W', 'Abbaneo, D', 'Alemany, R', 'Bazarko, A O', 'Becker, U', 'Bright-Thomas, P G', 'Cattaneo, M', 'Cerutti, F', 'Dissertori, G', 'Drevermann, H', 'Forty, Roger W', 'Frank, M', 'Hagelberg, R', 'Hansen, J B', 'Harvey, J', 'Janot, P', 'Jost, B', 'Kneringer, E', 'Lehraus, Ivan', 'Mato, P', 'Minten, A', 'Moneta, L', 'Pacheco, A', 'Pusztaszeri, J F', 'Ranjard, F', 'Rizzo, G', 'Rolandi, Luigi', 'Rousseau, D', 'Schlatter, D', 'Schmitt, M', 'Schneider, O', 'Tejessy, W', 'Teubert, F', 'Tomalin, I R', 'Wachsmuth, Horst Werner', 'Wagner, A', 'Ajaltouni, Ziad J', 'Barrès, A', 'Boyer, C', 'Falvard, A', 'Ferdi, C', 'Gay, P', 'Guicheney, C', 'Henrard, P', 'Jousset, J', 'Michel, B', 'Monteil, S', 'Montret, J C', 'Pallin, D', 'Perret, P', 'Podlyski, F', 'Proriol, J', 'Rosnet, P', 'Rossignol, J M', 'Fearnley, Tom', 'Hansen, J D', 'Hansen, J R', 'Hansen, P H', 'Nilsson, B S', 'Rensch, B', 'Wäänänen, A', 'Daskalakis, G', 'Kyriakis, A', 'Markou, C', 'Simopoulou, Errietta', 'Vayaki, Anna', 'Blondel, Alain', 'Brient, J C', 'Machefert, F P', 'Rougé, A', 'Rumpf, M', 'Valassi, A', 'Videau, H L', 'Boccali, T', 'Focardi, E', 'Parrini, G', 'Zachariadou, K', 'Cavanaugh, R J', 'Corden, M', 'Georgiopoulos, C H', 'Hühn, T', 'Jaffe, D E', 'Antonelli, A', 'Bencivenni, G', 'Bologna, G', 'Bossi, F', 'Campana, P', 'Capon, G', 'Casper, David William', 'Chiarella, V', 'Felici, G', 'Laurelli, P', 'Mannocchi, G', 'Murtas, F', 'Murtas, G P', 'Passalacqua, L', 'Pepé-Altarelli, M', 'Curtis, L', 'Dorris, S J', 'Halley, A W', 'Knowles, I G', 'Lynch, J G', ""O'Shea, V"", 'Raine, C', 'Scarr, J M', 'Smith, K', 'Teixeira-Dias, P', 'Thompson, A S', 'Thomson, E', 'Thomson, F', 'Turnbull, R M', 'Buchmüller, O L', 'Dhamotharan, S', 'Geweniger, C', 'Graefe, G', 'Hanke, P', 'Hansper, G', 'Hepp, V', 'Kluge, E E', 'Putzer, A', 'Sommer, J', 'Tittel, K', 'Werner, S', 'Wunsch, M', 'Beuselinck, R', 'Binnie, David M', 'Cameron, W', 'Dornan, Peter J', 'Girone, M', 'Goodsir, S M', 'Martin, E B', 'Morawitz, P', 'Moutoussi, A', 'Nash, J', 'Sedgbeer, J K', 'Spagnolo, P', 'Stacey, A M', 'Williams, M D', 'Ghete, V M', 'Girtler, P', 'Kuhn, D', 'Rudolph, G', 'Betteridge, A P', 'Bowdery, C K', 'Buck, P G', 'Colrain, P', 'Crawford, G', 'Finch, A J', 'Foster, F', 'Hughes, G', 'Jones, R W L', 'Sloan, Terence', 'Whelan, E P', 'Williams, M I', 'Giehl, I', 'Hoffmann, C', 'Jakobs, K', 'Kleinknecht, K', 'Quast, G', 'Renk, B', 'Rohne, E', 'Sander, H G', 'Van Gemmeren, P', 'Zeitnitz, C', 'Aubert, Jean-Jacques', 'Benchouk, C', 'Bonissent, A', 'Bujosa, G', 'Carr, J', 'Coyle, P', 'Diaconu, C A', 'Ealet, A', 'Fouchez, D', 'Konstantinidis, N P', 'Leroy, O', 'Motsch, F', 'Payre, P', 'Talby, M', 'Sadouki, A', 'Thulasidas, M', 'Tilquin, A', 'Trabelsi, K', 'Aleppo, M', 'Antonelli, M', 'Ragusa, F', 'Berlich, R', 'Blum, Walter', 'Büscher, V', 'Dietl, H', 'Ganis, G', 'Gotzhein, C', 'Kroha, H', 'Lütjens, G', 'Lutz, G', 'Männer, W', 'Moser, H G', 'Richter, R H', 'Rosado-Schlosser, A', 'Schael, S', 'Settles, Ronald', 'Seywerd, H C J', 'Saint-Denis, R', 'Stenzel, H', 'Wiedenmann, W', 'Wolf, G', 'Boucrot, J', 'Callot, O', 'Chen, S', 'Cordier, A', 'Davier, M', 'Duflot, L', 'Grivaz, J F', 'Heusse, P', 'Höcker, A', 'Jacholkowska, A', 'Jacquet, M', 'Kim, D W', 'Le Diberder, F', 'Lefrançois, J', 'Lutz, A M', 'Nikolic, I A', 'Schune, M H', 'Serin, L', 'Simion, S', 'Tournefier, E', 'Veillet, J J', 'Videau, I', 'Zerwas, D', 'Azzurri, P', 'Bagliesi, G', 'Bettarini, S', 'Bozzi, C', 'Calderini, G', 'Ciulli, V', ""Dell'Orso, R"", 'Fantechi, R', 'Ferrante, I', 'Giassi, A', 'Gregorio, A', 'Ligabue, F', 'Lusiani, A', 'Marrocchesi, P S', 'Messineo, A', 'Palla, Fabrizio', 'Sanguinetti, G', 'Sciabà, A', 'Sguazzoni, G', 'Steinberger, Jack', 'Tenchini, Roberto', 'Vannini, C', 'Venturi, A', 'Verdini, P G', 'Blair, G A', 'Bryant, L M', 'Chambers, J T', 'Gao, Y', 'Green, M G', 'Medcalf, T', 'Perrodo, P', 'Strong, J A', 'Von Wimmersperg-Töller, J H', 'Botterill, D R', 'Clifft, R W', 'Edgecock, T R', 'Haywood, S', 'Maley, P', 'Norton, P R', 'Thompson, J C', 'Wright, A E', 'Bloch-Devaux, B', 'Colas, P', 'Fabbro, B', 'Kozanecki, Witold', 'Lançon, E', 'Lemaire, M C', 'Locci, E', 'Pérez, P', 'Rander, J', 'Renardy, J F', 'Rosowsky, A', 'Roussarie, A', 'Schuller, J P', 'Schwindling, J', 'Trabelsi, A', 'Vallage, B', 'Black, S N', 'Dann, J H', 'Kim, H Y', 'Litke, A M', 'McNeil, M A', 'Taylor, G', 'Booth, C N', 'Boswell, R', 'Brew, C A J', 'Cartwright, S L', 'Combley, F', 'Kelly, M S', 'Lehto, M H', 'Newton, W M', 'Reeve, J', 'Thompson, L F', 'Affholderbach, K', 'Böhrer, A', 'Brandt, S', 'Cowan, G D', 'Foss, J', 'Grupen, Claus', 'Lutters, G', 'Saraiva, P', 'Smolik, L', 'Stephan, F', 'Apollonio, M', 'Bosisio, L', 'Della Marina, R', 'Giannini, G', 'Gobbo, B', 'Musolino, G', 'Pütz, J', 'Rothberg, J E', 'Wasserbaech, S R', 'Williams, R W', 'Armstrong, S R', 'Charles, E', 'Elmer, P', 'Ferguson, D P S', 'González, S', 'Greening, T C', 'Hayes, O J', 'Hu, H', 'Jin, S', 'McNamara, P A', 'Nachtman, J M', 'Nielsen, J', 'Orejudos, W', 'Pan, Y B', 'Saadi, Y', 'Scott, I J', 'Walsh, J', 'Wu Sau Lan', 'Wu, X', 'Yamartino, J M', 'Zobernig, G']",['Searches for supersymmetry in the photon(s) plus missing energy channels at $\\sqrt{s}$ = 161 GeV and 172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'sparticle, decay modes', 'supersymmetry, symmetry breaking', 'supergravity', 'sparticle, pair production', 'neutrino, pair production', 'photon, electroproduction', 'final state, ((n)photon missing-energy)', 'channel cross section, upper limit', 'mass, neutralino', 'mass, selectron', 'gravitino, LSP', 'neutralino, LSP', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'electron positron --> photon neutrino antineutrino', 'electron positron --> 2photon', '161, 172 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-122', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710009']","['Searches for supersymmetric particles in channels with one or more photons and missing energy have been performed with data collected by the ALEPH detector at LEP. The data consist of 11.1 \\pb\\ at $\\sqrt{s} = 161 ~\\, \\rm GeV$, 1.1 \\pb\\ at 170 \\gev\\ and 9.5 \\pb\\ at 172 GeV. The \\eenunu\\ cross se ction is measured. The data are in good agreement with predictions based on the Standard Model, and are used to set upper limits on the cross sections for anomalous photon production. These limits are compared to two different SUSY models and used to set limits on the neutralino mass. A limit of 71 \\gevsq\\ at 95\\% C.L. is set on the mass of the lightest neutralin o ($\\tau_{\\chi_{1}^{0}} \\leq $ 3 ns) for the gauge-mediated supersymmetry breaking and LNZ models.']",['1997-09-24']
2036,['eng'],"['Crittenden, J A']",['Recent Results from Investigations of Diffractive Vector Meson Production with the ZEUS Detector at HERA'],['Particle Physics - Experimental Results'],"['talk, Egmond aan Zee 1997/05/10', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'vector meson, electroproduction', 'vector meson, photoproduction', 'diffraction, production', 'rho(770)0', 'Phi(1020)', 'J/psi(3100)', 'momentum transfer, high', 'differential cross section, transverse momentum', 'dependence, momentum transfer', 'energy dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709031'],"['We present results from recent investigations of diffractive vector meson production using the ZEUS detector at HERA. These consist of measurements of rho production in the region of photon virtuality 0.25 < Q^2 < 0.85 GeV^2, of rho, phi, and J/psi production for values of the momentum transfer to the proton 0.3 < |t| < 4.0 GeV^2, and of elastic J/psi production both in photoproduction and for Q^2 > 2 GeV^2.']",['1997-09-30']
2037,['eng'],"['Kuhlen, M']",['Low-x hadronic final states at HERA'],['Particle Physics - Experimental Results'],"['review, Madrid 1997/06/18', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, electroproduction', 'p, structure function', 'small-x', 'transverse energy, energy flow', 'rapidity dependence', 'Lipatov equation', 'Altarelli-Parisi equation', 'effect, hadronization', 'charged particle, transverse momentum', 'jet, electroproduction', 'production, small-angle', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709030'],"['Measurements of the hadronic final state at HERA are reviewed, which aim at the investigation of the parton dynamics of the proton at small Bjorken x.']",['1997-09-30']
2038,['eng'],"['Glasman, C']",['Jet Cross Sections and Jet Shapes in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['talk, Madrid 1997/06/18', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, hadroproduction', 'event shape analysis', 'photon, structure function', 'momentum spectrum, parton', 'jet, transverse energy', 'differential cross section, rapidity dependence', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709029'],['Studies on the structure of the photon are presented by means of the extraction of a leading order effective parton distribution in the photon and measurements of inclusive jet differential cross sections in photoproduction. Measurements of the internal structure of jets have been performed and are also presented as a function of the transverse energy and pseudorapidity of the jets.'],['1997-09-29']
2039,['eng'],"['Adams, J']",['Search for Light Gluinos via the Spontaneous Appearance of $\\pi^+ \\pi^-$ Pairs with an 800 GeV/c Proton Beam at Fermilab'],['Particle Physics - Experimental Results'],"['p nucleus, interaction', 'beryllium', 'neutral particle, secondary beam', 'search for, gluino', 'bound state, (gluon gluino)', 'bound state, decay', 'bound state, mass', 'pi, pair production', 'mass spectrum, (pi+ pi-)', 'K0(L), hadronic decay', 'flux, ratio', 'upper limit', 'mass, dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709028'],"['We searched for the appearance of pi+pi- pairs with invariant mass greater than 648 MeV in a neutral beam. Such an observation could signify the decay of a long-lived light neutral particle. We find no evidence for this decay. Our null result severely constrains the existence of an R0 hadron, which is the lightest bound state of a gluon and a light gluino, and thereby also the possibility of a light gluino. Depending on the photino mass, we exclude the R0 in the mass and lifetime ranges of 1.2 -- 4.6 GeV and 2E-10 -- 7E-4 seconds, respectively. (To Appear in Phys. Rev. Lett.)']",['1997-09-26']
2040,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for Unstable Heavy and Excited Leptons in $e^+ e^-$ Collisions at $\\sqrt{s}$ = 170-172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'heavy lepton, pair production', 'heavy lepton, excited state', 'heavy lepton, decay', 'excited state, decay', 'charged current', 'excited state, radiative decay', 'mass, lower limit', 'model, composite', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '170, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709027'],"['We have searched for unstable neutral and charged heavy leptons, N and L^+/-, and for excited states of neutral and charged leptons, nu*, e*, mu* and tau*, in e^+e^- collisions at centre-of-mass energies of 170 and 172 GeV using the OPAL detector at LEP. No evidence for their existence was found. From the analysis of charged-current decays of pair-produced unstable heavy leptons, and of charged-current and photonic decays of pair-produced excited leptons, lower limits on their masses are derived. From the analysis of charged-current and photonic decays of singly-produced excited leptons, upper limits on the ratio of the coupling to the compositeness scale, f/Lambda, are determined for masses up to the kinematic limit.']",['1997-09-24']
2041,['eng'],"['Cheu, E']",['An Expression of Interest to Detect and Measure the Direct CP Violating Decay $K_{L}\\to \\pi 0 \\nu \\overline{\\nu}$ and Other Rare Decays at Fermilab Using the Main Injector'],['Detectors and Experimental Techniques'],"['K0(L), semileptonic decay', 'K0(L), rare decay', 'violation, CP', 'K0, secondary beam', 'calorimeter, electromagnetic', 'cesium, iodine', 'calorimeter, sandwich', 'lead', 'scintillation counter, fibre', 'magnetic spectrometer', 'electronics', 'trigger', 'data acquisition', 'efficiency', 'background', 'numerical calculations', 'counters and detectors, proposed', 'proposed experiment, Fermilab', 'tables', 'K0(L) --> pi0 neutrino antineutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709026'],"[""We, the KAMI (Kaons at the Main Injector) collaboration, express our interest to continue the experimental program of rare kaon decay physics at Fermilab using the Main Injector. KAMI's primary physics goals shall be: 1. The first detection of the rare, direct CP violating decay K_L --> pi0 nu nu_bar and measurement of its branching ratio with an accuracy of 10%, corresponding to a measurement of the CP violating parameter eta with 5% accuracy; and 2. Studies of various other rare decay processes such as K_L --> pi0ee, pi0mumu, pi0mue, pi+pi-e+e-,mu+mu-,e+e-, etc. with sensitivities of approximately 10E-13.""]",['1997-09-24']
2042,['eng'],"['Lee-Franzini, Juliet']",['Hidden and Open Beauty in CUSB'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'electron positron, annihilation', 'upsilon mesons, electroproduction', 'upsilon mesons, decay modes', 'hadron spectroscopy, beauty', 'beautiful meson', 'chi mesons, beauty', 'energy levels, fine structure', 'four-pi-detector, CUSB', 'Cornell CESR Stor', '((2)) ((3))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709025'],['We present a brief history and a summary of the physics results of CUSB at CESR.'],['1997-09-24']
2043,['eng'],"['Kirk, A']",['A search for non-$q\\overline{q}$ mesons in the WA102 experiment at the CERN Omega Spectrometer'],['Particle Physics - Experimental Results'],"['talk, Upton 1997/08/25', 'p p, exclusive reaction', 'diffraction', 'meson, hadroproduction', 'meson, exotic', 'glueball', 'exchange, pomeron', 'exchange, Regge', 'exchange, two-particle', 'mass spectrum, (pi+ pi-)', 'mass spectrum, (2pi+ 2pi-)', 'mass spectrum, (K+ K-)', 'p, transverse momentum', 'transverse momentum, difference', 'f0(1500)', 'f0(1710)', 'postulated particle, f2(1900)', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', '85, 300, 450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709024'],['A study of central meson production as a function of the difference in transverse momentum dPT of the exchanged particles shows that undisputed qqbar mesons are suppressed at small dPT whereas the glueball candidates are enhanced.'],['1997-09-24']
2044,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of triple gauge boson couplings from $W^+ W^-$ production at $\\sqrt{s}$ = 172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'W, electroproduction', 'W, pair production', 'coupling, (3gauge boson)', 'W, leptonic decay', 'W, hadronic decay', 'angular distribution', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> W+ W- anything', '172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709023'],"[""We present measurements of triple gauge boson coupling parameters using data recorded by the OPAL detector at LEP2 at a centre-of-mass energy of 172 GeV. A total of 120 W-pair candidates has been selected in the q q(bar) q q(bar), q q(bar) l nu(bar)_l, and l nu(bar)_l l(bar)' nu_l' decay channels, for an integrated luminosity of 10.4 pb^-1. We use these data to determine several different anomalous coupling parameters using the measured cross-section and the distributions of kinematic variables. We measure alpha_B-phi = 0.35 + 1.29 - 1.07 +/- 0.38, alpha_W-phi = 0.00 + 0.30 - 0.28 +/- 0.11, alpha_W = 0.18 + 0.49 - 0.47 +/- 0.23, Delta(g_1^z) = -0.03 + 0.40 -0.37 +/- 0.14, Delta(kappa_gamma^(HISZ)) = 0.03 + 0.55 - 0.51 +/- 0.20, and Delta(kappa) = 0.03 + 0.49 - 0.46 +/- 0.21. Combining the alpha_W-phi result with our previous result obtained from the 161 GeV data sample we measure alpha_W-phi = -0.08 + 0.28 - 0.25 +/- 0.10. All of these measurements are consistent with the Standard Model.""]",['1997-09-24']
2045,['eng'],"['Aschenauer, E C', 'Bähr, J', 'Gapienko, V A', 'Hoffmann, B', 'Kharchilava, A I', 'Lüdecke, H', 'Nahnhauer, R', 'Shanidze, R']",['Development of scintillating fiber detector technology for high rate particle tracking'],['Detectors and Experimental Techniques'],"['talk, Jerusalem 1997/08/19', 'tracks', 'scintillation counter, fibre', 'spatial resolution', 'radiation, damage', 'radiation, yield', 'optics, absorption', 'magnetic detector, HERA-B', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9710001'],"['The performance of a scintillating fiber detector prototype for tracking under high rate conditions is investigated. A spatial resolution of about100 micron is aimed for the detector. Further demands are low occupancy and radiation hardness up to 1 Mrad/year. Fibers with different radii and different wavelengths of the scintillation light from different producers have been extensively tested concerning light output, attenuation length and radiation hardness, with and without coupling them to light guides of different length and diameter. In a testrun at a 3 GeV electron beam the space dependent efficiency and spatial resolution of fiber bundels were measured by means of two external reference detectors with a precision of 50 micron. The light output profile across fiber roads has been determined with the same accuracy. Different technologies were adopted for the construction of tracker modules consisting of 14 layers of 0.5 mm fibers and 0.7 mm pitch. A winding technology provides reliable results to produce later fiber modules of about 25 cm x 25 cm area. We conclude that on the basis of these results a fiber tracker for high rate conditions can be built.']",['1997-10-03']
2046,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for a massive diphoton resonance at $\\sqrt{s}$ = 91-172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'photon, pair production', 'mass spectrum, two-photon', 'resonance, search for', 'Higgs particle, electroproduction', 'Z0, associated production', 'Higgs particle, radiative decay', 'channel cross section, branching ratio', 'upper limit', 'Higgs particle, mass', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '91-172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709022'],"['A search for the resonant production of high mass photon pairs associated with a leptonic or hadronic system has been performed using a total data sample of 25.7 pb^-1 taken at centre-of-mass energies between 130 GeV and 172 GeV with the OPAL detector at LEP. The observed number of events is consistent with the expected number from Standard Model processes. The observed candidates are combined with search results from sqrt{s} ~ M_Z to place limits on Br(H^0 -> gamma gamma) within the Standard Model for Higgs boson masses up to 77 GeV, and on the production cross section of any scalar resonance decaying into di-photons. Upper limits on Br(H^0 -> gamma gamma) x sigma(e^+e^- -> H^0 Z^0) of 290 - 830 fb are obtained over 40 < M_H < 160 GeV. Type-I two-Higgs-doublet scalars which couple only to gauge bosons are ruled out up to a mass of 76.5 GeV at the 95% confidence level.']",['1997-09-23']
2047,['eng'],"['Breitweg, J']",['Measurement of the Diffractive Structure Function F$_{2}^{D(4)}$ at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon p, interaction', 'diffraction, dissociation', 'cross section, momentum transfer', 'cross section, slope', 'diffraction, structure function', 'Regge poles', 'exchange, pomeron', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709021'],"['This paper presents the first analysis of diffractive photon dissociation events in deep inelastic positron-proton scattering at HERA in which the proton in the final state is detected and its momentum measured. The events are selected by requiring a scattered proton in the ZEUS leading proton spectrometer (LPS) with $\\xl>0.97$, where $\\xl$ is the fraction of the incoming proton beam momentum carried by the scattered proton. The use of the LPS significantly reduces the contamination from events with diffractive dissociation of the proton into low mass states and allows a direct measurement of $t$, the square of the four-momentum exchanged at the proton vertex. The dependence of the cross section on $t$ is measured in the interval $0.073<|t|<0.4$~$\\gevtwo$ and is found to be described by an exponential shape with the slope parameter $b=\\tslopeerr$. The diffractive structure function the momentum fraction of the struck quark with respect to $\\xpom$, and averaged over the $t$ interval $0.073<|t|<\\ftwodfourtmax$~$\\gevtwo$ and the photon virtuality range $5<Q^2<20~\\gevtwo$. In the kinematic range $4 \\times 10^{-4} < fitted with a form $\\xpoma$, yielding $a= \\ftwodfouraerr$. Upon integration over $t$, the structure function $\\ftwod$ is determined in a kinematic range extending to higher $\\xpom$ and lower $\\beta$ compared to our previous analysis; the results are discussed within the framework of Regge theory.']",['1997-09-23']
2048,['eng'],"['Söldner-Rembold, S']",['Photon Structure at LEP'],['Particle Physics - Experimental Results'],"['talk, Ringberg Castle 1997/05/25', 'electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'photon photon, interaction', 'photon, structure function', 'hadron, photoproduction', 'energy flow, hadronic', 'angular correlation', 'jet, hadroproduction', 'final state, (2jet)', 'quark, charm', 'quark, pair production', 'D*(2010)', 'cross section, energy dependence', 'transverse energy, dependence', 'rapidity dependence', 'experimental results', 'CERN LEP Stor', '((4))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709020'],['The structure of the photon is studied in photon interactions at high energies using photons radiated by the electron and positron beams at LEP. The current status of these measurements is reviewed.'],['1997-09-23']
2049,['eng'],"['Ootani, W', 'Minowa, M', 'Watanabe, T', 'Ito, Y', 'Kishimoto, Y', 'Miuchi, K', 'Inoue, Y', 'Ootuka, Y']",['First Results of Tokyo Dark Matter Search with a Lithium Fluoride Bolometer'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'search for, WIMP', 'scattering, WIMP nucleus', 'scattering, WIMP p', 'cross section, mass', 'spin, dependence', 'lithium, fluorine', 'bolometer, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709019'],['The First results of the Tokyo dark matter search programme using a 21-g lithium fluoride bolometer are presented. The background spectrum was measured in the surface laboratory. We derive an exclusion plot for the spin-dependently coupled Weakly Interacting Massive Particles (WIMPs) cross section.'],['1997-09-22']
2050,['eng'],"['Abe, F']",['Measurement of the $B^{0}\\overline{B}^{0}$ oscillation frequency using $\\pi-B$ meson charge-flavor correlations in $p\\overline{p}$ collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'B0, hadroproduction', 'B+, hadroproduction', 'B0 anti-B0, oscillation', 'particle identification, flavor', 'efficiency', 'correlation, (B pi)', 'charge correlation, flavor', 'quark, beauty', 'quark, hadronization', 'decay, B*2(5732)', 'B, semileptonic decay', 'B0, mass difference', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9712004'],"['We present a measurement of the B0 B0-bar oscillation frequency using a flavor tagging method based on correlations of B meson flavor with the charge of other particles produced in p p-bar collisions at sqrt{s} = 1.8 TeV. Such correlations are expected to arise from b quark hadronization and from B** decays. We partially reconstruct B mesons using the semileptonic decays B0 -> lepton D(*)- X. and B+ -> lepton D0-bar X$. From the oscillation frequency, we obtain the mass difference between the two B0 mass eigenstates, Delta m_d = 0.471 {+0.078} {-0.068}(stat) +- 0.034 (syst) hbar ps-1, and measure the efficiency and purity of this flavor tagging method for both charged and neutral B mesons.']",['1997-12-08']
2051,['eng'],"['Adloff, C']",['Low Q$^{2}$ Jet Production at HERA and Virtual Photon Structure'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon p, interaction', 'jet, photoproduction', 'momentum transfer, low', 'differential cross section, transverse energy', 'differential cross section, rapidity dependence', 'photon, resolved', 'quantum chromodynamics', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709017'],"['The transition between photoproduction and deep-inelastic scattering is investigated in jet production at the HERA ep collider, using data collected by the H1 experiment. Measurements of the differential inclusive jet cross-sections dsigep/dEt* and dsigmep/deta*, where Et* and eta* are the transverse energy and the pseudorapidity of the jets in the virtual photon-proton centre of mass frame, are presented for 0 < Q2 < 49 GeV2 and 0.3 < y < 0.6. The interpretation of the results in terms of the structure of the virtual photon is discussed. The data are best described by QCD calculations which include a partonic structure of the virtual photon that evolves with Q2.']",['1997-09-17']
2052,['eng'],"['Brandt, A', 'Erhan, S', 'Kuzucu-Polatoz, A', 'Medinnis, M', 'Ozdes, N', 'Schlein, Peter E', 'Zeyrek, M T', 'Zweizig, J G', 'Chèze, J B', 'Zsembery, J']",['Cross-section measurements of hard diffraction at the S$p\\overline{p}$S- Collider'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'diffraction', 'hard scattering', 'jet, hadroproduction', 'p, leading particle', 'flux, pomeron', 'sum rule, momentum', 'sum rule, violation', 'differential cross section', 'momentum transfer, dependence', 'x-dependence', 'spectrometer, experimental results', 'CERN SPS Coll', '630 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-126', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709015']","['The UA8 experiment previously reported the observation of jets in diffractive events containing leading protons (``hard diffraction""), which was interpreted as evidence for the partonic structure of an exchanged Reggeon, believed to be the \\pom . An analysis of the longitudinal momentum distribution of the 2-jet system in the \\pom -proton rest frame showed that the \\pom\\ structure is ``hard\'\', like $x(1-x)^1$, with an additional ``super-hard\'\' component near $x = 1$. In the present Letter, we report the final UA8 hard-diffractive (jet) cross section results and their interpretation. After corrections, the fraction of single diffractive events with mass from 118 to 189~GeV that have two scattered partons, each with $\\etj > 8$~GeV, is in the range 0.002 to 0.003 (depending on \\xp ). We determine the product, $fK$, of the fraction by which the \\pom \'s momentum sum rule is violated and the normalization constant of the \\pom -Flux-Factor of the proton. For a pure gluonic- or a pure $q\\bar{q}$-\\pom , respectively: $fK$ = ($0.30 \\pm 0.03 \\pm 0.09$) and ($0.56 \\pm 0.05 \\pm 0.17$) GeV$^{-2}$.']",['1997-10-02']
2053,['eng'],"['Cvach, J']",['Photoproduction of hadrons at HERA'],['Particle Physics - Experimental Results'],"['talk, Ringberg Castle 1997/05/25', 'positron p, colliding beams', 'positron p, inclusive reaction', 'exchange, one-photon', 'hadron, photoproduction', 'charged particle, spectra', 'K0(S), hadronic decay', 'Lambda, hadronic decay', 'jet, photoproduction', 'channel cross section, transverse momentum', 'rapidity dependence', 'energy dependence', 'momentum transfer, dependence', 'quantum chromodynamics, perturbation theory', 'fragmentation function', 'mass spectrum, two-photon', 'photon, direct production', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709014'],['New experimental results from photoproduction of hadrons at HERA are reviewed.'],['1997-09-17']
2054,['eng'],"['Aitala, E M']","['Search for the pentaquark via the $P^{0}_{\\overline{c}s} \\to \\phi,\\pi,p$ decay']",['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'search for, multiquark', 'bound state, (4quark antiquark)', 'decay, multiquark', 'mass spectrum, (Phi(1020) p pi)', 'mass, multiquark', 'channel cross section, branching ratio', 'upper limit', 'experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709013'],"['We report results of the first search for the pentaquark P_{{c bar}s} which is predicted to be a doublet of states: P^0_{{c bar}s}=({c bar} s u u d) and P^-_{{c bar}s}=({c bar} s d d u). A search was made for the decay P^0_{{c bar}s} --> phi,pi,p in data from Fermilab experiment E791, in which 500 GeV/c pi^- beam interacted with nuclear targets. We present upper limits at 90% confidence level for the ratio of cross section times branching fraction of this decay to that for the decay D_s --> phi,pi. The upper limits are 0.031 and 0.063 for M(P^0_{{c bar}s}) = 2.75 and 2.86 GeV/c^2, respectively, assuming a P^0_{{c bar}s} lifetime of 0.4 ps.']",['1997-09-16']
2055,['eng'],"['Alam, M S']",['Measurement of the Branching Fractions of $\\Lambda_{c}^{+}\\to p\\overline{K}n(\\pi)$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Lambda/c+, electroproduction', 'Lambda/c+, hadronic decay', 'Lambda/c+, branching ratio', 'mass spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Lambda/c+ --> p K- pi+ pi0', 'Lambda/c+ --> p anti-K0', 'Lambda/c+ --> p anti-K0 pi+ pi-', 'Lambda/c+ --> p anti-K0 pi0', 'Lambda/c+ --> p K- pi+', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709012'],"['Using data recorded by the CLEO-II detector at CESR, we report new measurements of the branching fractions for the decays of the charmed baryon $p\\bar{K}^0\\pi^0$, all measured relative to $pK^-\\pi^+$. The relative branching fractions are $0.67\\pm0.04\\pm0.11, 0.46\\pm0.02\\pm0.04,0.52\\pm0.04\\pm0.05$, and $0.66\\pm0.05\\pm0.07$ respectively.']",['1997-09-11']
2056,['ger'],"['Hadig, T']",['Untersuchungen zur Jet-Parton-Korrelation in der tief-inelastischen Streuung'],['Particle Physics - Experimental Results'],"['thesis', 'electron p, colliding beams', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'jet, multiplicity', 'jet, particle identification', 'correlation, (jet parton)', 'strong interaction, coupling constant', 'gluon, momentum spectrum', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709011'],"['The jet parton correlation has been studied for different cut scenarios and various jet algorithms. These migrations are getting important for measuring the strong coupling constant alpha_s and the NLO gluon density g(xi,Q^2) from jet rates in DIS at HERA.']",['1997-09-11']
2057,['eng'],"['Burrows, P N']",['Results on $\\alpha_{s}$ and QCD from (and above) the $Z^{0}$'],['Particle Physics - Experimental Results'],"['review, Bristol 1997/06/25', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, multiple production', 'final state, (3jet)', 'final state, (4jet)', 'quark, jet', 'gluon, jet', 'strong interaction, coupling constant', 'tau, semileptonic decay', 'event shape analysis', 'fragmentation function', 'dependence, flavor', 'scaling, violation', 'angular correlation', 'color', 'operator, Casimir', 'experimental results', '((3)) ((4)) ((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709010'],['Measurements of alpha_s from e+e- annihilation experiments are reviewed and compared with measurements from other processes. Highlights are presented of recent QCD studies in e+e- annihilation at the Z0 resonance.'],['1997-09-10']
2058,['eng'],"['Demarteau, M']",['Electroweak Results from Hadron Colliders'],['Particle Physics - Experimental Results'],"['talk, Capri 1997/06/22', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'photon, associated production', 'intermediate boson, pair production', 'intermediate boson, leptonic decay', 'W, mass', 'coupling, (3gauge boson)', 'Drell-Yan process', 'channel cross section, branching ratio', 'differential cross section, mass', 'model, composite', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709009'],['A review of recent electroweak results from hadron colliders is given. Properties of the W and Z gauge bosons using final states containing electrons and muons based on large integrated luminosities are presented. The emphasis is placed on the measurement of the mass of the W boson and the measurement of trilinear gauge boson couplings.'],['1997-09-09']
2059,['eng'],"['Maggiora, A']",['Hyperon polarization and vector meson production at 2.85 GeV'],['Particle Physics - Experimental Results'],"['talk, Nanjing 1997/08/16', 'p p, inclusive reaction', 'p, polarized beam', 'hyperon, hadroproduction', 'Lambda', 'Sigma', 'Sigma(1385)', 'K+, associated production', 'hyperon, polarization', 'hyperon, hadronic decay', 'vector meson, hadroproduction', 'vector meson, hadronic decay', 'Phi(1020)', 'omega(783)', 'Iizuka-Okubo-Zweig rule, violation', 'p, strangeness', 'quark, sea', 'analyzing power', 'angular distribution', 'mass spectrum', 'experimental results', 'Saclay PS', 'p p --> hyperon p K+', 'p p --> 2p vector meson', '2.50, 2.85 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709008'],"['Surprisingly large polarization in hyperon production by unpolarized proton beam has been known since long time. Huge inclusive hyperon polarization data are available in literature, few data are disponible on spin observables and none on exclusive hyperon measurements. Evidence of relevant violation of the OZI rule in several reactions are also shown in recent measurements. These two items, connected together by the hypothesis of existence of a sizeable $q \\bar{q}$ sea in the nucleon, can be studied using the DISTO is a spectrometer installed in the polarized proton beam of the Saturne accelerator in Saclay. The compact experimental set-up is designed to detect four or more charged particles signaling $\\Lambda$, $\\Sigma^{0}$, $Y^{*}$ or $\\phi$ production in An outline of the physical motivations and a brief description of the experimental apparatus is given as well as some preliminary results from the first production running']",['1997-09-09']
2060,['eng'],"['Lee-Franzini, Juliet', 'Franzini, P']",['CP Violation in the K-System'],['Particle Physics - Experimental Results'],"['review, Moscow 1997/02/18', 'violation, CP', 'K0 anti-K0, interference', 'K0, mass difference', 'K, rare decay', 'K0, hadronic decay', 'K0, semileptonic decay', 'K0, radiative decay', 'K0, regeneration', 'K0, beam', 'K0(L)', 'K0(S)', 'correlation', 'electron positron, annihilation', 'Phi(1020), electroproduction', 'anti-p p, annihilation', 'K, pair production', 'invariance, CPT', 'validity test', 'experimental results', 'proposed experiment', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709007'],"['CP violation in the K system is pedagogically reviewed. We discuss its manifestations in the neutral K meson systems, in rare K meson decays and in decays of charged K mesons. Results from classical experiments, and perspectives for upcoming experiments are included. We also briefly discuss the possibility of CPT tests.']",['1997-09-09']
2061,['eng'],"['Xing, Z']",['CP-violating Parameter $\\epsilon_B$ in $B_{d}^0-\\overline{B}^{0}_{d}$ Mixing'],['Particle Physics - Experimental Results'],"['B0 anti-B0, interference', 'parametrization', 'violation, CP', 'Upsilon(10570), hadronic decay', 'B0, pair production', 'B0, semileptonic decay', 'coherence', 'charge, dilepton', 'B0, hadronic decay', 'final state, (J/psi(3100) K)', 'decay, asymmetry', 'time dependence', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709005'],"['The parameter \\epsilon_B, analogous to \\epsilon_K in the neutral kaon system, has been used in some literature to describe CP violation in B^0_d-\\bar{B}^0_d mixing. We estimate the magnitude of \\epsilon_B within the standard model and obtain 0.16 \\leq |\\epsilon_B| \\approx {\\rm Im} \\epsilon_B \\leq 0.70 by use of current data. Hence ignorance of the |\\epsilon_B|^2 correction to some CP asymmetries of weak B_d decays may lead to large uncertainties and even misleading results. In particular, we find that the reported CLEO and OPAL constraints on |{\\rm Re}\\epsilon_B| should be modified by multiplying a factor (1+|\\epsilon_B|^2) \\approx 1.0 \\sim 1.5.']",['1997-09-09']
2062,['eng'],"['Abe, F']",['Properties of Jets in W Boson Events from $1.8 TeV \\overline{p}p$ Collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'W, leptonic decay', 'jet, associated production', 'jet, multiplicity', 'channel cross section, multiplicity', 'transverse energy, energy spectrum', 'mass spectrum, (2jet)', 'angular correlation, (2jet)', 'quantum chromodynamics, perturbation theory', 'gluon, radiation', 'fragmentation, parton', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W (n)jet anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709016'],['We present a study of events with W bosons and hadronic jets produced in pbar p collisions at a center of mass energy of 1.8 TeV. The data consist of 51400 W^+/- -> e^+/- nu decay candidates from 108 pb^-1 of integrated luminosity collected with the CDF detector at the Tevatron Collider. The cross sections and jet production properties have been measured for W + \\geq 1 to \\geq 4 jet events. The data are compared to predictions of leading order QCD matrix element calculations with added gluon radiation and simulated fragmentation.'],['1997-09-17']
2063,['eng'],"['Adloff, C']",['Measurement of the Inclusive Di-Jet Cross Section in Photoproduction and Determination of an Effective Parton Distribution in the Photon'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, photoproduction', 'final state, (2jet)', 'photon, structure function', 'transverse momentum, parton', 'differential cross section, transverse energy', 'cross section, factorization', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709004'],['The double-differential inclusive di-jet cross section in photoproduction processes is measured with the H1 detector at HERA. The cross section is determined as a function of the average transverse jet energy E_T^jets for ranges of the fractional energy x_gamma^jets of the parton from the photon side. An effective leading order parton distribution in the photon is determined at large parton fractional energies for scales between 80<p_T^2<1250 GeV^2. The measurement is compatible with the logarithmic scale dependence that is predicted by perturbative QCD.'],['1997-09-08']
2064,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for the Standard Model Higgs Boson in $e^+ e^-$ Collisions at $\\sqrt{s}$ = 161-172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Higgs particle, search for', 'Higgs particle, mass', 'lower limit', 'Z0, associated production', 'Higgs particle, decay modes', 'Z0, decay modes', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161, 170, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709003'],"['This paper describes a search for the Standard Model Higgs boson using data from e^+e^- collisions collected at center-of-mass energies of 161, 170 and 172 GeV by the OPAL detector at LEP. The data collected at these energies correspond to integrated luminosities of 10.0, 1.0 and 9.4 pb^-1, respectively. The search is sensitive to the main final states from the process in which the Higgs boson is produced in association with a fermion anti-fermion pair, namely four jets, two jets with missing energy, and two jets produced together with a pair of electron, muon or tau leptons. One candidate event is observed, in agreement with the Standard Model background expectation. In combination with previous OPAL searches at center-of-mass energies close to the Z^0 resonance and the revised previous OPAL searches at 161 GeV, we derive a lower limit of 69.4 GeV for the mass of the Standard Model Higgs boson at the 95% confidence level.']",['1997-09-08']
2065,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Multi-photon final states in $e^+ e^-$ collisions at $\\sqrt{s}$ = 130-172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'photon, multiple production', 'photon, multiplicity', 'quantum electrodynamics, Lambda parameter', 'angular distribution', 'coupling, (positron electron photon)', 'search for, new interaction', 'resonance, search for', 'channel cross section', 'electron, excited state', 'mass, lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2photon', 'electron positron --> 3photon', '130-172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709002'],"['The process e^+e^- -> gamma gamma (gamma) is studied using data recorded with the OPAL detector at LEP. The data sample corresponds to a total integrated luminosity of 25.38 pb^{-1} taken at centre-of-mass energies of 130-172 GeV. The measured cross-sections agree well with the expectation from QED. In a combined fit using data from all centre-of-mass energies, the angular distribution is used to obtain improved limits on the cut-off parameters: Lambda_+ > 195 GeV and Lambda_- > 210 GeV (95% CL). In addition, limits on non-standard e^+e^-gamma couplings and contact interactions, as well as a 95% CL mass limit for an excited electron, M_{e^*} > 194 GeV for an e^+e^-gamma coupling kappa = 1, are determined.']",['1997-09-08']
2066,['eng'],"['García-Abia, P']",['Spin analysis of the process $e^{+}e^{-}\\rightarrow\\tau^{+}\\tau^{-}$ at LEP'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1997/04/21', 'electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, decay modes', 'tau, polarization', 'polarization, longitudinal', 'spin, correlation', 'lepton, universality', 'Weinberg angle', 'electroweak interaction', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709001'],"['Using the data collected by the four experiments at LEP during 1990-1994, a precise measurement of the tau longitudinal polarisation (P_tau) has been performed, as well as the measurement of the transverse-transverse and transverse-normal tau spin correlations. From the P_tau measurement, assuming lepton universality of the neutral currents, the effective weak mixing angle has been determined to be sin(theta_W) = 0.2325 +- 0.0006. The Standard Model predictions are consistent with the measured results.']",['1997-09-04']
2067,['eng'],"['Aitala, E M']",['Asymmetries Between the Production of $D_{s}^{-}$ and $D_{s}^{+}$ Mesons from 500 GeV/c $\\pi^{-}$ Nucleon Interactions as Functions of $x_F$ and square of $p_{t}^{2}$'],['Particle Physics - Experimental Results'],"['pi- nucleon, inclusive reaction', 'D/s, hadroproduction', 'D, hadroproduction', 'charge, asymmetry', 'x-dependence', 'transverse momentum, dependence', 'model, hadronization', 'string model, fragmentation', 'string model, coalescence', 'experimental results', 'Batavia TEVATRON PS', 'pi- nucleon --> D/s anything', 'pi- nucleon --> D anything', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708040'],"['This paper presents measurements of the production of Ds- mesons relative to Ds+ mesons as functions of x_F and square of p_t for a sample of 2445 Ds decays to phi pi. The Ds mesons were produced in Fermilab experiment E791 with 500 GeV/c pi- mesons incident on one platinum and four carbon foil targets. The acceptance-corrected integrated asymmetry in the x_F range -0.1 to 0.5 for Ds+- mesons is 0.032 +- 0.022 +- 0.022, consistent with no net asymmetry. The results, as functions of x_F and square of p_t, are compared to predictions and to the large production asymmetry observed for D+- mesons in the same experiment. These comparisons support the hypothesis that production asymmetries come from the fragmentation process and not from the charm quark production itself.']",['1997-08-29']
2068,['eng'],"['Battiston, R']",['The alpha magnetic spectrometer (AMS)'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1997/05/20', 'astrophysics', 'search for, missing-mass', 'search for, antimatter', 'violation, CP', 'time reversal, violation', 'K0(L), decay', 'B, decay', 'WIMP, annihilation', 'positron', 'helium, antinucleus', 'elements, cosmic radiation', 'photon', 'magnetic spectrometer, satellite', 'semiconductor detector', 'scintillation counter, time-of-flight', 'proposed experiment', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708039'],"['The AMS is a state of the art detector for extraterrestrial study of antimatter, matter and missing matter. After a precursor flight on STS91 in May 1998, AMS will be installed on the International Space Station where it will operate for three years. In this paper the AMS experiment is described and is physics potential reviewed.']",['1997-08-28']
2069,['eng'],"['Fernández, P']",['Determinations of $\\alpha_s$ using JADE data of $e^{+}e^{-}$ Annihilations at $\\sqrt{s}$ = 22 to 44 GeV'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1997/07/03', 'electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'jet, electroproduction', 'event shape analysis', 'quantum chromodynamics, perturbation theory', 'strong interaction, coupling constant', 'energy dependence', 'magnetic detector, JADE', 'experimental results', 'DESY PETRA Stor', '22, 35, 44 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708037'],"['Data recorded by the JADE experiment at the PETRA e^+e^- collider were used to measure distributions of new event shape observables. The distributions were compared with resummed QCD calulations (O(alpha_s^2)+NLLA), and the strong coupling constant alpha_s was determined at \\sqrt{s}= 22, 35 and 44 GeV. The results are in agreement with previous combined results of PETRA but have smaller uncertainties. Together with corresponding data from LEP, the energy dependence of alpha_s is significantly tested and is found to be in good agreement with the QCD expectation.']",['1997-08-27']
2070,['eng'],"['Biebel, O']",['Combined QCD analysis of $e^{+} e^{-}$ data at $\\sqrt{s}$ = 14 to 172 GeV'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1997/07/03', 'electron positron, annihilation', 'hadron, multiple production', 'jet, electroproduction', 'event shape analysis', 'quantum chromodynamics, perturbation theory', 'correction, higher-order', 'strong interaction, coupling constant', 'energy dependence', 'effect, hadronization', 'numerical calculations, interpretation of experiments', '14-172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708036'],"['A study of the energy dependence of event shape observables is presented. The strong coupling constant \\alpha_s has been determined from the mean values of six event shape observables. Power corrections, employed for the measurement of']",['1997-08-27']
2071,['eng'],"['Anastassov, A']",['Investigation of Semileptonic $B$ Meson Decay to P-Wave Charm Mesons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B-, semileptonic decay', 'charmed meson, production', 'D1(2420), hadronic decay', 'D*2(2460), hadronic decay', 'D*(2010)', 'B-, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B- --> D1(2420) lepton neutrino', 'B- --> D*2(2460) lepton neutrino', 'D1(2420) --> D*(2010) pi-', 'D*2(2460) --> D*(2010) pi-', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708035'],"['We have studied semileptonic $B$ meson decays with a P-wave charm meson in the final state using 3.29 x 10^6 B\\bar{B} events collected by the CLEO~II detector at the Cornell Electron-positron Storage Ring. We find a value for the exclusive semileptonic product branching fraction: Br(B^- -> D_1^0 l^- and an upper limit for Br(B^- -> D_2^{*0} l^- \\bar{\\nu}) x Br(D_2^{*0} -> D^{*+}\\pi^-) < 0.16%$ (90% C.L.). These results indicate that at least 20% of the total B^- semileptonic rate is unaccounted for by the observed exclusive decays, B^- -> D^0 l^- \\bar{\\nu}, B^- -> D^{*0} l^- \\bar{\\nu}, B^- -> D_1^0 l^-']",['1997-08-27']
2072,['eng'],"['Movilla-Fernández, P A', 'Biebel, O', 'Bethke, Siegfried', 'Kluth, S', 'Pfeifenschneider, P']",['A Study of Event Shapes and Determinations of $\\alpha_s$ using data of $e^{+}e^{-}$ Annihilations at $\\sqrt{s}$ = 22 to 44 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'hadron, multiple production', 'event shape analysis', 'yield, (2jet)', 'quantum chromodynamics, perturbation theory', 'correction, higher-order', 'strong interaction, coupling constant', 'energy dependence', 'magnetic detector, JADE', 'experimental results', 'DESY PETRA Stor', '22-44 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708034'],"['Data recorded by the JADE experiment at the PETRA $e^+e^-$ collider were used to measure the event shape observables thrust, heavy jet mass, wide and total jet broadening and the differential 2-jet rate in the Durham scheme. For the latter three observables, no experimental results have previously been presented at these energies. The distributions were compared with resummed QCD calulations ($O(\\alpha_s^2)$+NLLA), and the strong coupling constant results, \\alpha_s(22 GeV) = 0.161 ^{+0.016}_{-0.011}, \\alpha_s(35 GeV) = 0.143 ^{+0.011}_{-0.007}, \\alpha_s(44 GeV) = 0.137 ^{+0.010}_{-0.007}, are in agreement with previous combined results of PETRA albeit with smaller uncertainties. Together with corresponding data from LEP, the energy dependence of $\\alpha_s$ is significantly tested and is found to be in good agreement with the QCD expectation. Similarly, mean values of the observables were compared to analytic QCD predictions where hadronisation effects are absorbed in calculable power corrections.']",['1997-08-26']
2073,['eng'],"['Nemati, B']",['Search for Color-Suppressed $B$ Hadronic Decay Processes with CLEO'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'Upsilon(10570), hadronic decay', 'B0, pair production', 'B0, hadronic decay', 'B0, decay modes', 'final state, two-particle', 'D*(2010)', 'energy spectrum', 'B0, branching ratio', 'anti-B0, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708033'],"[""Using 3.1 fb$^{-1}$ of data accumulated at the $\\Upsilon$(4S) by the CLEO-II detector, corresponding to 3.3 million $B\\bar{B}$ pairs, we have searched for the color-suppressed $B$ hadronic decay processes: $\\bar{B}^0 \\to D^0 (D^{*0}) X^0$, where $X^0$ is a light neutral meson $\\pi^0$, $\\rho^0$, $\\eta$, $\\eta'$ or $\\omega$. No obvious signal is observed. We set 90 \\% C.L. upper limits on these modes, varying from $1.2 \\times 10^{-4}$ for $\\bar{B}^0 \\to D^0 \\pi^0$ to $1.9 \\times 10^{-3}$ for $\\bar{B}^0 \\to D^{*0} \\eta'$.""]",['1997-08-26']
2074,['eng'],"['Blackett, G R', 'Danyo, K', 'Handler, T', 'Pisharody, M', 'Condo, G T']",['The Photoproduction of the $b_{1}(1235)\\pi$ System'],['Particle Physics - Experimental Results'],"['photon p, exclusive reaction', 'pi, multiple production', 'Delta(1232)++, photoproduction', 'b1(1235), associated production', 'b1(1235), mass', 'b1(1235), width', 'resonance, search for', 'mass spectrum, (omega(783) pi)', 'mass spectrum, (b1(1235) pi)', 'bubble chamber(hydrogen), experimental results', 'SLAC Lab', 'photon p --> p 2pi+ 2pi- pi0', 'photon p --> b1(1235) Delta(1232)++', '19.3 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708032'],"['We report on a study of the reaction, $\\gamma p \\to p significant feature of this reaction is $\\Delta^{++}$ production which occurs with a cross section of $0.6\\pm 0.1 \\mu$b. An upper limit is set for the cross section for the reaction, $\\gamma p \\to \\Delta^{++}b_1^-(1235)$, and a search is made for resonances decaying to $b_1^\\pm\\pi^\\mp$.']",['1997-08-22']
2075,['eng'],"['Adler, Stephen Louis']",['Evidence for the Decay $K^{+} \\rightarrow \\pi^{+}\\nu\\overline{\\nu}$'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'K+, rare decay', 'K+, branching ratio', 'neutrino, pair production', 'experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708031'],"['An event consistent with the signature expected for the rare kaon decay K+ --> pi+ nu anti-nu has been observed. In the pion momentum region examined, 211<P<230 MeV/c, the backgrounds are estimated to contribute 0.08 +/- 0.03 events. If the event is due to K+ --> pi+ nu anti-nu, the branching ratio is (4.2 +9.7/-3.5) x E-10.']",['1997-08-21']
2076,['eng'],"['Marti i Garcia, S', 'Fuster, J A', 'Cabrera, S']",['Experimental determination of the $m_b(M_Z)$ in DELPHI'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1997/07/03', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'gluon, associated production', 'mass, beauty', 'energy dependence', 'renormalization group', 'final state, (3jet)', 'particle identification, flavor', 'magnetic detector, DELPHI', 'experimental results', 'CERN LEP Stor', 'Z0 --> quark antiquark', 'Z0 --> quark antiquark gluon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708030'],"['The running mass of the b quark as defined in the MS-bar renormalization scheme, m_b, was measured at the M_Z scale using 2.8 million hadronic Z^0 decays collected by the DELPHI experiment at LEP. The result is m_b(M_Z) = 2.67 +- 0.25 (stat.) +- 0.34 (frag.) +- 0.27(theo.) GeV/c^2 which differs from that obtained at the Upsilon scale, by m_b(M_\\Upsilon/2)-m_b(M_Z) = 1.49 +- 0.52 GeV/c^2. This measurement, performed far from the $b\\bar{b}$ production threshold, provides the first experimental observation of the running of the quark masses.']",['1997-08-21']
2077,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Multiplicity distributions of gluon and quark jets and tests of QCD analytic predictions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'jet, electroproduction', 'quark, jet', 'gluon, jet', 'final state, (3jet)', 'charged particle, multiplicity', 'multiplicity, moment', 'quantum chromodynamics, validity test', 'correction, higher-order', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708029'],"['Gluon jets are identified in e+e- hadronic annihilation events by tagging two quark jets in the same hemisphere of an event. The gluon jet is defined inclusively as all the particles in the opposite hemisphere. Gluon jets defined in this manner have a close correspondence to gluon jets as they are defined for analytic calculations, and are almost independent of a jet finding algorithm. The charged particle multiplicity distribution of the gluon jets is presented, and is analyzed for its mean, dispersion, skew, and curtosis values, and for its factorial and cumulant moments. The results are compared to the analogous results found for a sample of light quark (uds) jets, also defined inclusively. We observe differences between the mean, skew and curtosis values of gluon and quark jets, but not between their dispersions. The cumulant moment results are compared to the predictions of QCD analytic calculations. A calculation which includes next-to-next-to-leading order corrections and energy conservation is observed to provide a much improved description of the data compared to a next-to-leading order calculation without energy conservation. There is agreement between the data and calculations for the ratios of the cumulant moments between gluon and quark jets.']",['1997-08-20']
2078,['eng'],"['Amsler, Claude']",['Proton-Antiproton Annihilation and Meson Spectroscopy with the Crystal Barrel'],['Particle Physics - Experimental Results'],"['review, experimental results', 'anti-p p, annihilation', 'at rest', 'partial wave', 'meson, hadroproduction', 'meson, multiple production', 'meson, hadron spectroscopy', 'photon, associated production', 'meson, hadronic decay', 'meson, radiative decay', 'gauge boson, search for', 'spin, parity', 'meson, multiplicity', 'postulated particle, a0(1450)', 'f0(1370)', 'f0(1500)', 'postulated particle, f2(1565)', 'f1(1420)', 'glueball', 'four-pi-detector', 'CERN LEAR', 'bibliography', '0 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708025'],"['This report reviews the achievements of the Crystal Barrel experiment at the Low Energy Antiproton Ring (LEAR) at CERN. During seven years of operation Crystal Barrel has collected very large statistical samples in pbarp annihilation, especially at rest and with emphasis on final states with high neutral multiplicity. The measured rates for annihilation into various two-body channels and for electromagnetic processes have been used to test simple models for the annihilation mechanism based on the quark internal structure of hadrons. From three-body annihilations three scalar mesons, a0(1450), f0(1370) and f0(1500) have been established in various decay modes. One of them, f0(1500), may be identified with the expected ground state scalar glueball.']",['1997-08-19']
2079,['eng'],"['Adloff, C']",['Inclusive Measurement of Diffractive Deep-inelastic ep Scattering'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'electron p, deep inelastic scattering', 'rapidity, gap', 'diffraction, structure function', 'exchange, pomeron', 'exchange, Regge', 'quantum chromodynamics', 'structure function, pomeron', 'Altarelli-Parisi equation', 'momentum spectrum, parton', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708016'],"['A measurement is made of the cross section for the process ep --> eXY in deep-inelastic scattering with the H1 detector at HERA. The cross section is presented in terms of a differential structure function F_2^D(3)(x_P,beta,Q^2) of the proton over the kinematic range 4.5 < Q^2 < 75 GeV^2. The dependence of F_2^D(3) on x_P is found to vary with beta, demonstrating that a factorisation of F_2^D(3) with a single diffractive flux independent of beta and Q^2 is not tenable. An interpretation in which a leading diffractive exchange and a subleading reggeon contribute to F_2^D(3) reproduces well the x_P dependence of F_2^D(3) with values for the pomeron and subleading reggeon intercepts of alpha_P(0)=1.203 \\pm 0.020(stat.)\\pm 0.013(sys.) ^{+0.030}_{-0.035}(model} and alpha_reg(0)=0.50\\pm 0.11(stat.)\\pm 0.11 (sys.}^{+0.09}_{-0.10} (model), respectively. A fit is performed of the data using a QCD motivated model, in which parton distributions are assigned to the leading and subleading exchanges. In this model, the majority of the momentum of the pomeron must be carried by gluons in order for the data to be well described.']",['1997-08-18']
2080,['eng'],[],['Measurement of $R_{b}$ using a Vertex Mass Tag'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Z0, branching ratio', 'quark, beauty', 'quark, pair production', 'particle identification, beauty', 'semiconductor detector, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708015'],"['We report a new measurement of Rb = Gamma(Z0->b-bbar) / Gamma(Z0->hadrons) using a double tag technique, where the b hemisphere selection is based on the reconstructed mass of the B hadron decay vertex. The measurement was performed using a sample of 130k hadronic Z0 events, collected with the SLD at the SLC. The method utilizes the 3-D vertexing abilities of the CCD pixel vertex detector and the small stable SLC beams to obtain a high b-tagging efficiency and purity. We obtain Rb=0.2142+/-0.0034(stat.)+/-0.0015(syst.)+/-0.0002(R_c).']",['1997-08-18']
2081,['eng'],"['Abe, F']",['Search for First Generation Leptoquark Pair Production in $p\\overline{p}$ Collisions at $\\Sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'search for, leptoquark', 'scalar particle, leptoquark', 'leptoquark, pair production', 'decay, leptoquark', 'channel cross section, mass', 'upper limit', 'mass, leptoquark', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2leptoquark anything', 'leptoquark --> quark electron', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708017'],['We present a search for first generation leptoquark with 110pb^1 of data collected with the CDF detector. We set 95% C.L. cross section limits as a function of the leptoquark mass.'],['1997-08-18']
2082,['eng'],"['Acharya, B S']",['Scintillation Counters for the D0 Muon Upgrade'],['Detectors and Experimental Techniques'],"['muon, counters and detectors', 'upgrade', 'scintillation counter, fibre', 'optics, transformation', 'photoelectron, amplifier', 'performance', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9709018'],"['We present the results of an upgrade to the D0 muon system. Scintillating counters have been added to the existing central D0 muon system to provide rejection for cosmic ray muons and out-of-time background, and to provide additional fast timing information for muons in an upgraded Tevatron. Performance and results from the 1994-1996 Tevatron run are presented.']",['1997-09-19']
2083,['eng'],"['Dorigo, T']",['Search For New Particles in Multijet Final States at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1997/06/05', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'jet, multiplicity', 'new particle, search for', 'Higgs particle', 'sparticle', ""W'"", ""Z'"", 'quark, excited state', 'mass, upper limit', 'mass, lower limit', 'quark, truth', 'quark, pair production', 'mass, truth', 'mass spectrum, (2jet)', 'quantum chromodynamics, validity test', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708026'],"['We present the latest results of the searches for new particles in hadronic final states performed in proton-antiproton collisions at a center of mass energy of 1.8 TeV. The large data samples collected with the CDF and D0 detectors at the Tevatron collider between 1992 and 1995 allow searches for low cross section phenomena in dijet and multijet events, despite the hindrance of the high background from normal QCD processes. However, no signal for new physics is found, and the data show good agreement with QCD. Limits on the mass and on the cross section of the searched states can thus be set.']",['1997-08-19']
2084,['eng'],"['Bolton, T']",['Determining the CKM Parameter $V_{cd}$ from $\\nu N$ Charm Production'],['Particle Physics - Experimental Results'],"['neutrino nucleon, inclusive reaction', 'electron positron, annihilation', 'production, charm', 'muon, pair production', 'model, quark parton', 'quark, hadronization', 'charmed particle, semileptonic decay', 'charmed particle, branching ratio', 'Kobayashi-Maskawa angle', 'unitarity', 'fragmentation function, charm', 'quantum chromodynamics, perturbation theory', 'nuclear physics, effect', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708014'],"['The formalism for extracting the CKM parameter $V_{cd}$ from $\\nu N$ production of charm is discussed in some detail. The various model assumptions needed are clearly pointed out. A direct determination from neutrino induced dimuon production requires $\\nu N$ charm production data, $% \\nu N$ charm hadronization data, and the semi-muonic branching ratios for charmed hadrons. Hadronization data from FNAL E531 is re-analyzed to take advantage of better-determined properties of the charmed hadrons. A small bias in the original published result is removed. Neutrino induced charm fragmentation is compared to $e^{+}e^{-}$ charm fragmentation functions; the data are consistent with a common hadronization scheme. An updated value of the mean semi-muonic branching ratio for charmed hadrons produced in $\\nu N$ scattering for $E_\\nu >30$ GeV is obtained. This value is used to determine $% V_{cd}$ and its associated uncertainties. Prospects for improving the $% V_{cd} $ measurement to test the unitarity limit of the CKM matrix are described.']",['1997-08-15']
2085,['eng'],"['Breitweg, J']",['Observation of Isolated High-$E_{T}$ Photons in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'photon, direct production', 'transverse energy, high', 'jet, associated production', 'angular distribution', 'transverse energy, spectra', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> jet positron photon anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708038'],"['Events containing an isolated prompt photon with high transverse energy, together with a balancing jet, have been observed for the first time in photoproduction at HERA.The data were taken with the ZEUS detector, in a incoming photon energy participating in the production of the prompt photon and the jet, $x_\\gamma$, shows a strong peak near unity, consistent with LO QCD Monte Carlo predictions. In the transverse energy and pseudorapidity range $5\\le \\eTg < 10$ GeV, $-0.7 \\le \\eta^\\gamma < 0.8$, $\\eTj\\ge 5$ GeV, and $-1.5\\le \\eta^{jet}\\le 1.8$, with $\\xgO > 0.8,$ the measured cross section is $15.3 \\pm 3.8 \\pm 1.8 pb$, in good agreement with a recent NLO calculation.']",['1997-08-28']
2086,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lamarche, F', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Van den Plas, D', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Polarization and forward-backward asymmetry of $\\Lambda$ baryons in hadronic $Z^0$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'Lambda, polarization', 'polarization, longitudinal', 'angular distribution, asymmetry', 'model, hadronization', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-104', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708027']","['The longitudinal polarization, the transverse polarization, and the forward-backward asymmetry of Lambda baryons have been measured using a sample of 4.34 million hadronic Z^0 decays collected with the OPAL detector at LEP between 1990 and 1995. These results are important as an aid to the understanding of hadronization mechanisms. Significant longitudinal polarization has been observed at intermediate and high momentum. For x_E = 2 E_{Lambda}/\\sqrt{s}) > 0.3, the longitudinal polarization has been measured to be -32.9 +/- 5.5(stat) +/- 5.2(syst)%. We have observed no transverse polarization. A significant forward-backward asymmetry has been measured and can be described by a JETSET model.']",['1997-08-13']
2087,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barillari, T', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davis, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the photon structure function $F_{2}^{\\gamma}$ at low x'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'photon electron, deep inelastic scattering', 'photon, structure function', 'small-x', 'dependence, momentum transfer', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-103', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708028']","['Deep inelastic electron-photon scattering is studied using e+e- data collected by the OPAL detector at centre-of-mass energies sqrt{s_ee} ~ M_{Z^0}. The photon structure function F_2^gamma(x,Q^2) is explored in a Q^2 range of 1.1 to 6.6 GeV/c^2 at lower x values than ever before. To probe this kinematic region events are selected with a beam electron scattered into one of the OPAL luminosity calorimeters at scattering angles between 27 and 55 mrad. A measurement is presented of the photon structure function F_2^gamma(x,Q^2) at <Q^2> = 1.86 GeV^2 and 3.76 GeV^2 in five logarithmic x bins from 0.0025 to 0.2.']",['1997-08-13']
2088,['eng'],"['Adler, Stephen Louis', 'Atiya, M S', 'Chiang, I H', 'Frank, J S', 'Haggerty, J S', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'Sambamurti, A K', 'Stevens, A', 'Strand, R C', 'Witzig, C', 'Louis, W C', 'Akerib, D S', 'Ardebili, M', 'Convery, M R', 'Ito, M M', 'Marlow, D R', 'McPherson, R A', 'Meyers, P D', 'Selen, M A', 'Shoemaker, F C', 'Smith, A J S', 'Blackmore, E W', 'Bryman, D A', 'Felawka, L', 'Konaka, A', 'Kuno, Y', 'MacDonald, J A', 'Numao, T', 'Padley, P', 'Poutissou, J M', 'Poutissou, R', 'Roy, J D', 'Turcot, A S', 'Kitching, P', 'Nakano, T', 'Rozon, M', 'Soluk, R A']",['Observation of the Decay $K^{+} \\rightarrow \\pi^{+}\\mu^{+} \\mu^{-}$'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'K+, rare decay', 'K+, branching ratio', 'perturbation theory, chiral', 'experimental results', 'Brookhaven PS', 'K+ --> pi+ muon+ muon-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708012'],['We have observed the rare decay K+ --> pi+ mu+ mu- and measured the branching ratio Gamma(K+ --> pi+ mu+ mu-)/Gamma(K+ --> all) = (5.0 +/- 0.4 (stat.) +/- 0.7 (sys.) +/- 0.6 (theor.)) x 10^{-8}. We compare this result with predictions from chiral perturbation theory and estimates based on the decay K+ --> pi+ e+ e-.'],['1997-08-08']
2089,['eng'],"['Kitching, P', 'Nakano, T', 'Rozon, M', 'Soluk, R A', 'Adler, Stephen Louis', 'Atiya, M S', 'Chiang, I H', 'Frank, J S', 'Haggerty, J S', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'Sambamurti, A K', 'Stevens, A', 'Strand, R C', 'Witzig, C', 'Louis, W C', 'Akerib, D S', 'Ardebili, M', 'Convery, M', 'Ito, M M', 'Marlow, D R', 'McPherson, R A', 'Meyers, P D', 'Selen, M A', 'Shoemaker, F C', 'Smith, A J S', 'Blackmore, E W', 'Bryman, D A', 'Felawka, L', 'Konaka, A', 'Kuno, Y', 'MacDonald, J A', 'Numao, T', 'Padley, P', 'Poutissou, J M', 'Poutissou, R', 'Roy, J D', 'Turcot, A S']",['Observation of the Decay $K^{+} \\rightarrow \\pi^{+}\\gamma\\gamma$'],['Particle Physics - Experimental Results'],"['K+, radiative decay', 'K+, branching ratio', 'upper limit', 'pi+, momentum spectrum', 'perturbation theory, chiral', 'experimental results', 'Brookhaven PS', 'K+ --> pi+ 2photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708011'],"['The first observation of the decay K^+ --> pi^+ gamma gamma is reported. A total of 31 events was observed with an estimated background of 5.2 +- 3.3 events in the pi+ momentum range from 100 MeV/c to 180 MeV/c. The corresponding partial branching ratio, B(K+ -> pi+ gamma gamma, 100 MeV/c < P_pi^+ < 180 MeV/c), is (6.0 +- 1.4 (stat) +- 0.7 (sys) ) x 10^{-7}. No K^+ --> pi^+ gamma gamma decay was observed in the pi^+ momentum region greater than 215 MeV/c. The observed pi^+ momentum spectrum is compared with the predictions of chiral perturbation theory.']",['1997-08-08']
2090,['eng'],[],['Measurement of Inelastic J/$\\Psi$ Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'J/psi(3100), photoproduction', 'nondiffractive', 'J/psi(3100), leptonic decay', 'differential cross section, energy dependence', 'transverse momentum, spectra', 'fusion, photon gluon', 'color, singlet', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> J/psi(3100) positron anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708010'],"['We present a measurement of the inelastic, non diffractive J/$\\psi$ photoproduction cross section in the reaction $e^{+} p \\to e^{+} {J}/\\psi X$ with the ZEUS detector at HERA. The J/$\\psi$ was identified using both the within the range $0.4<z<0.9$ ($0.5<z<0.9$) for the muon (electron) decay mode, where $z$ is the fraction of the photon energy carried by the J/$\\psi$ in the proton rest frame. The cross section, the $p^2_T$ and the $z$ distributions, after having subtracted the contributions from resolved photon and diffractive proton dissociative processes, are given for the photon-proton centre of mass energy range $50<W<180$ GeV; $p^2_T$ is the square of the J/$\\psi$ transverse momentum with respect to the incoming proton beam direction. In the kinematic range $0.4 < z < 0.9$ and $p^2_T > 1$ GeV$^2$, NLO calculations of the photon-gluon fusion process based on the colour-singlet model are in good agreement with the data. The predictions of a specific leading order colour-octet model, as formulated to describe the CDF data on J/$\\psi$ hadroproduction, are not consistent with the data.']",['1997-08-07']
2091,['eng'],"['Daum, K']",['Open Heavy Flavor Production in Deeply Inelastic ep Scattering at HERA'],['Particle Physics - Experimental Results'],"['talk, Ringberg Castle 1997/05/25', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'quark, charm', 'quark, pair production', 'D0, hadroproduction', 'D*(2010), hadroproduction', 'charmed meson, hadronic decay', 'p, structure function', 'structure function, charm', 'small-x', 'fusion, gluon boson', 'differential cross section, energy dependence', 'dependence, momentum transfer', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '301 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708009'],"['Recent results on inclusive D^0 and D^{*+-} production in deeply inelastic ep scattering at sqrt(s)=301 GeV are summarized. The data have been collected by the H1 and ZEUS experiments at HERA. The total and the differential cross sections are discussed in the framework of LO and NLO QCD predictions. The data exhibit clear evidence for boson gluon fusion dominating open heavy flavor production in the kinematic range currently explored at HERA. The measurements of F_2^{cc}(x,Q^2) at small Bjorken x are presented. The prospects for future analyses of open charm and beauty production including detector upgrades and anticipated high luminosities are investigated.']",['1997-08-07']
2092,['eng'],"['Carli, T', 'Kuhlen, M']",['Bounds on QCD Instantons from HERA'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'hadron, electroproduction', 'quantum chromodynamics, instanton', 'decay, instanton', 'transverse energy, energy flow', 'rapidity dependence', 'charged particle, rapidity spectrum', 'particle flow', 'multiplicity, spectra', 'event shape analysis', 'production, upper limit', 'numerical calculations, Monte Carlo', 'interpretation of experiments, DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708008'],['Signals for processes induced by QCD instantons are searched for in HERA data on the hadronic final state in deep-inelastic scattering. The maximally allowed fraction of instanton induced events is found at 95% confidence level to be on the percent level in the kinematic domain 0.0001<x<0.01 and 5 < Q-squared < 100 GeV-squared. The most stringent limits are obtained from the multiplicity distributions.'],['1997-08-06']
2093,['eng'],"['Miller, D J']","['Two Photon Physics at LEP2, including data Monte-Carlo comparison']",['Particle Physics - Experimental Results'],"['talk, Oxford 1997/04/14', 'electron positron, inelastic scattering', 'exchange, two-photon', 'photon photon, inclusive reaction', 'photon photon, exclusive reaction', 'photon, structure function', 'jet, photoproduction', 'meson resonance, photoproduction', 'vector meson, pair production', 'numerical calculations, CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708006'],"['A partisan review of some of the most important $\\gamma\\gamma$ channels accessible at LEP 2, with special stress on the measurement of the photon structure function $F_{2}^{\\gamma}$ and on associated problems with Monte Carlo modelling.']",['1997-08-05']
2094,['eng'],"['Abbott, B']",['Experimental Search for Chargino and Neutralino Production via Gauge-Mediated Supersymmetry Breaking Models'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'sparticle, search for', 'sparticle, pair production', 'mass, chargino', 'mass, neutralino', 'lower limit', 'final state, two-photon', 'transverse energy, high', 'transverse energy, missing-energy', 'supersymmetry, symmetry breaking', 'gravitino', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2photon missing-energy anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708005'],"['We search for inclusive high $E_T$ diphoton events with large missing transverse energy in $p\\bar{p}$ collisions at $\\sqrt{s}$=1.8 TeV. Such events are expected from pair production of charginos and neutralinos within the framework of the minimal supersymmetric standard model with a light gravitino. No excess of events is observed. In that model, and assuming gaugino mass unification at the GUT scale, we obtain a 95% CL exclusion region in the supersymmetry parameter space and lower mass bounds of 150 GeV/c$^2$ for the lightest chargino and 75 GeV/c$^2$ for the lightest neutralino.']",['1997-08-05']
2095,['eng'],"['Goulianos, K']",['Results on Diffraction'],['Particle Physics - Experimental Results'],"['talk, Bristol 1997/06/25', 'anti-p p, inclusive reaction', 'p p, inclusive reaction', 'jet, hadroproduction', 'jet, pair production', 'electron p, deep inelastic scattering', 'p, structure function', 'hard scattering', 'diffraction', 'factorization', 'Regge poles', 'exchange, pomeron', 'cross section, energy dependence', 'rapidity, gap', 'model, pomeron', 'W, hadroproduction', 'numerical calculations', 'interpretation of experiments, DESY HERA Stor', 'interpretation of experiments, Batavia TEVATRON Coll', 'interpretation of experiments, CERN SPS Coll', 'approx. 300 GeV-cms (electron p), 1800 GeV-cms (anti-p p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708004'],['Results on hard diffraction from HERA and proton-antiproton Colliders are reviewed with emphasis on the factorization properties of the diffractive structure function of the proton and on the structure of the pomeron.'],['1997-08-05']
2096,['eng'],"['Talamonti, C']",['Status report of the NA48 experiment at the CERN SPS'],['Detectors and Experimental Techniques'],"['talk, Big Sky 1997/05/27', 'K0, hadronic decay', 'violation, CP', 'K0(L), secondary beam', 'K0(S), secondary beam', 'mass spectrum, (pi+ pi-)', 'mass spectrum, two-photon', 'magnetic spectrometer, experimental results', 'CERN SPS', 'K0 --> 2pi0', 'K0 --> pi+ pi-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708003'],['The aim of the NA48 experiment at the CERN SPS is to measure direct CP violation in neutral kaon decays thus determining the parameter NA48 with respect to previous experiments are high statistics and reduced systematic effects. The principle of the experiment and the performance of the detector components are presented.'],['1997-08-05']
2097,['eng'],"['Miller, D J']","[""An Experimenter's Highlights""]",['Particle Physics - Experimental Results'],"['review, Egmond aan Zee 1997/05/10', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'photon electron, deep inelastic scattering', 'electron p, deep inelastic scattering', 'photon, structure function', 'photon, resolved', 'jet, photoproduction', 'cross section']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708002'],"[""This selection concentrates more on $\\gamma \\gamma$ results, with some reference to the related HERA photoproduction data. Progress has been made on a wide range of topics, from $F_{2}^{\\gamma}$ to the ``stickiness'' of glueball candidates, but many channels still need better statistics and/or a real photon target before they can match the comparable $ep$ studies.""]",['1997-08-05']
2098,['eng'],"['Heath, G P']",['Charm Production at HERA'],['Particle Physics - Experimental Results'],"['talk', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'positron p, inclusive reaction', 'production, charm', 'D*(2010), photoproduction', 'p, structure function', 'structure function, charm', 'photon, resolved', 'D*(2010), hadronic decay', 'channel cross section, energy dependence', 'transverse momentum, spectra', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708001'],['Measurements of open charm production at HERA are reviewed. The paper covers both photoproduction and Deep Inelastic Scattering measurements from the ZEUS and H1 collaborations.'],['1997-08-05']
2099,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'Davies, R', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dienes, B', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Hossain, K R', 'Howard, R', 'Hüntemeyer, P', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Kayal, P I', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Mihara, S', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oh, A', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Pérez-Ochoa, R', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, J L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Trócsányi, Zoltán László', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Search for chargino and neutralino production at $\\sqrt{s}$ = 170 and 172 GeV at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'sparticle, search for', 'chargino, pair production', 'neutralino, pair production', 'mass, lower limit', 'charged particle, multiplicity', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '170, 172 GeV-cms']","['http://www.cern.ch/Opal/pubs/paper/index.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708018']","['A search for charginos and neutralinos, predicted by supersymmetric theories, has been performed using a data sample of 10.3 pb^-1 at centre-of-mass energies of sqrt(s) = 170 and 172 GeV with the OPAL detector at LEP. No evidence for these particles has been found. The results are combined with those from previous OPAL chargino and neutralino searches at lower energies to obtain limits. Exclusion regions at 95% C.L. of parameters of the Minimal Supersymmetric Standard Model are determined. Within this framework, for tan(beta) >= 1.0, lower mass limits are placed on the lightest chargino and the three lightest neutralinos. The 95% C.L. lower mass limit on the lightest chargino, assuming that it is heavier than the lightest neutralino by more than 10 GeV, is 84.5 GeV for the case of a large universal scalar mass (m_0 > ~1 TeV) and 65.7 GeV for the smallest m_0 compatible with current limits on the sneutrino and slepton masses. The lower limit on the lightest neutralino mass at 95% C.L. for tan(beta) >= 1.0 is 24.7 GeV for m_0 = 1 TeV and 13.3 GeV for the minimum m_0 scenario. These mass limits are higher for increasing values of tan(beta). The interpretation of the limits in terms of gluino and scalar quark mass limits is also given.']",['1997-08-07']
2100,['eng'],"['Suda, R', 'Watanabe, M', 'Enomoto, R', 'Iijima, T', 'Adachi, I', 'Hattori, H', 'Kuniya, T', 'Ooba, T', 'Sumiyoshi, T', 'Yoshida, Y']",['Monte-Carlo Simulation for an Aerogel Cherenkov Counter'],['Particle Physics - Experimental Results'],"['particle identification', 'Cherenkov counter, aerogel', 'Cherenkov counter, threshold', 'photoelectron', 'magnetic field', 'numerical calculations, Monte Carlo', 'magnetic detector, BELLE', 'KEK TRISTAN Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707042'],"['We have developed a Monte-Carlo simulation code for an aerogel \\v Cerenkov Counter which is operated under a strong magnetic field such as 1.5T. This code consists of two parts: photon transportation inside aerogel tiles, and one-dimensional amplification in a fine-mesh photomultiplier tube. It simulates the output photoelectron yields as accurately as 5% with only a single free parameter. This code is applied to simulations for a B-Factory particle-identification system.']",['1997-08-01']
2101,['eng'],"['Evangelista, C', 'Palano, A', 'Drijard, Daniel', 'Hamann, N H', 'Jones, R T', 'Mouëllic, B', 'Ohlsson, S', 'Perreau, J M', 'Eyrich, W', 'Moosburger, M', 'Pomp, S', 'Stinzing, F', 'Fischer, H', 'Franz, J', 'Rössle, E', 'Schmitt, H', 'Wirth, H', 'Buzzo, A', 'Kirsebom, K', 'Lo Vetere, M', 'Macri, M', 'Marinelli, M', 'Passaggio, S', 'Pia, M G', 'Pozzo, A', 'Robutti, E', 'Santroni, A', 'Debevec, P T', 'Eisenstein, R A', 'Harris, P G', 'Hertzog, D W', 'Hughes, S A', 'Reimer, P E', 'Ritter, J B', 'Geyer, R', 'Kilian, K', 'Oelert, Walter', 'Röhrich, K', 'Rook, M', 'Steinkamp, O', 'Korsmo, H', 'Stugu, B', 'Johansson, T']",['Measurement of the $\\overline{p}p \\to Ks Ks$ Reaction from 0.6 to 1.9 GeV/c'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'K0(S), pair production', 'K0(S), hadronic decay', 'f4(2220), branching ratio', 'upper limit', 'f2(2150)', 'channel cross section, energy dependence', 'angular distribution', 'experimental results', 'CERN LEAR', 'anti-p p --> 2K0(S) anything', 'f4(2220) --> p anti-p', 'f4(2220) --> 2K0(S)', '0.6-1.9 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707041'],"['The pbar p -> Ks Ks -> 4pi+/- cross section was measured at incident antiproton momenta between 0.6 and 1.9 GeV/c using the CERN Low Energy Antiproton Ring (LEAR). This investigation was part of a systematic study of in-flight antiproton-proton annihilations into two-neutral-meson final states in a search for hadronic resonances. A coarse scan of the pbar p -> Ks Ks cross section as a function of center-of-mass energy between 1.964 and 2.395 GeV/c^2 and a fine scan of the region surrounding the Xi(2220) are presented. Upper limits on the product branching ratio BR(Xi -> pbar p)BR(Xi -> Ks Ks) are determined for a wide range of mass and width assumptions based on the non-observation of the Xi(2220). A rise in the pbar p -> Ks Ks cross section is observed near 2.15 GeV/c^2, which is consistent with the f2(2150) resonance.']",['1997-07-29']
2102,['eng'],"['Heuring, T C']",['Production of Jets at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1997/04/21', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'angular distribution, (2jet)', 'channel cross section', 'transverse energy, dependence', 'quantum chromodynamics, perturbation theory', 'search for, composite', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707040'],"['Measurements of the inclusive jet cross section and the dijet angular distribution using data from the Tevatron are presented. Comparisons to NLO QCD show good agreement below 250 GeV, but CDF data show an excess at higher ET; qualitative agreement is seen between the CDF and DO cross sections. Analysis of the dijet angular distributions exclude quark compositeness below 2.1 TeV.']",['1997-07-29']
2103,['eng'],"['Bernardi, G']",['H1 Results in Deep Inelastic Scattering'],['Particle Physics - Experimental Results'],"['talk, Chicago 1997/04/14', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'diffraction, structure function', 'jet, electroproduction', 'event shape analysis', 'hadron, multiple production', 'strong interaction, coupling constant', 'small-x', 'p, structure function', 'structure function, longitudinal', 'momentum transfer, dependence', 'Lipatov equation', 'transverse momentum, spectra', 'final state, (2jet)', 'differential cross section', 'neutral current', 'charged current', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707039'],"['Recent deep inelastic results from the H1 collaboration are presented. The topics covered include inclusive diffractive physics, the determination of alpha_S using the event shapes, the study of the hadronic final state at low x with single particles and with jets, the structure function measurements in particular F_2 at low Q^2 and the high Q^2 physics both in neutral and charged current.']",['1997-07-29']
2104,['eng'],"['De Wolf, E A', 'Doyle, A T', 'Varelas, N', 'Zeppenfeld, Dieter']",['QCD Effects in Hadronic Final States'],['Particle Physics - Experimental Results'],"['review, Chicago 1997/04/14', 'lepton nucleon, deep inelastic scattering', 'electron positron, annihilation', 'anti-p p, interaction', 'hadron, electroproduction', 'hadron, photoproduction', 'hadron, hadroproduction', 'quantum chromodynamics, perturbation theory', 'jet', 'duality, parton hadron', 'energy spectrum', 'momentum spectrum', 'scaling, violation', 'multiple scattering', 'event shape analysis', 'transverse energy, high', 'angular distribution, (2jet)', 'momentum transfer, dependence', 'Lipatov equation', 'effect, instanton', 'intermediate boson, associated production', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707038'],"['Progress in the study of hadronic final states in deep inelastic scattering as well as $p\\bar{p}$, photoproduction and $e^+e^-$ annihilation, as presented at the DIS97 workshop, is reviewed.']",['1997-07-29']
2105,['eng'],"['Noyes, V A']",['Search for new physics at HERA'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1997/06/05', 'positron p, colliding beams', 'new particle, search for', 'fermion, excited state', 'excited state, radiative decay', 'selectron', 'squark, width', 'R parity, violation', 'squark, decay modes', 'coupling, squark', 'upper limit', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707037'],['Recent results on the searches for new physics in ep collisions at HERA using the ZEUS and H1 detectors are presented. No evidence for excited fermions or supersymmetric particles within the context of the Minimal Supersymmetric Standard Model nor R-parity violation has been found using an integrated luminosity of up to 20 inv pb. New limits have therefore been established.'],['1997-07-28']
2106,['eng'],"['Groer, L S']",['Present Searches for Higgs Signatures at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1997/06/05', 'anti-p p, colliding beams', 'Higgs particle, search for', 'Higgs particle, decay modes', 'intermediate boson, associated production', 'intermediate boson, leptonic decay', 'intermediate boson, hadronic decay', 'quark, truth', 'quark, pair production', 'quark, decay', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> Higgs particle W anything', 'anti-p p --> Higgs particle Z0 anything', 'anti-p p --> 2truth anything', 'truth --> Higgs particle beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707034'],['We present results for various searches for signatures of standard and non-standard model Higgs boson decays conducted at the collider detectors CDF and DO using ~ 100 pb^-1 of integrated luminosity each from the Tevatron Collider Run 1 (1992-96) at \\sqrt{s} = 1.8 TeV. No evidence for a Higgs boson decay is found and various limits are set.'],['1997-07-23']
2107,['eng'],"['Schwiening, J']","['DIRC, the Internally Reflecting Ring Imaging Cherenkov Detektor for BaBar']",['Detectors and Experimental Techniques'],"['talk, Leon 1997/07/07', 'particle identification', 'Cherenkov counter, ring imaging', 'optics, reflection', 'silicon, glass', 'magnetic detector, BaBar', 'SLAC PEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707035'],"['The DIRC is a Cherenkov imaging detector based on total internal reflection for the BaBar detector at PEP-II. The principles of the DIRC ring imaging Cherenkov technique are explained and its choice for the BaBar detector particle identification system is motivated. The detector design and the status of the R&D are discussed. Results of the measurement of the optical properties and radiation damage of the the radiators, long rectangular bars made of synthetic fused silica, are presented.']",['1997-07-24']
2108,['eng'],"['Abbott, B']",['Search for Scalar Leptoquark Pairs Decaying to Electrons and Jets in $\\overline{p}p$ Collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, leptoquark', 'leptoquark, pair production', 'decay, leptoquark', 'final state, (2jet positron electron)', 'mass, leptoquark', 'lower limit', 'channel cross section, mass', 'upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2leptoquark anything', 'leptoquark --> quark electron', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707033'],"['We have searched for the pair production of first generation scalar leptoquarks in the eejj channel using the full data set (123 pb-1) collected with the D0 detector at the Fermilab Tevatron during 1992--1996. We observe no candidates with an expected background of approximately 0.4 events. Comparing the experimental 95% confidence level upper limit to theoretical calculations of the cross section with the assumption of a 100% branching fraction to eq, we set a lower limit on the mass of a first generation scalar leptoquark of 225 GeV/c^2. The results of this analysis rule out the interpretation of the excess of high Q^2 events at HERA as leptoquarks which decay exclusively to eq.']",['1997-07-22']
2109,['eng'],"['Bailey, D S', 'Carter, R C', 'Foster, B', 'Harnew, N', 'Heath, G P', 'Jeffs, M D', 'Khatri, T', 'Lancaster, M', 'Lane, J B', 'McArthur, I C', 'McFall, J D', 'Milborrow, R S', 'Morgado, C J S', 'Morrissey, M C', 'Nash, J', 'Nixon, G', 'Phillips, D A', 'Postranecky, M', 'Quinton, S P H', 'Shield, P D', 'Topp-Jørgensen, S', 'Westlake, G', 'White, D J', 'Wilson, F F']",['The Design and Performance of the ZEUS Central Tracking Detector z-by-Timing System'],['Detectors and Experimental Techniques'],"['electron p, colliding beam detector', 'drift chamber, readout', 'signal processing, time', 'spatial resolution', 'calibration', 'data acquisition', 'tracks, resolution', 'performance', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707032'],"['The ZEUS Central Tracking Detector utilizes a time difference measurement to provide a fast determination of the z-coordinate of each hit. The z-by-timing measurement is achieved by using a Time-to-Amplitude Converter which has an intrinsic timing resolution of 36 ps, has pipelined readout, and has a multihit capability of 48 ns. In order to maintain the required sub-nanosecond timing accuracy, the technique incorporates an automated self-calibration system. The readout of the z-by-timing data utilizes a fully customized timing control system which runs synchronously with the HERA beam-crossing clock, and a data acquisition system implemented on a network of Transputers. Three dimensional space-points provided by the z-by-timing system are used as input to all three levels of the ZEUS trigger and for offline track reconstruction. The average z-resolution is determined to be 4.4 cm for multi-track events from positron-proton collisions in the ZEUS detector.']",['1997-07-21']
2110,['eng'],"['Gronberg, J B']",['Measurements of the Meson-Photon Transition Form Factors of Light Pseudoscalar Mesons at Large Momentum Transfer'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'pseudoscalar meson, photoproduction', 'pi0', 'eta', 'eta(958)', 'form factor, transition', 'momentum transfer, dependence', 'pseudoscalar meson, radiative decay', 'pseudoscalar meson, hadronic decay', 'quantum chromodynamics, perturbation theory', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tables', 'bibliography', 'electron positron --> pseudoscalar meson positron electron', 'pi0 --> 2photon', 'eta --> 2photon', 'eta --> 3pi', 'eta(958) --> eta 2pi', '10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707031'],"['Using the CLEO II detector, we have measured the differential cross sections for exclusive two-photon production of light pseudoscalar mesons $\\piz$, associated with the electromagnetic transitions $\\gamma^*\\gamma \\ra$ meson. We have measured these form factors in the momentum transfer ranges from 1.5 to 9, 20, and 30 $\\gevt$ for $\\piz$, $\\etaz$, and $\\etap$, respectively, and have made comparisons to various theoretical predictions.']",['1997-07-18']
2111,['eng'],"['Santoro, A F S']",['Diffractive Phenomena at Tevatron'],['Particle Physics - Experimental Results'],"['talk, Big Sky 1997/05/27', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'jet, pair production', 'rapidity, gap', 'diffraction', 'exchange, (2pomeron)', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707030'],['Preliminary results from the D0 experiment on jet production with rapidity gaps in $p\\bar{p}$ collisions are presented. A class of dijet events with a forward rapidity gap is observed at center-of-mass energies $\\sqrt{s}$ = 1800 GeV and 630 GeV. The number of events with rapidity gaps at both center-of-mass energies is significantly greater than the expectation from multiplicity fluctuations and is consistent with a hard single diffractive process. A class of events with two forward gaps and central dijets are also observed at 1800 GeV. This topology is consistent with hard double pomeron exchange. We also present proposed plans for extending these analysis into Run II through the use of a forward proton detector.'],['1997-07-17']
2112,['eng'],"['Edwards, K']",['Search for the Decay $\\tau^{-}\\to 4\\pi^{-}3\\pi^{+}(\\pi^{0})\\nu_{\\tau}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'tau-, branching ratio', 'upper limit', 'momentum spectrum, (3pi+ 4pi-)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> tau+ 3pi+ 4pi- neutrino/tau', 'electron positron --> tau+ 3pi+ 4pi- pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707029'],"['We have searched for the decay of the tau lepton into seven charged particles and zero or one pi0. The data used in the search were collected with the CLEO II detector at the Cornell Electron Storage Ring (CESR) and correspond to an integrated luminosity of 4.61 fb^(-1). No evidence for a signal is found. Assuming all the charged particles are pions, we set an upper limit on the branching fraction, B(tau- -> 4pi- 3pi+ (pi0) nu_tau) < 2.4 x 10^(-6) at the 90% confidence level. This limit represents a significant improvement over the previous limit.']",['1997-07-17']
2113,['eng'],"['Savinov, V']",['Measurements of the Meson-Photon Transition Form Factors of Light Pseudoscalar Mesons at Large Momentum Transfer'],['Particle Physics - Experimental Results'],"['talk, Egmond aan Zee 1997/05/10', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'pseudoscalar meson, photoproduction', 'pseudoscalar meson, decay modes', 'form factor, transition', 'pi0', 'eta', 'eta(958)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> pseudoscalar meson positron electron', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707028'],"[""Using the CLEO-II detector, we have measured the form factors associated with the electromagnetic transitions $\\gamma^*\\gamma \\to $ meson. We have measured these form factors in the momentum transfer ranges from 1.5 to 9, 20, and 30 GeV^2 for $\\pi^0, \\eta$, and $\\eta'$, respectively. We present a brief review of the final results of our analysis.""]",['1997-07-15']
2114,['eng'],"['Anderson, S']",['Study of the Decay $\\tau^- \\to 2\\pi^- \\pi^+ 3\\pi^0 \\nu_{\\tau}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau-, semileptonic decay', 'tau-, branching ratio', 'pi, multiple production', 'isospin', 'CVC model', 'mass spectrum, (pi+ 2pi- 3pi0)', 'mass spectrum, (pi+ pi- pi0)', 'omega(783)', 'eta', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> pi+ 2pi- 3pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707027'],"['The decay tau- -> 2pi- pi+ 3pi0 nu_tau has been studied with the CLEO II detector at the Cornell Electron Storage Ring (CESR). The branching fraction is measured to be (2.85 +/- 0.56 +/- 0.51) x 10^(-4). The result is in good agreement with the isospin expectation but somewhat below the Conserved-Vector-Current (CVC) prediction. We have searched for resonance substructure in the decay. Within the statistical precision, the decay is saturated by the channels tau- -> pi- 2pi0 omega nu_tau, 2pi- pi+ eta nu_tau, and pi- 2pi0 eta nu_tau. This is the first observation of this omega decay mode and the branching fraction is measured to be (1.89 +0.74/-0.67 +/- 0.40) x 10^(-4).']",['1997-07-15']
2115,['eng'],"['Heinson, A P']",['Measuring the CKM Matrix Element $V_{tb}$ at D0 and CDF'],['Particle Physics - Experimental Results'],"['talk, Honolulu 1997/03/24', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'quark, branching ratio', 'Kobayashi-Maskawa angle', 'final state, ((n)jet lepton)', 'final state, dilepton', 'particle identification, beauty', 'fusion, boson gluon', 'family, 4', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'anti-p p --> truth beauty anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707026'],"['I present measurements by the CDF collaboration of the Standard Model three generation CKM matrix element Vtb and of a special case extension with additional assumptions, using current Tevatron ttbar data. I then show how we can significantly improve the precision on Vtb and at the same time extend the measurement so it is not constrained by Standard Model assumptions, using single top production at the upgraded Tevatron.']",['1997-07-15']
2116,['eng'],[],['Measurement of the Proton Structure Function $F_2$ and $\\sigma_{tot}^{\\gamma ^* p}$ at Low $Q^2$ and Very Low $x$ at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inelastic scattering', 'photon p, interaction', 'p, structure function', 'structure function, small-x', 'momentum transfer, low', 'channel cross section, energy dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707025'],"['A small electromagnetic sampling calorimeter, installed in the ZEUS experiment in 1995, significantly enhanced the acceptance for very low $x$ and low $Q^2$ inelastic neutral current scattering, $e^{+}p\\to e^{+}X$, at HERA. A measurement of the proton structure function $F_2$ and the total virtual photon-proton ($\\gamma^*p$) cross-section is presented for $0.11 \\le Q^{2} \\le 0.65$ GeV$^2$ and $2 \\times 10^{-6} \\le x \\le 6 \\times 10^{-5}$, corresponding to a range in the $\\gamma^{*}p$ c.m. energy of $100 \\le W \\le 230$ GeV. Comparisons with various models are also presented.']",['1997-07-17']
2117,['eng'],"['Bassler, U', 'Bernardi, G']",['Some Properties of the Very High $Q^2$ Events of HERA'],['Particle Physics - Experimental Results'],"['positron p, deep inelastic scattering', 'momentum transfer, high', 'kinematics', 'data analysis method', 'radiative correction, initial-state interaction', 'mass spectrum', 'numerical calculations', 'interpretation of experiments, DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707024'],"['The kinematic reconstruction of neutral current high Q^2 events at HERA is discussed in detail using as an example the recently published events of the H1 and ZEUS collaborations at Q^2 > 15000 GeV^2 and M > 180 GeV, which are more numerous than expected from Standard Model predictions. Taking into account the complete information of these events, the mass reconstruction is improved and the difference between the average mass of the samples of the two experiments is reduced from 26+/-10 GeV to 17+/-7 GeV, but remains different enough to render unlikely an interpretation of the excess observed by the two collaborations as originating from the decay of a single narrow resonance.']",['1997-07-14']
2118,['eng'],"['Barberis, D', 'Beusch, Werner', 'Binon, Freddy G', 'Blick, A M', 'Close, Francis Edwin', 'Danielsen, K M', 'Dolgopolov, A V', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Inyakin, A V', 'Ishida, T', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinashi, T', 'Kinson, J B', 'Kirk, A', 'Klempt, W', 'Kolosov, V N', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Maljukov, S', 'Martinengo, P', 'Minashvili, I A', 'Myklebost, K', 'Nakagawa, T', 'Norman, K L', 'Olsen, J M', 'Peigneux, J P', 'Polovnikov, S A', 'Polyakov, V A', 'Prokoshkin, Yu', 'Romanovsky, V I', 'Rotscheidt, Herbert', 'Rumyantsev, V', 'Rusakovitch, N', 'Samoylenko, V D', 'Semenov, A A', 'Sené, M', 'Sené, R', 'Shagin, P M', 'Shimizu, H M', 'Singovsky, A V', 'Sobol, A E', 'Soloviev, A S', 'Stassinaki, M', 'Stroot, J P', 'Sugonyaev, V P', 'Takamatsu, K', 'Tchlatchidze, G A', 'Tsuru, T', 'Vasileiadis, G', 'Venables, M', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the $K\\overline{K}\\pi$ channel produced centrally in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, exclusive reaction', 'K, hadroproduction', 'pi, hadroproduction', 'mass spectrum, (K0(S) K pi)', 'mass spectrum, (2K0(S) pi0)', 'f1(1285), hadronic decay', 'f1(1420), hadronic decay', 'a0(980)', 'K*(892)', 'postulated particle, eta2(1620)', 'a2(1320)', 'spin, parity', 'Dalitz plot', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p K0(S) K pi', 'p p --> 2p 2K0(S) pi0', 'f1(1285) --> a0(980) pi', 'f1(1420) --> K*(892) K', 'eta2(1620) --> a2(1320) pi', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707022'],['Results are presented of an analysis of the reactions pp -> pf(k0k+pi-)ps and pp -> pf(K0K0pi0)ps at 450 GeV/c. Clear f1(1285) and f1(1420) signals are seen and a spin parity analysis shows that both have IG JPC=0+ 1++. The f1(1285) decays to a0(980)pi and the f1(1420) decays to K* Kbar. Both states have a similar dependence as a function of dPT consistent with what has been observed for other qqbar states. Evidence is also presented for a K*Kbar decay mode of the eta2(1620).'],['1997-07-10']
2119,['eng'],"['Barberis, D', 'Beusch, Werner', 'Binon, Freddy G', 'Blick, A M', 'Close, Francis Edwin', 'Danielsen, K M', 'Dolgopolov, A V', 'Donskov, S V', 'Earl, B C', 'Evans, D', 'French, Bernard R', 'Hino, T', 'Inaba, S', 'Inyakin, A V', 'Ishida, T', 'Jacholkowski, A', 'Jacobsen, T', 'Khaustov, G V', 'Kinashi, T', 'Kinson, J B', 'Kirk, A', 'Klempt, W', 'Kolosov, V N', 'Kondashov, A A', 'Lednev, A A', 'Lenti, V', 'Maljukov, S', 'Martinengo, P', 'Minashvili, I A', 'Myklebost, K', 'Nakagawa, T', 'Norman, K L', 'Olsen, J M', 'Peigneux, J P', 'Polovnikov, S A', 'Polyakov, V A', 'Prokoshkin, Yu', 'Romanovsky, V I', 'Rotscheidt, Herbert', 'Rumyantsev, V', 'Rusakovitch, N', 'Samoylenko, V D', 'Semenov, A A', 'Sené, M', 'Sené, R', 'Shagin, P M', 'Shimizu, H M', 'Singovsky, A V', 'Sobol, A E', 'Soloviev, A S', 'Stassinaki, M', 'Stroot, J P', 'Sugonyaev, V P', 'Takamatsu, K', 'Tchlatchidze, G A', 'Tsuru, T', 'Vasileiadis, G', 'Venables, M', 'Villalobos Baillie, Orlando', 'Votruba, M F', 'Yasu, Y']",['A study of the centrally-produced $\\pi^+ \\pi^- \\pi^+ \\pi^-$ channel in pp interactions at 450 GeV/c'],['Particle Physics - Experimental Results'],"['p p, exclusive reaction', 'pi, multiple production', 'mass spectrum, (2pi+ 2pi-)', 'spin, parity', 'f1(1285)', 'postulated particle, eta2(1620)', 'eta2(1870), hadronic decay', 'postulated particle, f0(2000)', 'mass enhancement, (1450)', 'mass enhancement, (1900)', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'p p --> 2p 2pi+ 2pi-', 'eta2(1620) --> a2(1320) pi', 'eta2(1870) --> a2(1320) pi', '450 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707021'],"['The reaction pp -> pf (pi+pi-pi+pi-) ps has been studied at 450 GeV/c in an experiment designed to search for gluonic states. A spin analysis has been performed and the dPT filter applied. In addition to the well known f1(1285) there is evidence for two JPC=2-+ states called the eta2(1620) and eta2(1875) and a broad scalar called the f0(2000). The production of these states as a function of the dPT kinematical filter shows the behaviour expected for qqbar states. In contrast, there is evidence for two states at 1.45 GeV and at 1.9 GeV which do not show the behaviour observed for qqbar states.']",['1997-07-10']
2120,['eng'],"['Newman, P R']",['Colour-Singlet Exchange in ep Interactions'],['Particle Physics - Experimental Results'],"['review, Chicago 1997/04/14', 'electron p, deep inelastic scattering', 'hadron, photoproduction', 'rapidity, gap', 'baryon, leading particle', 'diffraction, structure function', 'vector meson, photoproduction', 'jet, pair production', 'exchange, pomeron', 'momentum spectrum, pomeron', 'color, singlet', 'gluon, exchange', 'longitudinal momentum', 'dependence, momentum transfer', 'energy flow', 'channel cross section', 'quantum chromodynamics, Compton scattering', 'numerical calculations, interpretation of experiments', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707020'],"['Results presented at the DIS97 workshop by the H1, ZEUS and E665 collaborations on processes yielding large rapidity gaps and energetic leading baryons are reviewed. A consistent picture begins to emerge in which diffractive processes dominate when the fractional longitudinal momentum loss at the baryon vertex $\\xpom$ is small, with substantial contributions from other processes as $\\xpom$ increases. The diffractive mechanism in the deep-inelastic regime is found, both from inclusive measurements and final state studies, to involve the exchange of a gluon carrying a large fraction of the exchange momentum. Vector meson results show the transition from soft to hard production mechanisms with increasing precision.']",['1997-07-10']
2121,['eng'],"['Ammar, R']",['A Measurement of the Total Cross Section for $e^{+} e^{-} \\to$ hadrons at $\\sqrt{s}$=10.52 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'hadron, multiple production', 'cross section, hadronic', 'strong interaction, coupling constant', 'charged particle, multiplicity', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.52 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707018'],"['Using the CLEO detector at the Cornell Electron Storage Ring, we have made a measurement of R=sigma(e+e- ->hadrons)/sigma(e+e- ->mu+mu-) =3.56+/-0.01+/-0.07 at ECM=10.52 GeV. This implies a value for the strong coupling constant of alpha_s(10.52 GeV)=0.20+/-0.01+/-0.06, or alpha_s(M_Z)=0.13+/-0.005+/-0.03.']",['1997-07-09']
2122,['eng'],"['Brinkmann, R', 'Ginzburg, I F', 'Holtkamp, N', 'Jikia, G', 'Napoly, O', 'Saldin, E L', 'Schneidmiller, E A', 'Serbo, V', 'Silvestrov, G I', 'Telnov, V I', 'Undrus, A E', 'Yurkov, M I']",['Second Interaction Region for $\\gamma-\\gamma$ and $e^-\\gamma$ Collisions'],['Particle Physics - Experimental Results'],"['electron positron, linear collider', 'photon photon, colliding beams', 'photon electron, colliding beams', 'Higgs particle, coupling', 'gauge boson', 'quark, truth', 'supersymmetry', 'hadron, photoproduction', 'backscatter, laser', 'Compton scattering, multiple scattering', 'luminosity, beam monitoring', 'beam optics', 'free electron laser', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707017'],"['Linear colliders offer unique opportunities to study gamma-gamma (gg), gamma-electron (ge) interactions. Using the laser backscattering method one can obtain gg, ge colliding beams with an energy and luminosity comparable to that in e+e- collisions. This work is a part of the Conceptual Design of TESLA/SBLC linear colliders describing a second interaction region for gg, ge collisions. We consider here possible physics in high energy gg, ge collisions, e -> g conversion, requirements to lasers, collision schemes, attainable luminosities, backgrounds, possible lasers, optics at the interaction region and other associated problems.']",['1997-07-09']
2123,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Berlich, P', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hilse, T', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Howard, R', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Przysiezniak, H', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Rosvick, M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schulz, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['Measurement of the branching fractions and forward-backward asymmetries of the $Z^0$ into light quarks'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, hadroproduction', 'Z0, hadronic decay', 'quark, pair production', 'angular distribution, asymmetry', 'particle identification, flavor', 'symmetry, SU(2)', 'Z0, branching ratio', 'coupling, (Z0 quark)', 'coupling, left-handed', 'coupling, right-handed', 'dependence, flavor', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://www.cern.ch/Opal/pubs/paper/index.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707019']","['Using approximately 4.3 million hadronic Z^0 decays collected with the OPAL detector at LEP between 1990 and 1995, we measure the branching fractions of the Z^0 into up-type and down-type light quarks, R_q, and the forward-backward asymmetries, A_FB(q), using high-momentum stable particles as a tag. Adopting a method that employs double tagged events to determine the flavour tagging efficiencies, and assuming the flavour independence of strong interactions and SU(2) isospin symmetry, we measure: R_{d,s}/(R_d + R_u + R_s) = 0.371 +/- 0.016(stat.) +/- 0.016(syst.) and A_FB(d,s)= 0.068 +/- 0.035(stat.) +/- 0.011(syst.), assuming the branching fractions and forward-backward asymmetries of down and strange quarks to be equal. The results are essentially free of assumptions based on hadronisation models. These results are in agreement with the Standard Model expectations and are used to infer the left and right handed couplings of strange/down quarks to the Z^0, yielding g_L^{d,s} = -0.44^{+0.13}_{-0.09} and g_R^{d,s} = +0.13^{+0.15}_{-0.17}. The results for the up quark, R_u/(R_d + R_u + R_s) = 0.258 +/- 0.031(stat.) +/- 0.032(syst.) and A_FB(u)= 0.040 +/- 0.067(stat.) +/- 0.028(syst.), are fully negatively correlated and almost completely positively correlated, respectively, with the corresponding down-type results.']",['1997-07-03']
2124,['eng'],[],['A Search for Excited Fermions in $e^{+}p$ Collisions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'new particle, search for', 'electron, excited state', 'neutrino/e, excited state', 'quark, excited state', 'excited state, decay modes', 'channel cross section, branching ratio', 'upper limit', 'coupling, excited state', 'mass, excited state', 'mass spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9708007'],"['Using the ZEUS detector at HERA, we have searched for heavy excited states of electrons, neutrinos, and quarks in $e^+p$ collisions at a center-of-mass energy of 300~GeV. With an integrated luminosity of 9.4~pb$^{-1}$, no evidence was found for electroweak production and decay of such states. Limits on the production cross section times branching ratio and on the characteristic couplings, $f/\\Lambda$, are derived for masses up to 250~GeV. For the particular choice $f/\\Lambda = 1/M_{f^*}$, we exclude at the 95% confidence level excited electrons with mass between 30 and 200~GeV, excited electron neutrinos with mass between 40 and 96~GeV, and quarks excited electroweakly with mass between 40 and 169~GeV.']",['1997-08-06']
2125,['eng'],"['Abbott, B']",['Measurement of Dijet Angular Distributions and Search for Quark Compositeness'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'angular distribution, (2jet)', 'quark, composite', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707016'],['We have measured the dijet angular distribution in $\\sqrt{s}$=1.8 TeV $p\\bar{p}$ collisions using the D0 detector. Order $\\alpha^{3}_{s}$ QCD predictions are in good agreement with the data. At 95% confidence the data exclude models of quark compositeness in which the contact interaction scale is below 2 TeV.'],['1997-07-08']
2126,['eng'],"['Carli, T', 'Kuhlen, M']",['Confronting QCD Instantons with HERA Data'],['Particle Physics - Experimental Results'],"['talk, Chicago 1997/04/14', 'electron p, deep inelastic scattering', 'hadron, multiple production', 'quantum chromodynamics, nonperturbative', 'effect, instanton', 'quark gluon, fusion', 'transverse energy, energy flow', 'rapidity dependence', 'multiplicity, spectra', 'transverse momentum, spectra', 'numerical calculations, Monte Carlo', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707013'],['The sensitivity of existing HERA data on the hadronic final state in deep-inelastic scattering (DIS) to processes induced by QCD instantons is systematically investigated. The maximally allowed fraction of such processes in DIS is found to be on the percent level in the kinematic domain 0.0001 < x-Bjorken < 0.01 and 5 < Q squared < 100 GeV squared. The best limits are obtained from the multiplicity distribution.'],['1997-07-07']
2127,['eng'],"['Chekanov, S V']",['Angular Intermittency and Analytical QCD Predictions'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1997/03/22', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quantum chromodynamics, perturbation theory', 'multiplicity, moment', 'angular dependence', 'intermittency', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707012'],['We present a comparison of local multiplicity fluctuations in angular phase-space intervals with first-order QCD predictions. The data are based on 810k hadronic events at 91.2 GeV collected with the L3 detector at LEP during 1994.'],['1997-07-07']
2128,['eng'],"['Abe, K']",['Measurement of the B Hadron Energy Distribution in $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'B, energy spectrum', 'B, semileptonic decay', 'quark, fragmentation', 'quantum chromodynamics, perturbation theory', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707011'],['We have measured the B hadron energy distribution in Z0 decays using a sample of semi-leptonic B decays recorded in the SLD experiment at SLAC. The energy of each tagged B hadron was reconstructed using information from the lepton and a partially-reconstructed charm-decay vertex. We compared the scaled energy distribution with several models of heavy quark fragmentation. The average scaled energy was found to be <x_E_B> = 0.716+-0.011 (stat.) +0.021 -0.022 (syst.).'],['1997-07-04']
2129,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Berlich, P', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fukui, H', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hilse, T', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Howard, R', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Przysiezniak, H', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Rosvick, M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schulz, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['An updated study of B meson oscillations using dilepton events'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B/s0 anti-B/s0, oscillation', 'B0 anti-B0, oscillation', 'beautiful meson, semileptonic decay', 'final state, dilepton', 'B0, mass difference', 'B/s0, mass difference', 'lower limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://www.cern.ch/Opal/pubs/paper/index.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707010']","['This paper reports a study of B meson oscillations using hadronic Z^0 decays with two identified leptons, and updates a previous publication by including data collected in 1994. Decay times are reconstructed for each of the semileptonic B decays by forming vertices which include the lepton and by estimating the B meson momentum. The mass difference, Delta(m_d), between the two mass eigenstates in the B^0_d system is measured to be 0.430 +/- 0.043 + 0.028 - 0.030 ps^-1, where the first error is statistical and the second error is systematic. For the B^0_s system, a lower limit of Delta(m_s) > 2.2 ps^-1 is obtained at 95% C.L.']",['1997-07-03']
2130,['eng'],"['Meyer, C A']",['Meson Spectroscopy and the Search for Exotics'],['Particle Physics - Experimental Results'],"['review, Big Sky 1997/05/27', 'meson, hadron spectroscopy', 'meson, exotic', 'glueball, scalar', 'glueball, tensor', 'meson, hybrid', 'interference, (glueball scalar meson)', 'anti-p p, annihilation', 'pi- p, interaction', 'meson, hadroproduction', 'J/psi(3100), radiative decay', 'f0(1500)', 'f0(1750)', 'f4(2220)', 'f0(1370)', 'mass spectrum', 'Dalitz plot', 'experimental results', '((1)) ((2))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707008'],"['I will review the current status of exotic hadrons in the meson sector. There is currently strong evidence that a scalar glueball mixed into the normal scalar mesons has been found. There is also an interesting candidate for the tensor glueball state. Finally, I will discuss hybrid mesons with explicitly exotic quantum numbers.']",['1997-07-03']
2131,['eng'],"['Saunders, R L']",['Recent Photoproduction Results From ZEUS'],['Particle Physics - Experimental Results'],"['talk, Chicago 1997/04/14', 'positron p, colliding beams', 'jet, photoproduction', 'channel cross section', 'angular distribution, (2jet)', 'quantum chromodynamics', 'perturbation theory, higher-order', 'photon, direct production', 'transverse momentum, high', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707006'],"['Recent results from ZEUS for inclusive jet cross sections, dijet cross sections and dijet angular distributions are compared with NLO perturbative QCD calculations. The observation of isolated high $P_T$ photons (prompt photons) is also reported.']",['1997-07-03']
2132,['eng'],"['Adloff, C']",['Evolution of ep Fragmentation and Multiplicity Distributions in the Breit Frame'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, multiple production', 'small-x', 'kinematics, Breit frame', 'fragmentation function', 'dependence, momentum transfer', 'x-dependence', 'electron positron, annihilation', 'charged particle, multiplicity', 'energy spectrum', 'leading logarithm approximation', 'scaling, KNO', 'scaling, violation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707005'],"['Low x deep-inelastic ep scattering data, taken in 1994 at the H1 detector at HERA, are analysed in the Breit frame of reference. The evolution of the peak and width of the current hemisphere fragmentation function is presented as a function of Q and compared with e+e- results at equivalent centre of mass energies. Differences between the average charged multiplicity and the multiplicity of e+e- annihilations at low energies are analysed. Invariant energy spectra are compared with MLLA predictions. Distributions of multiplicity are presented as functions of Bjorken-x and Q^2, and KNO scaling is discussed.']",['1997-07-03']
2133,['eng'],"['Dusini, S', 'Ferrari, F', 'Lazzizzera, I', 'Sartori, A', 'Sidoti, A', 'Tecchiolli, G P']",['Searching the Higgs with the Neurochip TOTEM'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1997/04/21', 'p p, interaction', 'Higgs particle, search for', 'neural network, integrated circuit', 'Higgs particle, hadroproduction', 'Higgs particle, decay', 'Z0, pair production', 'background', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707004'],"['We show that neural network classifiers can be helpful in discriminating Higgs production events from the huge background at LHC, assuming the case of a mass value $M_H \\sim 200$ GeV. We use the high performance neurochip TOTEM, trained by the Reactive Tabu Search algorithm (RTS), which could be used for on-line purposes. Two different sets of input variables are compared.']",['1997-07-02']
2134,['eng'],"['Rooke, A M']",['Energy Flows and Jet Production in Tagged $e-\\gamma$ Events at LEP'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'photon electron, interaction', 'jet, photoproduction', 'jet, multiplicity', 'energy flow, hadronic', 'rapidity dependence', 'numerical calculations, Monte Carlo', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707003'],"['It has already been shown that the energy flow distributions in tagged events disagree with those predicted by QCD models, generating serious systematic errors in the unfolding of the photon structure function $F_{2}^{\\gamma}$. This new analysis uses the jet structure in the hadronic final state to identify the class of events which is in worst agreement with the models. A cone jet finder is used to select events with 0,1 or 2 jets whose transverse energy is greater than 3 GeV. Tagged electrons are detected in the OPAL forward detector at angles between 60 and 120 milliradians. As well as the QCD-based Monte Carlo models, HERWIG and PYTHIA, the simple F2GEN program is used to give a comparison sample of events with purely pointlike photon-quark coupling.']",['1997-07-02']
2135,['eng'],"['Lauber, J A', 'Lönnblad, L', 'Seymour, Michael H']",['Tuning MC Models to Fit DIS $e-\\gamma$ Scattering Events'],['Detectors and Experimental Techniques'],"['photon electron, deep inelastic scattering', 'photon, structure function', 'photon, transverse momentum', 'transverse energy', 'energy flow, hadronic', 'x-dependence', 'dependence, momentum transfer', 'rapidity dependence', 'gluon, radiation', 'quark, transverse momentum', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707002'],"['Monte Carlo models of DIS e-gamma scattering must describe hard emissions as well as the soft and collinear limits. Comparison with the observed experimental hadronic energy flow has shown that various models underestimate the high-p_T contribution, in particular at low-x. We have attempted to tune the Herwig, Pythia and Ariadne models to improve the agreement with the data, and to understand the physical implications of the changes required. Unless the physics of these processes is understood it will not be possible to unfold the photon structure functions F_2^\\gamma from the e^+e^- data without large model dependent systematic errors.']",['1997-07-02']
2136,['eng'],"['Butterworth, J M']",['Jet Photoproduction'],['Particle Physics - Experimental Results'],"['talk, Ringberg 1997/05/25', 'review, experimental results', 'electron p, deep inelastic scattering', 'electron p, inclusive reaction', 'jet, photoproduction', 'photon, structure function', 'p, structure function', 'photon, resolved', 'angular distribution, (2jet)', 'differential cross section, transverse energy', 'differential cross section, rapidity dependence', 'quantum chromodynamics', 'energy flow', 'event shape analysis', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707001'],"['The status of HERA data on jet photoproduction is reviewed, and some suggestions and prospects for further work are given.']",['1997-07-02']
2137,['eng'],"['Streets, K']",['D0 Results on W Boson Properties'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1997/06/05', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'electroweak interaction, coupling constant', 'lepton, universality', 'lepton, transverse momentum', 'W, mass', 'W, width', 'channel cross section, branching ratio', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'anti-p p --> Z0 anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706028'],"['Results from analyses of events with W and Z bosons are presented for the D0 Tevatron run 1B data samples. From the leptonic decays of the W and Z, the W and Z production cross sections and the W width are determined. Events in which the W decays into a tau and neutrino are used to determine the ratio of the electroweak gauge coupling constants as a measure of lepton universality. Using W and Z decays into electrons, the the W boson mass is measured.']",['1997-07-01']
2138,['eng'],"['Norman, D']",['Search for Leptoquarks at D0'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1997/06/05', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, leptoquark', 'leptoquark, pair production', 'mass, leptoquark', 'lower limit', 'decay, leptoquark', 'final state, (2jet 2lepton)', 'final state, (2jet lepton)', 'transverse energy, missing-energy', 'channel cross section, mass', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2leptoquark anything', 'leptoquark --> quark lepton', 'leptoquark --> quark neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706027'],['We present in this paper the current status of searches for leptoquarks at D0. These results include the use of next leading order theoretical predictions for the cross section for pair production of leptoquarks at hadron colliders. We also present a new optimized analysis for first generation leptoquarks with significant increase in sensitivity relative to earlier searches using D0 data. The mass limits derived from this first generation leptoquark search are relevant to the recently reported high mass events at HERA.'],['1997-07-01']
2139,['eng'],"['Kambara, H']",['Search for Leptoquarks at CDF'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1997/06/05', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'search for, leptoquark', 'leptoquark, pair production', 'mass, leptoquark', 'lower limit', 'final state, (2jet 2lepton)', 'channel cross section, mass', 'B0, leptonic decay', 'B/s0, leptonic decay', 'beautiful meson, branching ratio', 'upper limit', 'magnetic detector, CDF', 'experimental results', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706026'],"['We present the result of direct leptoquark searches based on 110 pb-1 of integrated luminosity collected by the Collider Detector at Fermilab during the 1992-93 and 1994-95 Tevatron runs at \\sqrt{s}=1.8 TeV. We present upper limits on the production cross sections as a function of the leptoquark mass. Using the NLO calculation of the leptoquark-pair production cross sections we extract lower-mass limits for first, second and third generation leptoquarks. We also present the result of an indirect search for Pati-Salam leptoquarks via exclusive e-mu decay modes of B^{0}_{s} and B^{0}_{d}.']",['1997-06-30']
2140,['eng'],"['Wightman, J A']",['Recent Results from the Search for New Phenomena at D0'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1997/03/02', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'transverse energy, high', 'search for, new interaction', 'leptoquark, decay modes', 'mass, leptoquark', 'lower limit', 'sparticle, pair production', 'slepton', 'sneutrino', 'chargino', 'channel cross section, mass', 'upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706024'],"['We present results from several new searches for physics beyond the Standard Model. We describe a search based on the scalar sum of the transverse energy of the event, a global quantity nearly independent of the event topology. We summarize our searches for first generation leptoquarks into all three decay channels, eq eq, eq nu q, and nu q nu q, and note that this is the first time that the triumvirate of decay channels has been searched. We do not find any evidence for production of first generation leptoquarks and set a lower limit on the mass of the leptoquark of 175 GeV/c^2, assuming the decay is exclusively into eq eq. We also present results from the first search for a third generation leptoquark with charge = +/- 1/3. Again, we find no evidence for its existence for a mass less than 80 GeV/c^2. Finally, we discuss one of our searches for supersymmetry, specifically the pair-production of selectrons, sneutrinos, and chi_2^0 where the decay yields final states with two photons plus missing transverse energy. We set limits on the production cross section ranging from 1 pb to 400 fb, depending on the mass. This analysis also sets a model-independent upper limit on the cross section times branching ratio to two photons + missing transverse energy + X of 185 fb at the 95% CL for transverse energy of the photons > 12 GeV with eta < 1.1 and missing transverse energy > 25 GeV.']",['1997-06-27']
2141,['eng'],"['Eitel, K']",['KARMEN'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1997/03/15', 'neutrino, oscillation', 'neutrino, particle source', 'neutrino, mass difference', 'neutrino, mixing angle', 'iron, shielding', 'scintillation counter, liquid', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706023'],"[""The neutrino experiment KARMEN is situated at the beam stop neutrino source ISIS. It provides nu_mu's, nu_e's and nu_mu_bar's in equal intensities from the pi+ mu+ decay at rest. The oscillation channels nu_mu->nu_e and nu_mu_bar->nu_e_bar are investigated with a 56t liquid scintillation calorimeter at a mean distance of 17.6m from the nu source. No evidence for oscillations could be found with KARMEN, resulting in 90% CL exclusion limits of sin(2th) < 8.5 10^-3 (nu_mu_bar->nu_e_bar) and sin(2th) < 4.0 10^-2 (nu_mu->nu_e) for Delta m^2 > 100eV^2. In 1996, the KARMEN neutrino experiment has been upgraded by an additional veto system. Vetoing of cosmic muons passing the 7000t massive iron shielding of the detector suppresses energetic neutrons from deep inelastic scattering of muons as well as from mu-capture in iron. Up to 1996, these neutrons penetrating into the detector represented the main background for the nu_mu_bar->nu_e_bar oscillation search. With an expected reduction of the background rate by a factor of 40 the experimental sensitivity for nu_mu_bar->nu_e_bar will be significantly enhanced towards sin(2th) = 10^-3 for large Delta m^2.""]",['1997-06-27']
2142,['eng'],"['Abbiendi, G']",['High Energy Photoproduction'],['Particle Physics - Experimental Results'],"['review, experimental results', 'positron p, colliding beams', 'positron p, deep inelastic scattering', 'photon p, interaction', 'jet, photoproduction', 'vector meson, photoproduction', 'charm, photoproduction', 'quantum chromodynamics, validity test', 'photon, structure function', 'p, structure function', 'photon, resolved', 'momentum spectrum, parton', 'parametrization', 'diffraction', 'nondiffractive', 'hard scattering', 'exchange, pomeron', 'color, singlet', 'rapidity, gap', 'transverse momentum, spectra', 'cross section, energy dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706022'],"['The study of photoproduction reactions has gained a unique opportunity with the HERA data. The high center of mass energy allows to carry out quantitative tests of QCD, to explore the substructure of both the photon and the proton and to shed new light on soft and diffractive processes. In this report we review the HERA results, comparing them with the reach of fixed target photoproduction experiments and complementary measurements from $e^{+}e^{-}$ and hadron colliders.']",['1997-06-26']
2143,['eng'],"['Kabuss, E M']",['Asymmetries from Semi-inclusive Polarized Deep Inelastic Scattering'],['Particle Physics - Experimental Results'],"['talk, Chicago 1997/04/14', 'muon nucleon, deep inelastic scattering', 'muon, polarized beam', 'nucleon, polarized target', 'hadron, electroproduction', 'asymmetry', 'quark, valence', 'quark, sea', 'quark, polarization', 'magnetic spectrometer, experimental results', 'CERN SPS', '100, 190 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706021'],"['The analysis of semi-inclusive data from deep inelastic scattering of polarized muons off polarized protons and deuterons by the SMC is presented. The resulting charged hadron asymmetries are used to determine polarized valence and sea quark distributions and their contributions to the nucleon spin. In addition, a new approach to derive inclusive asymmetries is discussed.']",['1997-06-26']
2144,['eng'],"['Bergfeld, T']",['First Observation of $\\tau \\to 3 \\pi \\eta \\nu_{\\tau}$ and $\\tau \\to f_{1} \\pi \\nu_{\\tau}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, semileptonic decay', 'eta', 'eta(958)', 'tau, branching ratio', 'upper limit', 'f1(1285), hadronic decay', 'mass spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> 3pi eta neutrino/tau', 'tau- --> f1(1285) pi neutrino/tau', 'f1(1285) --> eta 2pi', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706020'],"[""We have observed new channels for $\\tau$ decays with an $\\eta$ in the final state. We study 3-prong tau decays, using the $\\eta\\to\\gamma\\gamma$ and the $\\eta\\to\\gamma\\gamma$ channel. The measured branching fractions are =(3.4^{+0.6}_{-0.5}\\pm0.6)\\times10^{-4}$ and $\\B(\\tau^{-}\\to \\pi^{-}2\\piz\\eta\\nu_{\\tau} =(1.4\\pm0.6\\pm0.3)\\times10^{-4}$. We observe clear evidence for $f_1\\to\\eta\\pi\\pi$ substructure and measure We have also searched for $\\eta'(958)$ production and obtain 90% CL upper limits $\\B(\\tau^{-}\\to \\pi^{-}\\eta'\\nu_\\tau)<7.4\\times10^{-5}$ and""]",['1997-06-26']
2145,['eng'],"['Brandenburg, G']",['New measurement of $B\\to D^{*}\\pi$ branching fractions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B-, branching ratio', 'anti-B0, branching ratio', 'D*(2010), hadronic decay', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D*(2010) pi', 'D*(2010) --> D pi', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706019'],"['The unique kinematics of BB production at the Upsilon(4S) allow reconstruction of all kinematic quantities in the decay sequence B -> D* pi, D* -> D pi without reconstructing the D decay. Using 3.1 fb^{-1} accumulated at the Upsilon(4S) by the CLEO-II detector,we report measurements of BR(B0 -> D*+ pi-) = (2.81 +/- 0.11 +/- 0.21 +/- 0.05) x 10^{-3} and BR(B- -> D*0 pi-) = (4.34 +/- 0.33 +/- 0.34 +/- 0.18) x 10^{-3}.']",['1997-06-26']
2146,['eng'],"['Sinclair, L E']",['Recent Results from the study of QCD and Jets at HERA'],['Particle Physics - Experimental Results'],"['talk, Lake Louise 1997/02/16', 'electron p, colliding beams', 'positron p, colliding beams', 'electron p, deep inelastic scattering', 'hadron, electroproduction', 'jet, photoproduction', 'photon, resolved', 'fragmentation function', 'final state, (2jet)', 'channel cross section', 'photon, direct production', 'transverse energy, energy flow', 'event shape analysis', 'quantum chromodynamics', 'showers, parton', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706018'],"['The HERA experiments H1 and ZEUS have recently presented a number of interesting results from studies of the hadronic final state produced in $ep$ collisions. These studies have focussed on deep inelastic scattering events and on the photoproduction of jets, and also on the comparison of the final states produced in these two regimes. Some of these results are reviewed here.']",['1997-06-25']
2147,['eng'],"['Willocq, S']",['B physics at SLD'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1997/04/21', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'B, decay', 'decay, path length', 'B+, lifetime', 'B0, lifetime', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'time dependence', 'particle identification, flavor', 'semiconductor detector, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706017'],"['We review recent $B$ physics results obtained in polarized $e^+ e^-$ interactions at the SLC by the SLD experiment. The excellent 3-D vertexing capabilities of SLD are exploited to extract precise $\\bu$ and $\\bd$ lifetimes, as well as measurements of the time evolution of $B^0_d - \\overline{B^0_d}$ mixing.']",['1997-06-24']
2148,['eng'],"['Favara, A', 'Pieri, M']",['Confidence level estimation and analysis optimization'],['Detectors and Experimental Techniques'],"['statistical analysis', 'efficiency', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706016'],"['This note proposes a method, which can be applied to searches and more in general to any cross section measurement, to maximize the analysis sensitivity.']",['1997-06-24']
2149,['eng'],"['Yasuda, T']",['Tevatron Results on Gauge Boson Couplings'],['Particle Physics - Experimental Results'],"['talk, Stony Brook 1997/06/05', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', ""W', hadroproduction"", 'Z0, hadroproduction', 'photon, hadroproduction', 'gauge boson, pair production', 'coupling, (3gauge boson)', 'intermediate boson, leptonic decay', 'intermediate boson, hadronic decay', 'channel cross section', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706015'],"['Direct measurements of the trilinear gauge boson couplings by the CDF and D0 collaborations at Fermilab are reviewed. Limits on the anomalous couplings were obtained at a 95 % CL from four diboson production processes: W-gamma production with the subsequent W boson decay to e-nu or mu-nu, WW production with both the W boson decaying to e-nu or mu-nu, WW/WZ production with one of the gauge bosons decaying leptonically and the other gauge boson decaying to two jets, and Z-gamma production with the subsequent Z boson decay to e-e, mu-mu, or nu-nu. Limits were also obtained by a combined fit to W-gamma, WW to dileptons and WW/WZ semileptonic data samples.']",['1997-06-20']
2150,['eng'],"['Abbott, B']",['Measurement of the Top Quark Mass Using Dilepton Events'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, dilepton', 'mass, truth', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706014'],"['The D0 collaboration has performed a measurement of the top quark mass based on six candidate events for the process t tbar -> b W+ bbar W-, where the W bosons decay to e nu or mu nu. This sample was collected during an exposure of the D0 detector to an integrated luminosity of 125 pb^-1 of sqrt(s)=1.8 TeV p-pbar collisions. We obtain mt = 168.4 +- 12.3 (stat) +- 3.7 (sys) GeV/c^2, consistent with the measurement obtained using single-lepton events. Combination of the single-lepton and dilepton results yields mt = 172.0 +- 7.5 GeV/c^2.']",['1997-06-17']
2151,['eng'],"['Barate, R', 'Buskulic, D', 'Décamp, D', 'Ghez, Philippe', 'Goy, C', 'Lees, J P', 'Lucotte, A', 'Minard, M N', 'Nief, J Y', 'Pietrzyk, B', 'Casado, M P', 'Chmeissani, M', 'Comas, P', 'Crespo, J M', 'Delfino, M C', 'Fernández, E', 'Fernández-Bosman, M', 'Garrido, L', 'Juste, A', 'Martínez, M', 'Miquel, R', 'Mir, L M', 'Orteu, S', 'Padilla, C', 'Park, I C', 'Pascual, A', 'Perlas, J A', 'Riu, I', 'Sánchez, F', 'Teubert, F', 'Colaleo, A', 'Creanza, D', 'De Palma, M', 'Gelao, G', 'Iaselli, Giuseppe', 'Maggi, G', 'Maggi, M', 'Marinelli, N', 'Nuzzo, S', 'Ranieri, A', 'Raso, G', 'Ruggieri, F', 'Selvaggi, G', 'Silvestris, L', 'Tempesta, P', 'Tricomi, A', 'Zito, G', 'Huang, X', 'Lin, J', 'Ouyang, Q', 'Wang, T', 'Xie, Y', 'Xu, R', 'Xue, S', 'Zhang, J', 'Zhang, L', 'Zhao, W', 'Abbaneo, D', 'Alemany, R', 'Bazarko, A O', 'Becker, U', 'Bright-Thomas, P G', 'Cattaneo, M', 'Cerutti, F', 'Dissertori, G', 'Drevermann, H', 'Forty, Roger W', 'Frank, M', 'Hagelberg, R', 'Hansen, J B', 'Harvey, J', 'Janot, P', 'Jost, B', 'Kneringer, E', 'Knobloch, J', 'Lehraus, Ivan', 'Lutters, G', 'Mato, P', 'Minten, A', 'Moneta, L', 'Pacheco, A', 'Pusztaszeri, J F', 'Ranjard, F', 'Rizzo, G', 'Rolandi, Luigi', 'Schlatter, D', 'Schmitt, M', 'Schneider, O', 'Tejessy, W', 'Tomalin, I R', 'Wachsmuth, Horst Werner', 'Wagner, A', 'Ajaltouni, Ziad J', 'Barrès, A', 'Boyer, C', 'Falvard, A', 'Ferdi, C', 'Gay, P', 'Guicheney, C', 'Henrard, P', 'Jousset, J', 'Michel, B', 'Monteil, S', 'Montret, J C', 'Pallin, D', 'Perret, P', 'Podlyski, F', 'Proriol, J', 'Rosnet, P', 'Rossignol, J M', 'Fearnley, Tom', 'Hansen, J D', 'Hansen, J R', 'Hansen, P H', 'Nilsson, B S', 'Rensch, B', 'Wäänänen, A', 'Daskalakis, G', 'Kyriakis, A', 'Markou, C', 'Simopoulou, Errietta', 'Vayaki, Anna', 'Blondel, Alain', 'Brient, J C', 'Machefert, F P', 'Rougé, A', 'Rumpf, M', 'Valassi, A', 'Videau, H L', 'Focardi, E', 'Parrini, G', 'Zachariadou, K', 'Cavanaugh, R J', 'Corden, M', 'Georgiopoulos, C H', 'Hühn, T', 'Jaffe, D E', 'Antonelli, A', 'Bencivenni, G', 'Bologna, G', 'Bossi, F', 'Campana, P', 'Capon, G', 'Casper, David William', 'Chiarella, V', 'Felici, G', 'Laurelli, P', 'Mannocchi, G', 'Murtas, F', 'Murtas, G P', 'Passalacqua, L', 'Pepé-Altarelli, M', 'Curtis, L', 'Dorris, S J', 'Halley, A W', 'Knowles, I G', 'Lynch, J G', ""O'Shea, V"", 'Raine, C', 'Scarr, J M', 'Smith, K', 'Teixeira-Dias, P', 'Thompson, A S', 'Thomson, E', 'Thomson, F', 'Turnbull, R M', 'Geweniger, C', 'Graefe, G', 'Hanke, P', 'Hansper, G', 'Hepp, V', 'Kluge, E E', 'Putzer, A', 'Schmidt, M', 'Sommer, J', 'Tittel, K', 'Werner, S', 'Wunsch, M', 'Beuselinck, R', 'Binnie, David M', 'Cameron, W', 'Dornan, Peter J', 'Girone, M', 'Goodsir, S M', 'Martin, E B', 'Morawitz, P', 'Moutoussi, A', 'Nash, J', 'Sedgbeer, J K', 'Stacey, A M', 'Williams, M D', 'Girtler, P', 'Kuhn, D', 'Rudolph, G', 'Betteridge, A P', 'Bowdery, C K', 'Colrain, P', 'Crawford, G', 'Finch, A J', 'Foster, F', 'Hughes, G', 'Jones, R W L', 'Sloan, Terence', 'Whelan, E P', 'Williams, M I', 'Hoffmann, C', 'Jakobs, K', 'Kleinknecht, K', 'Quast, G', 'Renk, B', 'Rohne, E', 'Sander, H G', 'Van Gemmeren, P', 'Zeitnitz, C', 'Aubert, Jean-Jacques', 'Benchouk, C', 'Bonissent, A', 'Bujosa, G', 'Calvet, D', 'Carr, J', 'Coyle, P', 'Diaconu, C A', 'Konstantinidis, N P', 'Leroy, O', 'Motsch, F', 'Payre, P', 'Rousseau, D', 'Talby, M', 'Sadouki, A', 'Thulasidas, M', 'Tilquin, A', 'Trabelsi, K', 'Aleppo, M', 'Ragusa, F', 'Berlich, R', 'Blum, Walter', 'Büscher, V', 'Dietl, H', 'Ganis, G', 'Gotzhein, C', 'Kroha, H', 'Lütjens, G', 'Lutz, G', 'Männer, W', 'Moser, H G', 'Richter, R H', 'Rosado-Schlosser, A', 'Schael, S', 'Settles, Ronald', 'Seywerd, H C J', 'Saint-Denis, R', 'Stenzel, H', 'Wiedenmann, W', 'Wolf, G', 'Boucrot, J', 'Callot, O', 'Chen, S', 'Cordier, A', 'Davier, M', 'Duflot, L', 'Grivaz, J F', 'Heusse, P', 'Höcker, A', 'Jacholkowska, A', 'Jacquet, M', 'Kim, D W', 'Le Diberder, F', 'Lefrançois, J', 'Lutz, A M', 'Nikolic, I A', 'Schune, M H', 'Simion, S', 'Tournefier, E', 'Veillet, J J', 'Videau, I', 'Zerwas, D', 'Azzurri, P', 'Bagliesi, G', 'Batignani, G', 'Bettarini, S', 'Bozzi, C', 'Calderini, G', 'Carpinelli, M', 'Ciocci, M A', 'Ciulli, V', ""Dell'Orso, R"", 'Fantechi, R', 'Ferrante, I', 'Giassi, A', 'Gregorio, A', 'Ligabue, F', 'Lusiani, A', 'Marrocchesi, P S', 'Messineo, A', 'Palla, Fabrizio', 'Sanguinetti, G', 'Sciabà, A', 'Spagnolo, P', 'Steinberger, Jack', 'Tenchini, Roberto', 'Tonelli, G', 'Vannini, C', 'Venturi, A', 'Verdini, P G', 'Blair, G A', 'Bryant, L M', 'Chambers, J T', 'Gao, Y', 'Green, M G', 'Medcalf, T', 'Perrodo, P', 'Strong, J A', 'Von Wimmersperg-Töller, J H', 'Botterill, D R', 'Clifft, R W', 'Edgecock, T R', 'Haywood, S', 'Maley, P', 'Norton, P R', 'Thompson, J C', 'Wright, A E', 'Bloch-Devaux, B', 'Colas, P', 'Fabbro, B', 'Kozanecki, Witold', 'Lançon, E', 'Lemaire, M C', 'Locci, E', 'Pérez, P', 'Rander, J', 'Renardy, J F', 'Rosowsky, A', 'Roussarie, A', 'Schuller, J P', 'Schwindling, J', 'Trabelsi, A', 'Vallage, B', 'Black, S N', 'Dann, J H', 'Kim, H Y', 'Litke, A M', 'McNeil, M A', 'Taylor, G', 'Booth, C N', 'Boswell, R', 'Brew, C A J', 'Cartwright, S L', 'Combley, F', 'Kelly, M S', 'Lehto, M H', 'Newton, W M', 'Reeve, J', 'Thompson, L F', 'Affholderbach, K', 'Böhrer, A', 'Brandt, S', 'Cowan, G D', 'Foss, J', 'Grupen, Claus', 'Saraiva, P', 'Smolik, L', 'Stephan, F', 'Apollonio, M', 'Bosisio, L', 'Della Marina, R', 'Giannini, G', 'Gobbo, B', 'Musolino, G', 'Pütz, J', 'Rothberg, J E', 'Wasserbaech, S R', 'Williams, R W', 'Armstrong, S R', 'Charles, E', 'Elmer, P', 'Ferguson, D P S', 'González, S', 'Greening, T C', 'Hayes, O J', 'Hu, H', 'Jin, S', 'McNamara, P A', 'Nachtman, J M', 'Nielsen, J', 'Orejudos, W', 'Pan, Y B', 'Saadi, Y', 'Scott, I J', 'Walsh, J', 'Wu Sau Lan', 'Wu, X', 'Yamartino, J M', 'Zobernig, G']",['Search for pair-production of long-lived heavy charged particles in $e^+ e^-$ annihilation'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'new particle, search for', 'charged particle, heavy', 'charged particle, pair production', 'channel cross section, mass', 'upper limit', 'supersymmetry', 'smuon', 'stau', 'chargino', 'sparticle, mass', 'lower limit', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '139, 136, 161, 172 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-041', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706013']","['A search for pair-production of long-lived, heavy, singly-charged particles has been performed with data collected by the ALEPH detector at a centre-of-mass energy of 172 GeV. Data at \\sqrt{s} = 161, 136, and 130 GeV are also included to improve the sensitivity to lower masses. No candidate is found in the data. A model-independent 95 % confidence level upper limit on the production cross section at 172 GeV of 0.2-0.4 pb is derived for masses between 45 and 86 GeV/c^2. This cross section limit implies, assuming the MSSM, a lower limit of 67 (69) GeV/c^2 on the mass of right- (left-) handed long-lived scalar taus or scalar muons and of 86 GeV/c^2 on the mass of long-lived charginos.']",['1997-05-05']
2152,['eng'],"['Abbott, B']",['Color Coherent Radiation in Multijet Events from $p\\overline{p}$ Collisions at $\\sqrt{s}=1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'jet, hadroproduction', 'jet, multiple production', 'gluon, radiation', 'color, interference', 'color, coherence', 'correlation', 'rapidity dependence', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706012'],['We report on a study of color coherence effects in ppbar collisions at a center of mass energy sqrt(s)=1.8 TeV. The data were collected with the D0 detector during the 1992-1993 run of the Fermilab Tevatron Collider. We observe the presence of initial-to-final state color interference with the spatial correlations between soft and hard jets in multijet events in the central and in forward pseudorapidity regions. The results are compared to Monte Carlo simulations with different color coherence implementations and to the predictions of O(alpha_s^3) QCD calculations.'],['1997-06-27']
2153,['eng'],"['Raja, R']",['Top quark mass measurements from the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1997/03/15', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'mass, truth', 'quark, decay', 'final state, (W jet lepton)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706011'],['We review the measurements of the top quark mass by the CDF and D-Zero collaborations using Run I data in excess of 100 inverse picobarns. The D-Zero collaboration has recently updated its measurement of the top quark mass in the lepton + jets channel. The world average of the top quark mass from the CDF and D-Zero measurements in the lepton + jets channel now stands at 175.6 +/- 5.5 GeV/c**2.'],['1997-06-27']
2154,['eng'],"['Würthwein, F']",['B Decays to Two Charmless Pseudoscalar Mesons at CLEO'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1997/03/22', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'eta(958)', 'B+, branching ratio', 'B0, branching ratio', 'upper limit', 'final state, (0charmed particle)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> 2pseudoscalar meson', 'B+ --> eta(958) K+', 'B --> K pi', 'approx. 10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706010'],"[""Using 3.3 Million $B\\bar B$ pairs accumulated with the CLEO detector CLEO has measured ${\\cal B}(B^0\\to K^+\\pi^-) = (1.5^{+ 0.5}_{-0.4}\\pm 0.1\\pm 0.1)\\times 10^{-5}$, ${\\cal B}(B^+\\to K^0\\pi^+) = (2.3^{+1.1}_{-1.0}\\pm 0.2\\pm 0.2)\\times 10^{-5}$, and ${\\cal B}(B^+\\to \\eta^{'}K^+) = (7.8^{+ 2.7}_{-2.2}\\pm 1.0)\\times 10^{-5}$. These constitute the first observations of exclusive $B$\\ decays to charmless hadronic final states. Furthermore, a measurement of ${\\cal B}(B^+\\to h^+\\pi^0) = (1.6^{+ 0.6 +0.3}_{-0.5 -0.2}\\pm 0.1)\\times 10^{-5}$, as well as upper limits on various other $B$ decays to two charmless pseudoscalar mesons are presented. In particular, an upper limit of ${\\cal B}(B^0\\to \\pi^+\\pi^-) < 1.5\\times 10^{-5}$ @ 90%C.L. is placed. All of these results are still preliminary, and averaging over charge conjugate modes is always implied.""]",['1997-06-12']
2155,['eng'],"['Oyama, Y']",['Experimental study of high energy atmospheric neutrinos in Kamiokande'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'neutrino/mu, flux', 'neutrino/e, flux', 'neutrino nucleon, interaction', 'charged current', 'muon, flux', 'angular dependence', 'showers, electromagnetic', 'neutrino, oscillation', 'neutrino, mass difference', 'neutrino, mixing angle', 'upper limit', 'deep underground detector, KAMIOKANDE', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706008'],"['Possible neutrino oscillations are being searched for using high-energy (>~ 10GeV) atmospheric neutrinos in Kamiokande. Both the upward-going muon flux from muon neutrinos and high-energy electro-magnetic shower events from electron neutrinos agree with theoretical expectations, and no positive evidence for neutrino oscillations is found. The 90% C.L. upper limits on the neutrino oscillation parameters, (Delta m^2 and sin^2(2theta)) are found to be Delta m^2 = 5.6 x 10^-3 eV^2 for sin^2(2theta) = 1 and sin^2(2theta) = 0.60 for large Delta m^2 for nu-e <--> nu-mu oscillation. This result excludes most of the allowed region for the nu-e <--> nu-mu oscillation, which was obtained from a recent sub-multi-GeV atmospheric neutrino analysis.']",['1997-06-10']
2156,['eng'],[],['D* Production in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'quark, charm', 'quark, pair production', 'D*(2010), electroproduction', 'D*(2010), hadronic decay', 'channel cross section', 'differential cross section, transverse momentum', 'rapidity dependence', 'energy dependence', 'dependence, momentum transfer', 'quantum chromodynamics, perturbation theory', 'fusion, photon gluon', 'p, structure function', 'structure function, charm', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> D*(2010) positron anything', 'positron p --> 2charm positron anything', 'D*(2010) --> D0 pi+', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706009'],"['This paper presents measurements of D^{*\\pm} production in deep inelastic scattering from collisions between 27.5 GeV positrons and 820 GeV protons. The data have been taken with the ZEUS detector at HERA. The decay channel $D^{*+}\\to (D^0 \\to K^- \\pi^+) \\pi^+ $ (+ c.c.) has been used in the study. The $e^+p$ cross section for inclusive D^{*\\pm} production with $5<Q^2<100 GeV^2$ and $y<0.7$ is 5.3 \\pms 1.0 \\pms 0.8 nb in the kinematic region {$1.3<p_T(D^{*\\pm})<9.0$ GeV and $| \\eta(D^{*\\pm}) |<1.5$}. Differential cross sections as functions of p_T(D^{*\\pm}), $\\eta(D^{*\\pm}), W$ and $Q^2$ are compared with next-to-leading order QCD calculations based on the photon-gluon fusion production mechanism. After an extrapolation of the cross section to the full kinematic region in p_T(D^{*\\pm}) and $\\eta$(D^{*\\pm}), the charm contribution $F_2^{c\\bar{c}}(x,Q^2)$ to the proton structure function is determined for Bjorken $x$ between 2 $\\cdot$ 10$^{-4}$ and 5 $\\cdot$ 10$^{-3}$.']",['1997-06-27']
2157,['eng'],"['Bürgin, R']",['Dijet Production in Photon-Photon Collisions at $\\sqrt{s}_{ee}=161$ and $172 GeV^a$'],['Particle Physics - Experimental Results'],"['talk, Egmond aan Zee 1997/05/10', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'jet, photoproduction', 'final state, (2jet)', 'jet, energy flow', 'photon, resolved', 'angular distribution', 'channel cross section', 'transverse energy, dependence', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> 2jet positron electron', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706007'],['Dijet production is studied in collisions of quasi-real photons radiated by the LEP beams at e+e- centre-of-mass energies sqrt(s)_ee=161 and 172 GeV. Jets are reconstructed using a cone jet finding algorithm in the range |eta(jet)|<2 and E_T(jet)>3 GeV. The angular distributions of direct and double-resolved processes and the inclusive two-jet cross-section are measured. They are compared to next-to-leading order perturbative QCD calculations and the prediction of the leading order Monte Carlo generators PYTHIA and PHOJET.'],['1997-06-05']
2158,['eng'],"['Barate, R', 'Buskulic, D', 'Décamp, D', 'Ghez, Philippe', 'Goy, C', 'Lees, J P', 'Lucotte, A', 'Minard, M N', 'Nief, J Y', 'Pietrzyk, B', 'Casado, M P', 'Chmeissani, M', 'Comas, P', 'Crespo, J M', 'Delfino, M C', 'Fernández, E', 'Fernández-Bosman, M', 'Garrido, L', 'Juste, A', 'Martínez, M', 'Miquel, R', 'Mir, L M', 'Orteu, S', 'Padilla, C', 'Park, I C', 'Pascual, A', 'Perlas, J A', 'Riu, I', 'Sánchez, F', 'Teubert, F', 'Colaleo, A', 'Creanza, D', 'De Palma, M', 'Gelao, G', 'Iaselli, Giuseppe', 'Maggi, G', 'Maggi, M', 'Marinelli, N', 'Nuzzo, S', 'Ranieri, A', 'Raso, G', 'Ruggieri, F', 'Selvaggi, G', 'Silvestris, L', 'Tempesta, P', 'Tricomi, A', 'Zito, G', 'Huang, X', 'Lin, J', 'Ouyang, Q', 'Wang, T', 'Xie, Y', 'Xu, R', 'Xue, S', 'Zhang, J', 'Zhang, L', 'Zhao, W', 'Abbaneo, D', 'Alemany, R', 'Bazarko, A O', 'Becker, U', 'Bright-Thomas, P G', 'Cattaneo, M', 'Cerutti, F', 'Dissertori, G', 'Drevermann, H', 'Forty, Roger W', 'Frank, M', 'Hagelberg, R', 'Hansen, J B', 'Harvey, J', 'Janot, P', 'Jost, B', 'Kneringer, E', 'Knobloch, J', 'Lehraus, Ivan', 'Lutters, G', 'Mato, P', 'Minten, A', 'Moneta, L', 'Pacheco, A', 'Pusztaszeri, J F', 'Ranjard, F', 'Rizzo, G', 'Rolandi, Luigi', 'Rousseau, D', 'Schlatter, D', 'Schmitt, M', 'Schneider, O', 'Tejessy, W', 'Tomalin, I R', 'Wachsmuth, Horst Werner', 'Wagner, A', 'Ajaltouni, Ziad J', 'Barrès, A', 'Boyer, C', 'Falvard, A', 'Ferdi, C', 'Gay, P', 'Guicheney, C', 'Henrard, P', 'Jousset, J', 'Michel, B', 'Monteil, S', 'Montret, J C', 'Pallin, D', 'Perret, P', 'Podlyski, F', 'Proriol, J', 'Rosnet, P', 'Rossignol, J M', 'Fearnley, Tom', 'Hansen, J D', 'Hansen, J R', 'Hansen, P H', 'Nilsson, B S', 'Rensch, B', 'Wäänänen, A', 'Daskalakis, G', 'Kyriakis, A', 'Markou, C', 'Simopoulou, Errietta', 'Siotis, I', 'Vayaki, Anna', 'Blondel, Alain', 'Brient, J C', 'Machefert, F P', 'Rougé, A', 'Rumpf, M', 'Valassi, A', 'Videau, H L', 'Focardi, E', 'Parrini, G', 'Zachariadou, K', 'Cavanaugh, R J', 'Corden, M', 'Georgiopoulos, C H', 'Hühn, T', 'Jaffe, D E', 'Antonelli, A', 'Bencivenni, G', 'Bologna, G', 'Bossi, F', 'Campana, P', 'Capon, G', 'Casper, David William', 'Chiarella, V', 'Felici, G', 'Laurelli, P', 'Mannocchi, G', 'Murtas, F', 'Murtas, G P', 'Passalacqua, L', 'Pepé-Altarelli, M', 'Curtis, L', 'Dorris, S J', 'Halley, A W', 'Knowles, I G', 'Lynch, J G', ""O'Shea, V"", 'Raine, C', 'Scarr, J M', 'Smith, K', 'Teixeira-Dias, P', 'Thompson, A S', 'Thomson, E', 'Thomson, F', 'Turnbull, R M', 'Geweniger, C', 'Graefe, G', 'Hanke, P', 'Hansper, G', 'Hepp, V', 'Kluge, E E', 'Putzer, A', 'Schmidt, M', 'Sommer, J', 'Tittel, K', 'Werner, S', 'Wunsch, M', 'Beuselinck, R', 'Binnie, David M', 'Cameron, W', 'Dornan, Peter J', 'Girone, M', 'Goodsir, S M', 'Martin, E B', 'Morawitz, P', 'Moutoussi, A', 'Nash, J', 'Sedgbeer, J K', 'Spagnolo, P', 'Stacey, A M', 'Williams, M D', 'Ghete, V M', 'Girtler, P', 'Kuhn, D', 'Rudolph, G', 'Betteridge, A P', 'Bowdery, C K', 'Colrain, P', 'Crawford, G', 'Finch, A J', 'Foster, F', 'Hughes, G', 'Jones, R W L', 'Sloan, Terence', 'Whelan, E P', 'Williams, M I', 'Hoffmann, C', 'Jakobs, K', 'Kleinknecht, K', 'Quast, G', 'Renk, B', 'Rohne, E', 'Sander, H G', 'Van Gemmeren, P', 'Zeitnitz, C', 'Aubert, Jean-Jacques', 'Benchouk, C', 'Bonissent, A', 'Bujosa, G', 'Calvet, D', 'Carr, J', 'Coyle, P', 'Diaconu, C A', 'Konstantinidis, N P', 'Leroy, O', 'Motsch, F', 'Payre, P', 'Talby, M', 'Sadouki, A', 'Thulasidas, M', 'Tilquin, A', 'Trabelsi, K', 'Aleppo, M', 'Ragusa, F', 'Berlich, R', 'Blum, Walter', 'Büscher, V', 'Dietl, H', 'Ganis, G', 'Gotzhein, C', 'Kroha, H', 'Lütjens, G', 'Lutz, G', 'Männer, W', 'Moser, H G', 'Richter, R H', 'Rosado-Schlosser, A', 'Schael, S', 'Settles, Ronald', 'Seywerd, H C J', 'Saint-Denis, R', 'Stenzel, H', 'Wiedenmann, W', 'Wolf, G', 'Boucrot, J', 'Callot, O', 'Chen, S', 'Cordier, A', 'Davier, M', 'Duflot, L', 'Grivaz, J F', 'Heusse, P', 'Höcker, A', 'Jacholkowska, A', 'Jacquet, M', 'Kim, D W', 'Le Diberder, F', 'Lefrançois, J', 'Lutz, A M', 'Nikolic, I A', 'Schune, M H', 'Serin, L', 'Simion, S', 'Tournefier, E', 'Veillet, J J', 'Videau, I', 'Zerwas, D', 'Azzurri, P', 'Bagliesi, G', 'Bettarini, S', 'Bozzi, C', 'Calderini, G', 'Ciulli, V', ""Dell'Orso, R"", 'Fantechi, R', 'Ferrante, I', 'Giassi, A', 'Gregorio, A', 'Ligabue, F', 'Lusiani, A', 'Marrocchesi, P S', 'Messineo, A', 'Palla, Fabrizio', 'Sanguinetti, G', 'Sciabà, A', 'Steinberger, Jack', 'Tenchini, Roberto', 'Vannini, C', 'Venturi, A', 'Verdini, P G', 'Blair, G A', 'Bryant, L M', 'Chambers, J T', 'Gao, Y', 'Green, M G', 'Medcalf, T', 'Perrodo, P', 'Strong, J A', 'Von Wimmersperg-Töller, J H', 'Botterill, D R', 'Clifft, R W', 'Edgecock, T R', 'Haywood, S', 'Maley, P', 'Norton, P R', 'Thompson, J C', 'Wright, A E', 'Bloch-Devaux, B', 'Colas, P', 'Kozanecki, Witold', 'Lançon, E', 'Lemaire, M C', 'Locci, E', 'Pérez, P', 'Rander, J', 'Renardy, J F', 'Rosowsky, A', 'Roussarie, A', 'Schuller, J P', 'Schwindling, J', 'Trabelsi, A', 'Vallage, B', 'Black, S N', 'Dann, J H', 'Kim, H Y', 'Litke, A M', 'McNeil, M A', 'Taylor, G', 'Booth, C N', 'Boswell, R', 'Brew, C A J', 'Cartwright, S L', 'Combley, F', 'Kelly, M S', 'Lehto, M H', 'Newton, W M', 'Reeve, J', 'Thompson, L F', 'Affholderbach, K', 'Böhrer, A', 'Brandt, S', 'Cowan, G D', 'Foss, J', 'Grupen, Claus', 'Saraiva, P', 'Smolik, L', 'Stephan, F', 'Apollonio, M', 'Bosisio, L', 'Della Marina, R', 'Giannini, G', 'Gobbo, B', 'Musolino, G', 'Pütz, J', 'Rothberg, J E', 'Wasserbaech, S R', 'Williams, R W', 'Armstrong, S R', 'Charles, E', 'Elmer, P', 'Ferguson, D P S', 'González, S', 'Greening, T C', 'Hayes, O J', 'Hu, H', 'Jin, S', 'McNamara, P A', 'Nachtman, J M', 'Nielsen, J', 'Orejudos, W', 'Pan, Y B', 'Saadi, Y', 'Scott, I J', 'Walsh, J', 'Wu Sau Lan', 'Wu, X', 'Yamartino, J M', 'Zobernig, G']",['Search for sleptons in $e^+ e^-$ collisions at centre-of-mass energies of 161 GeV and 172 GeV'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'supersymmetry', 'search for, slepton', 'mass, slepton', 'lower limit', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706006'],"['The data recorded by the ALEPH experiment at LEP at centre-of-mass energies of 161 GeV and 172 GeV were analysed to search for sleptons, the supersymmetric partners of leptons. No evidence for the production of these particles was found. The number of candidates observed is consistent with the background expected from four-fermion processes and gammagamma-interactions. Improved mass limits at 95% C.L. are reported.']",['1997-06-05']
2159,['eng'],"['Browder, T E']",['A New Upper Limit on the Decay $\\eta \\to e^{+}e^{-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'eta, electroproduction', 'eta, leptonic decay', 'eta, rare decay', 'eta, branching ratio', 'upper limit', 'mass spectrum, (positron electron)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> eta anything', 'eta --> positron electron', 'approx. 10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706005'],"[""We have searched for the rare decay of the eta meson $\\eta \\to e^{+}e^{-}$ using the CLEO II detector. The $\\eta$'s were produced in $e^{+}e^{-}$ collisions with 10 GeV center-of-mass energy at the Cornell Electron Storage Ring (CESR). We find with 90% confidence the upper limit on the branching fraction $B(\\eta \\to e^{+}e^{-}) < 7.7\\times 10^{-5}$. The application of conventional elementary particle theory to this decay predicts a branching fraction of about $10^{-9}$.""]",['1997-06-05']
2160,['eng'],"['Beda, A G', 'Demidova, E V', 'Starostin, A S', 'Voloshin, M B']",['On the Feasibility of Low-Background Ge-NaJ Spectrometer for Neutrino Magnetic Moment Measurement'],['Detectors and Experimental Techniques'],"['neutrino, magnetic moment', 'spectrometer', 'germanium, crystal', 'scintillation counter, sodium-iodide', 'background', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706004'],['We analyze the possibility of using a low-background Ge-NaJ spectrometer in a reactor experiment for a search for neutrino magnetic moment down to $3 \\times 10^{-11}$ of the electron magneton. The properties of the so-far existing Ge low-background spectrometers are discussed and additional sources of background in a reactor experiment at a small depth are estimated. These estimates place specific requirements on the design of the spectrometer. The results of preliminary background measurements at a small depth of 5 m.w.e. with a dedicated spectrometer built in ITEP are reported.'],['1997-06-05']
2161,['eng'],"['Söldner-Rembold, S']",['Search for Single Leptoquark Production in Electron-Photon Scattering at $\\sqrt{s}$ = 161 and 172 GeV'],['Particle Physics - Experimental Results'],"['talk, Egmond aan Zee 1997/05/10', 'electron positron, colliding beams', 'photon electron, interaction', 'search for, leptoquark', 'scalar particle, leptoquark', 'equivalent photon approximation', 'decay, leptoquark', 'charge, leptoquark', 'mass, leptoquark', 'coupling, leptoquark', 'final state, (jet electron)', 'final state, (jet neutrino)', 'transverse energy, missing-energy', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161, 172 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706003'],"['A search for a first generation scalar leptoquark (LQ) has been performed using the data collected by the OPAL detector in 1996 at e+e- centre-of-mass energies sqrt{s} of 161 and 172 GeV. It is assumed that a single leptoquark can be produced in the process eq->LQ, where the initial state quark originates from a hadronic fluctuation of a quasi-real photon which has been radiated by one of the LEP beams. Lower limits at the 95 % confidence level on the mass of a first generation scalar leptoquark of 131 GeV for beta=0.5 and beta=1, coupling values lambda larger than sqrt{4*pi*alpha_em) and leptoquark charges -1/3 or -5/3 are obtained.']",['1997-06-05']
2162,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Berlich, P', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hilse, T', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Howard, R', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Przysiezniak, H', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Rosvick, M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schulz, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['An upper limit on the branching ratio for $\\tau$ decays into seven charged particles'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'tau, pair production', 'final state, (7charged particle)', 'tau, branching ratio', 'upper limit', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '91 GeV-cms']","['http://www.cern.ch/Opal/pubs/paper/index.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707023']","['We have searched for decays of the tau lepton into seven or more charged particles, using data collected with the OPAL detector from 1990 to 1995 in e^+e^- collisions at sqrt(s) ~ M_Z. No candidate events were found and an upper limit on the branching ratio for tau decays into seven charged particles of 1.8 x 10^-5 at the 95% confidence level was determined.']",['1997-05-30']
2163,['eng'],"['Adloff, C']",['Measurement of Event Shape Variables in Deep Inelastic $e^{+}p$ Scattering'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'jet, electroproduction', 'event shape analysis', 'jet, thrust', 'jet, mass', 'kinematics, Breit frame', 'dependence, momentum transfer', 'quantum chromodynamics, perturbation theory', 'effect, nonperturbative', 'strong interaction, coupling constant', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706002'],"['Deep inelastic e^+ scattering data, taken with the H1 detector at HERA are used to study the event shape variables thrust, jet broadening and jet mass in the current hemisphere of the Breit frame over a large range of momentum transfers Q between 7 GeV and 100 GeV. The data are compared with results from e^+e^- experiments. Using second order QCD calculations and an approach to relate hadronisation effects to power corrections an analysis of the Q dependences of the means of the event shape parameters is presented, from which both the power corrections and the strong coupling constant are determined without any assumption on fragmentation models. The power corrections of all event shape variables investigated follow a 1/Q behaviour and can be described by a common parameter alpha_0.']",['1997-06-03']
2164,['eng'],"['Gerdes, D W']",['Top Quark Production and Decay at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1997/03/15', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay modes', 'final state, dilepton', 'final state, ((n)jet lepton)', 'final state, ((n)jet)', 'quark, branching ratio', 'channel cross section', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'truth --> W beauty', 'truth --> W quark', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706001'],"['Recent measurements of the top quark production cross section and decay properties by the CDF and D0 experiments are described. The cross section has been measured in dilepton, lepton plus jets, and all-hadronic final states, and a measurement of $BR(t \\to Wb)/BR(t \\to Wq)$, where $q$ is any quark, has been performed. The results, though statistics-limited, are consistent with each other and with theoretical predictions.']",['1997-06-03']
2165,['eng'],"['Maggipinto, T', 'Nardulli, Giuseppe', 'Dusini, S', 'Ferrari, F', 'Lazzizzera, I', 'Sidoti, A', 'Sartori, A', 'Tecchiolli, G P']",['Role of Neural Networks in the Search of the Higgs Boson at LHC'],['Detectors and Experimental Techniques'],"['p p, inclusive reaction', 'Higgs particle, search for', 'background', 'neural network', 'efficiency', 'Higgs particle, leptonic decay', 'numerical calculations, Monte Carlo', 'p p --> Higgs particle anything', 'Higgs particle --> 2muon+ 2muon-', '1400 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705020'],['We show that neural network classifiers can be used to discriminate Higgs production from background at LHC for $ 150< M_H<200$ GeV. Two different NN are used.'],['1997-06-02']
2166,['eng'],"['Athans, M']",['Measurement of the $\\overline{B}\\to Dl\\overline{\\nu}$ Partial Width and Form Factor Parameters'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'anti-B, width', 'anti-B0, branching ratio', 'B-, branching ratio', 'energy spectrum, missing-energy', 'momentum, missing-energy', 'form factor, slope', 'Kobayashi-Maskawa angle', 'HQET model', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B- --> D0 lepton- antineutrino', 'anti-B0 --> D+ lepton- antineutrino', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705019'],"['We have studied the decay $\\bar{B} \\to D\\ell\\bar{\\nu}$, where $\\ell=e or rate normalization ${\\cal F}_D(1)|V_{cb}|$ and form factor slope fractions are ${\\cal B}(\\bar{B}^0 \\to D^+\\ell^-\\bar{\\nu})=(1.87 \\pm 0.15 \\pm 0.32)%$ and ${\\cal B}(B^- \\to D^0\\ell^-\\bar{\\nu})=(1.94 \\pm 0.15 \\pm 0.34)%$. The form factor parameters are in agreement with those measured in $\\bar{B} \\to D^*\\ell\\bar{\\nu}$ decays, as predicted by heavy quark effective theory.']",['1997-06-02']
2167,['eng'],"['Adloff, C']",['Photoproduction of $K^0$ and $\\Lambda$ at HERA and a Comparison with Deep Inelastic Scattering'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, inelastic scattering', 'positron p, deep inelastic scattering', 'photon p, inclusive reaction', 'Lambda, photoproduction', 'K0(S), photoproduction', 'strange particle, hadronic decay', 'rapidity spectrum', 'transverse momentum, spectra', 'photon, fragmentation', 'differential cross section, momentum transfer', 'nondiffractive', 'quantum chromodynamics, perturbation theory', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'photon p --> Lambda anything', 'photon p --> K0(S) anything', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705018'],"['Two-particle correlations in invariant mass are studied separately for like-sign and unlike-sign charged particles produced in deep inelastic positron-proton scattering in a new kinematical domain. The data were taken with the H1 detector at the HERA storage ring in 1994, in which 27.5 GeV positrons collided with 820 GeV protons at a centre of mass energy sqrt{s}=300 GeV. The observed enhancement of the like-sign correlations at low invariant masses is related to the dimensions of the hadronic source. The data are compared to different QCD models where the hadronization is performed with the string-fragmentation model. Results are presented for the first time separately for diffractive and non-diffractive scattering, in domains of four-momentum transfer, Bjorken-x, and hadronic center of mass energy, and in intervals of charged particle multiplicity. The observed source radii do not differ strongly from those measured in lower energy lepton-nucleon inelastic scattering, and e^+e^- annihilation.']",['1997-05-29']
2168,['eng'],"['Abe, K']",['Measurement of the Neutron Spin Structure Function $g_{2}^{n}$ and Asymmetry $A_{2}^{n}$'],['Particle Physics - Experimental Results'],"['electron nucleus, deep inelastic scattering', 'electron, polarized beam', 'helium, nuclide', 'helium, polarized target', 'n, structure function', 'structure function, spin', 'sum rule, Bjorken', 'effect, higher-twist', 'polarization, longitudinal', 'polarization, transverse', 'polarization, asymmetry', 'magnetic spectrometer, experimental results', 'SLAC Lab', '48.3 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705017'],"['We have measured the neutron structure function g$_{2}^{n}$ and the virtual photon-nucleon asymmetry A$_{2}^{n}$ over the kinematic range $0.014\\leq x \\leq 0.7$ and $1.0 \\leq Q^{2} \\leq 17.0$ by scattering 48.3 GeV longitudinally polarized electrons from polarized $^{3}$He. Results for A$_{2}^{n}$ are significantly smaller than the $\\sqrt{R}$ positivity limit over most of the measured range and data for g$_2^{n}$ are generally consistent with the twist-2 Wandzura-Wilczek prediction. Using our measured g$_{2}^{n}$ we obtain results for the twist-3 reduced matrix element $d_{2}^{n}$, and the integral experiment are combined with existing data for g$_{2}^{n}$ to obtain an average for $d_{2}^{n}$ and the integral $\\int$g$_{2}^{n}(x)dx$.']",['1997-05-26']
2169,['eng'],"['Dissertori, G']",['Measurements of the QCD colour factors at LEP and a limit on the light gluino'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1997/04/21', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'jet, multiplicity', 'quantum chromodynamics, validity test', 'perturbation theory, higher-order', 'operator, Casimir', 'color', 'differential cross section, formula', 'event shape analysis', 'angular distribution, (4jet)', 'gluino', 'strong interaction, coupling constant', 'angular correlation', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=OPEN-97-015', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705016']","['A summary of the measurements of the QCD colour factors at LEP is presented. Such measurements provide a test of the gauge group structure underlying the theory of strong interactions. A variety of methods have been applied by the various experiments, and perfect consistency with the expectation of QCD with SU(3) as gauge group is found.']",['1997-05-22']
2170,['eng'],"['Abbott, B']",['Search for the Trilepton Signature from the Associated Production of SUSY $^\\widetilde{\\chi}_{1}^{\\pm} ^\\widetilde{\\chi}_{2}^{0}$ Gauginos'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'sparticle, search for', 'gaugino, pair production', 'R parity, invariance', 'final state, (3lepton)', 'channel cross section, branching ratio', 'upper limit', 'mass, gaugino', 'mass, dependence', 'transverse energy, missing-energy', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2gaugino anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705015'],"[""We report on a search for the trilepton signature from the associated production of supersymmetric gaugino pairs, Chi_1^(+-) Chi_2^0, within the context of minimal supersymmetric models that conserve R-parity. This search uses 95 pb^-1 of data taken with the \\D0 detector at Fermilab's Tevatron collider at \\sqrt{s} = 1.8 TeV. No evidence of a trilepton signature has been found, and a limit on the production cross section times branching fraction to trileptons as a function of Chi_1^(+-) mass is given.""]",['1997-05-22']
2171,['eng'],"['Adloff, C']",['Proton Dissociative $\\rho$ and Elastic $\\phi$ Electroproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, elastic scattering', 'rho(770), electroproduction', 'Phi(1020), electroproduction', 'diffraction, production', 'p, dissociation', 'factorization, validity test', 'channel cross section, ratio', 'dependence, momentum transfer', 'transverse momentum, dependence', 'mass spectrum, (K+ K-)', 'polarization', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705014'],"['The electroproduction of rho mesons with proton diffractive dissociation for Q^2 > 7 GeV^2 and the elastic electroproduction of Phi mesons for Q^2 > 6 Gev^2 are studied in e^+ p collisions at HERA with the H1 detector, for an integrated luminosity of 2.8 pb-1. The dependence of the cross sections on P_t^2 and Q^2 is measured, and the vector meson polarisation obtained. The cross section ratio between proton dissociative and elastic production of rho mesons is measured and discussed in the framework of the factorisation hypothesis of diffractive vertices. The ratio of the elastic cross section for Phi and rho meson production is investigated as a function of Q^2.']",['1997-05-22']
2172,['eng'],"['Burrows, P N']",['Precise Tests of QCD in $e^+ e^-$ Annihilation'],['Particle Physics - Experimental Results'],"['lectures, Stanford 1996/08/19', 'electron positron, annihilation', 'electron positron, colliding beams', 'hadron, multiple production', 'quantum chromodynamics, validity test', 'quark, pair production', 'gluon, radiation', 'jet, multiplicity', 'coupling', 'Feynman graph', 'cross section, hadronic', 'strong interaction, coupling constant', 'Z0, hadronic decay', 'Z0, width', 'tau, semileptonic decay', 'model, hadronization', 'perturbation theory', 'renormalization', 'fragmentation function', 'scaling, violation', 'energy dependence', 'mass, truth', 'experimental results', 'bibliography', '((1)) ((2)) ((3)) ((4)) ((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705013'],"['A pedagogical review is given of precise tests of QCD in electron-positron annihilation. Emphasis is placed on measurements that have served to establish QCD as the correct theory of strong interactions, as well as measurements of the coupling parameter alpha-s. An outlook is given for future important tests at a high energy e+e- collider.']",['1997-05-20']
2173,['eng'],"['Alexander, J P']",['Determination of the Michel Parameters and the $\\tau$ Neutrino Helicity in $\\tau$ Decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, semileptonic decay', 'tau, leptonic decay', 'neutrino/tau, helicity', 'Michel parameter', 'model, weak interaction', 'symmetry, left-right', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> tau+ tau-', 'tau- --> lepton- neutrino/tau antineutrino', 'tau- --> pi- pi0 neutrino/tau', 'approx. 10 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705009'],"['Using the CLEO II detector at the $e^+e^-$ storage ring CESR, we have determined the Michel parameters $\\rho$, $\\xi$, and $\\delta$ in $\\tau^\\mp \\to l^\\mp\\nu\\bar{\\nu}$ decay as well as the tau neutrino helicity parameter $h_{\\nu_\\tau}$ in $\\tau^\\mp \\to \\pi^\\mp\\pi^0\\nu$ decay. From a data sample of $3.02\\times 10^6$ tau pairs produced at $\\sqrt{s}=10.6 GeV$, using events of the topology $e^+e^- \\to \\tau^+\\tau^- \\to (l^\\pm\\nu\\bar{\\nu}) result of the three samples is: $\\rho = 0.747\\pm 0.010\\pm 0.006$, $\\xi = 1.007\\pm 0.040\\pm 0.015$, $\\xi\\delta = 0.745\\pm 0.026\\pm 0.009$, and $h_{\\nu_\\tau} = -0.995\\pm 0.010\\pm 0.003$. The results are in agreement with the Standard Model V-A interaction.']",['1997-05-16']
2174,['eng'],"['Abbott, B']",['Limits on $WWZ$ and $WW\\gamma$ couplings from $p\\overline{p} \\to e \\nu jjX$ events at $\\sqrt{s} = 1.8 TeV$'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'intermediate boson, pair production', 'W, hadroproduction', 'Z0, hadroproduction', 'coupling, (2W photon)', 'coupling, (Z0 2W)', 'intermediate boson, hadronic decay', 'jet, pair production', 'W, leptonic decay', 'invariance, CP', 'transverse momentum, spectra', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', 'anti-p p --> Z0 W anything', 'anti-p p --> 2jet electron neutrino anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705010'],"['We present limits on anomalous WWZ and WW-gamma couplings from a search for WW and WZ production in p-bar p collisions at sqrt(s)=1.8 TeV. We use p-bar p -> e-nu jjX events recorded with the D0 detector at the Fermilab Tevatron Collider during the 1992-1995 run. The data sample corresponds to an integrated luminosity of 96.0+-5.1 pb^(-1). Assuming identical WWZ and WW-gamma coupling parameters, the 95% CL limits on the CP-conserving couplings are -0.33<lambda<0.36 (Delta-kappa=0) and -0.43<Delta-kappa<0.59 (lambda=0), for a form factor scale Lambda = 2.0 TeV. Limits based on other assumptions are also presented.']",['1997-05-16']
2175,['eng'],"['Dusini, S', 'Ferrari, F', 'Lazzizzera, I', 'Lee, P', 'Sartori, A', 'Sidoti, A', 'Tecchiolli, G P', 'Zorat, A']",['Totem'],['Detectors and Experimental Techniques'],"['talk, Berlin 1997/04/07', 'microprocessor', 'trigger', 'track data analysis', 'signal processing', 'p p, interaction', 'Higgs particle, search for', 'performance']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705008'],"['It is being proved that the neurochip \\Totem{} is a viable solution for high quality and real time computational tasks in HEP, including event classification, triggering and signal processing. The architecture of the chip is based on a ""derivative free"" algorithm called Reactive Tabu Search (RTS), highly performing even for low precision weights. ISA, VME or PCI boards integrate the chip as a coprocessor in a host computer. This paper presents: 1) the state of the art and the next evolution of the design of \\Totem{}; 2) its ability in the Higgs search at LHC as an example.']",['1997-05-14']
2176,['eng'],"['Bolton, T']",['High Energy Muon Momentum Estimation from Multiple Coulomb Scattering in Dense Detectors'],['Detectors and Experimental Techniques'],"['muon, tracks', 'muon, momentum', 'calorimeter', 'multiple scattering, Coulomb', 'drift chamber, alignment', 'magnetic field', 'spatial resolution, finite', 'neutrino nucleon, interaction', 'charged current', 'momentum resolution', 'statistical analysis', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705007'],"['A method is described for estimating muon track momentum from the distribution of hits along tracks in dense calorimeters due to multiple Coulomb scattering (MCS). The method requires only well-aligned conventional drift chambers or similar tracking devices and can be implemented with or without a magnetic field present. Neutrino experiments can use this technique to increase acceptance for large angle charged-current scattering events. Resolutions in a typical detector geometry vary from ~10% at p=20 GeV/c to ~50% for p=500 GeV/c, if the number of hits on the track is sufficient.']",['1997-05-12']
2177,['eng'],"['Barish, B C']",['First Observation of Inclusive $B$ Decays to the Charmed Strange Baryons $\\Xi_{c}^{0}$ and $\\Xi_{c}^{+}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, decay modes', 'charmed baryon, production', 'charmed baryon, hadronic decay', 'Xi/c0, branching ratio', 'Xi/c+, branching ratio', 'mass spectrum, (Xi- pi+ pi-)', 'mass spectrum, (Xi- pi+)', 'charmed baryon, momentum spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> Xi/c+ anything', 'B --> Xi/c0 anything', 'Xi/c+ --> Xi- pi+ pi-', 'Xi/c0 --> Xi- pi+', 'approx. 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705005'],"['Using data collected in the region of the Upsilon(4S) resonance with the CLEO II detector operating at the Cornell Electron Storage Ring CESR, we present the first observation of B mesons decaying into the charmed strange baryons Xi_c0 and Xi_c+. We find 79 +/- 27 Xi_c0 and 125 +/- 28 Xi_c+ candidates from B decays, leading to product branching fractions of BR(Bbar -> Xi_c0 X)BR(Xi_c0 -> Xi- pi+) = (0.144 +/- 0.048 +/- 0.021) x 10^-3 and BR(Bbar -> Xi_c+ X)BR(Xi_c+ -> Xi- pi+ pi+) = (0.453 +/- 0.096 +0.085-0.065) x 10^-3.']",['1997-05-09']
2178,['eng'],"['Balest, R']",['Observation of the Decay $D_{s}^{+}\\to \\omega\\pi^{+}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D/s+, electroproduction', 'D/s+, hadronic decay', 'D/s+, branching ratio', 'mass spectrum, (omega(783) pi+)', 'mass spectrum, (eta pi+)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D/s+ --> omega(783) pi+', 'D/s+ --> eta pi+', 'approx. 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705006'],"['Using e+e- annihilation data collected by the CLEO~II detector at CESR, we have observed the decay Ds+ to omega pi+. This final state may be produced through the annihilation decay of the Ds+, or through final state interactions. We find a branching ratio of [Gamma(Ds+ to omega pi+)/Gamma(Ds+ to eta pi+)]=0.16+-0.04+-0.03, where the first error is statistical and the second is systematic.']",['1997-05-09']
2179,['eng'],"['Astafyeva, N M', 'Dremin, I M', 'Kotelnikov, K A']",['Pattern Recognition in High Multiplicity Events'],['Detectors and Experimental Techniques'],"['track data analysis', 'multiplicity, high', 'transformation, wavelet', 'nucleus nucleus, nuclear reaction', 'lead', 'charged particle, multiple production', 'rapidity spectrum', 'jet', 'numerical calculations', 'interpretation of experiments, CERN SPS Coll', '158 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705003'],"['In very high energy collisions, many particles are produced and distributed in the available phase space volume in various ways. With advent of new accelerator facilities (especially, for nucleus-nucleus collisions), the problem of pattern recognition in high multiplicity events becomes very actual in order to classify such events and to separate those of them with some special features (e.g. ring-like events, jets and other regular patterns). This paper presents the first attempt to use wavelet technique for pattern recognition in nucleus-nucleus collisions. After describing the method in general, we demonstrate its power by applying it to a single event of Pb-Pb collision at 158A GeV with 1072 charged particles produced and discuss results obtained for some other events. Further extension of the method is proposed.']",['1997-05-08']
2180,['eng'],"['Dittmar, Michael', 'Pauss, Felicitas', 'Zürcher, D']",['Towards a Precise Parton Luminosity Determination at the CERN LHC'],['Detectors and Experimental Techniques'],"['p p, storage ring', 'luminosity, parton', 'luminosity, monitoring', 'p p, inclusive reaction', 'p, structure function', 'intermediate boson, hadroproduction', 'intermediate boson, leptonic decay', 'lepton, rapidity spectrum', 'momentum spectrum, parton', 'quark, valence', 'quark, sea', 'gluon', 'numerical calculations, Monte Carlo', 'CERN LHC Coll']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705004', 'http://documents.cern.ch/archive/electronic/other/uploader/LHC98/dittmar.ps.gz']","['A new approach to determine the LHC luminosity is investigated. Instead of employing the proton-proton luminosity measurement, we suggest to measure directly the parton-parton luminosity. It is shown that the electron and muon pseudorapidity distributions, originating from the decay of W+, W- and Z0 bosons produced at 14 TeV pp collisions (LHC), constrain the x distributions of sea and valence quarks and antiquarks in the range from about 3 x 10**-4 to about 10**-1 at a Q**2 of about 10**4 GeV**2. Furthermore, it is demonstrated that, once the quark and antiquark structure functions are constrained from the W+,W- and Z0 production dynamics, other quark-antiquark related scattering processes at the LHC like q-qbar --> W+W- can be predicted accurately. Thus, the lepton pseudorapidity distributions provide the key to a precise parton luminosity monitor at the LHC, with accuracies of about +-1% compared to the so far considered goal of +-5%.']",['1997-05-08']
2181,['eng'],"['Kaplan, D M']",['A Future Charm Facility'],['Detectors and Experimental Techniques'],"['talk, Santa Monica 1997/02/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'charmed particle, hadroproduction', 'charmed particle, decay modes', 'charmed particle, rare decay', 'violation, CP', 'neutral current, flavor changing', 'lepton number, violation', 'D0 anti-D0, interference', 'magnetic spectrometer, proposed', 'proposed experiment, Batavia TEVATRON Coll', '2000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705002'],"['The ""BTeV/C0"" experiment at Fermilab could reconstruct >10^9 charm decays, four orders of magnitude beyond the largest extant sample. The experiment is likely to run during Tevatron Run II (ca. 2000--2005). In addition to ""programmatic"" charm physics such as spectroscopy, lifetimes, and QCD tests, it will have significant new-physics reach in the areas of CP violation, flavor-changing neutral-current and lepton-number-violating decays, and $D^0\\bar{D^0}$ mixing, and could observe direct CP violation in Cabibbo-suppressed D decays if it occurs at the level predicted by the Standard Model.']",['1997-05-05']
2182,['eng'],"['Adloff, C', 'Charlet, M']",['Bose-Einstein Correlations in Deep Inelastic $e^{+}p$ Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, electroproduction', 'correlation, two-particle', 'charge correlation', 'boson, statistics', 'diffraction', 'nondiffractive', 'quantum chromodynamics', 'string model, fragmentation', 'multiplicity, dependence', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9705001'],"['Two-particle correlations in invariant mass are studied separately for like-sign and unlike-sign charged particles produced in deep inelastic positron-proton scattering in a new kinematical domain. The data were taken with the H1 detector at the HERA storage ring in 1994, in which 27.5 GeV positrons collided with 820 GeV protons at a centre of mass energy sqrt{s}=300 GeV. The observed enhancement of the like-sign correlations at low invariant masses is related to the dimensions of the hadronic source. The data are compared to different QCD models where the hadronization is performed with the string-fragmentation model. Results are presented for the first time separately for diffractive and non-diffractive scattering, in domains of four-momentum transfer, Bjorken-x, and hadronic center of mass energy, and in intervals of charged particle multiplicity. The observed source radii do not differ strongly from those measured in lower energy lepton-nucleon inelastic scattering, and e^+e^- annihilation.']",['1997-05-05']
2183,['eng'],"['Glenzinski, D A']",['Recent LEP 2 Results from OPAL'],['Particle Physics - Experimental Results'],"['talk, Cracow 1997/01/04', 'electron positron, colliding beams', 'electron positron, annihilation', 'event shape analysis', 'quantum chromodynamics', 'electroweak interaction, validity test', 'fermion, pair production', 'new particle, search for', 'Higgs particle', 'chargino', 'neutralino', 'final state, (4jet)', 'mass spectrum, (2jet)', 'W, pair production', 'W, mass', 'cross section, energy dependence', 'coupling, (3gauge boson)', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', '161.3 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704019'],"['In 1996, after another set of upgrades, LEP began running for the first time at center-of-mass energies above the W-pair production threshold. This new energy regime is rich in physics and offers new tests of the Standard Model, increased sensitivity for search physics, and precision W physics. We summarize the recent results from OPAL using 9.9 pb^-1 of data collected at \\sqrt s = 161.3 GeV from June to August 1996.']",['1997-05-01']
2184,['eng'],"['Ackerstaff, K', 'Alexander, Gideon', 'Allison, J', 'Altekamp, N', 'Anderson, K J', 'Anderson, S', 'Arcelli, S', 'Asai, S', 'Axen, D A', 'Azuelos, G', 'Ball, A H', 'Barberio, E', 'Barlow, R J', 'Bartoldus, R', 'Batley, J R', 'Baumann, S', 'Bechtluft, J', 'Beeston, C', 'Behnke, T', 'Bell, A N', 'Bell, K W', 'Bella, G', 'Bentvelsen, S', 'Berlich, P', 'Bethke, Siegfried', 'Biebel, O', 'Biguzzi, A', 'Bird, S D', 'Blobel, Volker', 'Bloodworth, Ian J', 'Bloomer, J E', 'Bobinski, M', 'Bock, P', 'Bonacorsi, D', 'Boutemeur, M', 'Bouwens, B T', 'Braibant, S', 'Brigliadori, L', 'Brown, R M', 'Burckhart, H J', 'Burgard, C', 'Bürgin, R', 'Capiluppi, P', 'Carnegie, R K', 'Carter, A A', 'Carter, J R', 'Chang, C Y', 'Charlton, D G', 'Chrisman, D', 'Clarke, P E L', 'Cohen, I', 'Conboy, J E', 'Cooke, O C', 'Cuffiani, M', 'Dado, S', 'Dallapiccola, C', 'Dallavalle, G M', 'De Jong, S', 'del Pozo, L A', 'Desch, K', 'Dixit, M S', 'do Couto e Silva, E', 'Doucet, M', 'Duchovni, E', 'Duckeck, G', 'Duerdoth, I P', 'Eatough, D', 'Edwards, J E G', 'Estabrooks, P G', 'Evans, H G', 'Evans, M', 'Fabbri, F L', 'Fanti, M', 'Faust, A A', 'Fiedler, F', 'Fierro, M', 'Fischer, H M', 'Fleck, I', 'Folman, R', 'Fong, D G', 'Foucher, M', 'Fürtjes, A', 'Futyan, D I', 'Gagnon, P', 'Gary, J W', 'Gascon, J', 'Gascon-Shotkin, S M', 'Geddes, N I', 'Geich-Gimbel, C', 'Geralis, T', 'Giacomelli, Giorgio', 'Giacomelli, P', 'Giacomelli, R', 'Gibson, V', 'Gibson, W R', 'Gingrich, D M', 'Glenzinski, D A', 'Goldberg, J', 'Goodrick, M J', 'Gorn, W', 'Grandi, C', 'Gross, E', 'Grunhaus, J', 'Gruwé, M', 'Hajdu, C', 'Hanson, G G', 'Hansroul, M', 'Hapke, M', 'Hargrove, C K', 'Hart, P A', 'Hartmann, C', 'Hauschild, M', 'Hawkes, C M', 'Hawkings, R', 'Hemingway, Richard J', 'Herndon, M', 'Herten, G', 'Heuer, R D', 'Hildreth, M D', 'Hill, J C', 'Hillier, S J', 'Hilse, T', 'Hobson, P R', 'Homer, R James', 'Honma, A K', 'Horváth, D', 'Howard, R', 'Hutchcroft, D E', 'Igo-Kemenes, P', 'Imrie, D C', 'Ingram, M R', 'Ishii, K', 'Jawahery, A', 'Jeffreys, P W', 'Jeremie, H', 'Jimack, Martin Paul', 'Joly, A', 'Jones, C R', 'Jones, G', 'Jones, M', 'Jost, U', 'Jovanovic, P', 'Junk, T R', 'Karlen, D A', 'Kartvelishvili, V G', 'Kawagoe, K', 'Kawamoto, T', 'Keeler, Richard K', 'Kellogg, R G', 'Kennedy, B W', 'Kirk, J', 'Klier, A', 'Kluth, S', 'Kobayashi, T', 'Kobel, M', 'Koetke, D S', 'Kokott, T P', 'Kolrep, M', 'Komamiya, S', 'Kress, T', 'Krieger, P', 'Von Krogh, J', 'Kyberd, P', 'Lafferty, G D', 'Lahmann, R', 'Lai, W P', 'Lanske, D', 'Lauber, J', 'Lautenschlager, S R', 'Layter, J G', 'Lazic, D', 'Lee, A M', 'Lefebvre, E', 'Lellouch, Daniel', 'Letts, J', 'Levinson, L', 'Lloyd, S L', 'Loebinger, F K', 'Long, G D', 'Losty, Michael J', 'Ludwig, J', 'Macchiolo, A', 'Macpherson, A L', 'Mannelli, M', 'Marcellini, S', 'Markus, C', 'Martin, A J', 'Martin, J P', 'Martínez, G', 'Mashimo, T', 'Mättig, P', 'McDonald, W J', 'McKenna, J A', 'Mckigney, E A', 'McMahon, T J', 'McPherson, R A', 'Meijers, F', 'Menke, S', 'Merritt, F S', 'Mes, H', 'Meyer, J', 'Michelini, Aldo', 'Mikenberg, G', 'Miller, D J', 'Mincer, A', 'Mir, R', 'Mohr, W', 'Montanari, A', 'Mori, T', 'Morii, M', 'Müller, U', 'Nagai, K', 'Nakamura, I', 'Neal, H A', 'Nellen, B', 'Nisius, R', ""O'Neale, S W"", 'Oakham, F G', 'Odorici, F', 'Ogren, H O', 'Oldershaw, N J', 'Oreglia, M J', 'Orito, S', 'Pálinkás, J', 'Pásztor, G', 'Pater, J R', 'Patrick, G N', 'Patt, J', 'Pearce, M J', 'Petzold, S', 'Pfeifenschneider, P', 'Pilcher, J E', 'Pinfold, James L', 'Plane, D E', 'Poffenberger, P R', 'Poli, B', 'Posthaus, A', 'Przysiezniak, H', 'Rees, D L', 'Rigby, D', 'Robertson, S', 'Robins, S A', 'Rodning, N L', 'Roney, J M', 'Rooke, A M', 'Ros, E', 'Rossi, A M', 'Rosvick, M', 'Routenburg, P', 'Rozen, Y', 'Runge, K', 'Runólfsson, O', 'Ruppel, U', 'Rust, D R', 'Rylko, R', 'Sachs, K', 'Saeki, T', 'Sarkisian, E K G', 'Sbarra, C', 'Schaile, A D', 'Schaile, O', 'Scharf, F', 'Scharff-Hansen, P', 'Schenk, P', 'Schieck, J', 'Schleper, P', 'Schmitt, B', 'Schmitt, S', 'Schöning, A', 'Schröder, M', 'Schultz-Coulon, H C', 'Schulz, M', 'Schumacher, M', 'Schwick, C', 'Scott, W G', 'Shears, T G', 'Shen, B C', 'Shepherd-Themistocleous, C H', 'Sherwood, P', 'Siroli, G P', 'Sittler, A', 'Skillman, A', 'Skuja, A', 'Smith, A M', 'Snow, G A', 'Sobie, Randall J', 'Söldner-Rembold, S', 'Springer, R W', 'Sproston, M', 'Stephens, K', 'Steuerer, J', 'Stockhausen, B', 'Stoll, K', 'Strom, D', 'Szymanski, P', 'Tafirout, R', 'Talbot, S D', 'Tanaka, S', 'Taras, P', 'Tarem, S', 'Teuscher, R J', 'Thiergen, M', 'Thomson, M A', 'von Törne, E', 'Towers, S', 'Trigger, I', 'Tsur, E', 'Turcot, A S', 'Turner-Watson, M F', 'Utzat, P', 'Van Kooten, R', 'Verzocchi, M', 'Vikas, P', 'Vokurka, E H', 'Voss, H', 'Wäckerle, F', 'Wagner, A', 'Ward, C P', 'Ward, D R', 'Watkins, P M', 'Watson, A T', 'Watson, N K', 'Wells, P S', 'Wermes, N', 'White, J S', 'Wilkens, B', 'Wilson, G W', 'Wilson, J A', 'Wolf, G', 'Wyatt, T R', 'Yamashita, S', 'Yekutieli, G', 'Zacek, V', 'Zer-Zion, D']",['A study of B meson oscillations using hadronic $Z^0$ decays containing leptons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'B0 anti-B0, oscillation', 'B0, mass difference', 'B/s0 anti-B/s0, oscillation', 'B/s0, mass difference', 'particle identification, flavor', 'B0, semileptonic decay', 'decay, time', 'jet, charge', 'lepton, charge', 'charge, symmetry breaking', 'violation, CP', 'violation, CPT', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']","['http://www.cern.ch/Opal/pubs/paper/index.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707009']","['An event sample enriched in semileptonic decays of b hadrons is selected using an inclusive lepton selection from approximately 3.0 million hadronic Z^0 decays collected with the OPAL detector. This sample is used to investigate B meson oscillations by reconstructing a proper decay time for the parent of each lepton, using a jet charge method to estimate the production flavour of this parent, and using the lepton charge to tag the decay flavour. We measure the mass difference between the two B^0_d mass eigenstates Delta(m_d) = 0.444 +/- 0.029 + 0.020 - 0.017 ps^-1. For the B^0_s system, we find Delta(m_s) > 3.1 ps ^-1 at the 95% confidence level. This limit varies only a little if alternative limit setting approaches are adopted. Regions at higher Delta(m_s) are also excluded with some methods for setting the limit. By studying the charge symmetry of the B^0_d mixing structure, we are able to constrain possible CP and CPT violating effects. We measure the CP violation parameter Re(epsilon_B) = -0.006 +/- 0.010 +/- 0.006 and the indirect CPT violating parameter Im(delta_B) = -0.020 +/- 0.016 +/- 0.006. If we invoke CPT symmetry, then we obtain Re(epsilon_B) = 0.002 +/- 0.007 +/- 0.003.']",['1997-04-28']
2185,['eng'],"['Marti i Garcia, S']",['Review of the measurements of the strong coupling constant at LEP 2'],['Particle Physics - Experimental Results'],"['talk, Chicago 1997/04/14', 'electron positron, colliding beams', 'electron positron, annihilation', 'quark, pair production', 'jet, multiple production', 'strong interaction, coupling constant', 'event shape analysis', 'energy dependence', 'experimental results', 'CERN LEP Stor', '91, 133, 161, 176 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704016'],"['Since 1995, LEP has steadily increased the center of mass energy of the colliding beams, from the M_Z resonance to 133, 161 and 172 GeV. New measurements of the strong coupling constant, alpha_s, at these energies have been performed by the LEP experiments, L3, ALEPH, OPAL and DELPHI. In this article, the new results are summarized, and combined with the previous LEP measurement of alpha_s(M_Z) in order to obtain an updated LEP average of alpha_s(M_Z) = 0.120 +- 0.005.']",['1997-04-29']
2186,['eng'],"['Gibbons, L K']",['Status of weak quark mixing'],['Particle Physics - Experimental Results'],"['review, Warsaw 1996/07/25', 'Kobayashi-Maskawa angle', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'B0, mass difference', 'B/s0, mass difference', 'B, rare decay', 'K, rare decay', 'B, semileptonic decay', 'electron positron, annihilation', 'anti-p p, interaction', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704017'],['The experimental status of the Cabibbo-Kobayashi-Maskawa matrix is reviewed. Measurements discussed include B0_(s)-\\bar{B}0_(s) mixing and several rare B and K decays with implications for |V_td| and |V_ts|. Extraction of |V_cb| and |V_ub| from studies of semileptonic B decay is also discussed.'],['1997-04-29']
2187,['eng'],"['Asner, D M']",['Search for the Decays $B^0 \\to D^{(*)+} D^{(*)-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, hadronic decay', 'D*(2010)', 'B0, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> 2D*(2010)', 'B0 --> D*(2010) D', 'B0 --> D+ D-', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704014'],"['Using the CLEO-II data set we have searched for the Cabibbo-suppressed decays B^0 -> D^{(*)+} D^{(*)-}. For the decay B^0 -> D^{*+} D^{*-}, we observe one candidate signal event, with an expected background of 0.022 +/- 0.011 events. This yield corresponds to a branching fraction of Br(B^0 -> D^{*+} D^{*-}) = (5.3^{+7.1}_{-3.7}(stat) +/- 1.0(syst)) x 10^{-4} and an upper limit of Br(B^0 -> D^{*+} D^{*-}) < 2.2 x 10^{-3} at the 90% CL. For B^0 -> D^{*\\pm} D^\\mp and B^0 -> D^+ D^-, no significant excess of signal above the expected background level is seen, and we calculate the 90% CL upper limits on the branching fractions to be Br(B^0 -> D^{*\\pm} D^\\mp) < 1.8 x 10^{-3} and Br(B^0 -> D^+ D^-) < 1.2 x 10^{-3}.']",['1997-04-28']
2188,['eng'],"['Abachi, S']",['Measurement of the Top Quark Pair Production Cross Section in $p\\overline{p}$ Collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, dilepton', 'final state, ((n)jet lepton)', 'channel cross section, mass', 'mass, truth', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704015'],"['We present a measurement of the ttbar production cross section in ppbar collisions at root(s) = 1.8TeV by the D0 experiment at the Fermilab Tevatron. The measurement is based on data from an integrated luminosity of approximately 125 pb^-1 accumulated during the 1992-1996 collider run. We observe 39 ttbar candidate events in the dilepton and lepton+jets decay channels with an expected background of 13.7+-2.2 events. For a top quark mass of 173.3GeV/c^2, we measure the ttbar production cross section to be 5.5+-1.8 pb.']",['1997-04-28']
2189,['eng'],"['Bonvicini, G']",['Search for Neutrinoless $\\tau$ Decays Involving $\\pi^{0}$ or $\\eta$ Mesons'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, pair production', 'tau, rare decay', 'decay, search for', 'final state, (0neutrino)', 'pseudoscalar meson, production', 'pi0', 'eta', 'tau, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau --> pseudoscalar meson lepton', 'tau --> 2pseudoscalar meson lepton', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704010'],"['We have searched for lepton family number violating decays of the $\\tau$ lepton using final states with an electron or a muon and one or more $\\pi^0$ or the CLEO II detector at the Cornell Electron Storage Ring (CESR) and correspond to an integrated luminosity of 4.68 $fb^{-1}$. No evidence for signals was found, resulting in much improved limits on the branching fractions for the one-meson modes and the first upper limits for the two-meson modes.']",['1997-04-21']
2190,['eng'],"['Derrick, Malcolm']",['Study of Photon Dissociation in Diffractive Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'photon p, interaction', 'hadron, photoproduction', 'diffraction, production', 'photon, dissociation', 'cross section, ratio', 'mass spectrum', 'rapidity, gap', 'Regge poles, triple-Regge limit', 'exchange, pomeron', 'exchange, Regge', 'nondiffractive', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300.3 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704008'],"['Diffractive dissociation of quasi-real photons at a photon-proton centre of mass energy of W ~ 200 GeV is studied with the ZEUS detector at HERA. The process under consideration is gamma p -> X N, where X is the diffractively dissociated photon system of mass M_X and N is either a proton or a nucleonic system with mass M_N < 2GeV. The cross section for this process in the interval 3 < M_X < 24 GeV relative to the total photoproduction cross section was measured to be sigma^partial_D / sigma_tot = 6.2 +- 0.2(stat) +- 1.4(syst)%. After extrapolating this result to the mass interval of m_phi^2 < M_X^2 < 0.05 W^2 and correcting it for proton dissociation, the fraction of the total cross section attributed to single diffractive photon dissociation, gamma p -> X p, is found to be sigma_SD / sigma_tot = 13.3 +- 0.5(stat) +- 3.6(syst)%. The mass spectrum of the dissociated photon system in the interval 8 < M_X < 24 GeV can be described by the triple pomeron (PPP) diagram with an effective pomeron intercept of alpha_P(0) = 1.12 +- 0.04(stat) +- 0.08(syst). The cross section for photon dissociation in the range 3 < M_X < 8 GeV is significantly higher than that expected from the triple pomeron amplitude describing the region 8 < M_X < 24 GeV. Assuming that this discrepancy is due to a pomeron-pomeron-reggeon (PPR) term, its contribution to the diffractive cross section in the interval 3 < M_X < 24 GeV is estimated to be f_PPR = 26 +- 3(stat) +- 12(syst)%.']",['1997-04-18']
2191,['eng'],"['Crittenden, J A']",['Exclusive Production of Neutral Vector Mesons at the Electron-Proton Collider HERA'],['Particle Physics - Experimental Results'],"['review, experimental results', 'positron p, colliding beams', 'electron p, colliding beams', 'electron p, deep inelastic scattering', 'photon p, exclusive reaction', 'hadron, electroproduction', 'vector meson, photoproduction', 'vector meson, decay modes', 'small-x', 'channel cross section, energy dependence', 'rho(770)0', 'omega(783)', 'Phi(1020)', 'J/psi(3100)', 'psi(3685)', 'yield, ratio', 'dependence, momentum transfer', 'differential cross section, slope', 'helicity, amplitude analysis', 'p, dissociation', 'Regge poles', 'angular distribution', 'magnetic detector, ZEUS', 'magnetic detector, H1', 'upgrade, proposed', 'polarized beam', 'ion, beam', 'DESY HERA Stor', 'bibliography', 'electron p --> vector meson p electron', '((5)) ((6))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704009'],"['The first five years of operation of the multi-purpose experiments ZEUS and H1 at the electron-proton storage ring facility HERA have opened a new era in the study of vector-meson production in high-energy photon-proton interactions. The high center-of-mass energy available at this unique accelerator complex allows investigations in hitherto unexplored kinematic regions, providing answers to long-standing questions concerning the energy-dependence of the rho, omega, phi, and J/psi production cross sections. The excellent angular acceptance of these detectors, combined with that of specialized tagging detectors at small production angles, has permitted measurements of elastic and inelastic production processes for both quasi-real photons and those of virtuality exceeding the squared mass of the vector meson. This report provides a quantitative picture of the present status of these studies, comparing them to the extensive measurements in this field at lower energies and summarizing topical developments in theoretical work motivated by the new data.']",['1997-04-18']
2192,['eng'],"['Abe, F']",['The $\\mu\\tau$ and $e\\tau$ Decays of Top Quark Pairs Produced in $p\\overline{p}$ Collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'quark, decay', 'final state, dilepton', 'tau, semileptonic decay', 'particle identification, beauty', 'channel cross section', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', 'W --> tau neutrino/tau', 'tau --> (n)hadron neutrino/tau', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704007'],"['We present evidence for dilepton events from t tbar production with one electron or muon and one hadronically decaying tau lepton from the decay t tbar -> (l nu_l) (tau nu_tau) b bbar, (l=e, mu), using the Collider Detector at Fermilab (CDF). In a 109 pb^-1 data sample of p pbar collisions at sqrt(s) = 1.8 TeV we expect ~1 signal event and a total background of ~2 events; we observe 4 candidate events (2 e tau and 2 mu tau). Three of these events have jets identified as b candidates, compared to an estimated background of 0.28+-0.02 events.']",['1997-04-16']
2193,['eng'],"['Wolf, G']",['The Kinematics of Deep Inelastic Scattering in the Presence of Initial State Radiation'],['Particle Physics - Experimental Results'],"['data analysis method', 'lepton nucleon, deep inelastic scattering', 'radiation, initial-state interaction', 'hadron, electroproduction', 'kinematics', 'energy spectrum', 'angular distribution', 'photon, energy', 'forward scattering', 'momentum transfer', 'x-dependence', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704006'],"['Initial state radiation (ISR) in deep inelastic scattering of charged leptons on nucleons can lead to substantial shifts in the reconstruction of $Q^2$ and the scaling variables $x$ and $y$. By measuring at least three out of the four variables: energy and production angle of the lepton and the hadron system, the energy of the ISR photon emitted under zero degrees can be determined. The ISR effect is illustrated for experimentation at HERA with different methods of kinematic reconstruction.']",['1997-04-14']
2194,['eng'],"['Mallot, G K']",['Spin structure functions'],['Particle Physics - Experimental Results'],"['talk, Mexico City 1996/06/19', 'talk, Amsterdam 1996/09/10', 'lepton nucleon, deep inelastic scattering', 'lepton nucleon, inclusive reaction', 'lepton deuteron, deep inelastic scattering', 'lepton deuteron, inclusive reaction', 'exchange, one-photon', 'photon nucleon, interaction', 'structure function, spin', 'polarization, asymmetry', 'charged particle, electroproduction', 'sum rule, validity test', 'sum rule, violation', 'quark, fragmentation function', 'quark, flavor', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704005'],"['The experimental status of the spin-dependent structure functions as obtained from the deep inelastic scattering experiments at CERN, SLAC, and DESY is reviewed. All data show a violation of the Ellis-Jaffe sum rule. The Bjorken sum rule is found to be valid and is tested to the 10 % level.']",['1997-04-10']
2195,['eng'],"['Rogalla, M', 'Eich, T', 'Evans, N', 'Joost, S', 'Kienzle-Focacci, M N', 'Geppert, R', 'Göppert, R', 'Irsigler, R', 'Ludwig, J', 'Runge, K', 'Schmid, T']",['Radiation damage to neutron and proton irradiated GaAs particle detectors'],['Detectors and Experimental Techniques'],"['semiconductor detector', 'gallium, arsenic', 'radiation, damage', 'n, radiation', 'p, radiation', 'dosimetry', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704002'],"['The radiation damage in 200 um thick Schottky diodes made on semi-insulating (SI) undoped GaAs Liquid Encapsulated Czochralski (LEC) bulk material with resistivities between 0.4 and 8.9*10E7 Ohm*cm were studied using alpha-spectroscopy, signal response to minimum ionising particles (MIP), I-V and CV-measurements. The results have been analysed to investigate the influence of the substrate resistivity on the detector performance after neutron and proton irradiation. The leakage current density, signal response to alpha-particles and MIPs show a strong dependence on the resistivity before and after irradiation. An observed decrease of the electron mean free drift length before and after irradiation with increasing substrate resistivity can be explained by a model involving the different ionisation ratios of defects, which are introduced by the irradiation. Comparison of the radiation damage due to neutrons and protons gives a hardness factor of 7+-0.9 for 24 GeV/c protons. The best detectors show a response to MIPs of 5250 e- at 200 V reverse bias after a irradiation level of 2*10E14 p/cm^2.']",['1997-04-07']
2196,['eng'],"['Ellison, J']",['W Boson Physics at the Fermilab Tevatron'],['Particle Physics - Experimental Results'],"['talk, Cracow 1997/01/04', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'channel cross section, branching ratio', 'W, width', 'W, mass', 'mass spectrum, transverse', 'photon, associated production', 'gauge boson, pair production', 'coupling, (3gauge boson)', 'charge, asymmetry', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704001'],"['We present electroweak physics results from the D0 and CDF experiments using data from p \\bar p collisions at \\sqrt s = 1.8 TeV. Measurements of the cross sections times branching ratios for W and Z production, the inclusive width of the W boson and the W boson mass are presented. Direct tests of the WW\\gamma and WWZ trilinear gauge boson couplings are also presented based on studies of diboson production.']",['1997-04-03']
2197,['eng'],[],['The doubly Cabibbo-suppressed decay $D^+ \\to K^+ \\pi^- \\pi^+$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'tin', 'D+, hadroproduction', 'D+, hadronic decay', 'D+, branching ratio', 'mass spectrum, (K+ pi+ pi-)', 'Dalitz plot', 'K*(892)', 'rho(770)0', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> K+ pi+ pi-', 'D+ --> rho(770)0 K+', 'D+ --> K*(892) pi+', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9706025'],['We report the observation of the doubly Cabibbo-suppressed decay $D^+\\to K^+ a signal of 59 \\pm 13 events we measured the ratio of the branching fraction for this mode to that of the Cabibbo-favored decay $D^+\\to K^- \\pi^+ \\pi^+$ to be $B(D^+ \\to K^+ \\pi^- \\pi^+) / B(D^+ \\to K^- \\pi^+ \\pi^+) = (7.7 \\pm 1.7 \\pm 0.8) \\times 10^{-3}$. A Dalitz plot analysis was performed to search for resonant structures.'],['1997-06-27']
2198,['eng'],"['Mallot, G K']",['Deep inelastic scattering from unpolarised targets'],['Particle Physics - Experimental Results'],"['review, Erice 1995/08/03', 'lepton nucleon, deep inelastic scattering', 'lepton deuteron, deep inelastic scattering', 'neutrino nucleon, deep inelastic scattering', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'p, structure function', 'n, structure function', 'structure function, ratio', 'structure function, x-dependence', 'momentum transfer, dependence', 'sum rule, Gottfried', 'quantum chromodynamics, perturbation theory', 'effect, higher-twist', 'strong interaction, coupling constant', 'model, rescaling', 'gluon, momentum spectrum', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703014'],"['In this paper the experimental status of unpolarised structure functions is reviewed. In particular the latest results from the NMC, E665, CCFR, and HERA experiments are discussed. Emphasis is put on the fixed-target experiments, which cover with high precision the x region relevant for the present polarised DIS experiments.']",['1997-03-27']
2199,['eng'],"['Bartelt, J']",['Studies of the Cabibbo-Suppressed Decays $D^+ \\to \\pi^0 \\l^+ \\nu$ and $D^+ \\to \\eta e^+ \\nu_e$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D+, electroproduction', 'D+, semileptonic decay', 'D+, branching ratio', 'Kobayashi-Maskawa angle', 'D+, decay constant', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'D+ --> pi0 lepton+ neutrino', 'D+ --> anti-K0 lepton+ neutrino', 'D+ --> eta positron neutrino/e', 'D+ --> pi0 positron neutrino/e', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703013'],"['Using 4.8 fb$^{-1}$ of data taken with the CLEO II detector, the branching fraction for the Cabibbo-suppressed decay $D^+\\to\\pi^0\\ell^+\\nu$ measured relative to the Cabibbo favored decay $D^+\\to\\bar{K^0}\\ell^+\\nu$ is found to be $0.046\\pm 0.014\\pm 0.017$. Using $V_{cs}$ and $V_{cd}$ from unitarity constraints, we determine $| f_+^{\\pi}(0)/f_+^K(0)|^2=0.9\\pm 0.3\\pm 0.3$ We also present a 90% confidence level upper limit for the branching ratio of the decay $D^+ \\to \\eta e^+\\nu_e$ relative to that for $D^+ \\to \\pi^0 e^+\\nu_e$ of 1.5.']",['1997-03-26']
2200,['eng'],"['Akimov, D Y', 'Burenkov, A N', 'Churakov, D L', 'Kuzichev, V F', 'Morgunov, V L', 'Smirnov, G N', 'Solovov, V N']","['Development of High Pressure Xe Scintillation Proportional Counter for Experiments in ""Low-Background"" Physics']",['Particle Physics - Experimental Results'],"['proportional chamber, scintillation counter', 'scintillation counter, fibre', 'optics, transformation', 'energy resolution', 'radiation, yield']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703011'],"['Characteristics of a scintillation proportional counter with WLS fiber optics readout is described. The possibility of detection of the proportional scintillation signal produced by the single electron of primary ionization is shown. The counter can be applied for the experiments in ""low--background"" physics which require a low energy threshold.']",['1997-03-21']
2201,['eng'],"['Adloff, C']","['A Measurement of the Proton Structure Function $F_2(x,Q^2)$ at Low x and Low $Q^2$ at HERA']",['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'p, structure function', 'structure function, x-dependence', 'dependence, momentum transfer', 'photon p, interaction', 'total cross section, energy dependence', 'parametrization', 'Regge poles', 'vector dominance', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703012'],"['The results of a measurement of the proton structure function F_2(x,Q^2)and the virtual photon-proton cross section are reported for momentum transfers squared Q^2 between 0.35 GeV^2 and 3.5 GeV^2 and for Bjorken-x values down to 6 10^{-6} using data collected by the HERA experiment H1 in 1995. The data represent an increase in kinematic reach to lower x and Q^2 values of about a factor of 5 compared to previous H1 measurements. Including measurements from fixed target experiments the rise of F_2 with decreasing x is found to be less steep for the lowest Q^2 values measured. Phenomenological models at low Q^2 are compared with the data.']",['1997-03-21']
2202,['eng'],"['Godang, R']",['Limit on the Two-Photon Production of the Glueball Candidate $f_{J}(2220)$ at CLEO'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'f4(2220), photoproduction', 'f4(2220), hadronic decay', 'glueball', 'K0(S), pair production', 'width, branching ratio', 'upper limit', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> f4(2220) positron electron', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703009'],"['We use the CLEO detector at the Cornell electron-positron storage ring, CESR, to search for the two-photon production of the glueball candidate f_J(2220) in its decay to K_s K_s. We present a restrictive upper limit on the product of the two-photon partial width and the K_s K_s branching fraction. We use this limit to calculate a lower limit on the stickiness, which is a measure of the two-gluon coupling relative to the two-photon coupling. This limit on stickiness indicates that the f_J(2220) has substantial glueball content.']",['1997-03-19']
2203,['eng'],"['Anthony, P L', 'Becker-Szendy, R A', 'Bosted, P E', 'Cavalli-Sforza, M', 'Keller, L P', 'Kelley, L A', 'Klein, S R', 'Niemi, G D', 'Perl, Martin Lewis', 'Rochester, L S', 'White, J L']",['Bremsstrahlung Suppression due to the LPM and Dielectric Effects in a Variety of Materials'],['Particle Physics - Experimental Results'],"['electron nucleus, interaction', 'bremsstrahlung', 'cross section', 'effect, Landau-Pomeranchuk-Migdal', 'effect, dielectric', 'multiple scattering', 'effect, interference', 'photon electron, interaction', 'photon, energy spectrum', 'dependence, mass number', 'target, dependence', 'calorimeter, bismuth-germanate', 'experimental results', 'SLAC Lab', '8-25 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703016'],"['The cross section for bremsstrahlung from highly relativistic particles is suppressed due to interference caused by multiple scattering in dense media, and due to photon interactions with the electrons in all materials. We present here a detailed study of bremsstrahlung production of 200 keV to 500 MeV photons from 8 and 25 GeV electrons traversing a variety of target materials. For most targets, we observe the expected suppressions to a good accuracy. We observe that finite thickness effects are important for thin targets.']",['1997-03-31']
2204,['eng'],"['Abachi, S']",['Direct Measurement of the Top Quark Mass'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'mass, truth', 'final state, ((n)jet lepton)', 'statistical analysis', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703008'],['We measure the top quark mass m_t using t tbar pairs produced in the D0 detector by root(s) = 1.8 TeV p pbar collisions in a 125 pb^-1 exposure at the Fermilab Tevatron. We make a two constraint fit to m_t in t tbar --> b W^+ bbar W^- final states with one W decaying to q qbar and the other to e nu or mu nu. Events are binned in fit mass versus a measure of probability for events to be signal rather than background. Likelihood fits to the data yield m_t = 173.3 +- 5.6 (stat) +- 6.2 (syst) GeV/c^2.'],['1997-03-13']
2205,['eng'],"['Adamovich, M I', 'Alexandrov, Yu A', 'Barberis, D', 'Beck, M', 'Bérat, C', 'Beusch, Werner', 'Boss, M', 'Brons, S', 'Brückner, W', 'Buénerd, M', 'Busch, C', 'Büscher, C', 'Charignon, F', 'Chauvin, J', 'Chudakov, E A', 'Dersch, U', 'Dropmann, F', 'Engelfried, J', 'Faller, F', 'Fournier, A', 'Gerassimov, S G', 'Godbersen, M', 'Grafström, P', 'Haller, T', 'Heidrich, M', 'Hubbard, E', 'Hurst, R B', 'Königsmann, Kay C', 'Konorov, I', 'Keller, N', 'Martens, K', 'Martin, P', 'Masciocchi, S', 'Michaels, R', 'Müller, U', 'Neeb, H', 'Newbold, D', 'Newsom, C R', 'Paul, S', 'Pochodzalla, J', 'Potashnikova, I K', 'Povh, B', 'Ren, Z', 'Rey-Campagnolle, M', 'Rosner, G', 'Rossi, L', 'Rudolph, H', 'Scheel, C V', 'Schmitt, L', 'Siebert, Hans-Wolfgang', 'Simon, A', 'Smith, V', 'Thilmann, O', 'Trombini, A', 'Vesin, E', 'Volkemer, B', 'Vorwalter, K', 'Walcher, T', 'Wälder, G', 'Werding, R', 'Wittmann, E', 'Zavertyaev, M V']","['$\\Xi ^{-}$ Production by $\\Sigma ^{-}$,$\\pi^{-}$ and Neutrons in the Hyperon Beam Experiment at CERN']",['Particle Physics - Experimental Results'],"['hadron nucleus, inclusive reaction', 'Sigma-, secondary beam', 'pi-, secondary beam', 'n, secondary beam', 'carbon', 'copper', 'Xi-, hadroproduction', 'Xi-, hadronic decay', 'differential cross section, transverse momentum', 'differential cross section, x-dependence', 'effect, leading particle', 'dependence, mass number', 'magnetic detector, OMEGA', 'experimental results', 'CERN SPS', 'hadron nucleus --> Xi- anything', 'Xi- --> Lambda pi-', 'Lambda --> p pi-', '450 GeV/c (p)']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-023', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703007']","['Inclusive cross sections for \\ximin\\ hyperon production in high-energy \\sigmamin, \\pimin\\ and neutron induced interactions were measured by the experiment WA89 at CERN. Secondary \\sigmamin\\ and \\pimin\\ beams with average momenta of 345~\\gevc1 and a neutron beam of average momentum 65~\\gevc1 were produced by primary protons of 450~\\gevc1\\ from the CERN SPS. Both single and double differential cross sections are presented as a function of the transverse momentum and the Feynman variable $x_F$. A strong leading effect for \\ximin\\ produced by \\sigmamin\\ is observed. The influence of the target mass on the \\ximin\\ cross section is explored by comparing reactions on copper and carbon nuclei.']",['1997-03-10']
2206,['eng'],"['Gibbons, L K']",['The Inclusive Decays $B\\to D X$ and $B\\to D^* X$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, decay modes', 'charmed meson, hadronic decay', 'D*(2010), polarization', 'momentum dependence', 'yield, charm', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D anything', 'B --> D*(2010) anything', 'D*(2010) --> D pi', 'D0 --> K- pi+', 'D+ --> K- 2pi+', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703006'],"[""We report new measurements of the differential and total branching ratios for inclusive B decay to D^0, D^+ and D^{*+} and the first measurement of the same quantities for inclusive B decay to $D^{*0}$. Here B is the mixture of B_d and B_u from $\\Upsilon(4S)$ decay. Furthermore, since more than one charm particle (or antiparticle) of the same kind can be produced in B decay, here ``inclusive B branching ratio'' is used to mean the average number of charm particles and their antiparticles of a certain species produced in B decay. We obtain the following results (the first error is statistical, the second systematic of this analysis, the third is propagated from other measurements): ${\\cal B}(B\\to D^0 X) = (0.636\\pm 0.014\\pm 0.019\\pm 0.018), {\\cal B}(B\\to D^+ X) = (0.235\\pm 0.009\\pm 0.009\\pm 0.024), {\\cal B}(B\\to D^{*0} X) = (0.247\\pm 0.012\\pm 0.018\\pm 0.018), {\\cal B}(B\\to D^{*+} X) = (0.239\\pm 0.011\\pm 0.014\\pm 0.009)$. The following ratio of branching ratios is not affected by most of the systematic errors: ${\\cal B}(B\\to D^{*0} X)/{\\cal B}(B\\to D^{*+} X) = (1.03\\pm 0.07\\pm 0.09\\pm 0.08).$ We also report the first measurement of the momentum-dependent $D^{*0}$ polarization and a new measurement of the $D^{*+}$ polarization in inclusive B decay. Using these measurements and other CLEO results and making some additional assumptions, we calculate the average number of c and $\\bar c$ quarks produced in B decay to be $< n_c > = 1.10\\pm 0.05$.""]",['1997-03-07']
2207,['eng'],"['Ackerstaff, K']",['Measurement of the Neutron Spin Structure Function $g_1^n$ with a Polarized $^3He$ Target'],['Particle Physics - Experimental Results'],"['positron nucleus, deep inelastic scattering', 'polarized target, internal', 'helium, nuclide', 'positron, polarized beam', 'polarization, longitudinal', 'n, structure function', 'structure function, spin', 'moment, structure function', 'Regge poles', 'structure function, x-dependence', 'dependence, momentum transfer', 'magnetic detector, HERMES', 'experimental results', 'DESY HERA Stor', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703005'],"['Results are reported from the HERMES experiment at HERA on a measurement of the neutron spin structure function $g_1^n(x,Q^2)$ in deep inelastic scattering using 27.5 GeV longitudinally polarized positrons incident on a polarized $^3$He internal gas target. The data cover the kinematic range $0.023<x<0.6$ and $1 (GeV/c)^2 < Q^2 <15 (GeV/c)^2$. The integral $\\int_{0.023}^{0.6} g_1^n(x) dx$ evaluated at a fixed $Q^2$ of $2.5 (GeV/c)^2$ is $-0.034\\pm 0.013(stat.)\\pm 0.005(syst.)$. Assuming Regge behavior at low $x$, the first moment $\\Gamma_1^n=\\int_0^1 g_1^n(x) dx$ is $-0.037\\pm 0.013(stat.)\\pm 0.005(syst.)\\pm 0.006(extrapol.)$.']",['1997-03-05']
2208,['eng'],[],['Measurement of $\\tau$ polarization in $e ^+ e^-$ annihilation at $\\sqrt{s}=58 GeV$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, polarization', 'asymmetry', 'tau, leptonic decay', 'tau, semileptonic decay', 'angular distribution, asymmetry', 'magnetic detector, VENUS', 'experimental results', 'KEK TRISTAN Stor', '58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703003'],"['The polarization of tau leptons in the reaction e+ e- --> tau+ tau- has been measured using a e+e- collider, TRISTAN, at the center-of-mass energy of 58 GeV. From the kinematical distributions of daughter particles in tau --> e nu nu-bar, mu nu nu-bar, rho nu or pi(K) nu decays, the average polarization of tau- and its forward-backward asymmetry have been evaluated to be 0.012 +- 0.058 and 0.029 +- 0.057, respectively.']",['1997-03-04']
2209,['eng'],"['Berg, B', 'Riedler, J']",['Signal Confidence Limits from a Neural Network Data Analysis'],['Detectors and Experimental Techniques'],"['track data analysis', 'neural network', 'statistical analysis']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703001'],"['Let $N$ experimental data be given, such that $N=N_s+N_b$, ($N_s\\ll N_b)$, where $N_s$ is the number of signals, $N_b$ the number of background events, and both are unknown. Assume that a neural network (NN) has been trained, such that it will tag signals with efficiency $F_s$ and background data with $F_b$, $(1> F_s\\gg F_b >0)$. Applying the NN yields $N^Y<N$ tagged events. From the knowledge of $N^Y$ we find the a-posteriori likelihood $P(N_s)$ that there are actually $N_s$ signals in the data set. Once $P(N_s)$ is given, confidence limits for the signal probability follow. Subsequently, we compare our results with those obtained by starting off with a maximum entropy type of assumption for the a-priori likelihood that there are $N_s$ signals in the data. Certain difficulties are encountered in the latter case.']",['1997-03-03']
2210,['eng'],"['Harr, R F', 'Liapis, C', 'Karchin, P E', 'Biino, C', 'Erhan, S', 'Hofmann, W', 'Kreuzer, P K', 'Lynn, D', 'Medinnis, M', 'Palestini, S', 'Pesando, L', 'Punturo, M', 'Schlein, Peter E', 'Wilkens, B', 'Zweizig, J G']",['Pseudorapidity Distribution of Charged Particles in $p\\overline{p}$ Collisions at root(s)= 630 GeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'hadron, multiple production', 'charged particle, rapidity spectrum', 'semiconductor detector, vertex', 'experimental results', 'CERN SPS', '630 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703002'],"['Using a silicon vertex detector, we measure the charged particle pseudorapidity distribution over the range 1.5 to 5.5 using data collected from PbarP collisions at root s = 630 GeV. With a data sample of 3 million events, we deduce a result with an overall normalization uncertainty of 5%, and typical bin to bin errors of a few percent. We compare our result to the measurement of UA5, and the distribution generated by the Lund Monte Carlo with default settings. This is only the second measurement at this level of precision, and only the second measurement for pseudorapidity greater than 3.']",['1997-03-03']
2211,['eng'],"['Jessop, C P']",['Measurement of the Decay Amplitudes and Branching Fractions of $B\\to J/\\psi K^{*}$ and $B\\to J/\\psi K$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, hadronic decay', 'B+, branching ratio', 'B0, branching ratio', 'decay, amplitude analysis', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> J/psi(3100) K*(892)', 'B --> J/psi(3100) K', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702013'],"['Using data taken with the CLEO II detector, we present the first full angular analysis in the color-suppressed modes B0 --> J/psi K*0 and B+ --> J/psi K*+. This leads to a complete determination of the decay amplitudes of these modes. In addition, we update the branching fractions for B --> J/psi K and B --> J/psi K*.']",['1997-02-26']
2212,['eng'],"['Apanasevich, L']",['Production of charm mesons at high transverse momentum in 515 GeV/c $\\pi^-$ nucleon collisions'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'beryllium', 'copper', 'D+, hadroproduction', 'D-, hadroproduction', 'transverse momentum, high', 'D, hadronic decay', 'mass spectrum, (K 2pi)', 'differential cross section, transverse momentum', 'channel cross section, energy dependence', 'magnetic detector, experimental results', 'Batavia TEVATRON PS', 'D+ --> K- 2pi+', 'D- --> K+ 2pi-', '515 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702014'],"['We present results on the production of high transverse momentum charm mesons in collisions of 515 GeV/c negative pions with beryllium and copper targets. The experiment recorded a large sample of events containing high transverse momentum showers detected in an electromagnetic calorimeter. From these data, a sample of charm mesons has been reconstructed via their decay into the fully charged K pi pi mode. A measurement of the single inclusive transverse momentum distribution of charged D mesons from 1 to 8 GeV/c is presented. An extrapolation of the measured differential cross section yields an integrated charged D cross section of 11.4+-2.7(stat)+-3.3(syst) microbarns per nucleon for charged D mesons with Feynman x greater than zero. The data are compared with expectations based upon next-to-leading order perturbative QCD, as well as with results from PYTHIA. We also compare our integrated charged D cross section with measurements from other experiments.']",['1997-02-26']
2213,['eng'],"['Höcker, A']",['Vector and Axial-Vector Spectral Functions and QCD'],['Particle Physics - Experimental Results'],"['talk, Estes Park 1996/09/16', 'electron positron, annihilation', 'tau, electroproduction', 'tau-, semileptonic decay', 'tau-, branching ratio', 'tau-, width', 'current, vector', 'current, axial-vector', 'spectral representation, moment', 'quantum chromodynamics, sum rule', 'pi, polarizability', 'symmetry, chiral', 'strong interaction, coupling constant', 'effect, nonperturbative', 'mass spectrum', 'numerical calculations', 'interpretation of experiments, ALEPH', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703004'],"['We present new results of the tau hadronic spectral function analysis using data accumulated by the ALEPH detector at LEP during the years 1991-94. In addition to the vector spectral functions, the axial-vector spectral functions and, separately, the tau --> 3pi nu as well as the tau --> pi 2pi0 nu spectral functions are determined from their respective unfolded, i.e., physical invariant mass spectra. The spectral functions are applied to QCD chiral sum rules in order to extract information about saturation at the tau mass scale. Using the the semi-leptonic tau decay rate for vector and axial-vector currents in addition to spectral moments, we obtain precise measurements of the strong coupling constant alpha_s(M_tau) and the contributing non-perturbative power terms. The evolution to the Z mass yields alpha_s(M_Z) = 0.1219 +/- 0.0019.']",['1997-03-04']
2214,['eng'],"['Budd, H S']",['CMS Central Hadron Calorimeter'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1996/05/21', 'calorimeter, hadronic', 'copper', 'scintillation counter, fibre', 'optics, transformation', 'energy resolution', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102032'],['We present a description of the CMS central hadron calorimeter. We describe the production of the 1996 CMS hadron testbeam module. We show the results of the quality control tests of the testbeam module. We present some results of the 1995 CMS hadron testbeam.'],['2001-02-15']
2215,['eng'],"['Budd, H S', 'Bodek, Arie', 'De Barbaro, P', 'Ruggiero, D', 'Skup, E']",['Fiber R and D for the CMS HCAL'],['Particle Physics - Experimental Results'],"['talk, Notre Dame 1997/11/02', 'calorimeter, hadronic', 'scintillation counter', 'optics, transformation', 'optics, fibre', 'optics, reflection', 'optics, absorption', 'radiation, yield', 'radiation, damage', 'magnetic detector, CMS', 'CERN LHC Coll']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0102031'],"['This paper documents the fiber R and D for the CMS hadron barrel calorimeter (HCAL). The R and D includes measurements of fiber flexibility, splicing, mirror reflectivity, relative light yield, attenuation length, radiation effects, absolute light yield, and transverse tile uniformity. Schematics of the hardware for each measurement are shown. These studies are done for different diameters and kinds of multiclad fiber.']",['2001-02-13']
2216,['eng'],"['Abachi, S']",['Study of the $ZZ\\gamma$ and $Z\\gamma\\gamma$ Couplings in $Z(\\nu\\nu)\\gamma$ Production'],['Particle Physics - Experimental Results'],"['anti-p p, inclusive reaction', 'photon, hadroproduction', 'transverse energy, missing-energy', 'Z0, associated production', 'Z0, leptonic decay', 'neutrino, pair production', 'coupling, (2Z0 photon)', 'coupling, (Z0 2photon)', 'transverse energy, energy spectrum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> photon missing-energy anything', 'anti-p p --> Z0 photon', 'Z0 --> neutrino antineutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702011'],"['We have measured the ZZ-gamma and Z-gamma-gamma couplings by studying p-bar p -> (missing ET) gamma + X events at sqrt(s)=1.8 TeV with the D0 detector at the Fermilab Tevatron Collider. This first study of hadronic Z-gamma production in the neutrino decay channel gives the most stringent limits on anomalous couplings available. A fit to the transverse energy spectrum of the photon in the candidate event sample, based on a data set corresponding to an integrated luminosity of 13.1 pb^(-1), yields 95% CL limits on the anomalous CP-conserving ZZ-gamma couplings of |h^Z_(30)|<0.9, |h^Z_(40)|<0.21, for a form-factor scale Lambda = 500 GeV. Combining these results with our previous measurement using Z -> ee and mu-mu yields the limits:|h^Z_(30)|<0.8, |h^Z_(40)|<0.19 (Lambda = 500 GeV) and |h^Z_(30)|<0.4, |h^Z_(40)|<0.06 (Lambda = 750 GeV).']",['1997-02-24']
2217,['eng'],"['Cremaldi, L']",['Search for Mixing and CP Violation in Charm Decays'],['Particle Physics - Experimental Results'],"['talk, Montreal 1996/08/27', 'pi nucleon, inclusive reaction', 'charmed meson, hadroproduction', 'D*(2010), cascade decay', 'D0, hadronic decay', 'D0, semileptonic decay', 'D+, hadronic decay', 'D0 anti-D0, interference', 'mass spectrum', 'charge, asymmetry', 'violation, CP', 'experimental results', 'Batavia TEVATRON PS', 'D0 --> K+ K-', 'D0 --> pi+ pi-', 'D+ --> 3pi', 'D+ --> 2K pi', 'D0 --> K lepton antineutrino']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011089'],"['Standard model mixing and CP violation are expected to be small in the charm sector. Some argue that only in the presence of new physics do we currently expect to observe these effects. Fermilab experiment E791 has the largest sample of reconstructed charm decays recorded to date. We have made an exhaustive search for D0 D0-bar mixing and CP violation in this data. We present the charm mixing limits on the mixing parameter r_mix using hadronic and semileptonic decays, and also present preliminary limits on the CP asymmetry parameter, A_CP, for Cabibbo suppressed decays.']",['2000-12-20']
2218,['eng'],"['Reyes, M A']",['Spin-Parity Analysis of the Centrally produced $K_{s}K_{s}$ system at 800 GeV'],['Particle Physics - Experimental Results'],"['talk, Dinkelsbuehl 1996/08/27', 'p p, inelastic scattering', 'p p, exclusive reaction', 'K0(S), pair production', 'f0(1500), hadroproduction', 'spin, parity', 'f0(1710)', 'mass spectrum, (2K0(S))', 'angular distribution', 'partial wave analysis', 'spectrometer, experimental results', 'Batavia TEVATRON PS', 'p p --> 2p 2K0(S)', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702010'],"['Results are presented of the spin-parity analysis on a sample of centrally produced mesons in the reaction (p p -> p_{slow} K_s K_s p_{fast}) with 800 GeV protons on liquid hydrogen. The spin-parity analysis in the mass region between threshold and 1.58 GeV/c^2 shows that the (K_s K_s) system is produced mainly in S-wave. The f_0(1500) is clearly observed in this region. Above 1.58 GeV/c^2 two solutions are possible, one with mainly S-wave and another with mainly D-wave. This ambiguity prevents a unique determination of the spin of the f_J(1710) meson.']",['1997-02-21']
2219,['eng'],"['Adloff, C']",['Observation of Events at Very High $Q^2$ in ep Collisions at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'momentum transfer, high', 'neutral current', 'charged current', 'electroweak interaction, validity test', 'transverse momentum, missing-energy', 'positron, energy spectrum', 'angular distribution', 'spectra, momentum transfer', 'mass spectrum', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702012'],"['Measurements of ep scattering with squared 4-momentum transfer Q^2 up to 35000 GeV^2 are compared with the expectation of the standard deep-inelastic model of lepton-nucleon scattering (DIS). For Q^2 > 15000 GeV^2, N_{obs} =12 neutral current candidate events are observed where the expectation is N_DIS = 4.71 \\pm 0.76 events. In the same Q^2 range, N_{obs} =4 charged current candidates are observed where the expectation is N_{DIS} = 1.77 \\pm 0.87 events. The probability P(N \\geq N_{obs}) that the DIS model signal N fluctuates to N \\geq N_{obs} in a random set of experiments is 6 10^{-3} for neutral current and 0.14 for charged current. The difference in the observed and expected number of Neutral Current events is mostly due to events at large masses M = sqrt{xs} in which the positron is backscattered at large y = Q^2/M^2.']",['1997-02-24']
2220,['eng'],"['Breitweg, J']",['Comparison of ZEUS Data with Standard Model Predictions for $e^+ p \\to e^+ X$ Scattering at High x and $Q^2$'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'momentum transfer, high', 'electroweak interaction, validity test', 'statistical analysis', 'background', 'spectra, x-dependence', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> positron anything', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702015'],"['Using the ZEUS detector at HERA, we have studied the reaction e^+ p -> e^+ X for Q^2 > 5000 GeV^2 with a 20.1 pb^{-1} data sample collected during the years 1994 to 1996. For Q^2 below 15000 GeV^2, the data are in good agreement with Standard Model expectations. For Q^2 > 35000 Gev^2, two events are observed while 0.145+-0.013 events are expected. A statistical analysis of a large ensemble of simulated Standard Model experiments indicates that with probability 6.0%, an excess at least as unlikely as that observed would occur above some Q^2 cut. For x>0.55 and y>0.25, four events are observed where 0.91+-0.08 events are expected. A statistical analysis of the two-dimensional distribution of the events in x and y yields a probability of 0.72% for the region x>0.55 and y>0.25 and a probability of 7.8% for the entire Q^2 > 5000 GeV^2 data sample. The observed excess above Standard Model expectations is particularly interesting because it occurs in a previously unexplored kinematic region.']",['1997-02-26']
2221,['eng'],"['Rosner, Jonathan L', 'Wilkerson, J F']",['Detection of the RF Pulse Associated With Cosmic Ray Air Showers'],['Astrophysics and Astronomy'],"['microwaves, cosmic radiation', 'showers, air']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702008'],"['Initial results of a project to detect the radio-frequency pulse associated with extensive air showers of cosmic rays are described briefly. This work is being performed at the CASA/MIA array in Utah, with the intention of designing equipment that can be used in conjunction with the Auger Giant Array proposal.']",['1997-02-17']
2222,['eng'],"['Abe, K']",['Measurement of Leading Particle Effects in Decays of $Z^{0}$ Bosons into Light Flavors'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'effect, leading particle', 'quark, jet', 'antiquark, jet', 'hadron, momentum', 'p', 'Lambda', 'K', 'K*(892)', 'yield, (particle antiparticle)', 'momentum dependence', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702009'],"['We present evidence for leading particle production in hadronic decays of the Z0 boson to light-flavor jets. A polarized electron beam was used to tag quark and antiquark jets, and a vertex detector was employed to reject heavy-flavor events. Charged hadrons were identified with a Cherenkov ring imaging detector. In the quark jets, more high-momentum p, Lambda, K-, and anti-K*0 were observed than their antiparticles, and vice versa for antiquark jets, providing direct evidence that the higher-momentum particles in jets are more likely to carry the primary quark or antiquark from the Z0 decay, and that s-s(bar) production is suppressed in fragmentation.']",['1997-02-17']
2223,['eng'],"['Artuso, M']",['Study of the $B^{0}$ semileptonic decay spectrum at the upsilon(4S) resonance'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B0, pair production', 'B0, semileptonic decay', 'lepton, momentum spectrum', 'B0, branching ratio', 'B+, branching ratio', 'lifetime, ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702007'],"[""We have made a first measurement of the lepton momentum spectrum in a sample of events enriched in neutral B's through a partial reconstruction of B0 --> D*- l+ nu. This spectrum, measured with 2.38 fb**-1 of data collected at the Upsilon(4S) resonance by the CLEO II detector, is compared directly to the inclusive lepton spectrum from all Upsilon(4S) events in the same data set. These two spectra are consistent with having the same shape above 1.5 GeV/c. From the two spectra and two other CLEO measurements, we obtain the B0 and B+ semileptonic branching fractions, b0 and b+, their ratio, and the production ratio f+-/f00 of B+ and B0 pairs at the Upsilon(4S). We report b+/b0=0.950 (+0.117-0.080) +- 0.091, b0 = (10.78 +- 0.60 +- 0.69)%, and b+ = (10.25 +- 0.57 +- 0.65)%. b+/b0 is equivalent to the ratio of charged to neutral B lifetimes, tau+/tau0.""]",['1997-02-14']
2224,['eng'],"['Adams, D']",['Spin Structure of the Proton from Polarized Inclusive Deep-Inelastic Muon-Proton Scattering'],['Particle Physics - Experimental Results'],"['muon p, deep inelastic scattering', 'muon p, polarized beam', 'p, polarized target', 'p, structure function', 'structure function, spin', 'structure function, small-x', 'quantum chromodynamics, perturbation theory', 'moment, structure function', 'operator product expansion', 'sum rule, Bjorken', 'factorization', 'charge, axial', 'model, quark parton', 'cross section, asymmetry', 'magnetic spectrometer, experimental results', 'CERN SPS', 'bibliography', '100, 190 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702005'],"['We have measured the spin-dependent structure function $g_1^p$ in inclusive deep-inelastic scattering of polarized muons off polarized protons, in the kinematic range $0.003 < x < 0.7$ and $1 GeV^2 < Q^2 < 60 GeV^2$. A next-to-leading order QCD analysis is used to evolve the measured $g_1^p(x,Q^2)$ to a fixed $Q^2_0$. The first moment of $g_1^p$ at $Q^2_0 = 10 GeV^2$ is $\\Gamma^p = 0.136\\pm 0.013(stat.) \\pm 0.009(syst.)\\pm 0.005(evol.)$. This result is below the prediction of the Ellis-Jaffe sum rule by more than two standard deviations. The singlet axial charge $a_0$ is found to be $0.28 required to bring $\\Delta \\Sigma$ in agreement with the Quark-Parton Model. A combined analysis of all available proton and deuteron data confirms the Bjorken sum rule.']",['1997-02-13']
2225,['eng'],"['Sultansoy, S F']","['""Four Ways to TeV Scale"", Ankara\'97 Workshop and Something Else']",['Particle Physics - Experimental Results'],"['talk, Ankara 1997/04/09', 'colliding beams, proposed', 'electron p, linac-ring collider', 'photon p, colliding beams', 'photon nucleus, colliding beams', 'free electron laser', 'electroweak interaction', 'new particle, search for', 'family, 4', 'supersymmetry', 'model, composite', 'supergravity', 'numerical calculations', 'bibliography']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007043'],"[""The first Part contains the invited talk given at the First International Workshop on Linac-Ring Type ep and $gamma$p Colliders (9-11 April 1997, Ankara, Turkey). Four known types of colliders, which may give an opportunity to achieve TeV center of mass energies in the near future (10-15 years), are discussed. Parameters of the linac-ring type ep and $gamma$p machines are roughly estimated. Some speculations on TeV scale physics are given. The physics goals of the TeV energy ep and $gamma$p colliders are considered. Information about the Ankara'97 Workshop, including Workshop Conclusion and Recommendations, is presented in Part II. The third Part includes some clarifications forced by unpleasant developments, which take place after the Workshop. Finally, an Appeal to ICFA, ECFA and ACFA is presented in Part IV.""]",['2000-07-21']
2226,['eng'],"['Adloff, C']",['Diffraction Dissociation in Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'hadron, photoproduction', 'diffraction, dissociation', 'rapidity, gap', 'differential cross section, mass', 'Regge poles, multi-Regge', 'exchange, pomeron', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702003'],"['A study is presented of the process gamma p -->XY, where there is a large rapidity gap between the systems X and Y. Measurements are made of the differential cross section as a function of the invariant mass mx of the system produced at the photon vertex. Results are presented at centre of mass energies of W_gp = 187 GeV and W_gp = 231 GeV, both where the proton dominantly remains intact and, for the first time, where it dissociates. Both the centre of mass energy and the mx^2 dependence of HERA data and those from a fixed target experiment may simultaneously be described in a triple-Regge model. The low mass photon dissociation process is found to be dominated by diffraction, though a sizable subleading contribution is present at larger masses. The pomeron intercept is extracted and found to be alpha_pom(0) = 1.068 \\pm 0.016 (stat.) \\pm 0.022 (syst.) \\pm 0.041 (model), in good agreement with values obtained from total and elastic hadronic and photoproduction cross sections. The diffractive contribution to the process gamma p --> Xp with mx^2 / W_gp^2 < 0.05 is measured to be 22.2 \\pm 0.6 (stat.) \\pm 2.6 (syst.) \\pm 1.7 (model) % of the total gamma p cross section at W_gp = 187 GeV.']",['1997-02-06']
2227,['eng'],"['Abe, F']",['Search for New Particles Decaying to Dijets at CDF'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'mass spectrum, (2jet)', ""W'"", 'axigluon', 'coloron', 'rho(770), technicolor', 'quark, diquark', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2jet anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702004'],"[""We have used 106 pb^-1 of data collected with the Collider Detector at Fermilab to search for new particles decaying to dijets. We exclude at the 95% confidence level models containing the following new particles: axigluons and flavor universal colorons with mass between 200 and 980 GeV/c, excited quarks with mass between 80 and 570 GeV/c^2 and between 580 and 760 GeV/c^2, color octet technirhos with mass between 260 and 480 GeV/c^2, W' bosons with mass between 300 and 420 GeV/c^2, and E_6 diquarks with mass between 290 and 420 GeV/c^2.""]",['1997-02-11']
2228,['eng'],"['Abe, K']",['Measurement of the B+ and B0 Lifetimes from Semileptonic Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'B, semileptonic decay', 'B+, lifetime', 'B0, lifetime', 'lifetime, ratio', 'track data analysis, vertex', 'decay, path length', 'B, charge', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702001'],"['The lifetimes of B+ and B0 mesons are measured using a sample of 150,000 hadronic Z0 decays collected by the SLD experiment at the SLC between 1993 and 1995. The analysis identifies the semileptonic decays of B mesons and reconstructs the B meson decay length and charge by vertexing the lepton with a partially reconstructed D meson. This new method results in a sample of 634 (584) charged (neutral) decays with high charge purity. The ratio of B+ : B0 decays in the charged (neutral) sample is 3:1 (1:3). A maximum likelihood fit yields t(B+) = 1.61 +0.13 -0.12(stat) +/- 0.07(syst) ps, t(B0) = 1.56 +0.14 -0.13(stat) +/- 0.10(syst) ps, and t(B+)/t(B0) = 1.03 +0.16 -0.14(stat) +/- 0.09(syst).']",['1997-02-03']
2229,['eng'],"['Abe, K']",['Measurement of the B+ and B0 Lifetimes using Topological Vertexing'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'B, semileptonic decay', 'B+, lifetime', 'B0, lifetime', 'lifetime, ratio', 'track data analysis, vertex', 'decay, path length', 'B, charge', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9702002'],"['The lifetimes of B+ and B0 mesons have been measured using a sample of 150,000 hadronic Z0 decays collected by the SLD experiment at the SLC between 1993 and 1995. The analysis reconstructs the decay length and charge of the B meson using a novel topological vertexing technique. This method results in a high statistics sample of 6033 (3665) charged (neutral) vertices with good charge purity. A maximum likelihood fit procedure finds: t(B+) = 1.67 +/- 0.07(stat) +/- 0.06(syst) ps, t(B0) = 1.66 +/- 0.08(stat) +/- 0.08(syst) ps, t(B+)/t(B0) = 1.01 +0.09-0.08(stat) +/- 0.05(syst).']",['1997-02-03']
2230,['eng'],"['Rogalla, M', 'Eich, T', 'Evans, N', 'Geppert, R', 'Göppert, R', 'Irsigler, R', 'Ludwig, J', 'Runge, K', 'Schmid, T', 'Marder, D G']",['Analysis of Trapping and Detrapping in Semi-Insulating GaAs Detectors'],['Detectors and Experimental Techniques'],"['semiconductor detector', 'gallium, arsenic', 'efficiency', 'electronics, impedance', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701018'],['To investigate the trapping and detrapping in SI-GaAs particle detectors we analyzed the signals caused by 5.48 MeV alpha particles with a charge sensitive preamplifier. From the bias and temperature dependence of these signals we determine the activation energies of two electron traps. Additional simulation and measurements of the lifetime as a function of resistivity have shown that the EL2+ is the dominant electron trap in semi-insulating GaAs.'],['1997-02-19']
2231,['eng'],"['Seligman, W G']",['A New Determination of $\\alpha_{S}$ From Neutrino-Nucleon Scattering'],['Particle Physics - Experimental Results'],"['neutrino nucleus, deep inelastic scattering', 'antineutrino nucleus, deep inelastic scattering', 'neutrino/mu', 'iron', 'charged current', 'p, structure function', 'dependence, momentum transfer', 'quantum chromodynamics, Lambda parameter', 'strong interaction, coupling constant', 'lepton deuteron, deep inelastic scattering', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '30-360 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701017'],"['We present a new determination of the proton structure functions $F_{2}$ and $xF_{3}$ from the CCFR $\\nu $-Fe deep inelastic scattering (DIS) experiment. Comparisons to high-statistics charged-lepton scattering results for $F_{2}$ from the NMC, E665, SLAC, and BCDMS experiments, after correcting for quark-charge and heavy-target effects, indicate good agreement for $x>0.1$ but some discrepancy at lower x. The $Q^{2}$ evolution of the structure functions yields the quantum chromodynamics (QCD) scale parameter $\\Lambda _{% the strong coupling constant at the scale of mass of the Z-boson of $\\alpha _{S}(M_{Z}^{2})=0.119 \\pm 0.002$(exp.)$\\pm 0.004$(theory) and is one of the most precise measurements of this quantity.']",['1997-01-29']
2232,['eng'],"['Paulini, M']",['Heavy Flavour Physics'],['Particle Physics - Experimental Results'],"['review, Stanford 1996/08/19', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, truth', 'quark, pair production', 'quark, decay', 'channel cross section', 'mass, truth', 'beautiful particle, lifetime', 'lifetime, ratio', 'B+', 'B0', 'B/s0', 'Lambda/b0', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'time dependence', 'beautiful meson, decay modes', 'violation, CP', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701019'],['We review the status of heavy flavour physics at the Fermilab Tevatron collider by summarizing recent top quark and B physics results from CDF and DO. In particular we discuss the measurement of the top quark mass and top production cross section as well as B meson lifetimes and time dependent BB= mixing results. An outlook of perspectives for top and B physics in Run II starting in 1999 is also given.'],['1997-02-19']
2233,['eng'],"['Bhadra, S', 'Bohnet, I', 'Cardy, M L', 'Dosselli, U', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K', 'Hanna, D', 'Holm, U', 'Johnson, K F', 'Khakzad, M', 'Levman, G', 'Lim, J N', 'Löhr, B', 'Martin, J F', 'Muhl, C', 'Neumann, T', 'Rohde, M', 'Schmidke, W B', 'Stairs, D G', 'Tiecke, H G', 'Voci, C']",['Design and Test of a Forward Neutron Calorimeter for the ZEUS Experiment'],['Detectors and Experimental Techniques'],"['n, counters and detectors', 'calorimeter, small-angle', 'lead', 'scintillation counter', 'optics, transformation', 'photoelectron, amplifier', 'charge exchange', 'showers', 'numerical calculations, Monte Carlo', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701015'],"['A lead scintillator sandwich sampling calorimeter has been installed in the HERA tunnel 105.6 m from the central ZEUS detector in the proton beam direction. It is designed to measure the energy and scattering angle of neutrons produced in charge exchange ep collisions. Before installation the calorimeter was tested and calibrated in the H6 beam at CERN where 120 GeV electrons, muons, pions and protons were made incident on the calorimeter. In addition, the spectrum of fast neutrons from charge exchange proton-lucite collisions was measured. The design and construction of the calorimeter is described, and the results of the CERN test reported. Special attention is paid to the measurement of shower position, shower width, and the separation of electromagnetic showers from hadronic showers. The overall energy scale as determined from the energy spectrum of charge exchange neutrons is compared to that obtained from direct beam hadrons.']",['1997-01-28']
2234,['eng'],"['Richman, J D']",['Progress in Understanding Heavy Flavor Decays'],['Particle Physics - Experimental Results'],"['review, Warsaw 1996/07/25', 'quark, heavy', 'quark, decay', 'charmed particle, electroproduction', 'charmed particle, decay modes', 'beautiful particle, electroproduction', 'beautiful particle, hadroproduction', 'beautiful particle, decay modes', 'leptonic decay', 'semileptonic decay', 'hadronic decay', 'rare decay', 'HQET model', 'quantum chromodynamics, sum rule', 'factorization', 'beautiful particle, lifetime', 'B', 'B/s', 'Lambda/b0', 'form factor, slope', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701014'],"['I review new results on particles containing a charm or bottom quark, focusing on measurements that give insight into the dynamics of the decay process. Leptonic and semileptonic decays are the simplest modes, and they provide detailed tests of theoretical predictions based on methods such as lattice QCD, heavy quark effective theory, and QCD sum rules. Although hadronic decays are much more complicated, the factorization hypothesis makes predictions that, at least for certain processes, are in accord with measurements. I also emphasize the importance of precise measurements of branching fractions for normalizing modes, whose uncertainties propagate into many other quantities. Rare hadronic decays are now becoming accessible to several experiments, and I discuss new results and their implications. Finally, I review b-hadron lifetime measurements, which are steadily improving in precision and which indicate a significant difference between B-meson and b-baryon lifetimes.']",['1997-01-28']
2235,['eng'],"['Rogalla, M', 'Eich, T', 'Evans, N', 'Geppert, R', 'Göppert, R', 'Irsigler, R', 'Ludwig, J', 'Runge, K', 'Schmid, T']",['Radiation studies for GaAs in the ATLAS Inner Detector'],['Detectors and Experimental Techniques'],"['semiconductor detector, microstrip', 'gallium, arsenic', 'radiation, damage', 'n, radiation', 'dosimetry', 'numerical calculations', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701011'],['We estimate the hardness factors and the equivalent 1 MeV neutron fluences for hadrons fluences expected at the GaAs positions wheels in the ATLAS Inner Detector. On this basis the degradation of the GaAs particle detectors made from different substrates as a function of years LHC operation is predicted.'],['1997-01-23']
2236,['eng'],"['Coan, T E']",['$\\tau$ Neutrino Helicity from $h^{\\pm}$ Energy Correlations'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'tau, electroproduction', 'tau, pair production', 'tau, semileptonic decay', 'energy, correlation', 'neutrino/tau, helicity', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> tau+ tau-', 'tau --> hadron neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701012'],"['We report a measurement of the magnitude of the tau neutrino helicity from tau-pair events taken with the CLEO detector at the CESR electron-positron storage ring. Events in which each tau undergoes the decay tau -> h nu, with h a charged pion or kaon, are analyzed for energy correlations between the daughter hadrons, yielding |xi| = 2*|h_nu| = 1.03 +/- 0.06 +/- 0.04, with the first error statistical and the second systematic.']",['1997-01-23']
2237,['eng'],"['Anderson, S']",['$\\Lambda\\overline{\\Lambda}$ Production in Two-Photon Interactions at CLEO'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'exchange, two-photon', 'photon photon, exclusive reaction', 'Lambda, pair production', 'Lambda, hadronic decay', 'channel cross section, energy dependence', 'quark, diquark', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Lambda Antilambda positron electron', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701013'],"['Using the CLEO detector at the Cornell $e^+e^-$ storage ring, CESR, we study the two-photon production of $\\Lambda \\overline{\\Lambda}$, making the first observation of $\\gamma \\gamma \\to \\Lambda \\overline{\\Lambda}$. We present the cross-section for $ \\gamma \\gamma \\to \\Lambda \\overline{\\Lambda}$ as a function of the $\\gamma \\gamma$ center of mass energy and compare it to that predicted by the quark-diquark model.']",['1997-01-23']
2238,['eng'],"['Merritt, K W']",['Searches for New Physics at the Tevatron'],['Particle Physics - Experimental Results'],"['review, Minneapolis 1996/08/10', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'new particle, search for', 'search for, new interaction', 'supersymmetry', 'sparticle, pair production', 'leptoquark', 'gauge boson, heavy', 'family, 4', 'Higgs particle, charged particle', 'angular distribution, (2jet)', 'Drell-Yan process', 'mass spectrum, dilepton', 'coupling, (3gauge boson)', 'model, technicolor', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701009'],"['This paper summarizes searches at the Fermilab Tevatron for a wide variety of signatures for physics beyond the Standard Model. These include searches for supersymmetric particles, in the two collider detectors and in one fixed target experiment. Also covered are searches for leptoquarks, dijet resonances, heavy gauge bosons, and particles from a fourth generation, as well as searches for deviations from the Standard Model predictions in dijet angular distributions, dilepton mass distributions, and trilinear gauge boson couplings.']",['1997-01-21']
2239,['eng'],"['McFarland, K S']",['A Precision Measurement of Electroweak Parameters in Neutrino-Nucleon Scattering'],['Particle Physics - Experimental Results'],"['neutrino nucleon, deep inelastic scattering', 'neutral current', 'charged current', 'cross section, ratio', 'Weinberg angle', 'W, mass', 'renormalization, on-shell', 'coupling, (quark neutrino)', 'coupling, (Z0 quark)', 'model, composite', 'four-fermion interaction', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701010'],"['The CCFR collaboration reports a precise measurement of electroweak parameters derived from the ratio of neutral-current to charged-current cross-sections in neutrino-nucleon scattering at the Fermilab Tevatron. This ratio of cross-sections measures the neutral current couplings to quarks, which implies a determination of sin^2 theta_W (on-shell) = 0.2236 +/- 0.0028(expt.) +/- 0.0030(model) for m_top=175 GeV, m_Higgs=150 GeV. This is equivalent to M_W=80.35+/-0.21 GeV. The good agreement of this measurement with Standard Model expectations implies the exclusion of additional neutrino-neutrino-quark-quark contact interactions at 95% confidence at a mass scale of 1-8 TeV, depending on the form of the contact interaction.']",['1997-01-21']
2240,['eng'],"['Gan, K K']",['Review of Rare and Forbidden $\\tau$ Decays'],['Particle Physics - Experimental Results'],"['talk, Estes Park 1996/09/16', 'tau-, rare decay', 'tau-, decay modes', 'tau-, branching ratio', 'anomaly, chiral', 'second-class current', 'Cabibbo model', 'tau-, radiative decay', 'branching ratio, upper limit', 'mass spectrum', 'Feynman graph', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9707007'],"['This is a review of rare and forbidden decays of the $\\tau$ lepton. For the rare decays, this includes new results on the chiral anomaly decay and the observations of the Cabibbo-suppressed decay $\\tauketa$ and the internal conversion decay $\\taueee$. For the forbidden decays, there are new upper limits on the radiative decays $\\tauegamma$ and $\\taumugamma$. Some forbidden decays which have not been previously searched for are also suggested.']",['1997-07-03']
2241,['eng'],"['Bishai, M']",['Analyses of $D^{+} \\to K_{S}^{0} K^{+}$ and $D^{+} \\to K_{S}^{0} \\pi^{+}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'D, electroproduction', 'D+, hadronic decay', 'D+, branching ratio', 'K0(S), hadronic decay', 'mass spectrum, (K0(S) K+)', 'mass spectrum, (K0(S) pi+)', 'isospin, amplitude analysis', 'partial wave', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> D+ anything', 'D+ --> K0(S) K+', 'D+ --> K0(S) pi+', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701008'],"['Using data collected with the CLEO II detector at the Cornell Electron Storage Ring, we present new measurements of the branching fractions for $D^+ CLEO measurements to extract the ratios of isospin amplitudes and phase shifts for $D \\to KK$ and $D \\to K\\pi$.']",['1997-01-14']
2242,['eng'],"['Alam, M S']",['Study of Gluon versus Quark Fragmentation in $\\Upsilon \\to gg\\gamma$ and $e^{+}e^{-} \\to q\\overline{q}\\gamma$ Events at $\\sqrt{s}=10 GeV$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(9460), electroproduction', 'Upsilon(9460), radiative decay', 'quark, fragmentation', 'gluon, fragmentation', 'charged particle, multiplicity', 'mass, (2jet)', 'multiplicity, ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Upsilon(9460)', 'Upsilon(9460) --> 2gluon photon', 'Upsilon(9460) --> quark antiquark photon', '9.46, 10.52 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701006'],"['Using data collected with the CLEO II detector at the Cornell Electron Storage Ring, we determine the ratio R(chrg) for the mean charged multiplicity observed in Upsilon(1S)->gggamma events, to the mean charged multiplicity observed in e+e- -> qqbar gamma events. We find R(chrg)=1.04+/-0.02+/-0.05 for jet-jet masses less than 7 GeV.']",['1997-01-13']
2243,['eng'],"['Schmelling, M']",['Status of the Strong Coupling Constant'],['Particle Physics - Experimental Results'],"['review, Warsaw 1996/07/25', 'strong interaction, coupling constant', 'electron positron, annihilation', 'cross section, hadronic', 'Z0, branching ratio', 'tau, branching ratio', 'sum rule', 'quark, heavy', 'quark, pair production', 'threshold', 'quarkonium, heavy', 'lattice field theory', 'scaling, violation', 'neutrino nucleus, deep inelastic scattering', 'quantum chromodynamics, Lambda parameter', 'perturbation theory, higher-order', 'quark, fragmentation function', 'gluon, fragmentation function', 'hadron hadron, inclusive reaction', 'event shape analysis', 'electron p, interaction', 'jet, multiple production', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701002'],"['The current status of measurements of the strong coupling constant from different reactions is reviewed. Including new results presented at the 1996 ICHEP conference, a global average alpha_s(Mz) = 0.118 +- 0.003 is obtained.']",['1997-01-10']
2244,['eng'],"['Kettell, S H']",['A search for the rare decay $K^+ \\to \\pi^+ \\nu \\nu$'],['Particle Physics - Experimental Results'],"['talk, St. Goar 1996/10/03', 'K+, semileptonic decay', 'K+, radiative decay', 'K+, branching ratio', 'upper limit', 'mass spectrum, (pi+ muon+ muon-)', 'mass spectrum, two-photon', 'Kobayashi-Maskawa angle', 'spectrometer, experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino', 'K+ --> pi+ muon+ muon-', 'K+ --> pi+ 2photon', 'K+ --> muon+ neutrino/mu photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701003'],"['Recent results from the first phase of the E787 experiment and an update on the current status are presented. From the first phase the limit on the K+ -> pi+ nu nu (pnn) branching ratio is BR(pnn) < 2.4e-9 (90%CL). An observation of the decay K+ -> pi+ mu mu has been made using two separate techniques. An observation of the decay K+ -> pi+ gamma gamma has been made and the distribution of two photon invariant mass is inconsistent with phase space but consistent with chiral perturbation theory. A description of recent upgrades to the detector follows. With the upgraded detector the pnn decay should soon be observable. A discussion of the expected sensitivity for pnn during the current running period is presented. Possible improvements, in order to make a significant measurement of |Vtd|, are discussed. One result from the upgraded detector is a measurement of the structure dependent part (SD+) of the decay K+ -> mu+ nu gamma with a branching ratio of BR(SD+) = (1.33 +/- 0.12 +/- 0.18)e-5.']",['1997-01-10']
2245,['eng'],"['Gary, J W']",['Test of QCD Analytic Predictions for Gluon and Quark Jet Differences'],['Particle Physics - Experimental Results'],"['talk, Faro 1996/09/01', 'electron positron, annihilation', 'jet, electroproduction', 'quark, jet', 'gluon, jet', 'final state, (3jet)', 'quantum chromodynamics', 'showers, parton', 'charged particle, multiplicity', 'multiplicity, ratio', 'energy dependence', 'numerical calculations, Monte Carlo', 'electron positron --> quark antiquark gluon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701005'],"['Differences between the properties of gluon and quark jets have been convincingly established by experiments at LEP. Quantitative tests of QCD analytic predictions for these differences have not been possible, however, because of differences between the theoretical and experimental definitions of the jets and event samples. Here, a new method to compare gluon and quark jet properties is described, which uses an inclusive definition of the jets in analogy to theoretical calculations. Using this new method, a value 1.552+-0.041(stat.)+-0.061(syst.) is found for the ratio of the mean charged particle multiplicity in gluon jets to that in quark jets, in agreement with a recent analytic calculation which incorporates energy conservation.']",['1997-01-10']
2246,['eng'],"['Drell, P']",['Experimental Aspects of the Standard Model'],['Particle Physics - Experimental Results'],"['lectures, Boulder 1996/06/02', 'electroweak interaction, validity test', 'lepton nucleon, interaction', 'neutral current', 'charged current', 'electron positron, annihilation', 'hadron hadron, interaction', 'counters and detectors', 'calorimeter', 'colliding beam detector', 'strong interaction, coupling constant', 'cross section, hadronic', 'radiative correction', 'Z0, electroproduction', 'Z0, mass', 'coupling, Yukawa', 'quark, truth', 'B, lifetime', 'Kobayashi-Maskawa angle', 'Higgs particle, search for', 'quark, composite', 'neutrino, oscillation', 'experimental methods', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701001'],"[""This is a series of lectures intended to introduce high energy theorists to the marvels of the Standard Model from an experimentalist's point of view.""]",['1997-01-08']
2247,['eng'],"['Akimov, D Y', 'Belogurov, S G', 'Burenkov, A N', 'Churakov, D', 'Kuzichev, V F', 'Morgunov, V', 'Smirnov, G', 'Solovov, V N']",['Scintillation proportional Xe counter with WLS fiber readout for low-energy X-rays'],['Detectors and Experimental Techniques'],"['astrophysics, missing-mass', 'neutrino, magnetic moment', 'proportional chamber, scintillation counter', 'xenon', 'optics, transformation', 'efficiency']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9703017'],"['A gas Xe based scintillation proportional counter with cylindrical geometry and wavelength shifting (WLS) fiber readout for X-rays of energy 0.5 - 100 keV is proposed. With such a design large sizes and sensitive area of the counter with a fairly well uniformity is possible. The counter could be used for ""dark matter"" search and neutrino magnetic moment measurement and for detection of small amounts or traces of radioactive elements in substances or environment.']",['1997-04-01']
2248,['eng'],"['Ludovici, L', 'Zucchelli, P']","['Conceptual study of an ""anti-tagged"" experiment searching for $\\nu _\\mu \\to \\nu _e$ oscillation']",['Detectors and Experimental Techniques'],"['neutrino, oscillation', 'neutrino/mu, secondary beam', 'neutrino/e, background', 'trigger', 'neutrino, mixing angle', 'neutrino, mass difference', 'Cherenkov counter', 'photon, counters and detectors', 'numerical calculations, Monte Carlo', 'proposed experiment', 'CERN Lab', '19.2 GeV (p)']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-96-181', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9701007']","[""We study the feasibility, from the conceptual point of view, %of a high energy, appearance , zero background experiment to detect %$\\nu_\\mu \\rightarrow \\nu_e$ oscillations with maximum sensitivity % ($sin^2 2 \\theta = 10^{-4}$) %in the $\\Delta m^2 \\simeq 1 \\; eV^2$ region, %fully covering the area where the LSND experiment claims evidence. Partial %overlap with the atmospheric neutrino region ($\\Delta m^2 \\simeq 0.01 \\; eV^2$ %at maximum mixing) is also foreseen. The ``natural'' $\\nu_e$ %background of the neutrino beam, due to $K,\\mu$ decays in the decay tunnel, % is controlled by using % a hadron blind detector that vetoes , by time concidence, an eventual %$\\nu_e$ signal in %the neutrino detector ({\\sl anti-tagging technique}). %The existing CERN PS beamline could be resurrected %because of the ideal $L/E$ ratio and the proton availability before the %LHC era. %----- %We study the feasibility, from the conceptual point of view, %of a high energy, zero background appearance experiment to detect %$\\nu_\\mu \\rightarrow \\nu_e$ oscillations with maximum sensitivity %in the $\\dm2 \\simeq 1 \\; eV^2$ region, %fully covering the area where the LSND experiment claims evidence and also %partially overlapping the atmospheric neutrino region. The ``natural'' $\\nu_e$ %background of the neutrino beam, due to K and $\\mu$ decays in the decay tunnel, %is suppressed by a hadron blind detector that vetoes, by time coincidence, %a possible $\\nu_e$ signal in the neutrino detector %({\\sl anti-tagging technique}). %The PS accelerator at CERN offers the ideal $L/E$ ratio and %the proton availability before the LHC era. %----- We study the conceptual feasibility of a high energy, ``short baseline'', zero background experiment to search for \\numtonue\\ oscillations and fully covering the area where the LSND experiment claims evidence. The natural \\nue\\ background of the \\num\\ beam, from $K$ and $\\mu$ decays in the decay tunnel, is suppressed by a hadron blind detector that vetoes, by time coincidence, a possible \\nue\\ signal in the neutrino detector ({\\sl anti-tagging technique}). We discuss this new idea and we study a possible implementation in the old neutrino line of the PS accelerator, which at CERN offers the ideal $L/E$ ratio. In the anti-tagged \\num\\ beam, the \\nue\\ contamination can be reduced by more than two orders of magnitude over conventional beams, down to $\\nue/\\num = 5\\cdot 10^{-5}$. In an ideal appearance experiment using a $300\\; t$ detector one would expect after two years $112$ events according to the LSND result, with a background of $1.1\\div 2.4$ events. In case of a negative search, the $90\\%$ C.L. upper limit in the mixing angle would be $\\sin2tme < 1.8\\cdot 10^{-4}$ for large \\dm2\\ and $\\dm2 <3.3\\cdot 10^{-2}\\; eV^2$ for maximal mixing.""]",['1996-12-12']
2249,['eng'],"['Burkot, W', 'Coghen, T', 'Czyzewski, J', 'Wittek, W', 'Aderholz, Michael', 'Guy, J', 'Jones, G T', 'Katz, U F', 'Marage, P', 'Morrison, Douglas Robert Ogston', 'Myatt, Gerald', 'Schmitz, N', 'Venus, W A']",['Nuclear Attenuation of Fast Hadrons Produced in Charged-Current Neutrino and Antineutrino Interactions in Neon'],['Particle Physics - Experimental Results'],"['neutrino nucleus, interaction', 'interaction, neutrino nucleus', 'antineutrino, interaction', 'interaction, antineutrino', 'neon', 'charged current', 'hadron, neutrinoproduction', 'neutrinoproduction, hadron', 'fragmentation function', 'neutrino p, interaction', 'interaction, neutrino p', 'bubble chamber, experimental results', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612015'],"[""The production of hadrons in charged-current (anti)neutrino interactions is studied with the bubble chamber BEBC exposed ot the CERN (anti)neutrino wide-band beam. Fast-hadron production in a neon target is found to be attennuated as compared to that in a hydrogen target. This feature is discussed within the theoretical models based on the idea of a hadron formation length. The experimental results favour the `constituent' over the `yo-yo' length concept, and suggest a quark cross-section in the order of 3mb.""]",['1996-12-17']
2250,['eng'],"['Czyzewski, J']",['Correlations in transverse momentum in pion-proton and kaon-proton collisions at 250 GeV/c'],['Particle Physics - Experimental Results'],"['talk, Nijmegen 1996/06/30', 'pi+ p, interaction', 'K+ p, interaction', 'hadron, multiple production', 'multiplicity, moment', 'correlation, two-particle', 'transverse momentum, difference', 'rapidity', 'boson, statistics', 'particle source, spatial distribution', 'four-pi-detector, EHS', 'bubble chamber(hydrogen), experimental results', 'CERN SPS', '250 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612016'],"['We have measured the second-order normalized differential factorial moments as a function of the difference of transverse momentum ($\\Delta p_T$) in $\\p^+ p$ and $K^+ p$ collisions at 250 GeV/$c$. The second-order differential factorial moments for like-charged pairs reveal a strong increase with decreasing $\\Delta p_T$. In a small central rapidity window this increase is described by a simple power law. Such a behavior, if interpreted as originating from Bose-Einstein correlations, may indicate a structure of the transverse spatial distribution of the source similar to that recently predicted by Bia\\l{}as and Peschanski for color-dipole emission in onium-onium scattering. The power of the rise obtained in the fit agrees with the predicted value.']",['1996-12-17']
2251,['eng'],"['Hamel, L A', 'Lessard, L', 'Rainville, L', 'Sur, B', 'Zacek, V']",['A Superheated Droplet Detector for Dark Matter Search'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'sparticle, search for', 'recoil, energy', 'counters and detectors, droplet', 'production, bubble', 'thermodynamics, critical phenomena', 'solid-state counter', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612014'],"['We discuss the operation principle of a detector based on superheated droplets of Freon-12 and its feasibility for the search of weakly interacting cold dark matter particles. In particular we are interested in a neutralino search experiment in the mass range from 10 to 10^4 GeV/c^2 and with a sensitivity of better than 10^-2 events/kg/d. We show that our new proposed detector can be operated at ambient pressure and room temperature in a mode where it is exclusively sensitive to nuclear recoils like those following neutralino interactions, which allows a powerful background discrimination. An additional advantage of this technique is due to the fact that the detection material, Freon-12, is cheap and readily available in large quantities. Moreover we were able to show that piezoelectric transducers allow efficient event localization in large volumes.']",['1996-12-16']
2252,['eng'],"['Abachi, S']",['Search for Top Squark Pair Production in the Dielectron Channel'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'sparticle, search for', 'squark, truth', 'squark, pair production', 'decay, squark', 'final state, (positron electron)', 'transverse energy, missing-energy', 'channel cross section, branching ratio', 'upper limit', 'supersymmetry', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'squark --> beauty chargino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612009'],"['This report describes the first search for top squark pair production in the channel stop_1 stopbar_1 -> b bbar chargino_1 chargino_1 -> ee+jets+MEt using 74.9 +- 8.9 pb^-1 of data collected using the D0 detector. A 95% confidence level upper limit on sigma*B is presented. The limit is above the theoretical expectation for sigma*B for this process, but does show the sensitivity of the current D0 data set to a particular topology for new physics.']",['1996-12-13']
2253,['eng'],"['Abachi, S', 'Abbott, E']",['Search for Diphoton Events with Large Missing Transverse Energy in proton-antiproton collisions at $\\sqrt(s)$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'photon, pair production', 'transverse energy, missing-energy', 'supersymmetry', 'sparticle, pair production', 'sparticle, radiative decay', 'selectron', 'sneutrino', 'neutralino', 'sparticle, mass', 'channel cross section, branching ratio', 'upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2photon anything', 'anti-p p --> 2sparticle anything', 'sparticle --> 2photon', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612011'],"['A search for signals of new physics has been carried out in the channel p pbar -> gamma gamma + ETmiss. This signature is expected in various recently proposed supersymmetric (SUSY) models. We observe 842 events with two photons having transverse momentum ET(g) > 12 GeV and pseudorapidity |eta(g)| < 1.1. Of these, none have missing transverse energy (ETmiss) in excess of 25 GeV. The distribution of ETmiss is consistent with that of the expected background. We therefore set limits on production cross sections for selectron, sneutrino and neutralino pairs, decaying into photons. The limits range from about 400 fb to 1 pb depending on the sparticle masses. A general limit of 185 fb (95% C.L.) is set on sigma.B(pbar p -> gamma gamma ETmiss + X) where ET(g) > 12 GeV, |eta(g)| < 1.1, and ETmiss > 25 GeV.']",['1996-12-13']
2254,['eng'],"['Burrows, P N', 'Dixon, L', 'El-Khadra, A X', 'Gary, J W', 'Giele, W T', 'Harris, D A', 'Ritz, S', 'Schumm, B A']",['Prospects for the Precision Measurement of $\\alpha_s$'],['Detectors and Experimental Techniques'],"['talk, Snowmass 1996/06/25', 'strong interaction, coupling constant', 'measurement, error', 'lepton nucleon, deep inelastic scattering', 'nucleon, structure function', 'lepton, polarized beam', 'nucleon, polarized target', 'dependence, momentum transfer', 'sum rule', 'quantum chromodynamics', 'lattice field theory', 'quarkonium, energy levels', 'quarkonium, heavy', 'renormalization', 'approximation, quenching', 'quark, sea', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'hadron hadron, interaction', 'W, hadroproduction', 'jet, associated production', 'numerical calculations, interpretation of experiments', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612012'],['The prospects for the measurement of the strong coupling constant alpha_msbar(M_Z) to a relative uncertainty of 1% are discussed. Particular emphasis is placed on the implications relating to future High Energy Physics facilities.'],['1996-12-13']
2255,['eng'],"['Hinchliffe, Ian', 'Womersley, J']",['High Transverse Momentum Physics at the Large Hadron Collider'],['Detectors and Experimental Techniques'],"['talk, Snowmass 1996/06/25', 'p p, interaction', 'transverse momentum, high', 'gauge field theory, SU(3) x SU(2) x U(1)', 'electroweak interaction, symmetry breaking', 'Higgs particle, mass', 'supersymmetry', 'model, technicolor', 'model, composite', 'Higgs particle, hadroproduction', 'Higgs particle, decay modes', 'Higgs particle, multiplet', 'sparticle, search for', 'W, strong interaction', 'gauge boson, postulated particle', 'coupling, (3gauge boson)', 'mass, truth', 'quark, rare decay', 'magnetic detector, ATLAS', 'magnetic detector, CMS', 'numerical calculations, CERN LHC Coll', '14000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612006'],['This note summarizes the various physics studies done for the LHC. It concentrates on the processes involving the production of high mass states. Results are drawn from simulations performed by the CMS and ATLAS collaborations. The ability of the LHC to provide insight into the mechanism of electroweak symmetry breaking is exemplified.'],['1996-12-11']
2256,['eng'],"['Burrows, P N']",['Review of $\\alpha _s$ Measurements'],['Particle Physics - Experimental Results'],"['review, Cracow 1996/08/01', 'strong interaction, coupling constant', 'quantum chromodynamics, Lambda parameter', 'renormalization, dependence', 'electron positron, annihilation', 'hadron hadron, interaction', 'lepton nucleon, deep inelastic scattering', 'cross section, hadronic', 'Z0, width', 'tau, decay modes', 'tau, branching ratio', 'hadron, multiple production', 'event shape analysis', 'fragmentation function', 'scaling, violation', 'nucleon, structure function', 'structure function, polarization', 'jet, electroproduction', 'jet, hadroproduction', 'W, hadroproduction', 'photon, direct production', 'quarkonium, heavy', 'quarkonium, decay modes', 'quarkonium, energy levels', 'lattice field theory', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612007'],"[""Determinations of alpha_s are reviewed. Current results are limited to a precision of around 3-20%, largely by theoretical uncertainties. All measurements are consistent with a `world average' value of 0.118 +- 0.005 and there is no evodence of any discrepancy between `low-Q^2' and `high-Q^2' results.""]",['1996-12-11']
2257,['eng'],"['Aitala, E M']",['Search for CP Violation in Charged D Meson Decays'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'charmed meson, hadroproduction', 'D, hadronic decay', 'violation, CP', 'charge, asymmetry', 'mass spectrum', 'spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> K+ K- pi+', 'D+ --> Phi(1020) pi+', 'D+ --> K*(892) K+', 'D+ --> 2pi+ pi-', '500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612005'],"['We report results of a search for CP violation in the singly Cabibbo-suppressed decays D+ -> K- K+ pi+, phi pi+, K*(892)0 K+, and pi- pi+ pi+ based on data from the charm hadroproduction experiment E791 at Fermilab. We search for a difference in the D+ and D- decay rates for each of the final states. No evidence for a difference is seen. The decay rate asymmetry parameters A(CP), defined as the difference in the D+ and D- decay rates divided by the sum of the decay rates, are measured to be: A(CP)(K K pi) = -0.014 +/- 0.029, A(CP)(phi pi) = -0.028 +/- 0.036, A(CP)(K*(892) K) = -0.010 +/- 0.050, and A(CP)(pi pi pi) = -0.017 +/- 0.042.']",['1996-12-10']
2258,['eng'],"['Kasahara, S M']",['A Study of Cosmic Ray Composition in the Knee Region using Multiple Muon Events in the Soudan 2 Detector'],['Astrophysics and Astronomy'],"['cosmic radiation, primary', 'elements, cosmic radiation', 'p, cosmic radiation', 'muon, cosmic radiation', 'muon, multiplicity', 'cosmic radiation, flux', 'cosmic radiation, energy', 'deep underground detector, Soudan', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612004'],"['Deep underground muon events recorded by the Soudan 2 detector, located at a depth of 2100 meters of water equivalent, have been used to infer the nuclear composition of cosmic rays in the ""knee"" region of the cosmic ray energy spectrum. The observed muon multiplicity distribution favors a composition model with a substantial proton content in the energy region 800,000 - 13,000,000 GeV/nucleus.']",['1996-12-06']
2259,['eng'],"['Burrows, P N', 'Dawson, S', 'Orr, L', 'Smith, W H']",['QCD'],['Particle Physics - Experimental Results'],"['talk, Snowmass 1996/06/25', 'electron positron, annihilation', 'electron p, deep inelastic scattering', 'p p, interaction', 'anti-p p, inclusive reaction', 'quantum chromodynamics, validity test', 'strong interaction, coupling constant', 'nucleon, structure function', 'momentum spectrum, parton', 'parametrization', 'jet, hadroproduction', 'transverse energy, spectra', 'sum rule', 'quark, hadroproduction', 'quark, heavy', 'diffraction', 'rapidity, gap', 'structure function, polarization', 'spin, asymmetry']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612003'],"['Despite many experimental verifications of the correctness of our basic understanding of QCD, there remain numerous open questions in strong interaction physics and we focus on the role of future colliders in addressing these questions. We discuss possible advances in the measurement of $\\alpha_s$, in the study of parton distribution functions, and in the understanding of low $x$ physics at present colliders and potential new facilities. We also touch briefly on the role of spin physics in advancing our understanding of QCD.']",['1996-12-05']
2260,['eng'],"['Abramowicz, H']",['Tests of QCD at low $x$'],['Particle Physics - Experimental Results'],"['review, Warsaw 1996/07/25', 'hadron hadron, interaction', 'lepton p, deep inelastic scattering', 'Regge poles', 'exchange, pomeron', 'quantum electrodynamics, validity test', 'small-x', 'spectra, momentum transfer', 'p, structure function', 'structure function, longitudinal', 'gluon, momentum spectrum', 'structure function, charm', 'hadron, electroproduction', 'vector meson, electroproduction', 'strong interaction, coupling constant', 'diffraction', 'photon, structure function', 'Altarelli-Parisi equation', 'jet, photoproduction', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612001'],"['This talk reviews the latest measurements of the proton, Pomeron and photon structure functions. These measurements, especially at low $x$ and/or low $Q^2$ lead to new insight into the picture of hadronic interactions.']",['1996-12-02']
2261,['eng'],"['Adloff, C']","['Determination of the Longitudinal Proton Structure Function $F_{L}(x,Q^{2})$ at Low x']",['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'positron p, deep inelastic scattering', 'positron p, inclusive reaction', 'p, structure function', 'structure function, longitudinal', 'cross section, momentum transfer', 'cross section, x-dependence', 'Altarelli-Parisi equation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'positron p --> positron anything', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611017'],"['A measurement of the inclusive cross section for the deep-inelastic scattering of positrons off protons at HERA is presented at momentum transfers $8.5 \\leq Q^2 \\leq 35 GeV^2$ and large inelasticity $y = 0.7$, i.e. for the Bjorken-x range $0.00013 \\leq x \\leq 0.00055$. Using a next-to-leading order QCD fit to the structure function F_2 at lower y values, the contribution of F_2 to the measured cross section at high y is calculated and, by subtraction, the longitudinal structure function F_{L} is determined for the first time with an average value of $F_L=0.52 \\pm 0.03 (stat)$^ {+0.25}_{-0.22}$ (syst) at $Q^2=15.4 GeV^2$ and $x=0.000243$.']",['1996-11-25']
2262,['eng'],"['Demarteau, M']",['Electroweak Physics Results from the Tevatron'],['Particle Physics - Experimental Results'],"['review, Snowmass 1996/06/25', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'Z0, hadroproduction', 'W, hadroproduction', 'intermediate boson, leptonic decay', 'channel cross section, branching ratio', 'charge, asymmetry', 'angular distribution, asymmetry', 'W, mass', 'W, width', 'W, rare decay', 'W, radiative decay', 'gauge boson, pair production', 'coupling, (3gauge boson)', 'transverse momentum, spectra', 'mass spectrum, transverse', 'four-pi-detector, DZERO', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'bibliography', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611018'],"['An overview of recent electroweak physics results from the Tevatron is given. Properties of the W and Z gauge bosons using final states containing electrons and muons based on large integrated luminosities are presented. In particular, measurements of the W and Z production cross sections, the W-charge asymmetry and the measurement of the W-mass are summarized. Gauge boson self interactions are measured by studying gauge boson pair production and limits on anomalous gauge boson couplings are discussed.']",['1996-11-25']
2263,['eng'],"['Demarteau, M']",['Precision Electroweak Measurements'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'electroweak interaction, validity test', 'electron positron, colliding beams', 'electron positron, annihilation', 'anti-p p, colliding beams', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, pair production', 'quark, charm', 'quark, beauty', 'quark, truth', 'W, hadroproduction', 'Z0, hadroproduction', 'intermediate boson, leptonic decay', 'intermediate boson, width', 'angular distribution, asymmetry', 'Weinberg angle', 'Drell-Yan process', 'mass, transverse', 'W, mass', 'W, pair production', 'differential cross section, mass', 'coupling constant, vector', 'coupling constant, axial-vector', 'Z0, branching ratio', 'mass, truth', 'Higgs particle, mass', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611019'],"[""Recent electroweak precision measurements from e+e- and pbarp colliders are presented. Some emphasis is placed on the recent developments in the heavy flavor sector. The measurements are compared to predictions from the Standard Model of electroweak interactions. All results are found to be consistent with the Standard Model. The indirect constraint on the top quark mass from all measurements is in excellent agreement with the direct Mt measurements. Using the world's electroweak data in conjunction with the current measurement of the top quark mass, the constraints on the Higgs mass are discussed.""]",['1996-11-25']
2264,['eng'],"['Kobel, M']",['Measurements of Four-Fermion Production via Neutral Elektroweak Currents at LEP'],['Particle Physics - Experimental Results'],"['talk, Warsaw 1996/07/25', 'electron positron, colliding beams', 'electron positron, interaction', 'neutral current', 'final state, (4fermion)', 'quark, pair production', 'lepton, pair production', 'neutrino, pair production', 'multiplicity', 'momentum, missing-energy', 'experimental results', 'CERN LEP Stor', 'approx. 91, 130-136, 161 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611015'],['Four-fermion production via electroweak neutral currents has been measured by all four LEP collaborations at center-of-mass energies near the Z resonance and for the first time also at energies well above the Z peak. Essentially all possible final states have been covered in four different topologies.'],['1996-11-21']
2265,['eng'],"['Mallot, G K']",['Spin Physics with COMPASS'],['Particle Physics - Experimental Results'],"['talk, Amsterdam 1996/09/10', 'muon nucleus, inclusive reaction', 'quark, charm', 'quark, pair production', 'light nucleus, polarized target', 'fusion, photon gluon', 'gluon, polarization', 'D0, hadronic decay', 'D*(2010), cascade decay', 'nucleon, structure function', 'structure function, spin', 'magnetic spectrometer', 'proposed experiment, CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611016'],['The recently proposed COMPASS experiment at CERN attempts a measurement of the gluon polarisation with a precision of delta(Delta g/g) = 0.1. The experiment uses open charm muoproduction to tag the photon-gluon fusion process.'],['1996-11-21']
2266,['eng'],"['Halzen, Francis']",['Status of the AMANDA South Pole Neutrino Detector'],['Particle Physics - Experimental Results'],"['talk, Heidelberg 1996/09/16', 'neutrino, cosmic radiation', 'deep underground detector, AMANDA', 'Cherenkov counter', 'solids, water', 'photoelectron, amplifier', 'photon, path length', 'neutrino, energy', 'muon, neutrinoproduction', 'showers, electromagnetic']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611014'],"['Initial deployment of optical modules near 1 and 2 kilometer depth indicate that deep polar ice is the most transparent known natural solid. Experience with early data has revealed that a detector, conceived to measure muons tracks, can also measure energy of high energy neutrinos as well as bursts of MeV neutrinos, e.g. produced by supernovae and gamma ray bursts. We plan to complete AMANDA this austral summer to form a detector of 11 deep strings instrumented over 400 meters height with 300 optical modules. We will argue that ice is the ideal medium to deploy a future kilometer-scale detector and discuss the first deployment of 10 strings of kilometer length.']",['1996-11-20']
2267,['eng'],"['Barabash, L']","['Measurement of $xF_3$, $F_2$ Structure Functions and Gross-Llewellyn Smith Sum Rule with IHEP-JINR Neutrino Detector']",['Particle Physics - Experimental Results'],"['neutrino nucleon, interaction', 'antineutrino nucleon, interaction', 'neutrino/mu', 'nucleon, structure function', 'structure function, isoscalar', 'sum rule', 'structure function, x-dependence', 'quantum chromodynamics, Lambda parameter', 'strong interaction, coupling constant', 'calorimeter, experimental results', 'Serpukhov PS', '67, 70 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611012'],"['The isoscalar structure functions xF_3 and F_2 are measured as functions of x averaged over all Q^2 permissible for the range 6 to 28 GeV of incident (anti)neutrino energy. With the measured values of xF_3, the value of the Gross-Llewellyn Smith sum rule is found to be $\\int_{0}^{1}{F_3 dx} = 2.13\\pm0.38 (stat)\\pm 0.26 (syst)$. The QCD analysis of xF_3 provides interaction constant $\\alpha_S (M_Z)=0.120^{+3}_{-4}$ is larger than most of the deep inelastic scattering results.']",['1996-11-19']
2268,['eng'],"['Abe, K', 'Abt, I']",['An Improved Measurement of the Left-Right $Z^{0}$ Cross Section Asymmetry'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'polarization, asymmetry', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.28 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611011'],"['We present a new measurement of the left-right cross section asymmetry (ALR) for Z boson production by e+e- collisions. The measurement was performed at a center-of-mass energy of 91.28 GeV with the SLD detector at the SLAC Linear Collider (SLC). The luminosity-weighted average polarization of the SLC electron beam was (77.23+-0.52)%. Using a sample of 93,644 Z decays, we measure the pole-value of the asymmetry, ALR0, to be 0.1512+-0.0042(stat.)+-0.0011(syst.) which is equivalent to an effective weak mixing angle of sin**2(theta_eff)=0.23100+-0.00054(stat.)+-0.00014(syst.).']",['1996-11-19']
2269,['eng'],"['Romosan, A']",['A High Statistics Search for $\\nu-{\\mu}(\\overline{\\nu}\\mu) \\to \\nu-{e}(\\overline{\\nu}e)$ Oscillations in the Small Mixing Angle Regime'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'neutrino/mu', 'neutrino/e, flux', 'neutrino nucleon, interaction', 'charged current', 'showers, energy loss', 'neutrino, mixing angle', 'neutrino, mass difference', 'universality, (neutrino/mu neutrino/e)', 'calorimeter, experimental results', 'Batavia TEVATRON PS', '30-600 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611013'],"['Limits on $\\nu_\\mu (\\overline{\\nu}_\\mu) \\to \\nu_e (\\overline{\\nu}_e)$ oscillations based on a statistical separation of $\\nu_e N$ charged current interactions in the CCFR detector at Fermilab are presented. $\\nu_e$ interactions are identified by the difference in the longitudinal shower energy deposition pattern of $\\nu_e N \\rightarrow eX$ versus $\\nu_\\mu N \\to \\nu_\\mu X$ interactions. Neutrino energies range from 30 to 600 GeV with a mean of 140 GeV, and $\\nu_\\mu$ flight lengths vary from 0.9 km to 1.4 km. The lowest 90% confidence upper limit in $sin^2 2\\alpha$ of $1.1 \\times 10^{-3}$ is obtained at $\\Delta m^2 \\sim 300 eV^2$. For $sin^2 2\\alpha = 1$, $\\Delta m^2 > 1.6 eV^2$ is excluded, and for $\\Delta m^2 \\gg 1000 eV^2$, $sin^2 2\\alpha > 1.8 \\times 10^{-3}$ is excluded. This result is the most stringent limit to date for favoured by the LSND experiment. The $\\nu_\\mu$-to-$\\nu_e$ cross-section ratio was measured as a test of $\\nu_\\mu (\\bar\\nu_\\mu) \\leftrightarrow \\nu_e']",['1996-11-19']
2270,['eng'],"['Tkaczyk, S M']",['Quarkonium Production in $p-\\overline{p}$ Collisions at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Warsaw 1996/07/25', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quarkonium, charm', 'quarkonium, beauty', 'quarkonium, hadroproduction', 'quarkonium, leptonic decay', 'final state, dimuon', 'quarkonium, direct production', 'psi mesons', 'upsilon mesons', 'chi mesons, radiative decay', 'quark, beauty', 'quark, decay', 'decay, path length', 'differential cross section, transverse momentum', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611009'],"['Charmonium and bottomonium production is studied using $\\mu^+\\mu^-$ data samples collected by the CDF and D0 experiments during the 1992-96 p-pbar collider run at the Fermilab Tevatron. The inclusive cross sections as a function of the transverse momentum of reconstructed quarkonium states are measured. The results are compared with theoretical predictions, which take into account different quarkonium production mechanisms.']",['1996-11-18']
2271,['eng'],"['Bruins, E E W']",['Semi-inclusive spin asymmetries in polarised deep inelastic electron scattering'],['Particle Physics - Experimental Results'],"['talk, Amsterdam 1996/09/10', 'positron nucleus, deep inelastic scattering', 'positron nucleus, inclusive reaction', 'helium, nuclide', 'polarized target, internal', 'polarization, longitudinal', 'hadron, electroproduction', 'spin, asymmetry', 'pi0', 'diffraction, production', 'rho(770)0, hadronic decay', 'angular distribution', 'transparency', 'dependence, momentum transfer', 'magnetic spectrometer, HERMES', 'experimental results', 'DESY HERA Stor', '27.5 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611010'],"['In 1995, the HERMES experiment at DESY (Hamburg, Germany) has taken its first data, using the 27.5 GeV polarised HERA positron beam impinging on a longitudinally polarised internal $^3$He target. Preliminary results from the semi-inclusive physics program are presented.']",['1996-11-18']
2272,['eng'],"['Burrows, P N']",['Determination of $\\alpha_{s}(M_Z^2)$ from hadronic event shape observables in $e^+e^-$ annihilation'],['Particle Physics - Experimental Results'],"['talk, Warsaw 1996/07/25', 'electron positron, annihilation', 'Z0, electroproduction', 'hadron, multiple production', 'strong interaction, coupling constant', 'event shape analysis', 'quantum chromodynamics, perturbation theory', 'Pade approximation', 'renormalization', 'numerical calculations', 'interpretation of experiments, SLAC SLC Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612008'],"[""The determination of alpha_s(M_Z^2) using O(alpha_s^2) calculations of hadronic event observables in e+e- annihilation is reviewed. The large scatter among alpha_s(M_Z^2) values determined from different observables may be interpreted as arising from the effect of uncalculated higher-order contributions. The application of `optimised' perturbation theory and Padé approximants in an attempt to reduce this effect is discussed.""]",['1996-12-12']
2273,['eng'],"['Allison, W W M', 'Alner, G J', 'Ayres, D S', 'Barrett, W L', 'Bode, C', 'Border, P M', 'Brooks, C B', 'Cobb, J H', 'Cockerill, D J A', 'Cotton, R J', 'Courant, H', 'Demuth, D M', 'Fields, T H', 'Gallagher, H R', 'García-García, C', 'Goodman, M C', 'Gray, R N', 'Johns, K', 'Kafka, T', 'Kasahara, S M', 'Leeson, W', 'Litchfield, P J', 'Longley, N P', 'Lowe, M J', 'Mann, W A', 'Marshak, M L', 'May, E N', 'Milburn, R H', 'Miller, W H', 'Mualem, L M', 'Napier, A', 'Oliver, W', 'Pearce, G F', 'Perkins, Donald Hill', 'Peterson, E A', 'Petyt, D A', 'Price, L E', 'Roback, D M', 'Ruddick, K', 'Schmid, D J', 'Schneps, J', 'Schub, M H', 'Seidlein, R V', 'Shupe, M A', 'Stassinakis, A', 'Sundaralingam, N', 'Thomas, J', 'Thron, J L', 'Vasilev, V', 'Villaume, G', 'Wakely, S P', 'Wall, D', 'Werkema, S J', 'West, N', 'Wielgosz, U M']",['Measurement of the atmospheric neutrino flavour composition in Soudan 2'],['Particle Physics - Experimental Results'],"['neutrino, cosmic radiation', 'neutrino/mu, flux', 'neutrino/e, flux', 'flux, ratio', 'deep underground detector, Soudan', 'calorimeter, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611007'],['The atmospheric neutrino flavour ratio measured using a 1.52 kton-year exposure of Soudan 2 is found to be 0.72 +- 0.19 +0.05 -0.07 relative to the expected value from a Monte Carlo calculation. The possible background of interactions of neutrons and photons produced in muon interactions in the rock surrounding the detector has been investigated and is shown not to produce low values of the ratio.'],['1996-11-14']
2274,['eng'],"['Nemati, B']",['Measurement of the Direct Photon Spectrum in $\\Upsilon(1S)$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(9460), electroproduction', 'Upsilon(9460), radiative decay', 'Upsilon(9460), branching ratio', 'Upsilon(9460), width', 'momentum spectrum, (photon)', 'strong interaction, coupling constant', 'quantum chromodynamics, Lambda parameter', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Upsilon(9460) --> 2gluon photon', 'Upsilon(9460) --> 3gluon', '9.46, 10.52 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611020'],"['Using data taken with the CLEO II detector at the Cornell Electron Storage Ring, we have determined the ratio of branching fractions: $R_{\\gamma} \\equiv = (2.75 \\pm 0.04(stat.) \\pm 0.15(syst.))%$. From this ratio, we have determined the QCD scale parameter $\\Lambda_{\\overline{MS}}$ (defined in the modified minimal subtraction scheme) to be $\\Lambda_{\\overline{MS}}= 233 \\pm 11 \\pm 59$ MeV, from which we determine a value for the strong coupling constant']",['1996-11-27']
2275,['eng'],"['Woods, M']",['The polarized electron beam for the SLAC Linear Collider'],['Accelerators and Storage Rings'],"['talk, Amsterdam 1996/09/10', 'electron positron, linear collider', 'electron, polarized beam', 'particle source, polarized beam', 'polarization, beam monitoring', 'SLAC SLC Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611006'],"[""The SLAC Linear Collider has been colliding a polarized electron beam with an unpolarized positron beam at the Z^0 resonance for the SLD experiment since 1992. An electron beam polarization of close to 80% has been achieved for the experiment at luminosities up to 8x10^29 cm^-2 s^-1. This is the world's first and only linear collider, and is a successful prototype for the next generation of high energy electron linear colliders. This paper discusses polarized beam operation for the SLC, and includes aspects of the polarized source, spin transport and polarimetry. Presented at the 12th International Symposium on High Energy Spin Physics held at Amsterdam, The Netherlands September 10-14, 1996.""]",['1996-11-11']
2276,['eng'],"['Aïd, S']",['Scale Influence on the Energy Dependence of Photon-Proton Cross Sections'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'photon p, interaction', 'photon, fragmentation', 'hadron, photoproduction', 'cross section, energy dependence', 'charged particle, transverse momentum', 'quantum chromodynamics, perturbation theory', 'field theory, Regge', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611004'],['The scale dependence of the evolution of photoproduction cross sections with the photon-proton centre of mass energy W is studied using low Q^2 < 0.01 GeV^2 e^+p interactions collected by the H1 experiment at HERA. The value of the largest transverse momentum of a charged particle in the photon fragmentation region is used to define the hard scale. The slope of the $W$ dependence of the cross section is observed to increase steeply with increasing transverse momentum. The result is compared to measurements of the Q^2 evolution of the W dependence of the virtual photon-proton cross section. Interpretations in terms of QCD and in terms of Regge phenomenology are discussed.'],['1996-11-07']
2277,['eng'],"['Schumacher, R A']",['Photoproduction evidence for and against hidden-strangeness states near 2 GeV'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'carbon', 'baryon resonance, hadroproduction', 'baryon resonance, decay', 'mass spectrum, (Sigma0 K+)', 'mass spectrum, (Sigma(1385) K+)', 'quark, multiquark', 'K anti-K, molecule', 'photon p, exclusive reaction', 'baryon resonance, search for', 'baryon resonance, (2050)', 'strange particle, photoproduction', 'Sigma(1385)', 'Sigma0', 'K', 'K*(892)', 'Lambda', 'baryon resonance, width', 'channel cross section, energy dependence', 'numerical calculations, interpretation of experiments', 'p carbon --> Sigma0 K+', 'p carbon --> Sigma(1385) K+', 'photon p --> Lambda K pi', 'photon p --> Sigma K pi', 'photon p --> Sigma0 K']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611003'],"['Experimental evidence from coherent diffractive proton scattering has been reported for two narrow baryonic resonances which decay predominantly to strange particles. These states, with masses close to 2.0 GeV would, if confirmed, be candidates for hidden strangeness states with unusual internal structure. In this paper we examine the literature on strangeness photoproduction, to seek additional evidence for or against these states. We find that one state is not confirmed, while for the other state there is some mild supporting evidence favoring its existence. New experiments are called for, and the expected photoproduction lineshapes are calculated.']",['1996-11-06']
2278,['eng'],"['De Jongh, F', 'Michail, G']",['Time Dependent $B0 \\overline{B}^0$ Mixing at CDF'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'B0 anti-B0, interference', 'time dependence', 'B, semileptonic decay', 'B0, mass difference', 'final state, dilepton', 'magnetic detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'B --> D lepton neutrino', 'B --> D*(2010) neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9612010'],['We describe two measurements of Delta m_d. The first uses B -> nu l D(*) events and a same-side flavor tagging algorithm. The second uses dilepton events. From the average of these two measurements we find Delta m_d = 0.466 +- 0.037 +- 0.031 ps^{-1}.'],['1996-12-13']
2279,['eng'],"['Gadomski, S', 'Eerola, Paula Anna-Mari', 'Bannikov, A V']",['ATLAS sensitivity range for the $x_{s}$ measurement'],['Detectors and Experimental Techniques'],"['p p, inclusive reaction', 'B/s0, hadroproduction', 'B/s0 anti-B/s0, interference', 'B/s0, hadronic decay', 'D/s-', 'a1(1260)', 'asymmetry, time dependence', 'Kobayashi-Maskawa angle, unitarity', 'magnetic detector, ATLAS', 'time resolution', 'luminosity', 'efficiency', 'numerical calculations, Monte Carlo', 'CERN LHC Coll', 'p p --> B/s0 anything', 'B/s0 --> D/s- pi+', 'B/s0 --> D/s- a1(1260)', '14000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611001'],"['Previous results for the prospects of B_s mixing measurement in the ATLAS experiment at LHC are updated. The improved analysis method of the studied decay channels B_s -> D_s pi and B_s -> D_s a_1, combined with most recent values for the branching ratios and the B_s lifetime, leads to the new ATLAS sensitivity range for the x_s measurement: x_s^{max} = 42. An extensive study is done in order to estimate how x_s^{max} is influenced by the B-decay proper-time resolution of the vertex detector, as well as by the number of events and by the signal-to-background ratio.']",['1996-11-04']
2280,['eng'],"['Aitala, E M']",['Measurement of the Branching Ratio $B(D^{+} \\to \\rho^{0}l^{+}\\nu_{l})/ B(D^{+} \\to \\overline{K}^{*0}l^{+}\\nu _{l})$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D+, hadroproduction', 'D+, semileptonic decay', 'D+, branching ratio', 'rho(770)0', 'K*(892)', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> rho(770)0 lepton+ neutrino', 'D --> K*(892) lepton+ neutrino', 'rho(770)0 --> pi+ pi-', 'K*(892) --> K- pi+', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9611002'],"['We report a measurement of the branching ratio B(D+-->rho^0 l nu)/ B(D+-->K*0 l nu) from the Fermilab charm hadroproduction experiment E791. Based on signals of 49+-17 events in the D+--> rho^0 e nu mode and 54+-18 events in the D+--> rho^0 mu nu mode, we measure B(D+-->rho^0 e nu)/B(D+-->K*0 e nu) = 0.045+-0.014+-0.009, and B(D+-->rho^0 mu nu)/B(D+-->K*0 mu nu) = 0.051+-0.015+-0.009. Combining the results from both the electronic and muonic modes, we obtain B(D+-->rho^0 l nu)/B(D+-->K*0 l nu) = 0.047+-0.013. This result is compared to theoretical predictions.']",['1996-11-04']
2281,['eng'],"['Artuso, M']",['B Decay Studies at Cleo'],['Particle Physics - Experimental Results'],"['talk, Rome 1996/06/17', 'electron positron, colliding beams', 'electron positron, annihilation', 'Upsilon(10570), electroproduction', 'B, pair production', 'B, semileptonic decay', 'Kobayashi-Maskawa angle', 'D', 'D*(2010)', 'final state, (0charmed particle)', 'mass spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B0 --> D lepton neutrino', 'B0 --> D*(2010) lepton neutrino', 'B --> pi lepton neutrino', 'B --> rho(770) lepton neutrino', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610009'],"['Weak decays of heavy flavored hadrons are sensitive probes of several facets of the Standard Model. In particular the experimental study of B meson semileptonic decaysis starting to pin down the quark mixing parameters in the Cabibbo Kobayashi Maskawa matrix. In addition, some features of the non--perturbative regime of the strong interaction are probed by these decays. New results from the CLEO experiment at the CESR electron-positron collider, based on a data sample of up to 3.5 inverse femtobarn, provide crucial information on both of these aspects of heavy flavor phenomenology.']",['1996-11-01']
2282,['eng'],"['Telnov, V I']",['Laser cooling of electron beams for linear colliders'],['Accelerators and Storage Rings'],"['talk, Santa Barbara 1996/08/19', 'electron positron, linear collider', 'linear collider, proposed', 'beam cooling, laser', 'free electron laser', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610008'],['A novel method of electron beam cooling is considered which can be used for linear colliders. The electron beam is cooled during collision with focused powerful laser pulse. With reasonable laser parameters (laser flash energy about 10 J) one can decrease transverse beam emittances by a factor about 10 per one stage. The ultimate transverse emittances are much below of that given by other methods. Depolarization of a beam during the cooling is about 5-15% for one stage. This method is especially useful for photon colliders and open new possibilities for e+e- colliders and x-ray FEL based on high energy linacs.'],['1996-10-29']
2283,['eng'],"['Kuhlen, M']",['High-$p_T$ Particles in the Forward Region at HERA'],['Particle Physics - Experimental Results'],"['talk, Hamburg 1996/05/30', 'electron p, deep inelastic scattering', 'small-x', 'hadron, electroproduction', 'production, small-angle', 'transverse momentum, high', 'showers, parton', 'gluon, radiation', 'Lipatov equation', 'Altarelli-Parisi equation', 'multiplicity', 'rapidity dependence', 'transverse momentum, spectra', 'semiconductor detector, small-angle', 'luminosity', 'magnetic detector, H1', 'numerical calculations, DESY HERA Stor', '((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610004'],"['In order to probe the dynamics of parton evolution in deep inelastic scattering at small x, high-p_T particles produced centrally in pseudorapidity are studied. In the BFKL mechanism gluon radiation is expected to be more abundant than for DGLAP evolution with strong ordering of the gluon transverse momenta, leading to harder p_T spectra. The proposed measurements require charged particle tracking capability as much forward as possible in the HERA laboratory frame, for example with a Very Forward Silicon Tracker, and high luminosity for detailed studies.']",['1996-10-09']
2284,['eng'],"['Grunhaus, J', 'Kananov, S']",['Separation of $\\gamma$/$\\pi^0$ showers at high energies'],['Detectors and Experimental Techniques'],"['pi0, showers', 'photon, showers', 'showers, electromagnetic', 'particle identification, (pi0 photon)', 'shower detector, proposed', 'scintillation counter', 'lead', 'efficiency, energy dependence', 'hadron hadron, colliding beam detector', 'Higgs particle, radiative decay', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610005'],"['We have designed and carried out simulation studies of a two layer Shower Maximum Detector diagonally off-set (SMD-dos) optimized for the separation of 87+-4% and 32+-2%, respectively, for 30, 50 and 150 GeV incident energies. We find that the SMD-dos is superior to a conventional geometry single-layer or mutiple-layer shower maximum detector (SMD), of equal granularity, by an average factor of ~1.5 over the 50 to 150 GeV energy range. We also find that the SMD-dos gives better \\pi^0 rejection, for the same number of channels, than a SMD. At hadron - hadron colliders the signature of choice for the detection of the Higgs particle, in the mass range of 120 to 160 GeV, is via the decay H-->\\gamma\\gamma. The addition of a SMD-dos to the planned detectors at the LHC would significantly reduce the background to the \\gamma-signal coming from prolific \\pi^0 production.']",['1996-10-09']
2285,['eng'],"['Eerola, Paula Anna-Mari']",['B physics potential of ATLAS'],['Detectors and Experimental Techniques'],"['talk, Rome 1996/06/17', 'p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'muon, trigger', 'B0, hadronic decay', 'anti-B0, hadronic decay', 'decay, asymmetry', 'J/psi(3100), leptonic decay', 'violation, CP', 'B, excited state', 'jet, charge', 'B+, hadronic decay', 'B/s0, hadronic decay', 'B, rare decay', 'magnetic detector, ATLAS', 'numerical calculations, Monte Carlo', 'CERN LHC Coll', '14000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610002'],"['The B-physics potential of the ATLAS experiment at LHC is described. Simulation results are shown for the measurement of sin(2beta), with an emphasis on new tagging techniques. Other CP-violation measurements are described briefly. New limits are shown for the reach of the x_s-measurement, resulting from increased statistics and improved fitting methods. Some rare decay modes of B-mesons can be easily seen in ATLAS. Analyses of channels B-> mu+mu-(X) are presented here.']",['1996-10-08']
2286,['eng'],"['Kaplan, D M']",['Charmonium Production in Fermilab E789'],['Particle Physics - Experimental Results'],"['talk, Chicago 1996/06/13', 'p nucleus, inclusive reaction', 'beryllium', 'gold', 'J/psi(3100), hadroproduction', 'psi(3685), hadroproduction', 'D0, hadroproduction', 'J/psi(3100), leptonic decay', 'mass spectrum, dimuon', 'quantum chromodynamics, perturbation theory', 'color, octet', 'differential cross section, transverse momentum', 'differential cross section, x-dependence', 'dependence, mass number', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610003'],"['Using a sample of >10^5 J/psi to mu+mu- decays, Fermilab experiment 789 has studied production of J/psi and psi-prime in 800-GeV proton-nucleon collisions. Differential cross sections and nuclear dependences have been measured for charmonium as well as for charm and beauty production. While charm and beauty production are consistent with perturbative QCD calculations, charmonium cross sections exceed the predictions of the color-singlet model by large factors, suggesting that additional mechanisms (such as color-octet production) may play important roles. Nuclear dependences of production cross sections may offer a new tool for the detailed understanding of charmonium production.']",['1996-10-08']
2287,['eng'],"['Gerdes, D W']",['Top Quark Physics Results from CDF and D0'],['Particle Physics - Experimental Results'],"['talk, Snowmass 1996/06/25', 'Snowmass 1996/06/25, talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'channel cross section', 'mass, truth', 'truth, mass', 'quark, decay modes', 'decay modes, quark', 'quark, branching ratio', 'upper limit', 'Kobayashi-Maskawa angle', 'W, polarization', 'polarization, W', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'truth --> W beauty', 'truth --> Z0 quark', 'truth --> quark photon', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609013'],"[""I summarize recent top quark physics results from the Fermilab Tevatron experiments. Since the observation of the top quark by CDF and D0 in 1995, the experimental focus has shifted to a detailed study of the top quark's properties. This article describes recent measurements of the top quark production cross section, mass, kinematic properties, branching ratios, $V_{tb}$, and the W polarization in top decays.""]",['1996-09-30']
2288,['eng'],"['Anthony, P L', 'Arnold, R G', 'Band, H R', 'Borel, H', 'Bosted, P E', 'Breton, V', 'Cates, G D', 'Chupp, T E', 'Dietrich, F S', 'Erbacher, R D', 'Fellbaum, J', 'Fonvieille, H', 'Gearhart, R A', 'Holmes, R', 'Hughes, E W', 'Johnson, J R', 'Kawall, D', 'Keppel, C E', 'Kuhn, S E', 'Lombard-Nelsen, R M', 'Marroncle, J', 'Meyer, W T', 'Meziani, Z E', 'Middleton, H', 'Morgenstern, J', 'Newbury, N R', 'Petratos, G G', 'Prepost, R', 'Roblin, Y', 'Rock, S E', 'Shapiro, G', 'Smith, T', 'Souder, P A', 'Spengos, M', 'Staley, F', 'Stuart, L M', 'Szalata, Z M', 'Terrien, Y', 'Thompson, A K', 'White, J L', 'Woods, M', 'Xu, J', 'Young, C C', 'Zapalac, G H']",['Deep Inelastic Scattering of Polarized Electrons by Polarized $^3$He and the Study of the Neutron Spin Structure'],['Particle Physics - Experimental Results'],"['p nucleus, deep inelastic scattering', 'helium, polarized target', 'helium, nuclide', 'p, polarized beam', 'polarization, asymmetry', 'polarization, longitudinal', 'polarization, transverse', 'n, structure function', 'structure function, spin', 'moment, structure function', 'sum rule', 'Regge poles', 'magnetic spectrometer, experimental results', 'SLAC Linac', '19.42, 22.66 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610007'],"['The neutron longitudinal and transverse asymmetries $A^n_1$ and $A^n_2$ have been extracted from deep inelastic scattering of polarized electrons by a polarized $^3$He target at incident energies of 19.42, 22.66 and 25.51 GeV. The measurement allows for the determination of the neutron spin structure functions $g^n_1 (x,Q^2)$ and $g^n_2(x,Q^2)$ over the range $0.03 < x < 0.6$ at an average $Q^2$ of 2 (GeV$/c)^2$. The data are used for the evaluation of the Ellis-Jaffe and Bjorken sum rules. The neutron spin structure function $g^n_1 (x,Q^2)$ is small and negative within the range of our measurement, yielding an integral ${\\int_{0.03}^{0.6} g_1^n(x) dx}= -0.028 \\pm 0.006 (stat) \\pm 0.006 (syst) $. Assuming Regge behavior at low $x$, we extract $\\Gamma_1^n=\\int^1_0 g^n_1(x)dx = -0.031 \\pm 0.006 (stat)\\pm 0.009 (syst) $. Combined with previous proton integral results from SLAC experiment E143, we find $\\Gamma_1^p - evaluated using $\\alpha_s = 0.32\\pm 0.05$.']",['1996-10-15']
2289,['eng'],"['Torrence, E']",['Determination of Electroweak Parameters at the SLC'],['Particle Physics - Experimental Results'],"['talk, Warsaw 1996/07/25', 'electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'polarization, asymmetry', 'coupling, asymmetry', 'Weinberg angle', 'Z0, leptonic decay', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.28 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9610001'],"['We present an improved measurement of the left-right cross section asymmetry Alr for Z boson production by e+e- collisions. The measurement was performed at a center-of-mass energy of 91.28 GeV with the SLD detector at the SLAC Linear Collider (SLC) during the 1994-95 running period. The luminosity-weighted average polarization of the SLC electron beam during this run was measured to be (77.23 +/- 0.52)%. Using a sample of 93,644 hadronic Z decays, we measure the pole asymmetry Alr0 to be 0.1512 +/- 0.0042(stat.) +/- 0.0011(syst.) which is equivalent to an effective weak mixing angle of 0.23100 +/- 0.00054(stat.) +/- 0.00014(syst.). We also present a preliminary direct measurement of the Z-lepton coupling asymmetries A_e,A_mu, and A_tau extracted from the differential cross section observed in leptonic Z decays. We combine these results with our previous Alr measurement to obtain a combined determination of the weak mixing angle of 0.23061 +/- 0.00047.']",['1996-10-02']
2290,['eng'],"['Söldner-Rembold, S']",['Jet Production in Photon-Photon Interactions'],['Particle Physics - Experimental Results'],"['talk, Warsaw 1996/07/25', 'electron positron, colliding beams', 'exchange, two-photon', 'photon photon, interaction', 'jet, photoproduction', 'final state, (2jet)', 'cross section, rapidity dependence', 'cross section, transverse energy', 'quantum chromodynamics, perturbation theory', 'photon, resolved', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'electron positron --> jet positron electron anything', 'electron positron --> 2jet positron electron anything', '130, 136 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609018'],['The inclusive one- and two-jet cross-sections are measured in collisions of quasi-real photons at e+e- centre-of-mass energies of 130 and 136 GeV using the OPAL detector at LEP. Jets are reconstructed with a cone jet finding algorithm. The jet cross-sections are compared to next-to-leading order (NLO) perturbative QCD calculations. Transverse energy flows in jets are studied separately for direct and resolved two-photon events.'],['1996-09-30']
2291,['eng'],"['Abe, K', 'Abe, K', 'Abt, I']",['First Measurement of the Left-Right Charge Asymmetry in Hadronic Z Boson Decays and a New Determination of $sin^{2} \\theta_{W}^{eff}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'electron, polarized beam', 'Z0, electroproduction', 'Z0, hadronic decay', 'polarization, asymmetry', 'charge, asymmetry', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.27 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609019'],"['We present the first measurement of the left-right charge asymmetry A_Q^{obs} in hadronic Z boson decays. This was performed at E_cm = 91.27 GeV with the SLD at the SLAC Linear Collider with a polarized electron beam. Using 89838 events, we obtain A_Q^{obs}=0.225+-0.056+-0.019 which leads to a measurement of the electron left-right asymmetry parameter, A_e=0.162+-0.041+-0.014, and sin^2(theta_eff)=0.2297+-0.0052 +-0.0018. Also, the A_Q^{obs} measurement combined with the left-right cross section asymmetry determines A_e independently of the value of the electron-beam polarization.']",['1996-09-30']
2292,['eng'],"['Bauerdick, L A T', 'Glazov, A', 'Klein, M']",['Future Measurement of the Longitudinal Proton Structure Function at HERA'],['Particle Physics - Experimental Results'],"['talk, Hamburg 1995/09/25', 'talk, Hamburg 1996/02/07', 'talk, Hamburg 1996/05/30', 'electron p, deep inelastic scattering', 'exchange, one-photon', 'p, structure function', 'structure function, longitudinal', 'structure function, small-x', 'dependence, momentum transfer', 'cross section, error', 'numerical calculations, DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609017'],"['A study is presented of a possible future measurement of the longitudinal structure function $F_{L}(x,Q^{2})$ with different proton beam energies at HERA.']",['1996-09-26']
2293,['eng'],"['Raja, R']",['On Measuring the top quark mass using the dilepton decay modes'],['Particle Physics - Experimental Results'],"['talk, Snowmass 1996/06/25', 'anti-p p, annihilation', 'quark, truth', 'quark, pair production', 'quark, decay', 'W, leptonic decay', 'final state, dilepton', 'mass, truth', 'data analysis method, proposed', 'statistical analysis', 'spin, correlation', 'gluon, radiation', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609016'],['We demonstrate a new likelihood method for extracting the top quark mass from events of the type ttbar-->bW(l+nu)bW(l+nu) This method estimates the top quark mass correctly from an ensemble of dilepton events. The method proposed by Dalitz and Goldstein [1] is shown to result in a systematic underestimation of the top quark mass. Effects due to the spin correlations between the top and anti-top quarks are shown to be unimportant in estimating the mass of the top quark.'],['1996-09-23']
2294,['eng'],"['Bethke, Siegfried']",['Experimental Tests of Asymptotic Freedom'],['Particle Physics - Experimental Results'],"['review, Montpellier 1996/07/04', 'quantum chromodynamics, asymptotic freedom', 'strong interaction, coupling constant', 'energy dependence', 'electron positron, annihilation', 'electron p, interaction', 'jet, electroproduction', 'final state, (3jet)', 'anti-p p, interaction', 'jet, hadroproduction', 'jet, multiplicity', 'tau, semileptonic decay', 'mass spectrum', 'sum rule', 'Z0, electroproduction', 'Z0, width', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609014'],"['Measurements which probe the energy dependence of $\\alpha_s$, the coupling strength of the strong interaction, are reviewed. Jet counting in $e^+ e^-$ annihilation, combining results obtained in the centre of mass energy range from 22 to 133 GeV, provides direct evidence for an asymptotically free coupling, without the need to determine explicit values of $\\alpha_s$. Recent results from jet production in $e p$ and in $p \\overline{p}$ collisions, obtained in single experiments spanning large ranges of momentum transfer, $Q^2$, are in good agreement with the running of $\\alpha_s$ as predicted by QCD. Mass spectra of hadronic decays of $\\tau$-leptons are analysed to probe the running $\\alpha_s$ in the very low energy domain, $0.7 GeV^2 < Q^2 < M_\\tau^2$. An update of the world summary of measurements of $\\alpha_s(Q^2)$ consistently proves the energy dependence of $\\alpha_s$ and results in a combined average of $\\alpha_s(M_Z) = 0.118 \\pm 0.006$.']",['1996-09-20']
2295,['eng'],"['Nakada, Tatsuya']",['Future Prospects for Studying CP Violation in B-Meson Decays'],['Particle Physics - Experimental Results'],"['talk, Orsay 1996/05/30', 'B, decay modes', 'B/s, decay modes', 'violation, CP', 'electron positron, annihilation', 'electron p, interaction', 'B, electroproduction', 'B, pair production', 'anti-p p, interaction', 'p p, interaction', 'B, hadroproduction', 'Kobayashi-Maskawa angle', 'B0 anti-B0, oscillation', 'B/s0 anti-B/s0, oscillation', 'numerical calculations', 'proposed experiment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609015'],"['Experimental prospects for observing CP violation in B-meson decays are reviewed. Comparisons are made for various options: experiments at $e^+ e^-$ B-Meson Factories, HERA and the TEVATRON will produce results in near future. They will have a good chance to discover CP violation in B-meson decays. On a longer time scale, experiments at the LHC will aim at accurate measurements to make a precision test of the standard model in CP violation.']",['1996-09-20']
2296,['eng'],"['Rylko, R']",['On the Study of $B\\overline{B}$ Correlations a HERA-B'],['Particle Physics - Experimental Results'],"['talk, Hamburg 1995/09/25', 'talk, Hamburg 1996/02/07', 'talk, Hamburg 1996/05/30', 'B, hadroproduction', 'hadroproduction, B', 'B, pair production', 'pair production, B', 'angular correlation, (B anti-B)', 'momentum, correlation', 'event shape analysis', 'numerical calculations', 'magnetic detector, HERA-B', 'proposed experiment, DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609012'],"['We analyze the possibility of studying the heavy flavour hadroproduction properties at the HERA-B experiment. In addition to the high statistics single inclusive B spectra measurements, the measurement of the BBbar meson correlations is considered. The techniques of momentum estimators, widely used in the charm sector, are demonstrated to be useful for the BBbar correlation studies at HERA-B. The kinematic limits for the precision of the momentum estimator within which the pair spectra can be measured are determined. The errors are weakly dependent on the topology of the multibody B meson decay.']",['1996-09-18']
2297,['eng'],"['Abe, F']",['Measurement of Dijet Angular Distributions at CDF'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'angular distribution, (2jet)', 'quark, composite', 'quantum chromodynamics, perturbation theory', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON PS', '1800 Gev-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609011'],['We have used 106 pb^-1 of data collected in proton-antiproton collisions at sqrt(s)=1.8 TeV by the Collider Detector at Fermilab to measure jet angular distributions in events with two jets in the final state. The angular distributions agree with next to leading order (NLO) predictions of Quantum Chromodynamics (QCD) in all dijet invariant mass regions. The data exclude at 95% confidence level (CL) a model of quark substructure in which only up and down quarks are composite and the contact interaction scale is Lambda_ud(+) < 1.6 TeV or Lambda_ud(-) < 1.4 TeV. For a model in which all quarks are composite the excluded regions are Lambda(+) < 1.8 TeV and Lambda(-) < 1. 6 TeV.'],['1996-09-18']
2298,['eng'],"['Aïd, S']",['Search for Excited Fermions with the H1 Detector'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'electron p, inclusive reaction', 'electron, excited state', 'neutrino, excited state', 'quark, excited state', 'search for, excited state', 'excited state, decay', 'track data analysis, cluster', 'transverse energy, missing-energy', 'final state, (muon)', 'final state, ((n)jet)', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'electron* --> electron photon', 'electron* --> Z0 electron', 'electron* --> W electron', 'quark* --> quark photon', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609008'],"['We present a search for excited electrons, neutrinos and quarks using the H1 detector at the $ep$ collider HERA, based on data taken in 1994 with an integrated luminosity of 2.75 pb$^{-1}$. Radiative decays of excited quarks and neutrinos have been investigated as well as decays of excited electrons into all possible electroweak gauge bosons. No evidence for new particle production is found and exclusion limits are derived.']",['1996-09-30']
2299,['eng'],"['Grab, C']",['Rare D Meson Decays at HERA'],['Particle Physics - Experimental Results'],"['electron p, inclusive reaction', 'quark, charm', 'quark, pair production', 'charmed meson, rare decay', 'charmed meson, leptonic decay', 'charmed meson, hadronic decay', 'charmed meson, radiative decay', 'charmed meson, semileptonic decay', 'neutral current, flavor changing', 'violation, flavor', 'efficiency', 'background', 'numerical calculations, DESY HERA Stor', '((5))']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609007'],"['A status report on the prospects of measuring rare decays of charmed mesons at HERA is given. Based on actual experience with measuring charm at HERA, the sensitivity on limits of rare decays is estimated.']",['1996-09-16']
2300,['eng'],"['Del Duca, V', 'Gallo, E', 'Marage, P']",['Diffractive Interactions'],['Particle Physics - Experimental Results'],"['talk, Rome 1996/04/15', 'electron p, deep inelastic scattering', 'positron p, deep inelastic scattering', 'diffraction', 'hadron, electroproduction', 'hadron, photoproduction', 'rapidity, gap', 'structure function, diffraction', 'structure function, pomeron', 'differential cross section, mass', 'factorization, violation', 'momentum spectrum, parton', 'jet, photoproduction', 'vector meson, photoproduction', 'dependence, momentum transfer', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609009'],"['The general framework of diffractive deep inelastic scattering is introduced and reports given in the session on diffractive interactions at the International Workshop on Deep-Inelastic Scattering and Related Phenomena, Rome, April 1996, are presented.']",['1996-09-30']
2301,['eng'],"['Fuster, J A', 'Cabrera, S', 'Marti i Garcia, S']",['Experimental studies of QCD using flavour tagged jets with DELPHI'],['Particle Physics - Experimental Results'],"['talk, Montpellier 1996/07/04', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (quark antiquark gluon)', 'final state, (quark antiquark photon)', 'quark, jet', 'gluon, jet', 'quantum chromodynamics', 'particle identification, flavor', 'charged particle, multiplicity', 'multiplicity, ratio', 'jet, energy', 'mass, beauty', 'gluon, radiation', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609004'],"['Identified $b\\overline{b}g$ and $q\\overline{q}\\gamma$ events from DELPHI are used to measure the ratio of the mean charged particle multiplicity distribution between gluon and quark jets. The dependence of this ratio with the jet energy is established using about three million Z$^0$ decays. Results from all other detectors are discussed and compared. A nice agreement is found among all them. The ratio between the normalized total three-jet cross sections of $b\\overline{b}g$ and $q\\overline{q}g, q \\equiv u,d,s$ events is also determined. The preliminary value obtained indicates that $b$ quarks are experimentaly seen to radiate less than light quarks due to their higher mass. The suggested experimental error is $\\sim$300 MeV for the $b$ mass determination at the M$_Z$ scale.']",['1996-09-12']
2302,['eng'],"['Bazarko, A O']",['A Measurement of $R_b$ Using Multiple Tags'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, beauty', 'quark, pair production', 'Z0, branching ratio', 'particle identification, flavor', 'track data analysis', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'approx. 91 Gev-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609005'],['A new measurement of $R_b$ with the ALEPH detector at LEP using five mutually exclusive hemisphere tags is presented. The preliminary result is $R_b = 0.2158'],['1996-09-12']
2303,['eng'],"['Diwan, M V', 'Frank, J', 'Gordeev, A', 'Kettell, S H', 'Leipuner, L', 'Littenberg, L S', 'Ma, H', 'Polychronakos, V', 'Atoyan, G S', 'Issakov, V V', 'Karavichev, O V', 'Laptev, S V', 'Poblaguev, A A', 'Proskuryakov, A', 'Barakat, B', 'Elaasar, M', 'Greenwood, D', 'Johnston, K', 'Adair, R K', 'Larsen, R']",['Search for T Violation in $K_{\\mu 3}$ Decay'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'K+, semileptonic decay', 'K+, separated beam', 'time reversal, violation', 'pi0, radiative decay', 'muon+, polarization', 'magnetic field', 'calorimeter', 'proposed experiment, Brookhaven PS', 'K+ --> pi0 muon+ neutrino', '2 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609002'],"['We propose a new experiment at the AGS to search for the T-violating polarization of the muon normal to the decay plane of the K+ to mu+ pi0 nu decay. Motivated by the need for a stronger CP violation source to account for the baryon asymmetry of the Universe, the experiment aims to search for T-violation beyond the Standard Model. The experiment will be performed with in-flight decays from an intense 2 GeV/c separated K+ beam at the AGS. We expect to analyze 10**9 events to obtain the sensitivity of delta Pt = +- 0.00013 at 1 sigma, corresponding to the sensitivity of +-0.0007 to Im(xi), an improvement by 40 over the present limit.']",['1996-09-06']
2304,['eng'],"['Filip, P']",['Azimuthally Sensitive HBT Analysis'],['Particle Physics - Experimental Results'],"['talk, Berkeley 1996/07', 'scattering, heavy ion', 'hadron, multiple production', 'correlation, two-pion', 'boson, statistics', 'angular dependence', 'correlation function', 'pi, particle source', 'dependence, geometrical', 'nucleus nucleus, nuclear reaction', 'sulfur', 'lead', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609001'],['In the paper we investigate a possibility to perform shape-sensitive HBT analysis in transversal plane. We study presently used Side-Out decomposition of the correlation function and we do not find it to be very sensitive for the detection of a shape of source distribution in transversal plane. Therefore we suggest to use X-Y decomposition of the correlation function for the HBT analysis. We test the method suggested on artificial and non-central Pb-Pb 158GeV/n events produced by CASCUS generator. Further possible enhancement of the method is sketched.'],['1996-09-02']
2305,['eng'],"['Teige, S']",['Properties of the a0(980) meson'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'pi- p, exclusive reaction', 'a0(980), hadroproduction', 'a0(980), hadronic decay', 'a0(980), mass', 'a0(980), width', 'mass spectrum', 'coupling constant, (a0(980) eta pi)', 'coupling constant, (a0(980) K anti-K)', 'experimental results', 'Brookhaven PS', 'pi- p --> n eta pi+ pi-', 'a0(980) --> eta pi+', 'a0(980) --> K anti-K']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608017'],['The mass and width of the a0(980) have been independently determined from a nearly background free data sample and the coupling constants to the eta-pi and K-K-bar modes have been determined'],['1996-08-30']
2306,['eng'],[],['Search for Lepton Flavor Violation in ep Collisions at 300 GeV Center of Mass Energy'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'positron p, colliding beams', 'colliding beams, positron p', 'electron p, inclusive reaction', 'positron p, inclusive reaction', 'muon, electroproduction', 'electroproduction, muon', 'tau, electroproduction', 'electroproduction, tau', 'transverse momentum, high', 'violation, flavor', 'postulated particle, leptoquark', 'postulated particle, squark', 'mass, leptoquark', 'leptoquark, mass', 'mass, squark', 'squark, mass', 'R parity, violation', 'violation, R parity', 'coupling', 'mass, dependence', 'dependence, mass', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9704018'],"['Using the ZEUS detector at the HERA electron-proton collider, we have searched for lepton flavor violation in ep collisions at a center-of-mass energy s^1/2 of 300 GeV. Events of the type e + p -> lepton + X with a final-state lepton (mu or tau) of high transverse momentum, were sought. No evidence was found for lepton flavor violation in the combined 1993 and 1994 data samples, for which the integrated luminosities were 0.84 pb^-1 for e- p collisions and 2.94 pb^-1 for e+ p collisions. Limits on coupling vs. mass are provided for leptoquarks and R-parity violating squarks. For flavor violating couplings of electromagnetic strength, we set 95% confidence level lower limits on leptoquark masses between 207 GeV and 272 GeV, depending on the leptoquark species and final-state lepton. For leptoquark masses larger than 300 GeV, limits on flavor-changing couplings are determined, many of which supersede prior limits from rare decay processes.']",['1997-05-05']
2307,['eng'],"['Adair, R K', 'Atoyan, G S', 'Barakat, B', 'Diwan, M V', 'Imazato, J', 'Issakov, V V', 'Kuno, Y', 'Kycia, T F', 'Larsen, R', 'Leipuner, L', 'Ma, H', 'Poblaguev, A A', 'Ritchie, J']",['Muon Polarization Working Group Report'],['Particle Physics - Experimental Results'],"['talk, Upton 1996/05/13', 'K, separated beam', 'K, decay modes', 'muon, polarization', 'polarization, asymmetry', 'violation, CP', 'Kobayashi-Maskawa angle', 'proposed experiment, Brookhaven PS', 'K+ --> pi0 muon+ neutrino', 'K+ --> muon+ neutrino photon', 'K0(L) --> muon+ muon-', 'K+ --> pi+ muon+ muon-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608015'],"['We have examined the physics and the experimental feasibility at the AGS of various kaon decay processes in which the polarization of a muon in the final state is measured. Valuable information on CP violation, the CKM matrix or new physics can be obtained with these measurements and therefore they are well motivated. In particular, models of non-standard CP violation that produce the baryon asymmetry of the universe could also produce effects observable in these measurements. Limits from measurements such as the neutron and electron electric dipole moment, and epsilon-prime over epsilon in neutral kaon decays do not eliminate all of these models. We have made a more detailed examination of the measurement of the out of the plane muon polarization in Kmu3 decays. With our current knowledge of the AGS kaon beams and detector techniques it is possible to measure this polarization with an error approaching 10**-4. Such an experiment would be well justified since the sensitivity is well beyond the current direct experimental limit (5.3 times 10**-3) and the projected sensitivity (10**-3) of the currently running experiment at KEK in Japan.']",['1996-08-27']
2308,['eng'],"['Brooks, T C', 'Convery, M E', 'Davis, W L', 'Delsignore, K W', 'Jenkins, T L', 'Kangas, E', 'Knepley, M G', 'Kowalski, K L', 'Taylor, C C', 'Walker, W D', 'Colestock, P L', 'Hanna, B', 'Martens, M', 'Streets, J', 'Ball, R', 'Gustafson, H R', 'Jones, L W', 'Longo, M J', 'Bjorken, James D', 'Abashian, A', 'Morgan, N', 'Pruneau, C A']",['Preliminary Results from a Search for Disoriented Chiral Condensates at MiniMax'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'anti-p p, colliding beams', 'hadron, multiple production', 'pi, hadroproduction', 'yield, (pi+ pi- pi0)', 'multiplicity, moment', 'moment, ratio', 'pi, condensation', 'symmetry, chiral', 'search for, condensation', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608012'],"['We report on the progress of a search for disoriented chiral condensates (DCCs) in the far forward region at sqrt(s)=1.8 TeV. MiniMax is a small collider experiment situated at the C0 interaction region of the Tevatron and has been designed to measure the ratio of charged to neutral pions produced at eta near 4.1. The distribution of this ratio is expected to be very different for the generic binomial and DCC particle production models. We present a method used for the search using the factorial moments of particle generating functions, which can be extracted directly from the data. A preliminary comparison of robust ratios of measured values and those expected from the different models is also presented.']",['1996-08-21']
2309,['eng'],"['Bailey, M W']",['Charmonium and Bottomonium Production in $p \\overline{p}$ Collisions at CDF'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'quarkonium, hadroproduction', 'quarkonium, charm', 'quarkonium, beauty', 'beauty, decay', 'J/psi(3100), direct production', 'psi(3685), direct production', 'psi mesons, leptonic decay', 'final state, dimuon', 'differential cross section, transverse momentum', 'upsilon mesons, leptonic decay', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608014'],['We present measurements of charmonium and bottomonium production using a data sample collected by CDF during the 1992-93 p-pbar collider run at the Fermilab Tevatron.'],['1996-08-26']
2310,['eng'],"['Aitala, E M', 'Gounder, K']",['Observation of $D-\\pi$ Production Correlations in 500 GeV $\\pi^{-} - N$ Interactions'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D*(2010), hadroproduction', 'D0, hadroproduction', 'D+, hadroproduction', 'pi, hadroproduction', 'charmed meson, hadronic decay', 'charge correlation, (D pi)', 'charge correlation, (D*(2010) pi)', 'x-dependence', 'dependence, mass difference', 'model, fragmentation', 'resonance, effect', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> K- pi+', 'D+ --> K- 2pi+', 'D*(2010) --> D0 pi+', '500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001004'],"['We study the charge correlations between charm mesons produced in 500 GeV pi- - N interactions and the charged pions produced closest to them in phase space. With 110,000 fully reconstructed D mesons from experiment E791 at Fermilab, the correlations are studied as functions of the Dpi - D mass difference and of Feynman x. We observe significant correlations which appear to originate from a combination of sources including fragmentation dynamics, resonant decays, and charge of the beam.']",['2000-01-04']
2311,['eng'],"['Aïd, S', 'Andeson, M', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Babaev, A', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Braunschweig, W', 'Brisson, V', 'Bruel, P', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Calvet, D', 'Campbell, A J', 'Carli, T', 'Charlet, M', 'Chechelnitskii, S', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Cocks, S', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Cousinou, M C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davis, C L', 'De Wolf, E A', 'Delcourt, B', 'Di Nezza, P', 'Dirkmann, M', 'Dixon, P', 'Dlugosz, W', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duhm, H', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Evrard, E', 'Fahr, A B', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Gaede, F', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'Golec-Biernat, K J', 'González-Pineiro, B', 'Gorelov, I V', 'Grab, C', 'Greenshaw, T J', 'Griffiths, R K', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Hampel, M', 'Haynes, W J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hewitt, K', 'Hildesheim, W', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Hoffmann, D', 'Holtom, T', 'Hoppner, M', 'Horisberger, R P', 'Hudgson, V L', 'Hufnagel, H', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johnson, D P', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kander, M', 'Kant, D', 'Kaschowitz, R', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kaufmann, O', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Kolanski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Kuhlen, M', 'Kurca, T', 'Kurzhofer, J', 'Köhler, T', 'Köhne, J H', 'Küster, H', 'Lacour, D', 'Laforge, B', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Langenegger, U', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Levonian, S', 'Lindström, G', 'Lindstrøm, M', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lomas, J W', 'Lubimov, V', 'Lüke, D', 'López, G C', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Meyer, A', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moeck, J', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Negri, I', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Niggli, H', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Olsson, J E', 'Ozerov, D', 'Palmen, P', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Pawletta, H', 'Peppel, E', 'Phillips, J P', 'Pieuchot, A', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Pérez, E', 'Rabbertz, K', 'Reimer, P', 'Reinshagen, S', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riepenhausen, F', 'Riess, S', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rädel, G', 'Rüter, K', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schöning, A', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Specka, A E', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Squinabol, F', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Steiner, H', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stier, J', 'Stiewe, J', 'Stolze, K', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Tapprogge, Stefan', 'Tasevsky, M', 'Theissen, J', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Van den Plas, D', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'West, L R', 'Wiesand, S', 'Wilksen, T', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wobisch, M', 'Wünsch, E', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zini, P', 'Zomer, F', 'Zsembery, J', 'Zuber, K', 'Zur Nedden, M', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']",['Charged Particle Multiplicities in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron positron, colliding beams', 'positron positron, deep inelastic scattering', 'hadron, multiple production', 'charged particle, multiplicity', 'multiplicity, moment', 'energy dependence', 'dependence, momentum transfer', 'rapidity dependence', 'statistical analysis', 'scaling, KNO', 'transverse energy, energy flow', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608011'],"['Using the H1 detector at HERA, charged particle multiplicity distributions in deep inelastic ep scattering have been measured over a large kinematical region. The evolution with $W$ and $Q^2$ of the multiplicity distribution and of the multiplicity moments in pseudorapidity domains of varying size is studied in the current fragmentation region of the hadronic centre-of-mass frame. The results are compared with data from fixed target lepton-nucleon interactions, $e^+e^-$ annihilations and hadron-hadron collisions as well as with expectations from QCD based parton models. Fits to the Negative Binomial and Lognormal distributions are presented.']",['1996-08-19']
2312,['eng'],"['Abe, K']","['Measurement of the Charged Multiplicities in $b$, $c$ and Light Quark Events from $Z^{0}$ Decays']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'Z0, hadronic decay', 'quark, charm', 'quark, beauty', 'quark, pair production', 'charged particle, multiplicity', 'dependence, flavor', 'model, fragmentation', 'track data analysis, impact parameter', 'quantum chromodynamics, perturbation theory', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608008'],"['Average charged multiplicities have been measured separately in $b$, $c$ and light quark ($u,d,s$) events from $Z^0$ decays measured in the SLD experiment. Impact parameters of charged tracks were used to select enriched samples of $b$ and light quark events, and reconstructed charmed mesons were used to select $c$ quark events. We measured the charged multiplicities: $\\bar{n}_{uds} = 20.21 \\pm 0.10 (\\rm{stat.})\\pm 0.22(\\rm{syst.})$, $\\bar{n}_{c} = 21.28 \\pm 0.46(\\rm{stat.}) ^{+0.41}_{-0.36}(\\rm{syst.})$ $\\bar{n}_{b} = 23.14 \\pm 0.10(\\rm{stat.}) ^{+0.38}_{-0.37}(\\rm{syst.})$, from which we derived the differences between the total average charged multiplicities of $c$ or $b$ quark events and light quark events: $\\Delta \\bar{n}_c = 1.07 \\pm 0.47(\\rm{stat.})^{+0.36}_{-0.30}(\\rm{syst.})$ and $\\Delta \\bar{n}_b = 2.93 \\pm 0.14(\\rm{stat.})^{+0.30}_{-0.29}(\\rm{syst.})$. We compared these measurements with those at lower center-of-mass energies and with perturbative QCD predictions. These combined results are in agreement with the QCD expectations and disfavor the hypothesis of flavor-independent fragmentation.']",['1996-08-15']
2313,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Okrasinski, J R', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Mattingly, M C K', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, I', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Crittenden, J A', 'Deffner, R', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Grothe, M', 'Hartmann, H', 'Heinloth, K', 'Heinz, L', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mengel, S', 'Paul, E', 'Pfeiffer, M', 'Rembser, C', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Cottingham, W N', 'Dyce, N', 'Foster, B', 'George, S', 'Hayes, M E', 'Heath, G P', 'Heath, H F', 'Piccioni, D', 'Roff, D G', 'Tapper, R J', 'Yoshida, R', 'Arneodo, M', 'Ayad, R', 'Capua, M', 'Garfagnini, A', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Caldwell, A', 'Crtiglia, N', 'Jing, Z', 'Liu, W', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Jakubowski, Z', 'Przybycien, M B', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Dulinski, Z', 'Kotanski, Andrzej', 'Abbiendi, G', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Cases, G', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'GroBe-Knitter, J', 'Haas, T', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Iga, Y', 'Johnson, K F', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Mainusch, J', 'Manczak, O', 'Milewski, J', 'Monteiro, T', 'Ng, J S T', 'Notz, D', 'Ohrenberg, K', 'Piotrzkowski, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Surrow, B', 'Tassi, E', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Grabosch, H J', 'Mari, S M', 'Meyer, A', 'Schlenstedt, S', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Trefzger, T M', 'Wölfle, S', 'Bromley, J T', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Saxon, D H', 'Sinclair, L E', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Sinkus, R', 'Wick, K', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Brümmer, N', 'Butterworth, Ian', 'Harris, V L', 'Howell, G', 'Hung, B Y H', 'Lamberti, L', 'Long, K R', 'Miller, D B', 'Pavel, N', 'Prinias, A', 'Sedgbeer, J K', 'Sideris, D', 'Whitfield, A F', 'Mallik, U', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Cloth, P', 'Filges, E', 'An, S H', 'Cho, G H', 'Ko, B J', 'Lee, S B', 'Nam, S W', 'Park, H S', 'Park, S K', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Fernández, J P', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Laberga, L', 'Martínez, M', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Yung, L W', 'Lim, J N', 'Matthews, C G', 'Murray, W N', 'Ochs, A', 'Patel, P M', 'Riveline, M', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Tsurugai, T', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Van Sighem, A', 'Tiecke, H G', 'Verkerke, W', 'Vossebeld, J H', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Gilmore, J', 'Ginsburg, C M', 'Kim, C L', 'Li Chuan', 'Ling, T Y', 'Nylander, P', 'Park, I H', 'Romanowsky, T A', 'Bailey, D S', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Harmew, N', 'Lancaster, M', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Tickner, J R', 'Uijterwaal, H', 'Walczak, R', 'Waters, D S', 'Wilson, F F', 'Yip, T', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Zuin, F', 'Bulmahn, J', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Barberis, E', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Williams, D C', 'Biltzinger, J', 'Seifert, R J', 'Schwarzer, O', 'Walenta, A H', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Doeker, T', 'Levy, A', 'Inuzuka, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nakao, M', 'Suzuki, I', 'Tokushuku, K', 'Umemori, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Matsushita, T', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bénard, F', 'Brkic, M', 'Fagerstroem, C P', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sampson, C R', 'Simmons, D', 'Teuscher, R J', 'Butterworth, J M', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Sutton, M R', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Coldewey, C', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Badgett, W F', 'Breitweg, J', 'Chapin, D', 'Cross, R', 'Dasu, S', 'Foudas, C', 'Loveless, R J', 'Mattingly, S E', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Bhadra, S', 'Cardy, M L', 'Frisken, W R', 'Khakzad, M', 'Schmidke, W B']",['Measurement of Elastic Omega Photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'exchange, one-photon', 'photon p, exclusive reaction', 'omega(783), photoproduction', 'channel cross section', 'differential cross section, momentum transfer', 'differential cross section, slope', 'angular distribution', 'helicity, conservation law', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'electron p --> p omega(783) electron', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608010'],"['The reaction $\\gamma p \\rightarrow \\omega p$ $(\\omega \\rightarrow interactions using the \\mbox{ZEUS} detector at photon-proton centre-of-mass energies between $70$ and $90\\uni{GeV}$ and $|t| < 0.6\\uni{GeV}^2$, where $t$ is the squared four momentum transferred at the proton vertex. The elastic \\ome photoproduction cross section has been measured to be $\\sigma_{\\gamma cross section $d\\sigma_{\\gamma p\\rightarrow \\omega p} /d|t|$ has an exponential shape $\\mbox{e}^{-b |t|}$ with a slope $b = 10.0\\pm 1.2\\pm 1.3\\uni{GeV}^{-2}$. The angular distributions of the decay pions are consistent with {\\it s}-channel helicity conservation. When compared to low energy data, the features of $\\omega$ photoproduction as measured at HERA energies are in agreement with those of a soft diffractive process. Previous measurements of the $\\rho^0$ and $\\phi$ photoproduction cross sections at HERA show a similar behaviour.']",['1996-08-16']
2314,['eng'],"['Levy, A']",['The transition from the photoproduction to the DIS region'],['Particle Physics - Experimental Results'],"['talk, Rome 1996/04/15', 'electron p, interaction', 'electron p, deep inelastic scattering', 'momentum transfer, low', 'small-x', 'hadron, photoproduction', 'p, structure function', 'parametrization', 'dependence, momentum transfer', 'total cross section, energy dependence', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608009'],['This is a review of the existing ideas in modelling the transition from the photoproduction ($Q^2 = 0$) to the deep inelastic scattering region. The available data of the proton structure function are analyzed from the point of view of the total $\\gamma^* p$ cross section behavior with $W$ and the results are compared to different parameterizations. The question whether DIS processes are hard or soft is discussed.'],['1996-08-15']
2315,['eng'],"['McFarland, K S']",['Updated Electroweak Measurements from Neutrino-Nucleon Deeply Inelastic Scattering at CCFR'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1996/03/16', 'neutrino nucleon, deep inelastic scattering', 'neutral current', 'Weinberg angle', 'renormalization, on-shell', 'coupling, (quark neutrino)', 'model, composite', 'four-fermion interaction', 'postulated particle, leptoquark', 'neutrino, oscillation', 'calorimeter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608007'],"['We report the results of a study of electroweak parameters from observations of neutral-current $\\nu$N deeply inelastic scattering in the CCFR detector at the FNAL Tevatron Quadrupole Triplet neutrino beam. An improved extraction of the weak mixing angle in the on-shell renormalization scheme, incorporating additional data and with an improved technique for constraining systematic errors, is presented. Within the Standard Model, this result constrains the W mass with a precision comparable to that from direct measurements. The result is also presented in a model-independent form, as constraints on neutral-current quark-neutrino couplings, to facilitate comparisons with theories outside the Standard Model. Using this result, limits on new four-fermion interactions, leptoquarks and neutrino oscillations are presented. Prospects for a successor experiment, NuTeV (FNAL-E815), are also presented.']",['1996-08-14']
2316,['eng'],"['Becker, U']",['Baryon production in ALEPH'],['Particle Physics - Experimental Results'],"['talk, Novy Svet 1996/06/09', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'baryon, production', 'production, baryon', 'hyperon, hadronic decay', 'hadronic decay, hyperon', 'Sigma(1385)', 'Xi-', 'Xi(1530)', 'Omega-', 'Lambda/b0, hadronic decay', 'hadronic decay, Lambda/b0', 'Xi/b, hadronic decay', 'hadronic decay, Xi/b', 'Lambda, polarization', 'polarization, Lambda', 'Lambda/b0, polarization', 'polarization, Lambda/b0', 'energy spectrum', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'electron positron --> hyperon anything', 'electron positron --> beautiful baryon anything', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608004'],"['Several recent results of the ALEPH Collaboration covering different aspects of baryon production on the Z resonance are presented. In particular production rates of hyperons, the full kinematical reconstruction of the Lambda_b, observation of Xi_b in its semileptonic decay, and the measurements of the polarization of Lambda and Lambda_b baryons are discussed.']",['1996-08-07']
2317,['eng'],"['Sinervo, P K']",['Top Quark Studies at Hadron Colliders'],['Particle Physics - Experimental Results'],"['lectures, Stanford 1995/07/10', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay modes', 'decay modes, quark', 'final state, dilepton', 'dilepton, final state', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'transverse energy, missing-energy', 'particle identification, beauty', 'mass, truth', 'truth, mass', 'channel cross section', 'quark, branching ratio', 'mass spectrum, (2truth)', '(2truth), mass spectrum', ""mass, Z'"", ""Z', mass"", 'upper limit', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608005'],"['The techniques used to study top quarks at hadron colliders are presented. The analyses that discovered the top quark are described, with emphasis on the techniques used to tag b-quark jets in candidate events. The most recent measurements of top quark properties by the CDF and DZero collaborations are reviewed, including the top quark cross section, mass, branching fractions and production properties. Future top quark studies at hadron colliders are discussed, and predictions for event yields and uncertainties in the measurements of top quark properties are presented.']",['1996-08-07']
2318,['eng'],"['Pillai, M K', 'Hayashi, E', 'Maeshima, K', 'Grosso-Pilcher, C', 'De Barbaro, P', 'Bodek, Arie', 'Kim, B', 'Sakumoto, W']",['A search for Neutral Heavy Vector Gauge Bosons in $\\overline {p}p$ collisions at $\\sqrt{s}$ = 1.8 TeV'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/10', 'anti-p p, colliding beams', 'colliding beams, anti-p p', ""search for, Z'"", ""Z', leptonic decay"", ""leptonic decay, Z'"", 'channel cross section, branching ratio', 'upper limit', ""mass, Z'"", ""Z', mass"", 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', ""anti-p p --> Z' anything"", ""Z' --> positron electron"", ""Z' --> muon+ muon-"", '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608006'],"['A search for a neutral heavy vector gauge boson, Zprime, was conducted in pbar-p collisions using 110pb$^{-1}$ of data obtained at the Collider Detector at Fermilab. We present preliminary 95% CL limits on the production of Zprime in different models using its e+e- and mu+mu- decay modes.']",['1996-08-07']
2319,['eng'],"['Campagnari, C', 'Franklin, M']",['The discovery of the top quark'],['Particle Physics - Experimental Results'],"['review, experimental results', 'quark, truth', 'search for, truth', 'electron positron, annihilation', 'annihilation, electron positron', 'electroweak interaction', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, decay modes', 'decay modes, Z0', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'angular distribution, asymmetry', 'asymmetry, angular distribution', 'mass, truth', 'truth, mass', 'W, mass', 'mass, W', 'Higgs particle, mass', 'mass, Higgs particle', 'anti-p p, inclusive reaction', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'quark, hadroproduction', 'hadroproduction, quark', 'quark, decay modes', 'decay modes, quark', 'final state, dilepton', 'dilepton, final state', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'transverse energy, missing-energy', 'background', 'particle identification, beauty', 'channel cross section', 'W, hadronic decay', 'hadronic decay, W', 'coupling, (W truth beauty)', '(W truth beauty), coupling', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'proposed experiment', 'Batavia TEVATRON Coll', 'bibliography', 'truth --> W beauty', 'truth --> Higgs particle beauty', 'W --> truth beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608003'],"['Evidence for pair production of a new particle consistent with the Standard Model top quark has been reported recently by groups studying proton anti-proton collisions at 1.8 TeV center of mass energy at the Fermi National Accelerator Laboratory. In this paper we review the history of the search for the top quark in electron positron and proton anti-proton collisions. We report on a number of precise electro-weak measurements and the value of the top quark mass which can be extracted from these measurements within the context of the Standard Model. We review the theoretical predictions for top quark production and the dominant backgrounds. We describe the collider and the detectors that were used to measure the pair production process and follow on to describe the data from which the existence of the top quark is evinced. Finally, we present possible measurements that could be made in the future with more data, measurements of quantities that would confirm the nature of this particle, the details of its production in hadron collisions, and its decay properties.']",['1996-08-05']
2320,['eng'],"['Sivertz, M', 'Berger, B', 'Ehrlich, R', 'Bartlet, J', 'Csorna, S E', 'Jain, V', 'Marka, S', 'Kinoshita, K', 'Pomianowski, P A']",['A Compact Gas Cerenkov Detector with Novel Optics'],['Particle Physics - Experimental Results'],"['particle identification, (K pi)', 'Cherenkov counter, gas', 'Cherenkov counter, threshold', 'optics, reflection', 'photoelectron, amplifier', 'photoelectron, yield', 'numerical calculations, Monte Carlo', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607013'],"['We discuss the design and performance of a threshold Cerenkov counter for identification of charged hadrons. The radiator is pressurized gas, which is contained in thin-walled cylindrical modules. A mirror system of novel design transports Cerenkov photons to photomultiplier tubes. This system is compact, contains relatively little material, and has a large fraction of active volume. A prototype of a module designed for the proposed CLEO III detector has been studied using cosmic rays. Results from these studies show good agreement with a detailed Monte Carlo simulation of the module and indicate that it should achieve separation of pions and kaons at the 2.5-3.0sigma level in the momentum range 0.8-2.8 GeV/c. We predict performance for specific physics analyses using a GEANT-based simulation package.']",['1996-08-01']
2321,['eng'],"['Bamberger, Andreas']",['The Presampler for the Forward and Rear Calorimeter in the ZEUS Detector'],['Detectors and Experimental Techniques'],"['calorimeter, sandwich', 'scintillation counter, fibre', 'optics, transformation', 'radiation, yield', 'photoelectron, amplifier', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9609006'],"['The ZEUS detector at HERA has been supplemented with a presampler detector in front of the forward and rear calorimeters. It consists of a segmented scintillator array read out with wavelength-shifting fibers. We discuss its desi gn, construction and performance. Test beam data obtained with a prototype presampler and the ZEUS prototype calorimeter demonstrate the main function of this detector, i.e. the correction for the energy lost by an electron interacting in inactive material in front of the calorimeter.']",['1996-09-12']
2322,['eng'],"['Leone, S']",['New Observations of Top at CDF'],['Particle Physics - Experimental Results'],"['talk, Padua 1996/05/26', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'final state, (6jet)', '(6jet), final state', 'final state, dilepton', 'dilepton, final state', 'tau, semileptonic decay', 'semileptonic decay, tau', 'particle identification, beauty', 'transverse energy, missing-energy', 'channel cross section', 'mass, dependence', 'dependence, mass', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608002'],"['We report preliminary results from the analyses looking for top candidates in the channel with 6 jets in the final state (all hadronic) and in the dilepton channel with one tau lepton (tau dilepton), using a data sample of 110 pb^{-1} collected by the CDF experiment at the Fermilab Tevatron Collider.']",['1996-08-05']
2323,['eng'],"['Adolff, C', 'Andeson, M', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arndt, C', 'Aïd, S', 'Babaev, A', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Braunschweig, W', 'Brisson, V', 'Bruel, P', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Bán, J', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Calvet, D', 'Campbell, A J', 'Carli, T', 'Charlet, M', 'Chechelnitskii, S', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Cousinou, M C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davis, C L', 'De Wolf, E A', 'Delcourt, B', 'Di Nezza, P', 'Dirkmann, M', 'Dixon, P', 'Dlugosz, W', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duhm, H', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Evrard, E', 'Fahr, A B', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Gaede, F', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'Golec-Biernat, K J', 'González-Pineiro, B', 'Gorelov, I V', 'Grab, C', 'Greenshaw, T J', 'Griffiths, R K', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Hampel, M', 'Haynes, W J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hewitt, K', 'Hildesheim, W', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Hoffmann, D', 'Holtom, T', 'Hoppner, M', 'Horisberger, R P', 'Hudgson, V L', 'Hufnagel, H', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johannsen, K', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kander, M', 'Kant, D', 'Kaschowitz, R', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kaufmann, O', 'Kausch-Blecken von Schmeling, M', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Kolanski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Kuhlen, M', 'Kurca, T', 'Kurzhofer, J', 'Köhler, T', 'Köhne, J H', 'Küpper, A', 'Küster, H', 'Lacour, D', 'Laforge, B', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Langenegger, U', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Levonian, S', 'Lindström, G', 'Lindstrøm, M', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lomas, J', 'Lubimov, V', 'Lüke, D', 'López, G C', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Meyer, A', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moeck, J', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Niggli, H', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Palmen, P', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Pawletta, H', 'Peppel, E', 'Phillips, J P', 'Pieuchot, A', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Pérez, E', 'Rabbertz, K', 'Reimer, P', 'Reinshagen, S', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riepenhausen, F', 'Riess, S', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rädel, G', 'Rüter, K', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schöning, A', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Specka, A E', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Squinabol, F', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Steiner, H', 'Steinhart, J', 'Stella, B', 'Stellberger, A', 'Stier, J', 'Stiewe, J', 'Stolze, K', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Tapprogge, Stefan', 'Tasevsky, M', 'Theissen, J', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Tsipolitis, G', 'Turnau, J', 'Tutas, J', 'Tzamariudaki, K', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Van den Plas, D', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'West, L R', 'Wiesand, S', 'Wilksen, T', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wobisch, M', 'Wünsch, E', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zini, P', 'Zomer, F', 'Zsembery, J', 'Zuber, K', 'Zur Nedden, M', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']",['Inclusive $D^0$ and $D^*$ $^{\\pm}$ Production in Deep Inelastic $ep$ Collisions at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'positron p, colliding beams', 'colliding beams, positron p', 'electron p, inclusive reaction', 'D0, electroproduction', 'electroproduction, D0', 'D*(2010), electroproduction', 'electroproduction, D*(2010)', 'charmed meson, hadronic decay', 'hadronic decay, charmed meson', 'quark, charm', 'quark, pair production', 'pair production, quark', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'quantum chromodynamics, perturbation theory', 'fusion, intermediate boson gluon', 'channel cross section', 'p, structure function', 'structure function, x-dependence', 'p, charm', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'electron p --> D0 electron anything', 'electron p --> D*(2010) electron anything', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607012'],"['First results on inclusive D0 and D* production in deep inelastic $ep$ scattering are reported using data collected by the H1 experiment at HERA in 1994. Differential cross sections are presented for both channels and are found to agree well with QCD predictions based on the boson gluon fusion process. A charm production cross section for 10~GeV$^2\\le Q^2\\le100$~GeV$^2$ and $0.01\\le y\\le0.7$ of $\\sigma\\left(ep\\ rightarrow c\\overline cX\\right) = (17.4 \\pm 1.6 \\pm 1.7 \\pm 1.4)$~nb is derived. A first measurement of the charm contribution F2_charm(x,Q^2) to the proton structure function for Bjorken $x$ between $8\\cdot10^{-4}$ and $8\\cdot10^{-3}$ is presented. In this kinematic range a ratio F2_charm/F2= 0.237\\pm0.021{+0.043\\atop-0.039}$ is observed.']",['1996-07-24']
2324,['eng'],"['Abe, K']",['A Study of the Orientation and Energy Partition of Three-Jet Events in Hadronic $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, inclusive reaction', 'Z0, electroproduction', 'Z0, hadronic decay', 'final state, (3jet)', 'quark, jet', 'gluon, jet', 'jet, energy', 'angular distribution', 'quantum chromodynamics, perturbation theory', 'gluon, spin', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'electron positron --> quark antiquark gluon', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9608016'],"['We have measured the distributions of the jet energies in e+e- --> qq^bar g events, and of the three orientation angles of the event plane, using hadronic $Z^0$ decays collected in the SLD experiment at SLAC. We find that the data are well described by perturbative QCD incorporating vector gluons. We have also compared our data with models of scalar and tensor gluon production, and discuss limits on the relative contributions of these particles to three-jet production in e+e- annihilation.']",['1996-08-29']
2325,['eng'],"['Demarteau, M']",['Measurement of the $W$ Boson Mass'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'W, leptonic decay', 'leptonic decay, W', 'mass, transverse', 'transverse, mass', 'W, mass', 'mass, W', 'mass ratio, (Z0 W)', '(Z0 W), mass ratio', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'W --> electron neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607011'],"['A measurement of the mass of the $W$ boson is presented based on a sample of 5982 $W \\rightarrow e \\nu$ decays observed in $p\\overline{p}$ collisions at fit to the transverse mass spectrum, combined with measurements of the $Z$ boson mass, the $W$ boson mass is measured to be $M_W = 80.350 \\pm 0.140 (stat.) \\pm 0.165 (syst.) \\pm 0.160 (scale) GeV/c^2$.']",['1996-07-17']
2326,['eng'],"['Chekanov, S V']",['Local multiplicity fluctuations in Z decay'],['Particle Physics - Experimental Results'],"['talk, Nijmegen 1996/06/30', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'statistical analysis', 'multiplicity, fluctuation', 'multiplicity, moment', 'parametrization', 'angular dependence', 'rapidity', 'momentum, difference', 'numerical calculations, Monte Carlo', 'interpretation of experiments, L3']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607007'],"['Local multiplicity fluctuations of hadrons produced in the decay of Z^0 were studied on the basis of L3 data. In addition to the normalized-factorial-moment method, the fluctuations were studied for the first time by the use of bunching parameters. A strong multifractal structure was observed inside jets. JETSET 7.4 PS describes the fluctuations in the azimuthal angle defined with respect to the beam axis reasonably well. For the fluctuations in rapidity, defined with respect to the thrust axis and in the four-momentum-difference variable, JETSET 7.4 PS overestimates the fluctuations.']",['1996-07-10']
2327,['eng'],"['Röhrich, D']",['Strange and non-strange (anti-)baryon production at 200 GeV per nucleon'],['Particle Physics - Experimental Results'],"['talk, Budapest 1996/05/15', 'nucleon nucleon, inclusive reaction', 'p nucleus, inclusive reaction', 'nucleus nucleus, inclusive reaction', 'sulfur', 'silver', 'gold', 'baryon, hadroproduction', 'hadroproduction, baryon', 'antibaryon, hadroproduction', 'hadroproduction, antibaryon', 'p', 'Lambda', 'production, strangeness', 'strangeness, production', 'strange particle, multiplicity', 'rapidity spectrum', 'yield, (Lambda K pi)', 'yield, (Antilambda anti-p)', 'energy dependence', 'dependence, mass number', 'mass number, dependence', 'experimental results', 'CERN SPS', '< 200 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607005'],['Rapidity distributions of net hyperons (\\Lambda - \\overline{\\Lambda}) are compared to distributions of participant protons (p - \\overline{p}). Strangeness production (mean multiplicities of produced \\Lambda/\\Sigma^0 hyperons and \\langle K + \\overline{K} \\rangle) in central nucleus-nucleus collisions is shown for different collision systems at different energies. An enhanced production of \\overline{\\Lambda} compared to \\overline{p} is observed at 200 GeV per nucleon.'],['1996-07-09']
2328,['eng'],"['Bertin, A', 'Bruschi, M']",['New data on OZI rule violation in $\\overline{P}P$ annihilation at rest'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'annihilation, anti-p p', 'at rest', 'hydrogen, gas', 'hydrogen, liquid', 'Iizuka-Okubo-Zweig rule, violation', 'hadron, multiple production', 'multiple production, hadron', 'pi, hadroproduction', 'hadroproduction, pi', 'omega(783), hadroproduction', 'hadroproduction, omega(783)', 'Phi(1020), hadroproduction', 'hadroproduction, Phi(1020)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607006'],"['The results of a measurement of the ratio R =3D Y(phi pi+ pi-) / Y(omega = pi+ pi-) for antiproton annihilation at rest in a gaseous and in a liquid hydrogen target are presented. It was found that the value of this ratio increases with the decreasing of the dipion mass, which demonstrates the difference in the phi and omega production mechanisms. An indication on the momentum transfer dependence of the apparent OZI rule violation for phi production from the 3S1 initial state was found.']",['1996-07-11']
2329,['eng'],"['Gazdzicki, M', 'Röhrich, D']",['Strangeness in nuclear collisions'],['Particle Physics - Experimental Results'],"['p p, interaction', 'interaction, p p', 'nucleus nucleus, interaction', 'interaction, nucleus nucleus', 'central region', 'hadron, multiple production', 'multiple production, hadron', 'strange particle, multiplicity', 'yield, (strange particle pi)', 'production, strangeness', 'strangeness, production', 'dependence, mass number', 'mass number, dependence', 'energy dependence', 'entropy, production', 'production, entropy', 'model, statistical', 'quark gluon, plasma', 'experimental results', 'bibliography', '2.8-400.0 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607004'],"['Data on the mean multiplicity of strange hadrons produced in minimum bias proton--proton and central nucleus--nucleus collisions at momenta between 2.8 and 400 GeV/c per nucleon have been compiled. The multiplicities for nucleon--nucleon interactions were constructed. The ratios of strange particle multiplicity to participant nucleon as well as to pion multiplicity are larger for central nucleus--nucleus collisions than for nucleon--nucleon interactions at all studied energies. The data at AGS energies suggest that the latter ratio saturates with increasing masses of the colliding nuclei. The strangeness to pion multiplicity ratio observed in nucleon--nucleon interactions increases with collision energy in the whole energy range studied. A qualitatively different behaviour is observed for central nucleus--nucleus collisions: the ratio rapidly increases when going from Dubna to AGS energies and changes little between AGS and SPS energies. This change in the behaviour can be related to the increase in the entropy production observed in central nucleus-nucleus collisions at the same energy range. The results are interpreted within a statistical approach. They are consistent with the hypothesis that the Quark Gluon Plasma is created at SPS energies, the critical collision energy being between AGS and SPS energies.']",['1996-07-05']
2330,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Okrasinski, J R', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Mattingly, M C K', 'Anselmo, F', 'Antonioli, P', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, I', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Palmonari, F', 'Pesci, A', 'Polini, A', 'Sartorelli, G', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Amelung, C', 'Bornheim, A', 'Crittenden, J A', 'Deffner, R', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Grothe, M', 'Hartmann, H', 'Heinloth, K', 'Heinz, L', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mengel, S', 'Paul, E', 'Pfeiffer, M', 'Rembser, C', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Cottingham, W N', 'Dyce, N', 'Foster, B', 'George, S', 'Hayes, M E', 'Heath, G P', 'Heath, H F', 'Piccioni, D', 'Roff, D G', 'Tapper, R J', 'Yoshida, R', 'Arneodo, M', 'Ayad, R', 'Capua, M', 'Garfagnini, A', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Caldwell, A', 'Crtiglia, N', 'Jing, Z', 'Liu, W', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Jakubowski, Z', 'Przybycien, M B', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Przybycien, M B', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Dulinski, Z', 'Kotanski, Andrzej', 'Abbiendi, G', 'Bauerdick, L A T', 'Bhns, U', 'Beier, H', 'Bienlein, J K', 'Cases, G', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'GroBe-Knitter, J', 'Haas, T', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Iga, Y', 'Johnson, K F', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Mainusch, J', 'Manczak, O', 'Milewski, J', 'Monteiro, T', 'Ng, J S T', 'Notz, D', 'Ohrenberg, K', 'Piotrzkowski, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Surrow, B', 'Tassi, E', 'Vob, T', 'Westphal, D', 'Wolf, G', 'Wollmer, U', 'Youngman, C', 'Zeuner, W', 'Grabosch, H J', 'Kharchilava, A I', 'Mari, S M', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Gallo, E', 'Pelfer, P G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Trefzger, T M', 'Wölfle, S', 'Bromley, J T', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Saxon, D H', 'Sinclair, L E', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Sinkus, R', 'Wick, K', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Brümmer, N', 'Butterworth, Ian', 'Harris, V L', 'Howell, G', 'Hung, B Y H', 'Lamberti, L', 'Long, K R', 'Miller, D B', 'Pavel, N', 'Prinias, A', 'Sedgbeer, J K', 'Sideris, D', 'Whitfield, A F', 'Mallik, U', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Cloth, P', 'Filges, E', 'An, S H', 'Cho, G H', 'Ko, B J', 'Lee, S B', 'Nam, S W', 'Park, H S', 'Park, S K', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Fernández, J P', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Laberga, L', 'Martínez, M', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Yung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Riveline, M', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Tsurugai, T', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Korzhavina, I A', 'Kuzmin, V A', 'Lukina, O Yu', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Van Sighem, A', 'Tiecke, H G', 'Vossebeld, J H', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Gilmore, J', 'Li Chuan', 'Ling, T Y', 'Nylander, P', 'Park, I H', 'Romanowsky, T A', 'Bailey, D S', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Devenish, R C E', 'Harmew, N', 'Lancaster, M', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Tickner, J R', 'Uijterwaal, H', 'Walczak, R', 'Waters, D S', 'Wilson, F F', 'Yip, T', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Zuin, F', 'Bulmahn, J', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Shah, T P', 'Barberis, E', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Williams, D C', 'Biltzinger, J', 'Seifert, R J', 'Schwarzer, O', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Inuzuka, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nakao, M', 'Suzuki, I', 'Tokushuku, K', 'Umemori, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Matsushita, T', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bénard, F', 'Brkic, M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Polenz, S', 'Sampson, C R', 'Simmons, D', 'Teuscher, R J', 'Butterworth, J M', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Sutton, M R', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Coldewey, C', 'Eisenberg, Y', 'Hochman, D', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Badgett, W F', 'Breitweg, J', 'Chapin, D', 'Cross, R', 'Dasu, S', 'Foudas, C', 'Loveless, R J', 'Mattingly, S E', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Murray, W N', 'Schmidke, W B']",['Measurement of the F2 structure function in deep inelastic e$^{+}$p scattering using 1994 data from the ZEUS detector at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'p, structure function', 'structure function, small-x', 'x-dependence', 'dependence, momentum transfer', 'quantum chromodynamics, perturbation theory', 'Altarelli-Parisi equation', 'kinematics', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607002'],"['We present measurements of the structure function \\Ft\\ in e^+p scattering at HERA in the range 3.5\\;\\Gevsq < \\qsd < 5000\\;\\Gevsq. A new reconstruction method has allowed a significant improvement in the resolution of the kinematic variables and an extension of the kinematic region covered by the experiment. At \\qsd < 35 \\;\\Gevsq the range in x now spans 6.3\\cdot 10^{-5} < x < 0.08 providing overlap with measurements from fixed target experiments. At values of Q^2 above 1000 GeV^2 the x range extends to 0.5. Systematic errors below 5\\perc\\ have been achieved for most of the kinematic urray, W N']",['1996-07-04']
2331,['eng'],"['Heuring, T C']",['Jet decorrelation and jet shapes at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, La Thuile 1996/03/03', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'jet, hadroproduction', 'hadroproduction, jet', 'jet, event shape analysis', 'angular correlation, (2jet)', 'transverse energy, dependence', 'rapidity dependence', 'quantum chromodynamics, perturbation theory', 'renormalization, dependence', 'showers, parton', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607001'],"['We present results on measurements of jet shapes and jet azimuthal decorrelation from \\overline{p}p collisions at \\sqrt{s}=1.8 TeV using data collected during the 1992--1993 run of the Fermilab Tevatron. Jets are seen to narrow both with increasing E_T and increasing rapidity. While HERWIG, a parton shower Monte Carlo, predicts slightly narrower jets, it describes the trend of the data well; NLO QCD describes qualitative features of the data but is sensitive to both renormalization scale and jet definitions. Jet azimuthal decorrelation has been measured out to five units of pseudorapidity. While next--to--leading order QCD and a leading--log approximation based on BFKL resummation fail to reproduce the effect, HERWIG describes the data well.']",['1996-07-02']
2332,['eng'],"['Nachtman, J M']",['Searches at LEP 1.5'],['Particle Physics - Experimental Results'],"['review, Les Arcs 1996/03/16', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'new particle, search for', 'model, composite', 'lepton, excited state', 'quantum electrodynamics, Lambda parameter', 'heavy lepton, pair production', 'pair production, heavy lepton', 'final state, (4fermion)', '(4fermion), final state', 'sparticle, pair production', 'pair production, sparticle', 'mass, lower limit', 'lower limit, mass', 'magnetic detector, ALEPH', 'magnetic detector, DELPHI', 'magnetic detector, OPAL', 'magnetic detector, L3', 'experimental results', 'CERN LEP Stor', '130, 136 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606015'],"['The energy upgrade at LEP allows new regimes to be explored in the search for physics beyond the Standard Model. The searches for new physics using the ALEPH, DELPHI, L3, and OPAL data are described, and the results are presented.']",['1996-06-28']
2333,['eng'],"['Kodama, K', 'Torikai, S', 'Mokhtarani, A', 'Paolone, V S', 'Volk, J T', 'Wilcox, J O', 'Yager, P M', 'Edelstein, R M', 'Freyberger, A P', 'Gibaut, D B', 'Lipton, R J', 'Nichols, W R', 'Potter, D M', 'Russ, J S', 'Zhang, C', 'Zhang, Y', 'Jang, H I', 'Kim, J Y', 'Baller, B R', 'Stefanski, R J', 'Nakazawa, K', 'Chung, S H', 'Park, M S', 'Park, I G', 'Song, J S', 'Yoon, C S', 'Aryal, M', 'Reay, N W', 'Sidwell, R A', 'Stanton, N R', 'Yoshida, S', 'Chikawa, M', 'Hara, T', 'Aoki, S', 'Hoshino, K', 'Kobayashi, M', 'Komatsu, M', 'Miyanishi, M', 'Nakamura, M', 'Nakanishi, S', 'Niwa, K', 'Nomura, M', 'Okada, K', 'Tajima, H', 'Teraoka, K', 'Dunlea, J M', 'Frederiksen, S G', 'Kuramata, S', 'Lundberg, B G', 'Oleynik, G A', 'Reibel, K', 'Kalbfleisch, G R', 'Skubic, P L', 'Snow, J', 'Willis, S E', 'Nakamura, K', 'Okusawa, T', 'Yoshida, T', 'Okabe, H', 'Yokota, J', 'Ihara, N', 'Kazuno, M', 'Koya, T', 'Niu, E', 'Ogawa, S', 'Shibuya, H', 'Watanabe, S', 'Yasuda, N', 'Ehara, K', 'Horie, K', 'Sato, Y', 'Suzuki, K', 'Tezuka, I']",['Measurement of B(D$_{s}^{+}$ --> $\\mu^{+}\\nu_{\\mu}$)/B(D$_{s}^{+}$ --> $\\phi\\mu^{+}\\nu_{\\mu}$) and determination of the decay constant f$_{D_{s}}$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'D/s+, hadroproduction', 'hadroproduction, D/s+', 'D/s+, leptonic decay', 'leptonic decay, D/s+', 'D/s+, semileptonic decay', 'semileptonic decay, D/s+', 'D/s+, branching ratio', 'D/s+, decay constant', 'decay constant, D/s+', 'muon+, transverse momentum', 'nuclear emulsion', 'spectrometer, experimental results', 'Batavia TEVATRON Coll', 'D/s+ --> muon+ neutrino/mu', 'D/s+ --> Phi(1020) muon+ neutrino/mu', '600 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606017'],"['We have observed 23.2 \\pm 6.0_{-0.9}^{+1.0} purely-leptonic decays of D_s^+ -> \\mu^+ \\nu_\\mu from a sample of muonic one prong decay events detected in the emulsion target of Fermilab experiment E653. Using the D_s^+ -> \\phi \\mu^+ \\nu_\\mu yield measured previously in this experiment , we obtain B(D_s^+ ---> \\mu^+ \\nu_\\mu) / B(D_s^+ ---> \\phi \\mu^+ \\nu_\\mu) =0.16 \\pm 0.06 \\pm 0.03. In addition, we extract the decay constant f_{D_s}=194 \\pm 35 \\pm 20 \\pm 14 MeV.']",['1996-06-28']
2334,['eng'],"['Aitala, E M']",['Search for D$^{0}\\overline{D}^{0}$ mixing in semileptonic decay modes'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D*(2010), hadroproduction', 'hadroproduction, D*(2010)', 'D*(2010), hadronic decay', 'hadronic decay, D*(2010)', 'D0, semileptonic decay', 'semileptonic decay, D0', 'D0 anti-D0, interference', 'upper limit', 'charge correlation, (pi lepton)', 'experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> D*(2010) anything', 'D*(2010) --> D0 pi+', 'D0 --> K- lepton+ neutrino/e', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606016'],['We report the result of a search for D0 - D0_bar mixing in the data from hadroproduction experiment E791 at Fermilab. We use the D* tag and semileptonic decay vertices of D0 to look for wrong-sign decays with mixing time dependence.'],['1996-06-28']
2335,['eng'],"['Abachi, S']",['Search for anomalous WW and WZ production in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'intermediate boson, pair production', 'pair production, intermediate boson', 'intermediate boson, hadronic decay', 'hadronic decay, intermediate boson', 'W, leptonic decay', 'leptonic decay, W', 'final state, (2jet electron neutrino)', '(2jet electron neutrino), final state', 'W, transverse momentum', 'coupling, (2W photon)', '(2W photon), coupling', 'coupling, (Z0 2W)', '(Z0 2W), coupling', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', 'anti-p p --> Z0 W anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606013'],"['We present results from a search for anomalous WW and WZ production in ppbar collisions at sqrt(s) = 1.8 TeV. We used ppbar->evjjX events observed during the 1992-1993 run of the Fermilab Tevatron collider, corresponding to an integrated luminosity of 13.7 +- 0.7 pb^-1. A fit to the transverse momentum spectrum of the W boson yields direct limits on the CP-conserving anomalous WWgamma and WWZ coupling parameters of -0.9 < delta kappa < 1.1 (with lambda = 0) and -0.6 < lambda < 0.7 (with delta kappa = 0) at the 95% confidence level, for a form factor scale Lambda = 1.5 TeV, assuming that the WWgamma and WWZ coupling parameters are equal.']",['1996-06-25']
2336,['eng'],"['Allport, P P', 'Booth, P S L', 'Green, C', 'Greenall, A', 'Hanlon, M', 'Jackson, J N', 'Jones, T J', 'Richardson, J', 'Parzefall, U', 'Sheridan, A', 'Smith, N A']",['Performance of the ATLAS-A silicon detector with analogue read out'],['Particle Physics - Experimental Results'],"['tracks', 'semiconductor detector, microstrip', 'semiconductor detector, readout', 'integrated circuit', 'trigger', 'electronics, background', 'magnetic detector, ATLAS', 'CERN LHC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606012'],['The performace of an ATLAS-A silicon micro-strip detector prototype with FELIX 128 analogue read out chip has been studied. The noise level and the signal to noise ratio have been measured as a funtion of both detector bias and temperature. No evidence of micro-discharge was observed for detector bias voltages up to 300 V.'],['1996-06-20']
2337,['eng'],"['Sefkow, F']",['Heavy flavour production at HERA'],['Particle Physics - Experimental Results'],"['review, La Thuile 1996/03/03', 'electron p, colliding beams', 'colliding beams, electron p', 'positron p, colliding beams', 'colliding beams, positron p', 'exchange, one-photon', 'one-photon, exchange', 'quark, charm', 'quark, pair production', 'pair production, quark', 'J/psi(3100), photoproduction', 'photoproduction, J/psi(3100)', 'D*(2010), photoproduction', 'photoproduction, D*(2010)', 'p, structure function', 'structure function, charm', 'channel cross section, energy dependence', 'differential cross section', 'diffraction, production', 'production, diffraction', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606009'],"['Recent results from the experiments ZEUS and H1 on charm production in ep collisions are reviewed. The topics are elastic and inelastic J/\\psi photoproduction, D^* photoproduction differential cross sections and a first look at the proton structure function F_2^{c\\bar{c}}.']",['1996-06-19']
2338,['eng'],"['Sinclair, L E']",['Rapidity gaps in hard photoproduction'],['Particle Physics - Experimental Results'],"['talk, Eilat 1996/02/18', 'positron p, colliding beams', 'colliding beams, positron p', 'exchange, one-photon', 'one-photon, exchange', 'hadron, photoproduction', 'photoproduction, hadron', 'jet, photoproduction', 'photoproduction, jet', 'rapidity, gap', 'diffraction, dissociation', 'hard scattering', 'final state, (2jet)', '(2jet), final state', 'exchange, pomeron', 'pomeron, exchange', 'color, singlet', 'gluon, exchange', 'exchange, gluon', 'differential cross section, rapidity dependence', 'rapidity dependence, differential cross section', 'cross section, factorization', 'structure function, pomeron', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606010'],"['Recent results obtained from studies of diffractive processes in hard photoproduction performed by the ZEUS collaboration using data delivered by HERA in 1993 and 1994 are presented. In particular, we have found that (7 \\pm 3)\\% of events with two jets at a pseudorapidity interval of 3.5 to 4 are inconsistent with a non-diffractive production mechanism. These events may be interpreted as arising due to the exchange of a colour singlet object of negative squared invariant mass (-t) around 40~GeV^2. We have also probed the structure of the exchanged colour singlet object in low--t diffractive scattering. By comparing the results from photoproduction and electroproduction processes we find that between 30\\% and 80\\% of the momentum of the exchanged colour singlet object which is carried by partons is due to hard gluons.']",['1996-06-19']
2339,['eng'],"['Etzion, E']",['Analysis of the $\\tau$ Polarization and its Forward-Backward Asymmetry on the $Z^{0}$'],['Particle Physics - Experimental Results'],"['thesis', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'tau, pair production', 'pair production, tau', 'tau, polarization', 'polarization, tau', 'angular distribution, asymmetry', 'asymmetry, angular distribution', 'tau, leptonic decay', 'leptonic decay, tau', 'tau, semileptonic decay', 'semileptonic decay, tau', 'lepton, universality', 'Weinberg angle', 'coupling constant, vector', 'vector, coupling constant', 'coupling constant, axial-vector', 'axial-vector, coupling constant', 'magnetic detector, OPAL', 'experimental results', 'CERN LEP Stor', 'bibliography', 'electron positron --> tau+ tau-', 'tau --> lepton neutrino/tau antineutrino', 'tau --> pi neutrino/tau', 'tau --> K neutrino/tau', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606011'],"['This thesis describes a new a measurement of the tau lepton polarization and its forward-backward asymmetry at the Z resonance using the OPAL detector. This measurement is based on analyses of the tau->electron, muon and pion (Kaon) decays from a sample of 30663 tau-pair events collected in the polar angle range of Abs(cos(theta)) <0.68 during the 1990-1992 data taking period. Taking then the Standard Model with the V-A structure of the tau lepton decay, we measure the average tau polarization to be <p_tau>=(-13.5+/-2.9+/-2.2)% and the tau polarization forward-backward asymmetry to be AFBpol=(-11.0+/-3.5+/-0.5)% where the first error is statistical and the second systematic. Combining these figures with the OPAL <p_tau> and AFBpol measured with the tau->rho channel we get an average tau polarization, <p_tau>=(-14.9+/-1.9+/-1.3)% and for the asymmetry in the polarization, AFBpol=(-8.9+/-2.2+/-0.9)% . These results are consistent with lepton universality. Combining the two results we obtain for the electroweak mixing angle the value sin^2(theta_W)=0.2331+/-0.0023 within the context of the Standard Model, where the error includes both statistical and systematic uncertainties.']",['1996-06-19']
2340,['eng'],"['Etzion, E']",['Measurement of Rb at SLD'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1996/03/16', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'Z0, branching ratio', 'track data analysis, vertex', 'semiconductor detector, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606008'],"['We report a new measurement of Rb=Gamma(Z -> bb)/ Gamma(Z -> hadrons) using a double tag technique where the b selection is based on topological reconstruction of the mass of the B-decay vertex. The measurement was performed using a sample of 150k hadronic Z0 events collected with the SLD at the SLAC Linear Collider during the years 1993-1995. The method utilizes the 3-D vertexing abilities of the SLD CCD pixel vertex detector and the small stable SLC beams to obtain a high b tagging efficiency of 37% for a purity of 97.2%. The high purity reduces the systematics introduced by charm contamination and correlations with Rc. We obtain a result of Rb=0.2176+/-0.0033(stat.)+/-0.0017(syst.)+/-0.0008(Rc). (Presented at the XXXIst Rencontres de Moriond Electroweak Interactions and Unified Theories, Les Arcs, Savoie, France, March 16-23, 1996.)']",['1996-06-18']
2341,['eng'],"['Chen, E', 'Saulnier, M', 'Sun, W', 'Yamamoto, H']",['Tests of a high resolution time of flight system based on long and narrow scintillator'],['Particle Physics - Experimental Results'],"['fast logic, time-of-flight', 'scintillation counter, plastics', 'scintillation counter, fibre', 'photoelectron, amplifier', 'photoelectron, yield', 'time resolution', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606007'],"['We have tested a prototype time-of-flight system based on bulk scintillator block of dimensions 2.5 \\times 2.5 \\times 200 cm. Using a calibration scheme similar to the one used in actual collider experiments, we have achieved a resolution of 71 ps using Amperex XP2020/UR photomultipliers and 81 ps using proximity-focusing fine-mesh photomultipliers (Hamamatsu R2021). Results are also obtained for scintillating fiber blocks of the same dimensions. Good internal reflectivity of the bulk scintillator block resulted in resolutions superior to the fibre blocks. A single-photon pulsed laser system was used to study photomultipliers and the results were used in a Monte Carlo simulation of the system to study the critical elements that determine the resolution.']",['1996-06-17']
2342,['eng'],"['Agababian, N M']",['Large self-affine fractality in $\\pi^{+}$p and K$^{+}$p collisions at 250 GeV/c'],['Particle Physics - Experimental Results'],"['pi+ p, interaction', 'interaction, pi+ p', 'K+ p, interaction', 'interaction, K+ p', 'hadron, multiple production', 'multiple production, hadron', 'multiplicity, moment', 'fractals', 'phase space, anisotropy', 'scaling', 'transformation, affine', 'magnetic spectrometer, experimental results', 'CERN SPS', '250 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606005'],"['Taking into account the anisotropy of phase space in multiparticle production, a self-affine analysis of factorial moments was carried out on the NA22 data for $\\p^+\\Pp$ and $\\PK^+\\Pp$ collisions at 250 GeV/$c$. Within the transverse plane, the Hurst exponents measuring the anisotropy are consistent with unit value (i.e. no anisotropy). They are, however, only half that value when the longitudinal direction is compared to the transverse ones. Fractality, indeed, turns out to be self-affine rather than self-similar in multiparticle production. In three-dimensional phase space, power-law scaling is observed to be better realized in self-affine than in self-similar analysis.']",['1996-06-18']
2343,['eng'],"['Abe, F', 'Akimoto, H']",['Ratios of bottom meson branching fractions involving J/$\\psi$ mesons and determination of b quark fragmentation fractions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'beautiful meson, hadroproduction', 'hadroproduction, beautiful meson', 'beautiful meson, hadronic decay', 'hadronic decay, beautiful meson', 'beautiful meson, branching ratio', 'J/psi(3100)', 'B+', 'B0', 'B/s', 'model, decay', 'decay, model', 'fragmentation function, beauty', 'mass spectrum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B --> J/psi(3100) K', 'B --> J/psi(3100) K*(892)', 'B/s --> J/psi(3100) Phi(1020)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9607003'],[],['1996-07-04']
2344,['eng'],"['Saltzberg, D']",['Status of the search for $\\nu_{\\mu}$ --> $\\nu_{\\tau}$ oscillations with the CHORUS detector'],['Particle Physics - Experimental Results'],"['talk, Venice 1996/02/27', 'neutrino, oscillation', 'neutrino/mu, secondary beam', 'secondary beam, neutrino/mu', 'neutrino/tau', 'neutrino nucleon, interaction', 'interaction, neutrino nucleon', 'charged current', 'tau-, search for', 'tau-, decay modes', 'decay modes, tau-', 'neutrino, mixing angle', 'nuclear emulsion', 'scintillation counter, fibre', 'magnetic spectrometer', 'calorimeter', 'CERN SPS', '450 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606004'],"['The CHORUS experiment is searching for nu-mu to nu-tau oscillations using an 800 kilogram emulsion target and an electronic detector. Two of four years of running have been completed. The experiment will probe small mixing angles for squared neutrino mass differences greater than 10 eV^2, at least one order of magnitude better than previous limits.']",['1996-06-07']
2345,['eng'],"['Murayama, H', 'Peskin, Michael E']",['Physics opportunities of e+e- linear colliders'],['Particle Physics - Experimental Results'],"['review', 'electron positron, linear collider', 'linear collider, proposed', 'electron positron, interaction', 'interaction, electron positron', 'electron electron, interaction', 'interaction, electron electron', 'photon electron, interaction', 'interaction, photon electron', 'photon photon, interaction', 'interaction, photon photon', 'electroweak interaction, symmetry breaking', 'symmetry breaking, electroweak interaction', 'W, electroproduction', 'electroproduction, W', 'W, pair production', 'pair production, W', 'coupling, (Z0 2W)', '(Z0 2W), coupling', 'coupling, (2W photon)', '(2W photon), coupling', 'quark, truth', 'quark, pair production', 'pair production, quark', 'Higgs particle, electroproduction', 'electroproduction, Higgs particle', 'Higgs particle, coupling', 'coupling, Higgs particle', 'supersymmetry', 'sparticle, pair production', 'pair production, sparticle', 'sparticle, mass', 'mass, sparticle', 'sparticle, decay', 'decay, sparticle', 'p p, interaction', 'interaction, p p', 'scattering, W W', 'W W, scattering', 'Higgs particle, strong interaction', 'strong interaction, Higgs particle', 'model, technicolor', 'Goldstone particle', ""postulated particle, Z'"", 'proposed experiment', 'numerical calculations', 'bibliography', '500-1500 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606003'],"['We describe the anticipated experimental program of an e+e- linear collider in the energy range 500 GeV -- 1.5 TeV. We begin with a description of current collider designs and the expected experimental environment. We then discuss precision studies of the W boson and top quark. Finally, we review the range of models proposed to explain the physics of electroweak symmetry breaking and show, for each case, the central role that the linear collider experiments will play in elucidating this physics. (to appear in Annual Reviews of Nuclear and Particle Science)']",['1996-06-06']
2346,['eng'],"['Murayama, H']",['Physics prospects'],['Particle Physics - Experimental Results'],"['talk, Iwate 1995/09/08', 'electroweak interaction, symmetry breaking', 'symmetry breaking, electroweak interaction', 'electron positron, linear collider', 'Salam-Weinberg model', 'supersymmetry', 'Higgs particle, mass', 'mass, Higgs particle', 'Higgs particle, decay modes', 'decay modes, Higgs particle', 'Higgs particle, radiative decay', 'radiative decay, Higgs particle', 'Higgs particle, branching ratio', 'model, technicolor', 'sparticle, electroproduction', 'electroproduction, sparticle', 'sparticle, angular distribution', 'angular distribution, sparticle', 'transverse energy, missing-energy', 'W, pair production', 'pair production, W', 'Z0, pair production', 'pair production, Z0', 'linear collider, proposed', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606001'],"['The need to understand physics of electroweak symmetry breaking is reviewed. An electron positron linear collider will play crucial roles in that respect. It is discussed how the LHC and a linear collider need each other to understand symmetry breaking mechanism unambiguously. Two popular scenarios, supersymmetry and technicolor-like models, are used to demonstrate this point.']",['1996-06-05']
2347,['eng'],[],['Observation of Events with an Energetic Forward Neutron in Deep Inelastic Scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'n, electroproduction', 'electroproduction, n', 'production, small-angle', 'small-angle, production', 'n, leading particle', 'exchange, one-pion', 'one-pion, exchange', 'energy spectrum, (n)', '(n), energy spectrum', 'x-dependence', 'dependence, momentum transfer', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> n positron anything', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606006'],"['In deep inelastic neutral current scattering of positrons and protons at the center of mass energy of 300 GeV, we observe, with the ZEUS detector, events with a high energy neutron produced at very small scattering angles with respect to the proton direction. The events constitute a fixed fraction of the deep inelastic, neutral current event sample independent of Bjorken $x$ and $Q^2$ in the range $ 3 \\cdot 10^{-4} < \\xbj < 6\\cdot 10^{-3}$ and $10 < Q^2 < 100$~GeV$^2$.']",['1996-06-18']
2348,['eng'],"['Heinson, A P']",['Future top physics at the Tevatron and LHC'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1996/03/23', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, hadroproduction', 'hadroproduction, quark', 'quark, pair production', 'pair production, quark', 'cross section', 'mass, truth', 'truth, mass', 'quark, width', 'quark, branching ratio', 'quark, decay modes', 'decay modes, quark', 'coupling, (W truth beauty)', '(W truth beauty), coupling', 'Kobayashi-Maskawa angle', 'quark, polarization', 'polarization, quark', 'gluon, radiation', 'numerical calculations, CERN LHC Coll', 'numerical calculations, Batavia TEVATRON Coll', 'anti-p p --> truth anything', 'anti-p p --> 2truth anything', '1800, 14000 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605010'],"['Top quarks are produced at the Tevatron proton-antiproton collider at Fermilab and at the Large Hadron (proton-proton) Collider at CERN in two ways: as quark-antiquark pairs, and singly. For each mode, the cross sections and future experimental yields are presented. I then discuss some precision measurements that can be made using the anticipated large data sets. These measurements include the top quark mass, width and branching fractions, the electroweak Wtb coupling, and the CKM matrix element Vtb. Detailed studies of the top quark polarization and gluon radiation will also be possible, in addition to sensitive searches for ttbar resonances and rare decay modes.']",['1996-05-29']
2349,['eng'],"['Dittmar, Michael']",['Neutral current interference in the TeV region'],['Particle Physics - Experimental Results'],"['p p, interaction', 'interaction, p p', 'lepton, pair production', 'pair production, lepton', 'mass spectrum, dilepton', 'dilepton, mass spectrum', 'rapidity spectrum', 'neutral current, interference', 'angular distribution, asymmetry', 'asymmetry, angular distribution', 'charge, asymmetry', 'quark, composite', ""postulated particle, Z'"", 'numerical calculations, CERN LHC Coll', '14000 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9606002', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=scan&id=SCAN-9605176']","[""The possibilities to measure lepton forward--backward asymmetries at the LHC in the reaction pp(qqbar) --> l+l- are studied for dilepton events with masses above 400 GeV. It is shown that such measurements allow accurate tests of the neutral current interference structure up to about 2 TeV center of mass energies. The sensitivity of asymmetries at the LHC to new physics is demonstrated within the context of quark compositeness and exotic Z' scenarios.""]",['1996-06-05']
2350,['eng'],"['Derrick, Malcolm']",['Dijet angular distributions in direct and resolved photoproduction at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, inclusive reaction', 'exchange, one-photon', 'one-photon, exchange', 'jet, photoproduction', 'photoproduction, jet', 'photon, resolved', 'hard scattering', 'angular distribution, (2jet)', '(2jet), angular distribution', 'quantum chromodynamics', 'quark, exchange', 'exchange, quark', 'gluon, exchange', 'exchange, gluon', 'spin, parton', 'parton, spin', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605009'],"['Jet photoproduction, where the two highest transverse energy (\\ETJ) jets have \\ETJ above 6 GeV and a jet-jet invariant mass above 23~GeV, has been studied with the ZEUS detector at the HERA ep collider. Resolved and direct photoproduction samples have been separated. The cross section as a function of the angle between the jet-jet axis and the beam direction in the dijet rest frame has been measured for the two samples. The measured angular distributions differ markedly from each other. They agree with the predictions of QCD calculations, where the different angular distributions reflect the different spins of the quark and gluon exchanged in the hard subprocess.']",['1996-06-27']
2351,['eng'],"['Tapprogge, Stefan']",['Diffractive deep-inelastic scattering'],['Particle Physics - Experimental Results'],"['talk, Les Arcs 1996/03/23', 'electron p, colliding beams', 'electron p, deep inelastic scattering', 'structure function, diffraction', 'exchange, pomeron', 'dependence, momentum transfer', 'scaling, violation', 'Altarelli-Parisi equation', 'gluon', 'hadron, electroproduction', 'D*(2010), hadronic decay', 'energy flow', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605007'],"[""New results on diffractive deep-inelastic e p scattering at HERA are presented using data taken in 1994 with the H1 detector. The cross section for diffractive deep-inelastic scattering is measured in terms of a diffractive structure function F_2^{D(3)}(\\beta,Q^2, \\xpom) over an extended kinematic range. The dependence of F_2^{D(3)} on \\xpom is found not to depend on Q^2, but to depend on \\beta. Therefore the \\xpom dependence no longer factorizes. The Q^2 and \\beta dependence of F_2^{D(3)} is analyzed after an integration over the dependence on \\xpom. For fixed \\beta a clear rise with \\log Q^2 is observed, persisting up to high values of \\beta. In terms of the Altarelli-Parisi (DGLAP) QCD evolution equations, these scaling violations give clear indications for a gluon dominated process. Subsequently an attempt is made to quantify the parton content of the diffractive exchange using the DGLAP evolution. At the starting scale a ``leading'' gluon distribution is found which contributes about 80 \\% of the momentum in the diffractive exchange. Measurements of the hadronic final state (energy flow and production of D^{*} mesons) are found to be consistent with the predictions of a model of deep-inelastic electron pomeron scattering using the information on the parton content obtained.""]",['1996-05-22']
2352,['eng'],"['Roos, M', 'Khalfin, L A']",['Dangers of unphysical regions'],['Detectors and Experimental Techniques'],"['statistical analysis', 'neutrino, solar', 'neutrino, flux', 'flux, neutrino', 'radioactivity, chemistry', 'tritium, semileptonic decay', 'semileptonic decay, tritium', 'antineutrino/e, mass', 'mass, antineutrino/e', 'background']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605008'],"['We discuss the appearance of negative numbers of events in radiochemical experiments and negative squared antineutrino mass m^2_{\\bar{\\nu}_e} in tritium beta decay. Going beyond the standard discussion about how to extract upper limits in those cases, we show that the problem is much more profound. We explain the circumstances which are the likely cause of the persistently negative values of m^2_{\\bar{\\nu}_e} in all modern tritium beta decay experiments.']",['1996-05-22']
2353,['eng'],"['Kamon, T']","['New particle searches at Tevatron, 2']",['Particle Physics - Experimental Results'],"['talk, Les Arcs 1996/03/23', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'new particle, search for', 'sparticle, charged particle', 'postulated particle, gluino', 'postulated particle, leptoquark', ""postulated particle, W'"", ""postulated particle, Z'"", 'supergravity', 'final state, (3lepton missing-energy)', '(3lepton missing-energy), final state', 'final state, (2jet electron neutrino)', '(2jet electron neutrino), final state', 'final state, dilepton', 'dilepton, final state', 'cross section, upper limit', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605006'],"['Various recent results of new particle searches at the Fermilab Tevatron are presented. No evidence is found for supersymmetric particles (chargino, gluino), leptoquark bosons and heavy gauge bosons in p-pbar collisions at sqrt{s} = 1.8 TeV. Excluded mass regions for each particle are determined.']",['1996-05-21']
2354,['eng'],"['Yang, U K']",['A measurement of R = $\\sigma_{L}$/$\\sigma_{T}$ in deep inelastic neutrino-nucleon scattering at the Tevatron'],['Particle Physics - Experimental Results'],"['talk, Durham 1995/09/18', 'neutrino nucleon, deep inelastic scattering', 'deep inelastic scattering, neutrino nucleon', 'antineutrino nucleon, deep inelastic scattering', 'deep inelastic scattering, antineutrino nucleon', 'differential cross section', 'cross section, longitudinal', 'cross section, transverse', 'cross section, ratio', 'x-dependence', 'dependence, momentum transfer', 'experimental results', 'Batavia TEVATRON PS', '< 600 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605005'],"['Measurements of neutrino-nucleon and antineutrino-nucleon differential cross sections using the CCFR neutrino detector at Fermilab have been used to extract preliminary values of R ={\\sigma_L}/{\\sigma_T} in the kinematic region 0.01<x<0.6, and 4<Q^2<300 GeV^2. The new data provide the first measurements of R in the x<0.1 region. The x and Q^2 dependence of R is compared with a QCD based fit to previous data. The QCD fit, which provides an estimate of R in small x region where R has not been previously measured, is in good agreement with the new CCFR data.']",['1996-05-21']
2355,['eng'],"['Abe, F']",['Further properties of high-mass multijet events at the Fermilab proton-antiproton collider'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'jet, hadroproduction', 'hadroproduction, jet', 'jet, multiplicity', 'quantum chromodynamics, perturbation theory', 'showers, parton', 'model, phase space', 'parametrization', 'gluon, radiation', 'mass spectrum, ((n)jet)', '((n)jet), mass spectrum', 'angular distribution, ((n)jet)', '((n)jet), angular distribution', 'Dalitz plot', 'statistical analysis', 'numerical calculations, Monte Carlo', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605004'],"['The properties of high-mass multijet events produced at the Fermilab proton-antiproton collider are compared with leading order QCD matrix element predictions, QCD parton shower Monte Carlo predictions, and the predictions from a model in which events are distributed uniformly over the available multibody phase-space. Multijet distributions corresponding to (4N-4) variables that span the N-body parameter space are found to be well described by the QCD calculations for inclusive three-jet, four-jet, and five-jet events. The agreement between data, QCD Matrix Element calculations, and QCD parton shower Monte Carlo predictions suggests that 2 -> 2 scattering plus gluon radiation provides a good first approximation to the full LO QCD matrix element for events with three, four, or even five jets in the final state.']",['1996-05-14']
2356,['eng'],"['Bernardi, G']",['Structure function measurements at HERA and perturbative QCD'],['Particle Physics - Experimental Results'],"['talk, Santa Fe 1995/10/03', 'electron p, colliding beams', 'colliding beams, electron p', 'positron p, colliding beams', 'colliding beams, positron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'differential cross section', 'p, structure function', 'structure function, small-x', 'dependence, momentum transfer', 'exchange, pomeron', 'pomeron, exchange', 'quantum chromodynamics, perturbation theory', 'Altarelli-Parisi equation', 'gluon, momentum spectrum', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605003'],"['New results from the H1 and ZEUS collaborations on the measurement of cross-sections at very high Q^2 (up to 25000 GeV^2) and on the proton structure function F_2(x,Q^2) for momentum transfers squared Q^2 >= 1.5 GeV^2 and Bjorken x >= 3.5 10^{-5} are reported, using data collected at HERA mainly in 1994. No deviations from the Standard Model have been observed at high Q^2 and F_2 is seen to increase significantly with decreasing x, even in the lowest reachable Q^2 region. Comparisons at low Q^2 with fixed target experiments and with models based on pomeron exchange are presented. The F_2 results are well described by a Next to Leading Order QCD fit, and are consistent at the present level of precision with the rise at low x within this Q^2 range generated via the DGLAP evolution equations. The gluon density is extracted and being observed to rise at low x.']",['1996-05-09']
2357,['eng'],"['Aïd, S', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Babaev, A', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Braunschweig, W', 'Brisson, V', 'Bruel, P', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Bán, J', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Campbell, A J', 'Carli, T', 'Charlet, M', 'Chechelnitskii, S', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Cousinou, M C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Davis, C L', 'De Wolf, E A', 'Delcourt, B', 'Di Nezza, P', 'Dirkmann, M', 'Dixon, P', 'Dlugosz, W', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duhm, H', 'Düllmann, D', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Evrard, E', 'Fahr, A B', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Gaede, F', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'Golec-Biernat, K J', 'González-Pineiro, B', 'Gorelov, I V', 'Grab, C', 'Greenshaw, T J', 'Griffiths, R K', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Hadig, T', 'Haidt, D', 'Hajduk, L', 'Hampel, M', 'Haynes, W J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Hoffmann, D', 'Holtom, T', 'Hoppner, M', 'Horisberger, R P', 'Hudgson, V L', 'Hufnagel, H', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johannsen, K', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kander, M', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kaufmann, O', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Kolanski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Kuhlen, M', 'Kurca, T', 'Kurzhofer, J', 'Köhler, T', 'Köhne, J H', 'Küster, H', 'Lacour, D', 'Laforge, B', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Langenegger, U', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindström, G', 'Lindstrøm, M', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Lohmander, H', 'Lomas, J', 'Lubimov, V', 'Lüke, D', 'López, G C', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Merz, T', 'Meyer, A', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moeck, J', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Niggli, H', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Palmen, P', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Pawletta, H', 'Peppel, E', 'Phillips, J P', 'Pieuchot, A', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Pérez, E', 'Rabbertz, K', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riepenhausen, F', 'Riess, S', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rädel, G', 'Rüter, K', 'Sahlmann, N', 'Sankey, D P C', 'Schacht, P', 'Scharein, S', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schöning, A', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Specka, A E', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Squinabol, F', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Steiner, H', 'Stella, B', 'Stellberger, A', 'Stier, J', 'Stiewe, J', 'Stolze, K', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Tapprogge, Stefan', 'Tasevsky, M', 'Theissen, J', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Van den Plas, D', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wengler, T', 'Werner, M', 'West, L R', 'Wilksen, T', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wünsch, E', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zomer, F', 'Zsembery, J', 'Zuber, K', 'Zur Nedden, M', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']",['A search for selectrons and squarks at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'sparticle, search for', 'postulated particle, selectron', 'postulated particle, squark', 'sparticle, pair production', 'pair production, sparticle', 'sparticle, decay', 'decay, sparticle', 'supersymmetry', 'R parity, invariance', 'invariance, R parity', 'postulated particle, LSP', 'sparticle, mass', 'mass, sparticle', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'electron positron --> squark selectron anything', 'squark --> quark LSP', 'selectron --> electron LSP', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605002'],"['Data from electron-proton collisions at a center-of-mass energy of 300 GeV are used for a search for selectrons and squarks within the framework of the minimal supersymmetric model. The decays of selectrons and squarks into the lightest supersymmetric particle lead to final states with an electron and hadrons accompanied by large missing energy and transverse momentum. No signal is found and new bounds on the existence of these particles are derived. At 95\\% confidence level the excluded region extends to 65 GeV for selectron and squark masses, and to 40 GeV for the mass of the lightest supersymmetric particle.']",['1996-05-14']
2358,['eng'],"['Nakamura, I', 'Kawagoe, K']","['Measurement of BR(H --> c$\\overline{c}$, gg)/BR(H --> b$\\overline{b}$) in e+e- colliders at center-of-mass energy of 300 GeV']",['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'annihilation, electron positron', 'Higgs particle, electroproduction', 'electroproduction, Higgs particle', 'Higgs particle, hadronic decay', 'hadronic decay, Higgs particle', 'Higgs particle, leptonic decay', 'leptonic decay, Higgs particle', 'Higgs particle, branching ratio', 'Z0, associated production', 'associated production, Z0', 'Z0, decay modes', 'decay modes, Z0', 'quark, charm', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'gluon, pair production', 'pair production, gluon', 'tau, pair production', 'pair production, tau', 'supersymmetry', 'final state, (4jet)', '(4jet), final state', 'final state, (2jet)', '(2jet), final state', 'final state, (2jet 2lepton)', '(2jet 2lepton), final state', 'particle identification, flavor', 'numerical calculations, Monte Carlo', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604010'],"['Once a light Higgs boson is discovered at a future e+e- collider, the next target at the collider will be precise measurements of the Higgs boson properties. In this paper we report a simulation study on the measurement of the ratio Br(H->cc,gg)/Br(H->bb) at center of mass energy of 300 GeV, and show the possibility to constrain MSSM parameters from the measurement.']",['1996-05-01']
2359,['eng'],"['Rodríguez, J L']",['Factorization and color-suppression in hadronic b --> d$^{(*}$)n$\\pi$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Upsilon(10570), electroproduction', 'electroproduction, Upsilon(10570)', 'B, pair production', 'pair production, B', 'B0, hadronic decay', 'hadronic decay, B0', 'B-, hadronic decay', 'hadronic decay, B-', 'factorization, validity test', 'color', 'D', 'D*(2010)', 'rho(770)-', 'a1(1260)', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'B --> D (n)pi', 'B --> D*(2010) (n)pi', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604011'],"['The factorization hypothesis and color-suppression are investigated by analyzing the largest, to date, sample of B mesons. In all, 20 hadronic two-body decay modes are reconstructed using 2.04 fb^-1 of data collected with the CLEOII detector. We measure the branching fraction of five class I and five class III decay modes and set upper limits on branching fractions of ten class II decays. The branching fraction measurements are used to determine the BSW parameters a_1, and a_2/a_1. In addition, we measure the fraction of B-> D^{*+} rho^- decays which decay longitudinally polarized. The results are found to be consistent with factorization and color-suppression.']",['1996-05-01']
2360,['eng'],"['Filip, P']",['Transversal flow of pions as a consequence of rescattering process in non-central Pb+Pb 158 GeV/N heavy ion collisions'],['Particle Physics - Experimental Results'],"['nucleus nucleus, nuclear reaction', 'scattering, heavy ion', 'heavy ion, scattering', 'lead', 'pi, multiple production', 'multiple production, pi', 'transverse momentum, spectra', 'spectra, transverse momentum', 'angular distribution, asymmetry', 'asymmetry, angular distribution', 'particle flow, transverse', 'pi, gas', 'model, nuclear reaction', 'model, cascade', 'pi, multiple scattering', 'multiple scattering, pi', 'dependence, impact parameter', 'numerical calculations, Monte Carlo', '158 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9605001'],['Aim of this work was to test the idea of J.-Y.Ollitrault about the parallel squeeze-out type of transversal flow in mid-rapidity region. For this purpose we have performed a computer simulation of the expanding pion gas created in non-central Pb-Pb 158GeV/n collisions. A squeeze-out type of asymmetry parallel to impact parameter in azimuthal distribution of pions is found and studied. The asymmetry is explained as a consequence of geometry of non-central collisions and the rescattering process.'],['1996-05-02']
2361,['eng'],"['Raso, G']",['QCD studies at LEP I'],['Particle Physics - Experimental Results'],"['review, La Thuile 1996/03/03', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'Z0, leptonic decay', 'leptonic decay, Z0', 'width, ratio', 'tau, semileptonic decay', 'semileptonic decay, tau', 'strong interaction, coupling constant', 'coupling constant, strong interaction', 'dependence, flavor', 'quark, jet', 'gluon, jet', 'quark, beauty', 'jet, hadronization', 'fragmentation function', 'charged particle, multiplicity', 'experimental results', 'CERN LEP Stor', 'approx. 91 Gev-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604009'],['The high hadronic event statistics collected at the Z energy (LEP I) allowed a good understanding of the QCD dynamics. The coupling constant \\alpha_s has been measured with several methods giving a global average \\alpha_s(M_Z) = 0.122 \\pm 0.004. The flavour independence of \\alpha_s has been tested obtaining \\alpha_s^b/\\alpha_s^{udsc} = 0.997 \\pm 0.023. Quark-gluon jet differencies has been observed among which <n>_{gluon}/<n>_{quark} = 1.234 \\pm 0.027. A big role has been plaied by the silicon vertex detectors.'],['1996-04-29']
2362,['eng'],"['Derrick, Malcolm']",['Measurement of the reaction $\\gamma*$p --> $\\phi$p in deep inelastic e$^{+}$p scattering at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'Phi(1020), electroproduction', 'electroproduction, Phi(1020)', 'Phi(1020), photoproduction', 'photoproduction, Phi(1020)', 'rho(770), photoproduction', 'photoproduction, rho(770)', 'Phi(1020), hadronic decay', 'hadronic decay, Phi(1020)', 'mass spectrum, (K+ K-)', '(K+ K-), mass spectrum', 'channel cross section, energy dependence', 'quantum chromodynamics, perturbation theory', 'cross section, ratio', 'dependence, momentum transfer', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> Phi(1020) p positron', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604008'],"['The production of \\phi mesons in the reaction e^{+}p \\rightarrow e^{+} \\phi p (\\phi \\rightarrow K^{+}K^{-}), for 7 < Q^2 < 25 GeV^2 and for virtual photon-proton centre of mass energies (W) in the range 42-134 GeV, has been studied with the ZEUS detector at HERA. When compared to lower energy data at similar Q^2, the results show that the \\gamma^*p \\rightarrow \\phid p cross section rises strongly with W. This behaviour is similar to that previously found for the \\gamma^*p \\rightarrow \\rho^0 p cross section. This strong dependence cannot be explained by production through soft pomeron exchange. It is, however, consistent with perturbative QCD expectations, where it reflects the rise of the gluon momentum density in the proton at small x. The ratio of \\sigma (\\phi) / \\sigma (\\rho^0) which has previously been determined by ZEUS to be 0.065 \\pm 0.013 (stat.) in photoproduction at a mean W of 70 GeV, is measured to be 0.18 \\pm 0.05 (stat.) \\pm 0.03 (syst.) at a mean Q^2 of 12.3 GeV^2 and mean W of \\approx 100 GeV and is thus approaching at large Q^2 the value of 2/9 predicted from the quark charges of the vector mesons and a flavour independent production mechanism.']",['1996-05-02']
2363,['eng'],"['Aïd, S']",['A search for squarks of Rp-violating SUSY at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'supersymmetry', 'search for, squark', 'R parity, violation', 'violation, R parity', 'coupling, Yukawa', 'Yukawa, coupling', 'squark, decay modes', 'decay modes, squark', 'squark, truth', 'mass, squark', 'squark, mass', 'scattering, positron quark', 'positron quark, scattering', 'fusion, photon gluon', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604006'],"[""A search for squarks of R-parity violating supersymmetry is performed in ep collisions at HERA using H1 1994 e^+ data. Direct single production of squarks of each generation by e^+-quark fusion via a Yukawa coupling \\lambda' is considered. All possible R-parity violating decays and gauge decays of the squarks are taken into account. No significant deviation from the Standard Model predictions is found in the various multi-lepton and multi-jet final states studied and exclusion limits are derived. At 95\\% confidence level, the existence of first generation squarks is excluded for masses up to 240 \\GeV for coupling values \\lambda' \\gtrsim \\sqrt{ 4\\pi \\alpha_{em}}.The limits obtained are shown to be only weakly dependent on the free parameters of the Minimal Supersymmetric Standard Model. Stop squarks are excluded for masses up to 138 \\GeV for coupling \\lambda' \\times \\cos \\theta_t to e^+d pairs \\gtrsim 0.1 \\times \\sqrt{ 4\\pi \\alpha_{em}}, where \\theta_t is the mass mixing angle. Light stop squarks are furthermore searched for through pair production in \\gamma-gluon fusion processes. No signal is observed and exclusion limits are derived. Masses in the range 9 to 24.4 \\GeV are excluded at 95\\% confidence level for \\lambda' \\times \\cos \\theta_t > 10^{-4}.""]",['1996-05-16']
2364,['eng'],"['Sahu, S K', 'Wang, M Z', 'Suda, R', 'Enomoto, R', 'Peng, K C', 'Wang, C H', 'Adachi, I', 'Amami, M', 'Chang, Y H', 'Guo, R S', 'Hayashi, K', 'Iijima, T', 'Sumiyoshi, T', 'Yoshida, Y']",['Measurement of radiation damage on silica aerogel Cerenkov radiator'],['Detectors and Experimental Techniques'],"['Cherenkov counter, aerogel', 'silicon', 'optics, absorption', 'absorption, optics', 'optics, dispersion', 'radiation, damage', 'B, particle source', 'KEK TRISTAN Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604004'],"['We measured the radiation damage on silica aerogel \\v Cerenkov radiators originally developed for the B-factory experiment at KEK. Refractive index of the aerogel samples ranged from 1.012 to 1.028. The samples were irradiated up to 9.8~MRad of equivalent dose. Measurements of transmittance and refractive index were carried out and these samples were found to be radiation hard. Deteriorations in transparency and changes of refractive index were observed to be less than 1.3\\% and 0.001 at 90\\% confidence level, respectively. Prospects of using aerogels under high-radiation environment are discussed.']",['1996-04-12']
2365,['eng'],"['Aitala, E M']",['Mass splitting and production of $\\Sigma_{c}^{0}$ and $\\Sigma_{c}^{++}$ measured in 500 GeV $\\pi^{-}$-N interactions'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'Sigma/c++, hadroproduction', 'hadroproduction, Sigma/c++', 'Sigma/c0, hadroproduction', 'hadroproduction, Sigma/c0', 'mass difference, (Sigma/c Lambda/c+)', '(Sigma/c Lambda/c+), mass difference', 'Sigma/c, hadronic decay', 'hadronic decay, Sigma/c', 'Lambda/c+, hadronic decay', 'hadronic decay, Lambda/c+', 'mass spectrum', 'transverse momentum, spectra', 'spectra, transverse momentum', 'spectra, x-dependence', 'x-dependence, spectra', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> Sigma/c anything', 'Sigma/c --> Lambda/c+ pi', 'Lambda/c+ --> p K- pi+', '500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604007'],"[""From a sample of 2722 \\pm 78 \\Lambda_c^+ decaying to the pK^-\\pi^+ final state, we have observed, in the hadroproduction experiment E791 at Fermilab, 143 \\pm 20 \\Sigma_c^0 and 122 \\pm 18 \\Sigma_c^{++} through their decays to \\Lambda_c^+ \\pi^{\\pm}. The mass difference M(\\Sigma_c^0) - M(\\Lambda_c^+) is measured to be (167.38\\pm 0.29\\pm 0.15)\\,\\mbox{MeV}; for M(\\Sigma_c^{++}) - M(\\Lambda_c^+), we find (167.76\\pm 0.29\\pm0.15)\\,\\mbox{MeV}. The rate of \\Lambda_c^+ production from decays of the \\Sigma_c triplet is (22\\pm 2\\pm 3)\\,\\mbox{\\%} of the total \\Lambda_c^+ production assuming equal rate of production from all three, as measured for \\Sigma_c^0 and \\Sigma_c^{++}. We do not observe a statistically significant \\Sigma_c baryon-antibaryon production asymmetry. The x_F and p_t^2 spectra of \\Lambda_c^+ from \\Sigma_c decays are observed to be similar to those for all \\Lambda_c^+'s produced.""]",['1996-05-02']
2366,['eng'],"['Ellison, J']",['Electroweak physics results from the DZero detector at Fermilab'],['Particle Physics - Experimental Results'],"['talk, Zvenigorod 1995/09/20', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'gauge boson, pair production', 'pair production, gauge boson', 'intermediate boson, leptonic decay', 'leptonic decay, intermediate boson', 'Z0, hadronic decay', 'hadronic decay, Z0', 'channel cross section, branching ratio', 'W, width', 'coupling, (3gauge boson)', '(3gauge boson), coupling', 'electroweak interaction, validity test', 'validity test, electroweak interaction', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W+ anything', 'anti-p p --> Z0 anything', 'anti-p p --> Z0 photon anything', 'anti-p p --> W photon anything', 'anti-p p --> W+ W- anything', 'anti-p p --> Z0 W anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604001'],"[""We present electroweak physics results from the DZero experiment using data from collisions at \\sqrt{s} = 1.8 TeV, concentrating on single W and Z production cross sections and the production of electroweak gauge boson pairs. The inclusive cross sections times branching ratios for W and Z production have been measured and are used to determine the inclusive width of the W boson. Direct tests of the WW\\gamma and WWZ trilinear gauge boson couplings are derived from the study of diboson production. These measurements test the non-abelian self couplings of the W, Z and photon, one of the most direct consequences of the SU(2)_L \\times U(1)_Y gauge symmetry. We present measurements of the WW\\gamma coupling based on p pbar --> l \\nu \\gamma + X and limits on anomalous WWZ and WW\\gamma couplings based on searches for p \\pbar --> W^+ W^- + X --> l l' \\nu \\nubar + X and p \\pbar --> WW / WZ + X --> e \\nu + jets + X. We also present limits on the ZZ\\gamma and Z\\gamma\\gamma couplings based on p pbar --> l^+ l^- \\gamma + X events.""]",['1996-04-04']
2367,['eng'],"['Bernardi, G']",['Structure function measurement at HERA'],['Particle Physics - Experimental Results'],"['talk, Protvino 1995/06/26', 'electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'p, structure function', 'structure function, small-x', 'dependence, momentum transfer', 'x-dependence', 'quantum chromodynamics, perturbation theory', 'gluon, momentum spectrum', 'cross section, energy dependence', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603008'],"['Preliminary results on a measurement of the proton structure function F_2 are reported for momentum transfers squared Q^2 between 1.5~GeV^2 and 5000 GeV^2 and for Bjorken x between 5.10^{-5} and 0.32 using data collected by the HERA experiments H1 and ZEUS in 1994. F_2 increases significantly with decreasing x, even in the lowest reachable Q^2 region. The data are well described by a Next to Leading Order QCD fit, and support within the present precision that the rise at low x within this Q^2 range is generated ""radiatively"" via the DGLAP evolution equations. Prospects for future structure function measurements at HERA are briefly mentioned.']",['1996-03-28']
2368,['eng'],"['Aïd, S']",['Measurement of the Q$^{2}$ dependence of the charged and neutral current cross sections in e$^{\\pm}$p scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'positron p, colliding beams', 'colliding beams, positron p', 'hadron, electroproduction', 'electroproduction, hadron', 'charged current', 'neutral current', 'differential cross section, momentum transfer', 'momentum transfer, differential cross section', 'channel cross section, ratio', 'W, mass', 'mass, W', 'electroweak interaction, validity test', 'validity test, electroweak interaction', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603009'],['The Q^{2} dependence and the total cross sections for charged and neutral current processes are measured in e^{\\pm}p reactions for transverse momenta of the outgoing lepton larger than 25 GeV. Comparable size of cross sections for the neutral current process and for the weak charged current process are observed above Q^2~\\approx~5000~GeV^2 . Using the shape and magnitude of the charged current cross section we determine a propagator mass of m_{W} = 84\\ ^{+10}_{-7} GeV.'],['1996-04-02']
2369,['eng'],"['Saxon, D H']",['Particle physics in international collaboration'],['Particle Physics - Experimental Results'],"['talk, Aachen 1995/10', 'particle physics, history', 'particle physics, sociology']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603007'],"['Particle Physics in International Collaboration. Talk given at Kolloquiumstag ``125 Jahre Teilchenphysik in Aachen"", October 1995']",['1996-03-27']
2370,['eng'],"['Abachi, S']",['The isolated photon cross section in the central and forward rapidity regions in p-$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'rapidity, central region', 'photon, direct production', 'direct production, photon', 'photon, transverse energy', 'differential cross section, transverse energy', 'transverse energy, differential cross section', 'rapidity dependence', 'quantum chromodynamics, validity test', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603006'],"['A measurement of the cross section for production of single, isolated photons is reported for transverse energies in the range of 10-125 GeV, for two regions of pseudorapidity, |\\eta|<0.9 and 1.6<|\\eta|<2.5. The data represent 12.9 pb-1 of integrated luminosity accumulated in p-pbar collisions at sqrt{s} = 1.8 TeV and recorded with the D0 detector at the Fermilab Tevatron Collider.']",['1996-04-01']
2371,['eng'],"['Aïd, S']",['Elastic and inelastic photoproduction of J/$\\psi$ mesons at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, inclusive reaction', 'photon p, inelastic scattering', 'inelastic scattering, photon p', 'J/psi(3100), photoproduction', 'photoproduction, J/psi(3100)', 'psi(3685), photoproduction', 'photoproduction, psi(3685)', 'diffraction', 'p, dissociation', 'psi mesons, leptonic decay', 'leptonic decay, psi mesons', 'mass spectrum, dimuon', 'dimuon, mass spectrum', 'channel cross section, energy dependence', 'transverse momentum, spectra', 'spectra, transverse momentum', 'angular distribution', 'quantum chromodynamics, perturbation theory', 'exchange, pomeron', 'pomeron, exchange', 'color, singlet', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', 'positron p --> J/psi(3100) positron anything', 'positron p --> psi(3685) positron anything', 'psi mesons --> muon+ muon-', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603005'],"['Results on \\jpsi\\ production in e p interactionsin the H1 experiment at HERA are presented. The \\jpsi\\ mesons are produced by almost real photons (Q^2\\approx 0) and detected via their leptonic decays. The data have been taken in 1994 and correspond to an integrated luminosity of 2.7\\,\\mbox{pb}^{-1}. The \\gamma p cross section for elastic \\jpsi\\ production is observed to increase strongly with the \\cm\\ energy. The cross section for diffractive J/\\psi production with proton dissociation is found to be of similar magnitude as the elastic cross section. Distributions of transverse momentum and decay angle are studied and found to be in accord with a diffractive production mechanism. For inelastic \\jpsi\\ production the total \\gamma p cross section, the distribution of transverse momenta, and the elasticity of the \\jpsi\\ are compared to NLO QCD calculations in a colour singlet model and agreement is found. Diffractive \\psiprime\\ production has been observed and a first estimate of the ratio to \\jpsi\\ production in the HERA energy regime is given.']",['1996-05-02']
2372,['eng'],"['Aïd, S']","['A measurement and QCD analysis of the proton structure function F$_{2}$(x,Q$^{2}$) at HERA']",['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'photon, emission', 'emission, photon', 'p, structure function', 'structure function, small-x', 'dependence, momentum transfer', 'x-dependence', 'momentum transfer, low', 'quantum chromodynamics, perturbation theory', 'gluon, momentum spectrum', 'Altarelli-Parisi equation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'tables', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603004'],"['A new measurement of the proton structure function F_2(x,Q^2) is reported for momentum transfers squared Q^2 between 1.5~GeV^2 and 5000~GeV^2 and for Bjorken x between 3\\cdot 10^{-5} and 0.32 using data collected by the HERA experiment H1 in 1994. The data represent an increase in statistics by a factor of ten with respect to the analysis of the 1993 data. Substantial extension of the kinematic range towards low Q^2 and x has been achieved using dedicated data samples and events with initial state photon radiation. The structure function is found to increase significantly with decreasing x, even in the lowest accessible Q^2 region. The data are well described by a Next to Leading Order QCD fit and the gluon density is extracted.']",['1996-04-01']
2373,['eng'],"['Albuquerque, I F M']",['A search for light super symmetric baryons'],['Particle Physics - Experimental Results'],"['p nucleus, inclusive reaction', 'copper', 'hyperon, secondary beam', 'secondary beam, hyperon', 'new particle, search for', 'baryon, supersymmetry', 'bound state, (3quark gluino)', 'baryon, hadronic decay', 'hadronic decay, baryon', 'mass difference', 'production, upper limit', 'upper limit, production', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '800 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9604002'],"['We have searched for the production and decay of light super-symmetric baryons produced in 800 GeV/c proton copper interactions in a charged hyperon beam experiment. We observe no evidence for the decays R+(uud \\g^~) -> S(uds \\g^~) pi+ and X-(ssd \\g^~) -> S(uds \\g^~) pi- in the predicted parent mass and lifetime ranges of 1700-2500 Mev/c2 and 50-500 ps. Production upper limits for R+ at xF=0.47, Pt=1.4 GeV/c2 and X- at xF=0.48, Pt=0.65 GeV/c2 of less than 10^-3 of all charged secondary particles produced are obtained for all but the highest masses and shortest lifetimes predicted.']",['1996-04-09']
2374,['eng'],"['Kroll, I J']",['Masses and lifetimes of B hadrons'],['Particle Physics - Experimental Results'],"['review, Beijing 1995/08/10', 'electron positron, colliding beams', 'colliding beams, electron positron', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'beautiful particle, electroproduction', 'electroproduction, beautiful particle', 'beautiful particle, hadroproduction', 'hadroproduction, beautiful particle', 'beautiful particle, mass', 'mass, beautiful particle', 'beautiful particle, lifetime', 'beautiful particle, hadronic decay', 'hadronic decay, beautiful particle', 'beautiful particle, semileptonic decay', 'semileptonic decay, beautiful particle', 'B0', 'B/s0', 'B-', 'Lambda/b0', 'search for, B/c', 'B*(5320)', 'B, excited state', 'B/s, excited state', 'Sigma/b, excited state', 'lifetime, ratio', 'particle identification, beauty', 'experimental results', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602005'],"['The latest measurements of the masses and lifetimes of weakly decaying B~hadrons from experiments at e^+e^- and p\\bar{p} colliders are presented. These measurements include the lifetimes of the \\bar{B}^0, \\bar{B}^0_s, B^-, and b~baryons, as well as searches for the B_c~meson. The observation of B^*, p-wave B~mesons (B^{**}), and excited b~baryons using inclusive and exclusive B~hadron reconstruction are discussed. Results on b~quark flavour tagging are given. The latest measurements of the masses and lifetimes of weakly decaying B~hadrons from experiments at e^+e^- and p\\bar{p} colliders are presented. These measurements include the lifetimes of the \\bar{B}^0, \\bar{B}^0_s, B^-, and b~baryons, as well as searches for the B_c~meson. The observation of B^*, p-wave B~mesons (B^{**}), and excited b~baryons using inclusive and exclusive B~hadron reconstruction are discussed. Results on b~quark flavour tagging are given.']",['1996-02-15']
2375,['eng'],"['Abe, F']",['Properties of jets in Z boson events from 1.8 TeV $\\overline{p}$p collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'Z0, hadroproduction', 'hadroproduction, Z0', 'jet, associated production', 'associated production, jet', 'jet, multiplicity', 'Z0, leptonic decay', 'leptonic decay, Z0', 'quantum chromodynamics, perturbation theory', 'gluon, radiation', 'cross section, multiplicity', 'energy spectrum, transverse energy', 'transverse energy, energy spectrum', 'angular distribution', 'angular correlation, (2jet)', 'track data analysis, vertex', 'quark, beauty', 'quark, decay', 'decay, quark', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> Z0 (n)jet anything', 'Z0 --> positron electron', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603003'],['We present a study of events with Z bosons and hadronic jets produced in \\overline{p}p collisions at a center-of-mass energy of 1.8 TeV. The data consist of 6708 Z \\rightarrow e^+e^- decays from 106 pb^{-1} of integrated luminosity collected using the CDF detector at the Tevatron Collider. The Z + \\ge n jet cross sections and jet production properties have been measured for n = 1 to 4. The data compare well to predictions of leading order QCD matrix element calculations with added gluon radiation and simulated parton fragmentation.'],['1996-03-11']
2376,['eng'],"['Bianco, S']",['Charm lifetimes and semileptonic decays'],['Particle Physics - Experimental Results'],"['review, Brussels 1995/07/27', 'charmed particle, lifetime', 'charmed particle, semileptonic decay', 'semileptonic decay, charmed particle', 'charmed particle, branching ratio', 'D', 'D/s', 'Lambda/c+', 'Xi/c0', 'Xi/c+', 'Omega/c0', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602008'],"['This paper gives an experimental overview of current status and open questions on charm lifetimes and semileptonic decays, the latter including new results presented by E687 and CLEO at this Conference.']",['1996-02-28']
2377,['eng'],"['Aïd, S']",['Elastic electroproduction of $\\varrho$ and J/$\\psi$ mesons at large Q$^{2}$ at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, exclusive reaction', 'rho(770)0, electroproduction', 'electroproduction, rho(770)0', 'J/psi(3100), electroproduction', 'electroproduction, J/psi(3100)', 'diffraction, elastic scattering', 'elastic scattering, diffraction', 'vector dominance', 'momentum transfer, slope', 'cross section', 'decay, angular distribution', 'angular distribution, decay', 'rho(770)0, polarization', 'polarization, rho(770)0', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', '300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602007'],"['The total cross sections for the elastic electroproduction of \\rh0 and J/\\Psi mesons for Q^2 > 8 GeV^2 and \\langle W \\rangle \\simeq 90 GeV/c^2 are measured at HERA with the H1 detector. The measurements are for an integrated electron-proton luminosity of \\simeq~3~pb^{-1}. The dependences of the total virtual photon-proton (\\gamma^* p) cross sections on Q^2, W and the momentum transfer squared to the proton (t), and, for the \\rho, the dependence on the polar decay angle (\\cos \\theta^*), are presented. The J/\\Psi : \\rh0 cross section ratio is determined. The results are discussed in the light of theoretical models and of the interplay of hard and soft physics processes.']",['1996-04-01']
2378,['eng'],"['Abramowicz, H', 'Horn, D', 'Naftaly, U', 'Sahar-Pikielny, C']",['An orientation selective neural network and its application to cosmic muon identification'],['Detectors and Experimental Techniques'],"['calorimeter', 'uranium', 'scintillation counter', 'neural network', 'muon, cosmic radiation', 'numerical calculations', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602006'],"['We propose a novel method for identification of a linear pattern of pixels on a two-dimensional grid. Following principles employed by the visual cortex, we employ orientation selective neurons in a neural network which performs this task. The method is then applied to a sample of data collected with the ZEUS detector at HERA in order to identify cosmic muons which leave a linear pattern of signals in the segmented uranium-scintillator calorimeter. A two dimensional representation of the relevant part of the detector is used. The results compared with a visual scan point to a very satisfactory cosmic muon identification. The algorithm performs well in the presence of noise and pixels with limited efficiency. Given its architecture, this system becomes a good candidate for fast pattern recognition in parallel processing devices.']",['1996-02-16']
2379,['eng'],"['Hamel, L A', 'Lessard, L', 'Zacek, V', 'Sur, B']",['Dark matter search with moderately superheated liquids'],['Particle Physics - Experimental Results'],"['talk, Rome 1995/11/13', 'astrophysics, missing-mass', 'missing-mass, astrophysics', 'sparticle, search for', 'sparticle, neutral particle', 'postulated particle, WIMP', 'scattering, sparticle nucleus', 'sparticle nucleus, scattering', 'recoil, energy spectrum', 'energy spectrum, recoil', 'counters and detectors, droplet', 'production, bubble', 'bubble, production', 'performance', 'background', 'experimental methods, proposed', 'proposed, experimental methods']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602004'],"['We suggest the use of moderately superheated liquids in the form of superheated droplet detectors for a new type of neutralino search experiment. The advantage of this method for Dark Matter detection is, that the detector material is cheap, readily available and that it is easily possible to fabricate a large mass detector. Moreover the detector can be made ""background blind"", i.e. exclusively sensitive to nuclear recoils.']",['1996-02-15']
2380,['eng'],"['Derrick, Malcolm']",['Measurement of the diffractive cross section in deep inelastic scattering'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'photon p, interaction', 'interaction, photon p', 'diffraction', 'cross section, energy dependence', 'mass, dependence', 'dependence, mass', 'parametrization', 'background, nondiffractive', 'model, pomeron', 'p, structure function', 'structure function, diffraction', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602010'],"['Diffractive scattering of \\gamma^* p \\to X + N, where N is either a proton or a nucleonic system with M_N~<~4~GeV has been measured in deep inelastic scattering (DIS) at HERA. The cross section was determined by a novel method as a function of the \\gamma^* p c.m. energy W between 60 and 245~GeV and of the mass M_X of the system X up to 15~GeV at average Q^2 values of 14 and 31~GeV^2. The diffractive cross section d\\sigma^{diff} /dM_X is, within errors, found to rise linearly with W. Parameterizing the W dependence by the form d\\sigma^{diff}/dM_X \\propto (W^2)^{(2\\overline{\\mbox{\\alpha_{_{I\\hspace{-0.2em}P}}}} -2)} the DIS data yield for the pomeron trajectory \\overline{\\mbox{\\alpha_{_{I\\hspace{-0.2em}P}}}} = 1.23 \\pm 0.02(stat) \\pm 0.04 (syst) averaged over t in the measured kinematic range assuming the longitudinal photon contribution to be zero. This value for the pomeron trajectory is substantially larger than \\overline{\\mbox{\\alpha_{_{I\\hspace{-0.2em}P}}}} extracted from soft interactions. The value of \\overline{\\mbox{\\alpha_{_{I\\hspace{-0.2em}P}}}} measured in this analysis suggests that a substantial part of the diffractive DIS cross section originates from processes which can be described by perturbative QCD. From the measured diffractive cross sections the diffractive structure function of the proton F^{D(3)}_2(\\beta,Q^2, \\mbox{x_{_{I\\hspace{-0.2em}P}}}) has been determined, where \\beta is the momentum fraction of the struck quark in the pomeron. The form F^{D(3)}_2 = constant \\cdot (1/ \\mbox{x_{_{I\\hspace{-0.2em}P}}})^a gives a good fit to the data in all \\beta and Q^2 intervals with a = 1.46 \\pm 0.04 (stat) \\pm']",['1996-04-01']
2381,['eng'],"['Abe, F']",['Search for chargino-neutralino production in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'sparticle, pair production', 'pair production, sparticle', 'sparticle, charged particle', 'sparticle, neutral particle', 'sparticle, leptonic decay', 'leptonic decay, sparticle', 'final state, (3lepton)', '(3lepton), final state', 'supersymmetry', 'channel cross section, branching ratio', 'upper limit', 'sparticle, mass', 'mass, sparticle', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603001'],"['We have searched for chargino-neutralino production (\\chichi) in 1.8 TeV \\ppb\\sp collisions, followed by their leptonic decays \\chione\\dk\\chizero\\lnu\\psp and \\chitwo\\dk\\chizero\\lplm. These trilepton events are expected within a framework of the Minimal Supersymmetric Standard Model (MSSM). In a 19.1 pb^{-1} data sample collected with the Collider Detector at Fermilab, no trilepton events were observed. Upper limits on \\sigma(\\ppb\\dk\\chichi)\\cdot BR(\\chichi\\dk 3 \\ell + X) were obtained for various MSSM parameter space regions, yielding new 95\\% confidence level lower limits for the neutralino (\\chitwo) mass which extended as high as 49 \\mgev.']",['1996-03-05']
2382,['eng'],"['Afanasiev, A M', 'Glamazdin, A V']",['Atomic electron motion for Møller polarimetry in a double-arm mode'],['Particle Physics - Experimental Results'],"['electron, polarized beam', 'polarized beam, electron', 'beam monitoring, polarization', 'polarization, beam monitoring', 'electron electron, elastic scattering', 'elastic scattering, electron electron', 'cross section, asymmetry', 'correction, binding energy', 'atom, binding energy', 'Newport News CEBAF Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602002'],"['We analyse an effect of electron Fermi motion at atomic shells on the accuracy of electron beam polarization measurements with a M\\""oller polarimeter operating in a double--arm mode. It is demonstrated that the effect can result in either {\\it increase} or {\\it decrease} of the measured polarization depending on the detector positions. The effect is simulated for the M\\""oller polarimeter to be installed at CEBAF Hall A.']",['1996-02-07']
2383,['eng'],"['Aïd, S']",['Energy flow in the hadronic final state of diffractive and non-diffractive deep-inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'hadron, electroproduction', 'electroproduction, hadron', 'hadron, multiple production', 'multiple production, hadron', 'transverse energy, energy flow', 'diffraction', 'nondiffractive', 'model, interaction', 'interaction, model', 'model, pomeron', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602001'],"['An investigation of the hadronic final state in diffractive and non--diffractive deep--inelastic electron--proton scattering at HERA is presented, where diffractive data are selected experimentally by demanding a large gap in pseudo --rapidity around the proton remnant direction. The transverse energy flow in the hadronic final state is evaluated using a set of estimators which quantify topological properties. Using available Monte Carlo QCD calculations, it is demonstrated that the final state in diffractive DIS exhibits the features expected if the interaction is interpreted as the scattering of an electron off a current quark with associated effects of perturbative QCD. A model in which deep--inelastic diffraction is taken to be the exchange of a pomeron with partonic structure is found to reproduce the measurements well. Models for deep--inelastic ep scattering, in which a sizeable diffractive contribution is present because of non--perturbative effects in the production of the hadronic final state, reproduce the general tendencies of the data but in all give a worse description.']",['1996-02-13']
2384,['eng'],"['Derrick, Malcolm']",['Measurement of elastic $\\phi$ photoproduction at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'photon p, exclusive reaction', 'Phi(1020), photoproduction', 'photoproduction, Phi(1020)', 'Phi(1020), hadronic decay', 'hadronic decay, Phi(1020)', 'mass spectrum, (K+ K-)', '(K+ K-), mass spectrum', 'differential cross section, momentum transfer', 'momentum transfer, differential cross section', 'differential cross section, slope', 'slope, differential cross section', 'channel cross section', 'energy dependence', 'angular distribution', 'spin, density matrix', 'density matrix, spin', 'helicity, conservation law', 'diffraction', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'photon p --> Phi(1020) p', 'Phi(1020) --> K+ K-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601009'],"['The production of \\phi mesons in the reaction e^{+}p \\rightarrow e^{+} \\phi p (\\phi \\rightarrow K^{+}K^{-}) at a median Q^{2} of 10^{-4} \\ \\rm{GeV^2} has been studied with the ZEUS detector at HERA. The differential \\phi photoproduction cross section d\\sigma/dt has an exponential shape and has been determined in the kinematic range 0.1<|t|<0.5 \\ \\rm{GeV^2} and 60 < W < 80 \\ \\rm{GeV}. An integrated cross section of \\sigma_{\\gamma p \\rightarrow \\phi p} = 0.96 \\pm 0.19^{+0.21}_{-0.18} \\rm{\\mu b} has been obtained by extrapolating to {\\it t} = 0. When compared to lower energy data, the results show a weak energy dependence of both \\sigma_{\\gamma p \\rightarrow \\phi p} and the slope of the t distribution. The \\phi decay angular distributions are consistent with s-channel helicity conservation. From lower energies to HERA energies, the features of \\phi photoproduction are compatible with those of a soft diffractive process.']",['1996-02-02']
2385,['eng'],"['Abe, F']",['Inclusive jet cross section in $\\overline{p}$p collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'sparticle, pair production', 'pair production, sparticle', 'neutralino', 'chargino', 'sparticle, leptonic decay', 'leptonic decay, sparticle', 'final state, (3lepton)', '(3lepton), final state', 'supersymmetry', 'channel cross section, branching ratio', 'upper limit', 'sparticle, mass', 'mass, sparticle', 'lower limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601008'],"['The inclusive jet differential cross section has been measured for jet transverse energies, E_T, from 15 to 440 GeV, in the pseudorapidity region 0.1\\leq | \\eta| \\leq 0.7. The results are based on 19.5 pb^{-1} of data collected by the CDF collaboration at the Fermilab Tevatron collider. The data are compared with QCD predictions for various sets of parton distribution functions. The cross section for jets with E_T>200\\ GeV is significantly higher than current predictions based on O(\\alpha_s^3) perturbative QCD calculations. Various possible explanations for the high-E_T\\ excess are discussed.']",['1996-02-02']
2386,['eng'],"['Abe, K']",['Factorial and Cumulant Moments in $e^{+}e^{-} \\to$ Hadrons at the $Z^{0}$ Resonance'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'hadron, multiple production', 'multiple production, hadron', 'charged particle, multiplicity', 'multiplicity, moment', 'correlation', 'quantum chromodynamics, perturbation theory', 'statistical analysis', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601010'],"['We present the first experimental study of the ratio of cumulant to factorial moments of the charged-particle multiplicity distribution in high-energy particle interactions, using hadronic Z^0 decays collected by the SLD experiment at SLAC. We find that this ratio, as a function of the moment-rank q, decreases sharply to a negative minimum at q=5, which is followed by quasi-oscillations. These features are insensitive to experimental systematic effects and are in qualitative agreement with expectations from next-to-next-to-leadin g-order perturbative QCD.']",['1996-02-13']
2387,['eng'],"['Gounder, K', 'Cremaldi, L']",['$D-\\pi$ Production Correlations in 500 GeV $\\pi-N$ Interactions'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/11', 'pi- nucleon, inclusive reaction', 'charmed meson, hadroproduction', 'pi, associated production', 'charge correlation, (D pi)', 'D, hadronic decay', 'D*(2010), hadronic decay', 'effect, fragmentation', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> charmed meson pi anything', 'D0 --> K- pi+', 'D+ --> K- 2pi+', 'D*(2010) --> D0 pi+', '500 GeV']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0008061'],"['We study the charge correlations between charm mesons produced in 500 GeV pi- N interactions and the charged pions produced closest to them in phase space. With 110,000 fully reconstructed D mesons from experiment E791 at Fermilab, the correlations are studied as functions of the D-pi - D mass difference and of Feynman x. We observe significant correlations which appear to originate from a combination of sources including fragmentation dynamics, resonant decays, and charge of the beam.']",['2000-08-25']
2388,['eng'],"['Awes, T C']",['Azimuthal correlations in the target fragmentation region of high energy nuclear collisions'],['Particle Physics - Experimental Results'],"['p nucleus, nuclear reaction', 'nucleus nucleus, nuclear reaction', 'oxygen', 'silicon', 'gold', 'target, fragmentation', 'fragmentation, target', 'hadron, multiple production', 'multiple production, hadron', 'yield, (deuteron p pi)', 'angular correlation', 'rapidity spectrum', 'dependence, mass number', 'mass number, dependence', 'dependence, impact parameter', 'correlation function', 'pi, multiple scattering', 'multiple scattering, pi', 'pi, absorption', 'absorption, pi', 'experimental results', 'Berkeley Bevalac', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601007'],"[""Results on the target mass dependence of proton and pion pseudorapidity distributions and of their azimuthal correlations in the target rapidity range -1.73 \\le \\eta \\le 1.32 are presented. The data have been taken with the Plastic-Ball detector set-up for 4.9~GeV p\\,+\\,Au collisions at the Berkeley BEVALAC and for 200 A\\cdotGeV/c p-, O-, and S-induced reactions on different nuclei at the CERN-SPS. The yield of protons at backward rapidities is found to be proportional to the target mass. Although protons show a typical ``back-to-back'' correlations, a ``side-by-side'' correlation is observed for positive pions, which increases both with target mass and with impact parameter of a collision. The data can consistently be described by assuming strong rescattering phenomena including pion absorption effects in the entire excited target nucleus.""]",['1996-01-26']
2389,['eng'],"['Summers, D', 'Bracker, S', 'Gounder, K', 'Hendrix, K']",['An Efficient Multiprocessor Management System for Event-Parallel Computing'],['Particle Physics - Experimental Results'],"['talk, Minneapolis 1996/08/11', 'data management', 'computer, vector', 'microprocessor, multiprocessor', 'performance', 'Batavia TEVATRON PS']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007003'],"[""Performance of software using TCP/IP sockets to distribute events to UNIX workstations is described. This simple software was written at the University of Mississippi to control UMiss farm reconstruction of 8 billion raw events, part of Fermilab E791's data. E791 reconstructed HEP's largest data set to study charm physics.""]",['2000-07-04']
2390,['eng'],"['Heinson, A P']",['Top quark physics at the DZero experiment'],['Particle Physics - Experimental Results'],"['talk, Zvenigorod 1995/09/19', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'mass, truth', 'truth, mass', 'channel cross section', 'quark, decay', 'decay, quark', 'final state, dilepton', 'dilepton, final state', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'final state, ((n)jet)', '((n)jet), final state', 'mass difference, (truth W)', '(truth W), mass difference', 'transverse energy, missing-energy', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601006'],"['In this paper I present the latest results on top quark physics from the DZero collaboration since the discovery of the top quark in March 1995. I summarize the discovery results, discuss progress since the discovery, and show how we can measure the top quark mass using three separate techniques. The measurements were made at the Fermilab Tevatron, a ppbar collider with sqrt(s) = 1.8 TeV, using 50 pb^-1 data collected from 1992 to early 1995.']",['1996-01-18']
2391,['eng'],"['Doyle, A T']",['Diffraction at HERA'],['Particle Physics - Experimental Results'],"['talk, Durham 1995/09/18', 'electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'photon pi, interaction', 'interaction, photon pi', 'diffraction', 'rapidity, gap', 'vector meson, photoproduction', 'photoproduction, vector meson', 'channel cross section, energy dependence', 'structure function, x-dependence', 'structure function, momentum transfer', 'jet, photoproduction', 'photoproduction, jet', 'model, pomeron', 'cross section, rapidity dependence', 'background', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601005'],"['Measurements of diffractive phenomena observed at HERA are reviewed. A short introduction to the theoretical background is presented. The review focuses on the current experimental directions and discusses the exclusive production of vector mesons, the deep inelastic structure of diffraction and complementary information from jet structures. Emphasis is placed on the current sources of background and the experimental uncertainties.']",['1996-01-17']
2392,['eng'],"['Aïd, S']",['Elastic photoproduction of $\\varrho^{0}$ mesons at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, exclusive reaction', 'rho(770)0, photoproduction', 'photoproduction, rho(770)0', 'channel cross section, energy dependence', 'differential cross section, momentum transfer', 'momentum transfer, differential cross section', 'differential cross section, slope', 'slope, differential cross section', 'angular distribution', 'helicity, conservation law', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'photon p --> p rho(770)0', 'rho(770)0 --> pi+ pi-', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601004'],"['The cross section for the elastic photoproduction of \\r0\\ mesons (\\gamma p \\rightarrow \\rho^0 p) has been measured with the H1 detector at HERA for two average photon-proton centre-of-mass energies of 55 and 187~GeV. TheFcenterline lower energy point was measured by observing directly the \\rho^{0} decay giving a cross section of 9.1\\pm 0.9\\,(\\stat)\\pm 2.5\\,(\\syst)\\;\\mub. The logarithmic slope parameter of the differential cross section, {\\rm d}\\sigma/{\\rm d}t is found to be 10.9 \\pm 2.4\\,(\\stat) \\pm 1.1\\,(\\syst)\\;GeV^{-2}. The \\r0\\ decay polar angular distribution is found to be consistent with s-channel helicity conservation. The higher energy cross section was determined from analysis of the lower part of the hadronic invariant mass spectrum of diffractive photoproduction and found to be 13.6\\pm 0.8\\,(\\stat)\\pm 2.4\\,(\\syst)\\;\\mub.']",['1996-01-18']
2393,['eng'],"['Jain, V']",['Recent results from CLEO on charm and bottom hadrons'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Upsilon(10570), electroproduction', 'electroproduction, Upsilon(10570)', 'B, pair production', 'pair production, B', 'B, decay modes', 'decay modes, B', 'B, branching ratio', 'rho(770)', 'eta(958)', 'charmed meson, production', 'production, charmed meson', 'quarkonium, charm', 'Lambda/c+', 'Xi/c0', 'quark, beauty', 'quark, decay modes', 'decay modes, quark', 'D/s*(2110), hadronic decay', 'hadronic decay, D/s*(2110)', 'isospin, violation', 'violation, isospin', 'D/s, semileptonic decay', 'semileptonic decay, D/s', 'eta(958)', 'correlation, (Lambda/c+ lepton)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'beauty --> 2charm strangeness', 'beauty --> charm up down', 'beauty --> charm lepton neutrino', 'B --> charmed particle anything', 'B --> quarkonium anything', 'D/s*(2110) --> D/s pi0', 'D/s --> eta lepton neutrino', 'D/s --> eta(958) lepton neutrino', 'B0 --> pi+ lepton- neutrino', 'B0 --> rho(770)+ lepton neutrino', 'approx. 10.58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601002'],"['In this talk, I present new results from CLEO on charm and bottom hadrons. Most of the talk will be on the issue of the B semileptonic branching fraction, its connection to the number of charm quarks produced in the decay of a b quark, and the rate for the b -> ccbars transition']",['1996-01-12']
2394,['eng'],"['Abe, F']",['Search for charged Higgs decays of the top quark using hadronic $\\tau$ decays'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'Higgs particle, production', 'production, Higgs particle', 'Higgs particle, charged particle', 'Higgs particle, leptonic decay', 'leptonic decay, Higgs particle', 'tau, semileptonic decay', 'semileptonic decay, tau', 'charged particle, multiplicity', 'transverse energy, missing-energy', 'mass, truth', 'truth, mass', 'Higgs particle, mass', 'mass, Higgs particle', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'truth --> Higgs particle beauty', 'Higgs particle --> tau neutrino/tau', 'tau --> (n)hadron neutrino/tau', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601003'],"['We present the result of a search for charged Higgs decays of the top quark, produced in p\\bar{p} collisions at \\surd s = 1.8~TeV. When the charged Higgs is heavy and decays to a tau lepton, which subsequently decays hadronically, the resulting events have a unique signature: large missing transverse energy and the low-charged-multiplicity tau. Data collected in the period 1992-1993 at the Collider Detector at Fermilab, corresponding to 18.7\\pm0.7~pb^{-1}, exclude new regions of combined top quark and charged Higgs mass, in extensions to the standard model with two Higgs doublets.']",['1996-01-17']
2395,['eng'],"['Belz, J E']",['Search for the weak decay of an H dibaryon'],['Particle Physics - Experimental Results'],"['p nucleus, interaction', 'interaction, p nucleus', 'copper', 'neutral particle, secondary beam', 'secondary beam, neutral particle', 'diffraction, dissociation', 'postulated particle, H baryon', 'H baryon, hadroproduction', 'hadroproduction, H baryon', 'baryon resonance, dibaryon', 'dibaryon, baryon resonance', 'decay, H baryon', 'H baryon, decay', 'Lambda, hadroproduction', 'hadroproduction, Lambda', 'differential cross section, ratio', 'ratio, differential cross section', 'upper limit', 'magnetic spectrometer, experimental results', 'Brookhaven PS', 'p copper --> H baryon anything', 'H baryon --> Lambda n', 'H baryon --> Sigma0 n', 'H baryon --> Lambda photon', 'Lambda --> p pi-', '24 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9603002'],"['We have searched for a neutral H dibaryon decaying via H\\rightarrow\\Lambda n and H\\rightarrow\\Sigma^0 n. Our search has yielded two candidate events from which we set an upper limit on the H production cross section. Normalizing to the inclusive \\Lambda production cross section, we find (d\\sigma_H/d\\Omega)\\,/\\,(d\\sigma_\\Lambda/d\\Omega) < 6.3\\times 10^{-6} at 90\\% C.L., for an H of mass \\approx\\,2.15~GeV/c^2.']",['1996-03-08']
2396,['eng'],"['Aitala, E M', 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Aryal, M', 'Ashery, D', 'Astorga, J', 'Banerjee, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Carvalho, H S', 'Costa, I', 'Cremaldi, L M', 'Darling, C L', 'Denisenko, K', 'Fernández, A', 'Gagnon, P', 'Gerzon, S A', 'Göbel, C', 'Gounder, K', 'Granite, D', 'Halling, A M', 'Herrera, G', 'Hurvits, G', 'James, C', 'Kasper, P A', 'Kondakis, N', 'Kwan, S', 'Langs, D C', 'Leslie, J', 'Lichtenstadt, J', 'Lundberg, B G', 'Manacero, A', 'MayTal-Beck, S', 'Meadows, B', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', ""O'Shaughnessy, K F"", 'Peng, K C', 'Perera, L P', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Reay, N W', 'Reidy, J J', 'Reis, A C', 'Rubin, H A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A J', 'Sheaff, M', 'Sidwell, R A', 'Slaughter, A J', 'Smith, J G', 'Sokoloff, M D', 'Stanton, N R', 'Sugano, K', 'Summers, D J', 'Takach, S F', 'Thorne, K S', 'Tripathi, A K', 'Watanabe, S', 'Weiss-Babai, R', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yi, D', 'Zaliznyak, R', 'Zhang, C']",['Asymmetries between the production of D+ and D- mesons from 500 GeV/c pi- nucleon interactions as a function of x$_{F}$ and p$_{t}^{2}$'],['Particle Physics - Experimental Results'],"['pi- nucleus, inclusive reaction', 'carbon', 'platinum', 'D+, hadroproduction', 'hadroproduction, D+', 'D-, hadroproduction', 'hadroproduction, D-', 'cross section, asymmetry', 'effect, leading particle', 'x-dependence', 'transverse momentum, dependence', 'model, fragmentation', 'quantum chromodynamics, perturbation theory', 'mass spectrum, (K 2pi)', '(K 2pi), mass spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> D anything', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9601001'],"['We present asymmetries between the production of D+ and D- mesons in Fermilab experiment E791 as a function of xF and pt**2. The data used here consist of 74,000 fully-reconstructed charmed mesons produced by a 500 GeV/c pi- beam on C and Pt foils. The measurements are compared to results of models which predict differences between the production of heavy-quark mesons that have a light quark in common with the beam (leading particles) and those that do not (non-leading particles). While the default models do not agree with our data, we can reach agreement with one of them, PYTHIA, by making a limited number of changes to parameters used.']",['1996-01-05']
2397,['eng'],"['Enomoto, R']",['Observation of highly virtual photon-photon collisions to hadrons at TRISTAN'],['Particle Physics - Experimental Results'],"['photon photon, interaction', 'interaction, photon photon', 'electron positron, colliding beams', 'colliding beams, electron positron', 'hadron, photoproduction', 'photoproduction, hadron', 'cross section, hadronic', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', '58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512010'],"['We have observed highly virtual (Q^2>1.05~GeV^2) photon-photon collisions to hadronic final states at \\sqrt{s_{e^+e^-}}=58~GeV. The integrated luminosity of the data sample was 241pb^{-1}. Both scattered beam-electrons and scattered beam-positrons were detected using low-angle calorimeters (i.e., both photons were highly virtual, ``double-tag""); we obtained 115 hadronic events with an estimated background of 10.2\\pm1.1. The cross section obtained was 4.11\\pm0.66pb in the 2<W_{\\gamma \\gamma}<25 GeV and Q^2_{\\gamma, min}>2 GeV region, while the lowest order quark-parton model predicted 3.00pb.']",['1996-01-12']
2398,['eng'],"['Daoudi, M']",['Tau physics with polarized beams'],['Particle Physics - Experimental Results'],"['talk, Brussels 1995/07/27', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'polarized beam', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'tau, pair production', 'pair production, tau', 'tau, semileptonic decay', 'semileptonic decay, tau', 'tau, leptonic decay', 'leptonic decay, tau', 'tau, polarization', 'polarization, tau', 'energy spectrum, (lepton)', '(lepton), energy spectrum', 'energy spectrum, (pi)', '(pi), energy spectrum', 'Michel parameter', 'neutrino/tau, helicity', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'tau --> pi neutrino/tau', 'tau --> electron neutrino/tau antineutrino/e', 'tau --> muon neutrino/tau antineutrino/mu', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512009'],"['We present the first results on tau physics using polarized beams. These include measurements of the \\tau Michel parameters \\xi and \\xi\\delta and the \\tau neutrino helicity h_\\nu. The measurements were performed using the SLD detector at the Stanford Linear Collider (SLC). (Invited talk at the 1995 International Europhysics Conference on High Energy Physics, Brussels, Belgium, July 27 - August 2, 1995.)']",['1996-04-03']
2399,['eng'],"['De Jongh, F']",['B physics with the CDF run II upgrade'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'B, hadroproduction', 'hadroproduction, B', 'B, hadronic decay', 'hadronic decay, B', 'J/psi(3100)', 'violation, CP', 'particle identification, flavor', 'B/s0 anti-B/s0, interference', 'B, rare decay', 'rare decay, B', 'Kobayashi-Maskawa angle', 'magnetic detector, CDF', 'experimental results', 'proposed experiment', 'upgrade', 'Batavia TEVATRON Coll', 'anti-p p --> B anything', 'B0 --> J/psi(3100) K0(S)', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512008'],"['We summarize Run I results relevant to an analysis of the CP asymmetry in B\\to J/\\psi K_s, the CDF upgrade plans for Run II, and some of the main B physics goals related to the exploration of the origin of CP violation.']",['1996-04-03']
2400,['eng'],"['Abachi, S']","[""Search for right-handed W bosons and heavy W' in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV""]",['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'new particle, search for', 'W, right-handed', ""postulated particle, W'"", ""W', leptonic decay"", ""leptonic decay, W'"", 'neutrino, right-handed', 'neutrino, massive', 'massive, neutrino', 'neutrino, semileptonic decay', 'semileptonic decay, neutrino', ""mass, W'"", ""W', mass"", 'final state, (2jet 2electron)', '(2jet 2electron), final state', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', ""anti-p p --> W' anything"", ""W' --> electron neutrino"", 'neutrino --> 2jet electron', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512007'],"['We report on a search for right-handed W bosons (W_R). We used data collected with the D\\O \\ detector at the Fermilab Tevatron p\\bar p collider at \\sqrt{s}=1.8 TeV to search for W_R decays into an electron and a massive right-handed neutrino W_R^\\pm \\rightarrow e^\\pm N_R. Using the inclusive electron data, we set mass limits independent of the N_R decay: m_{W_R}>650 GeV/c^2 and m_{W_R}>720 GeV/c^2 at the 95\\% confidence level, valid for m_{N_R}<\\frac{1}{2}m_{W_R} and m_{N_R} \\ll m_{W_R} respectively. The latter also represents a new lower limit on the mass of a heavy left-handed W boson (W^\\prime) decaying into e \\nu. In addition, limits on m_{W_R} valid for larger values of the N_R mass are obtained assuming that N_R decays to an electron and two jets.']",['1996-05-02']
2401,['eng'],"['Anlauf, H', 'Dahmen, H D', 'Manakos, P', 'Ohl, T']","['UNIBAB, version 2.2']",['Particle Physics - Experimental Results'],"['electron positron, elastic scattering', 'elastic scattering, electron positron', 'scattering, wide-angle', 'wide-angle, scattering', 'radiative correction', 'photon, showers', 'programming, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512006'],['This manual describes version 2.2 of the Monte Carlo event generator UNIBAB for large angle Bhabha scattering at LEP and SLC. UNIBAB implements higher order electromagnetic radiative corrections and the effects of soft photon exponentiation in a photon shower approach. Weak corrections are included through the use of an electroweak library.'],['1995-12-18']
2402,['eng'],"['Browder, T E']",['Review of hadronic and rare B decays'],['Particle Physics - Experimental Results'],"['review, Brussels 1995/07/27', 'B, electroproduction', 'electroproduction, B', 'B, hadroproduction', 'hadroproduction, B', 'B, pair production', 'pair production, B', 'B, hadronic decay', 'hadronic decay, B', 'B, semileptonic decay', 'semileptonic decay, B', 'B, rare decay', 'rare decay, B', 'B, branching ratio', 'yield, (charmed meson)', 'yield, (psi meson)', 'correlation, (Lambda/c+ lepton)', 'correlation, (D/s lepton)', 'model, decay', 'decay, model', 'quark, beauty', 'quark, hadronic decay', 'hadronic decay, quark', 'quark, branching ratio', 'W, emission', 'emission, W', 'polarization', 'Feynman graph, higher-order', 'experimental results', 'beauty --> 2charm strangeness', 'beauty --> charm up down', 'beauty --> strangeness photon', 'beauty --> strangeness gluon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9602009'],"['We review recent results on rare and hadronic B decays from the CLEO, CDF and LEP experiments.']",['1996-02-28']
2403,['eng'],"['Franzini, P']",['CP and rare decays'],['Particle Physics - Experimental Results'],"['review, Beijing 1995/08/10', 'violation, CP', 'K0(L), hadronic decay', 'hadronic decay, K0(L)', 'K0(S), hadronic decay', 'hadronic decay, K0(S)', 'K0, rare decay', 'rare decay, K0', 'anti-K0, rare decay', 'rare decay, anti-K0', 'decay, asymmetry', 'asymmetry, decay', 'decay, amplitude analysis', 'amplitude analysis, decay', 'invariance, CPT', 'violation, CPT', 'K0(L), rare decay', 'rare decay, K0(L)', 'K0(S), rare decay', 'rare decay, K0(S)', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512005'],"['CP violation experiments, new measurements of the parameters of the neutral \\K\\ system and searches for rare decays are summarized. Perspectives for the near future are presented.']",['1995-12-08']
2404,['eng'],"['Abachi, S']",['Search for W\\Til $_{1}$ Z\\Til $_{2}$ production via trilepton final states in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, annihilation', 'annihilation, anti-p p', 'anti-p p, inclusive reaction', 'final state, (3lepton)', '(3lepton), final state', 'supersymmetry', 'postulated particle, gaugino', 'sparticle, hadroproduction', 'hadroproduction, sparticle', 'sparticle, associated production', 'associated production, sparticle', 'sparticle, decay modes', 'decay modes, sparticle', 'sparticle, branching ratio', 'upper limit', 'sparticle, mass', 'mass, sparticle', 'lepton, transverse momentum', 'transverse energy, missing-energy', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512004'],"['We have searched for associated production of the lightest chargino, \\widetilde{W}_1, and next-to-lightest neutralino, \\widetilde{Z}_2, of the Minimal Supersymmetric Standard Model in p\\bar{p}\\ collisions at \\mbox{\\sqrt{s} =\\ 1.8\\ TeV} using the \\D0 detector at the Fermilab Tevatron collider. Data corresponding to an integrated luminosity of 12.5\\pm 0.7\\ \\ipb\\ were examined for events containing three isolated leptons. No evidence for \\widetilde{W}_1\\widetilde{Z }_2\\ pair production was found. Limits on \\sigma(\\widetilde{W}_1\\widet ilde{Z}_2)Br(\\widetilde{W}_1\\rightarrow l\\nu\\widetilde{Z}_1)Br(\\wideti lde{Z}_2\\rightarrow l\\bar{l}\\widetilde{Z}_1)\\ are presented.']",['1995-12-07']
2405,['eng'],"['Piotrzkowski, K']",['Measurement of the longitudinal polarization of the HERA electron beam using crystals and the ZEUS luminosity monitor'],['Accelerators and Storage Rings'],"['talk, Aarhus 1995/07/10', 'electron p, storage ring', 'electron, polarized beam', 'polarized beam, electron', 'polarization, longitudinal', 'longitudinal, polarization', 'polarization, beam monitoring', 'beam monitoring, polarization', 'luminosity, beam monitoring', 'beam monitoring, luminosity', 'bremsstrahlung, polarization', 'polarization, bremsstrahlung', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512003'],['A measurement of the longitudinal polarization of the electron beam at HERA utilizing coherent interactions of high energy photons in crystals is proposed. Modification of existing facilities would allow an independent polarization measurement and a verification of birefringence phenomena in crystals for 20--30~GeV photons. Relevant experimental issues and systematic uncertainties are also presented.'],['1995-12-06']
2406,['eng'],"['Aïd, S']",['A search for leptoquarks at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'search for, leptoquark', 'fusion, positron quark', 'coupling, leptoquark', 'leptoquark, coupling', 'coupling, Yukawa', 'Yukawa, coupling', 'mass, leptoquark', 'leptoquark, mass', 'lower limit', 'decay, leptoquark', 'leptoquark, decay', 'final state, (quark lepton)', '(quark lepton), final state', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512001'],"['A search for leptoquarks at HERA was performed in H1 using 1994 e^+ p data corresponding to an integrated luminosity of about 3 \\pb^{-1}. Single leptoquarks were searched for in direct positron-quark fusion processes taking into account possible decays into lepton-quark pairs of either the first, the second, or the third generation. No significant deviation from the Standard Model predictions is found in the various final states studied and mass dependent exclusion limits are derived on the Yukawa couplings of the leptoquarks. Compared with earlier results from an analysis of e^-p data, exclusion limits are considerably improved for leptoquarks which could be produced via e^+-{\\it valence~quark} fusion. For leptoquarks with lepton flavour conserving couplings, masses up to 275 \\GeV (depending on the leptoquark type) are excluded for coupling values larger than \\sqrt{ 4 \\pi \\alpha_{em}}. For leptoquarks with lepton flavour violating couplings, masses up to 225 \\GeV are excluded for the first time in a direct search for couplings with leptons of the second or third generation larger than \\sqrt{ 4 \\pi \\alpha_{em}}. Fourteen possible combinations of couplings are studied and stringent exclusion limits comparable or better than any existing direct or indirect limits are obtained for each leptoquark type.']",['1995-12-06']
2407,['eng'],"['Kaplan, D M']",['Charm2000'],['Particle Physics - Phenomenology'],"['talk', 'p nucleus, inclusive reaction', 'charmed particle, hadroproduction', 'hadroproduction, charmed particle', 'D, pair production', 'pair production, D', 'D, decay modes', 'decay modes, D', 'anti-D, decay modes', 'decay modes, anti-D', 'violation, CP', 'asymmetry', 'final-state interaction', 'partial wave', 'neutral current, flavor changing', 'lepton number, violation', 'D0 anti-D0, interference', 'electroweak interaction', 'HQET model', 'validity test', 'form factor', 'Kobayashi-Maskawa angle', 'numerical calculations', 'proposed experiment, Batavia TEVATRON PS', 'bibliography', '900 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9512002'],"['I discuss the physics reach of a fixed-target charm experiment which can reconstruct >10^8 charm decays, three orders of magnitude beyond the largest extant sample. Such an experiment may run at Fermilab shortly after the Year 2000. In addition to ""programmatic"" charm physics such as spectroscopy, lifetimes, and tests of QCD, this ""Charm2000"" experiment will have significant sensitivity to new physics in the areas of CP violation, flavor-changing neutral-current and lepton-number-violating decays, and mixing, and could observe direct CP violation in Cabibbo-suppressed decays at the level predicted by the Standard Model.']",['1995-12-04']
2408,['eng'],"['Aïd, S', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Babaev, A', 'Bähr, J', 'Bán, J', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Bourov, S', 'Braemer, A', 'Brasse, F W', 'Braunschweig, W', 'Brisson, V', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Campbell, A J', 'Carli, T', 'Charles, F', 'Charlet, M', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Coutures, C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Delcourt, B', 'Del Buono, L', 'de Roeck, A', 'De Wolf, E A', 'Dixon, P', 'Di Nezza, P', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duboc, J', 'Düllmann, D', 'Dünger, O', 'Duhm, H', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Erlichmann, H', 'Eichenberger, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Evrard, E', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Forbush, M', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'González-Pineiro, B', 'Gorelov, I V', 'Goritchev, P A', 'Grab, C', 'Grässler, H', 'Grässler, R', 'Greenshaw, T J', 'Griffiths, R K', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Haack, J', 'Haidt, D', 'Hajduk, L', 'Hamon, O', 'Hampel, M', 'Hapke, M', 'Haynes, W J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hill, P', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Höppner, M', 'Horisberger, R P', 'Hudgson, V L', 'Huet, Patrick', 'Hütte, M', 'Hufnagel, H', 'Ibbotson, M', 'Itterbeck, H', 'Jabiol, M A', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Jönsson, L B', 'Johannsen, K', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Kalmus, Peter I P', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Ko, W', 'Köhler, T', 'Köhne, J H', 'Kolanoski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krämerkämper, T', 'Krasny, M W', 'Krehbiel, H', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Küster, H', 'Kuhlen, M', 'Kurca, T', 'Kurzhöfer, J', 'Kuznik, B', 'Lacour, D', 'Laforge, B', 'Lamarche, F', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Lanius, P', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindström, G', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lohmander, H', 'Lomas, J', 'López, G C', 'Lubimov, V', 'Lüke, D', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Masson, S', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Mercer, D', 'Merz, T', 'Meyer, C A', 'Meyer, H', 'Meyer, J', 'Meyer, P O', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Müller, G', 'Müller, K', 'Murín, P', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Palmen, P', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Pawletta, H', 'Peppel, E', 'Pérez, E', 'Phillips, J P', 'Pichler, C', 'Pieuchot, A', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Rabbertz, K', 'Rädel, G', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Ribarics, P', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riess, S', 'Rietz, M', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rüter, K', 'Rusakov, S V', 'Rybicki, K', 'Sahlmann, N', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'von Schlippe, W', 'Schmidt, D', 'Schmidt, G', 'Schöning, A', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schwanenberger, C', 'Sciacca, G F', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Stella, B', 'Stephens, K', 'Stier, J', 'Stiewe, J', 'Stösslein, U', 'Stolze, K', 'Strachota, J', 'Straumann, U', 'Struczinski, W', 'Sutton, J P', 'Tapprogge, Stefan', 'Chernyshov, V', 'Theissen, J', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van den Plas, D', 'Van Esch, P', 'Van Mechelen, P', 'Vartapetian, A H', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Waugh, B', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wellisch, H P', 'West, L R', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wright, A E', 'Wünsch, E', 'Wulff, N', 'Yiou, T P', 'Zácek, J', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zimmermann, W', 'Zomer, F', 'Zsembery, J', 'Zuber, K', 'Zur Nedden, M']",['Jets and energy flow in photon-proton collisions at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'transverse energy, energy flow', 'jet, electroproduction', 'electroproduction, jet', 'correlation', 'jet, event shape analysis', 'differential cross section', 'quantum chromodynamics', 'model, hard scattering', 'hard scattering, model', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511012'],"['Properties of the hadronic final state in photoproduction events with large transverse energy are studied at the electron-proton collider HERA. Distributions of the transverse energy, jets and underlying event energy are compared to \\overline{p}p data and QCD calculations. The comparisons show that the \\gamma p events can be consistently described by QCD models including -- in addition to the primary hard scattering process -- interactions between the two beam remnants. The differential jet cross sections d\\sigma/dE_T^{jet} and d\\sigma/d\\eta^{jet} are measured.']",['1995-12-01']
2409,['eng'],"['Hamacher, K', 'Weierstall, M']",['The next round of hadronic generator tuning heavily based on identified particle data'],['Particle Physics - Experimental Results'],"['review, experimental results', 'electron positron, colliding beams', 'colliding beams, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, decay modes', 'decay modes, Z0', 'hadron, electroproduction', 'electroproduction, hadron', 'event shape analysis', 'numerical calculations, Monte Carlo', 'tables', 'bibliography', 'magnetic detector, DELPHI', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511011'],"['Event shape and charged particle inclusive distributions determined from 750 000 hadronic Z events measured with the DELPHI detector at LEP are presented. The statistical and systematic precision of this data allows for a decisive confrontation with Monte Carlo models of the hadronization process and a better understanding of the structure of the Z hadronic final state. Improved tunings of the JETSET, ARIADNE and HERWIG parton shower models and the JETSET matrix element model are obtained by fitting the models to identified particle distributions from all LEP experiments and the DELPHI data presented. The description of the data distributions by the models is critically reviewed with special importance attributed to identified particles.']",['1995-11-28']
2410,['eng'],"['Derrick, Malcolm']",['Large inclusive charged particle distributions in deep inelastic scattering events at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'electron p, inclusive reaction', 'charged particle, electroproduction', 'electroproduction, charged particle', 'hadron, electroproduction', 'electroproduction, hadron', 'rapidity, gap', 'energy spectrum', 'transverse momentum, spectra', 'spectra, transverse momentum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511010'],"['A measurement of inclusive charged particle distributions in deep inelastic ep scattering for \\gamma^* p centre-of-mass energies 75< W < 175~GeV and momentum transfer squared 10< Q^2 < 160~GeV^2 from the ZEUS detector at HERA is presented. The differential charged particle rates in the \\gamma^* p centre-of-mass system as a function of the scaled longitudinal momentum, x_F, and of the transverse momentum, p_t^* and <\\!\\!p_t^{*\\,2}\\!\\!>\\,\\, , as a function of x_F, W and Q^2 are given. Separate distributions are shown for events with (LRG) and without (NRG) a rapidity gap with respect to the proton direction. The data are compared with results from experiments at lower beam energies, with the naive quark parton model and with parton models including perturbative QCD corrections. The comparison shows the importance of the higher order QCD processes. Significant differences of the inclusive charged particle rates between NRG and LRG events at the same W are observed. The value of <\\!\\!p_t^{*\\,2}\\!\\!>\\,\\, for LRG events with a hadronic mass M_X, which excludes the forward produced baryonic system, is similar to the <\\!\\!p_t^{*\\,2}\\!\\!>\\,\\, value observed in fixed target experiments at W \\approx M_X.']",['1995-11-28']
2411,['eng'],"['Abramowicz, H']",['Production of large rapidity gap events in ep interactions at HERA'],['Particle Physics - Experimental Results'],"['talk, Blois 1995/06/20', 'electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'hadron, electroproduction', 'electroproduction, hadron', 'rapidity, gap', 'diffraction, structure function', 'model, pomeron', 'jet, photoproduction', 'photoproduction, jet', 'rho(770)0, electroproduction', 'electroproduction, rho(770)0', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511007'],"['This is a short review of the properties of electron proton interactions characterized by the presence of large rapidity gaps (LRG) in the measured hadronic final state as obtained by the ZEUS Collaboration at the HERA Collider. In the deep inelastic neutral current ep interactions, the factorization properties of the LRG events interpreted as due to the diffractive dissociation of the virtual photon are compatible with expectations from the Regge phenomenology of soft interactions. The measurement of deep inelastic scattering combined with results from photoproduction of high p_T jets are successfully interpreted in terms of a factorizable Pomeron consisting of quarks and with a substantial contribution of a gluonic component. The first hints of a more complicated nature of the Pomeron are observed in the deep inelastic exclusive \\rho^o production, where a strong increase of the production cross section with energy is observed relative to the measurements of the NMC Collaboration at lower energy.']",['1995-11-17']
2412,['eng'],"['Levy, A']",['Soft interactions at high energy'],['Particle Physics - Phenomenology'],"['talk, Brussels 1995/07/27', 'hadron nucleon, interaction', 'interaction, hadron nucleon', 'photon p, interaction', 'interaction, photon p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'electron positron, inelastic scattering', 'inelastic scattering, electron positron', 'cross section, energy dependence', 'hadron, multiple production', 'multiple production, hadron', 'photon, structure function', 'gluon, momentum spectrum', 'jet, photoproduction', 'photoproduction, jet', 'jet, electroproduction', 'electroproduction, jet', 'elastic scattering', 'diffraction', 'exchange, two-photon', 'two-photon, exchange', 'rapidity, gap', 'exchange, pomeron', 'pomeron, exchange', 'structure function, pomeron', 'color, singlet', 'vector meson, photoproduction', 'photoproduction, vector meson', 'event shape analysis', 'model, fragmentation', 'multiple scattering', 'numerical calculations, interpretation of experiments', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511006'],"['Soft interactions are not easily disentangled from hard ones. In an operational definition of soft and hard processes one finds that at presently analyzed scales there is an interplay of soft and hard processes. As the scale increases, so does the amount of hard processes. So far, nothing is as soft nor as hard as we would like.']",['1995-11-14']
2413,['eng'],"['Fuster, J A', 'Martí, S']",['Charged particle production in the fragmentation of quark and gluon jets'],['Particle Physics - Experimental Results'],"['talk, Brussels 1995/07/27', 'electron positron, annihilation', 'annihilation, electron positron', 'jet, electroproduction', 'electroproduction, jet', 'final state, (3jet)', '(3jet), final state', 'quark, jet', 'gluon, jet', 'jet, fragmentation', 'charged particle, multiple production', 'multiple production, charged particle', 'multiplicity, energy dependence', 'angular distribution', 'jet, particle flow', 'fragmentation function', 'quantum chromodynamics', 'effect, string', 'effect, coherence', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511002'],"['Recent results on the total production and angular distribution of charged particles originated from the fragmentation of quark and gluon jets are presented. Experimental studies of the multiplicity as a function of the quark and gluon jet energy, the inter-jet particle flow and the individual fragmentation fucntions are reviewed and compared to expectations from QCD.']",['1996-04-03']
2414,['eng'],"['Vaca, F']",['A search for $\\lambda_{b}$ in $\\pi^{-}$ A collisions at 515 GeV/c'],['Particle Physics - Experimental Results'],"['thesis', 'pi- nucleus, inclusive reaction', 'beryllium', 'copper', 'Lambda/b0, hadroproduction', 'hadroproduction, Lambda/b0', 'Lambda/b0, hadronic decay', 'hadronic decay, Lambda/b0', 'channel cross section, branching ratio', 'upper limit', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'pi- nucleus --> Lambda/b0 anything', 'Lambda/b0 --> J/psi(3100) Lambda', 'J/psi(3100) --> muon+ muon-', 'Lambda --> p pi-', '515 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511003'],"['An extensive analysis was performed on 8.0 pb-1 of dimuon data produced in pi- - A collisions at 515 GeV/c to search for Lambda_b events in the decay channel Lambda_b --> J/psi Lambda^0, with J/psi --> mu^+ mu^- and Lambda^0 --> p pi^- (and for the conjugate reactions). The data was collected by the Fermilab fixed target experiments E672 and E706. Several cuts were applied to the Lambda^0 (and anti-Lambda^0) to make a clean Lambda^0 (and anti-Lambda^0) data sample. Among the cuts there was a K^0_s mass cut, in which if the Lambda^0 --> p pi^- (or conjugate reaction) had the mass of the K^0_s under the hypothesis of both tracks being pi^+ pi^-, the Lambda^0 (or anti-Lambda^0) candidates were rejected. The results show 2 events in the Lambda_b mass region. Using the E672/E706 measurement of the bb_bar cross-section, and considering the 2 Lambda_b event candidates as signal with zero background, an upper limit to F(Lambda_b) * Br(Lambda_b --> J/psi Lambda^0) was found to be less than 6.2x10^-2 at 90 % C. L. An upper limit was also calculate without using the K^0_s mass cut for the Lambda^0 s (and anti-Lambda^0 s), and again, requiring that the J/psi s originate from secondary vertices, giving that F(Lambda_b) * Br(Lambda_b --> J/psi Lambda^0) < 3.1x10^-2 at 90 % C. L. and F(Lambda_b) * Br(Lambda_b --> J/psi Lambda^0) < 3.2x10^-2 at 90 % C.L., respectively.']",['1996-04-03']
2415,['eng'],"['Kubota, Y']",['Measurement of the inclusive semi-electronic D$^{0}$ branching fraction'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'quark, charm', 'quark, pair production', 'pair production, quark', 'D*(2010), electroproduction', 'electroproduction, D*(2010)', 'D*(2010), hadronic decay', 'hadronic decay, D*(2010)', 'D0, semileptonic decay', 'semileptonic decay, D0', 'D0, branching ratio', 'angular correlation, (pi+ positron)', 'momentum spectrum, (positron)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> D*(2010) anything', 'D*(2010) --> D0 pi+', 'D0 --> positron neutrino/e anything', 'approx. 10 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511014'],"['Using the angular correlation between the \\pi^+ emitted in a D^{*+} \\rightarrow D^0 \\pi^+ decay and the e^+ emitted in the subsequent D^0 \\rightarrow Xe^+\\nu decay, we have measured the branching fraction for the inclusive semi-electronic decay of the D^0 meson to be: {\\cal B}(D^0 \\rightarrow X e^+ \\nu) = [6.64 \\pm 0.18 (stat.) \\pm 0.29 (syst.)] \\%. \\nonumber The result is based on 1.7 fb^{-1} of e^+e^- collisions recorded by the CLEO II detector located at the Cornell Electron Storage Ring (CESR). Combining the analysis presented in this paper with previous CLEO results we find, \\frac{{\\cal B} (D^0 \\rightarrow X e^+ \\nu)} {{\\cal B} (D^0 \\rightarrow K^- \\pi^+)} = 1.684 \\pm 0.056 (stat.) \\pm 0.093(syst.) \\nonumber and \\frac{{\\cal B}(D\\rightarrow K^-e^+\\nu)} {{\\cal B}(D\\rightarrow Xe^+\\nu)} = 0.581 \\pm 0.023 (stat.) \\pm 0.028(syst.). \\nonumber The difference between the inclusive rate and the sum of the measured exclusive branching fractions (measured at CLEO and other experiments) is (3.3 \\pm 7.2) \\% of the inclusive rate.']",['1995-12-06']
2416,['eng'],"['Adler, R', 'Angelopoulos, A', 'Apostolakis, Alkis', 'Aslanides, Elie', 'Backenstoss, Gerhard', 'Bee, C P', 'Behnke, O', 'Benelli, A', 'Bertin, V', 'Blanc, F', 'Bloch, P', 'Carlson, P J', 'Carroll, M', 'Carvalho, J', 'Cawley, E', 'Charalambous, S', 'Chardin, G', 'Chertok, M B', 'Cody, A', 'Danielsson, M', 'Dejardin, M', 'Derré, J', 'Ealet, A', 'Eckart, B', 'Eleftheriadis, C', 'Evangelou, I', 'Faravel, L', 'Fassnacht, P', 'Felder, C', 'Ferreira-Marques, R', 'Fetscher, W', 'Fidecaro, Maria', 'Filipcic, A', 'Francis, D', 'Fry, J', 'Gabathuler, Erwin', 'Gamet, R', 'Garreta, D', 'Gerber, H J', 'Go, A', 'Guyot, C', 'Haselden, A', 'Hayman, P J', 'Henry-Coüannier, F', 'Hollander, R W', 'Hubert, E', 'Jon-And, K', 'Kettle, P R', 'Kochowski, C', 'Kokkas, P', 'Kreuger, R', 'Le Gac, R', 'Leimgruber, F', 'Liolios, A', 'Machado, E', 'Mandic, I', 'Manthos, N', 'Marel, G', 'Mikuz, M', 'Miller, J', 'Montanet, F', 'Nakada, Tatsuya', 'Pagels, B', 'Papadopoulos, I M', 'Pavlopoulos, P', 'Pinto da Cunha, J', 'Policarpo, A', 'Polivka, G', 'Rickenbach, R', 'Roberts, B L', 'Ruf, T', 'Sakelliou, L', 'Sanders, P', 'Santoni, C', 'Schäfer, M', 'Schaller, L A', 'Schietinger, T', 'Schopper, A', 'Schune, P', 'Soares, A', 'Tauscher, Ludwig', 'Thibault, C', 'Touchard, F', 'Touramanis, C', 'Triantis, F A', 'Van Beveren, E', 'van Eijk, C W E', 'Varner, G S', 'Vlachos, S', 'Weber, P', 'Wigger, O', 'Wolter, M', 'Yéche, C', 'Zavrtanik, D', 'Zimmerman, D', 'Ellis, Jonathan Richard', 'López, J L', 'Mavromatos, Nikolaos E', 'Nanopoulos, Dimitri V']",['Test of CPT symmetry and quantum mechanics with experimental data from CPLEAR'],['Particle Physics - Experimental Results'],"['anti-p p, annihilation', 'annihilation, anti-p p', 'at rest', 'K, hadroproduction', 'hadroproduction, K', 'hadron, multiple production', 'multiple production, hadron', 'K0, hadronic decay', 'hadronic decay, K0', 'K0, semileptonic decay', 'semileptonic decay, K0', 'anti-K0, hadronic decay', 'hadronic decay, anti-K0', 'anti-K0, semileptonic decay', 'semileptonic decay, anti-K0', 'decay, asymmetry', 'asymmetry, decay', 'time dependence', 'parametrization', 'invariance, CPT', 'validity test, CPT', 'quantum mechanics, validity test', 'data analysis method', 'statistical analysis', 'experimental results', 'CERN LEAR', 'anti-p p --> K0 K- pi+', 'anti-p p --> anti-K0 K+ pi-', 'K0 --> pi+ pi-', 'K0 --> pi muon neutrino', '0 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511001'],['We use fits to recent published CPLEAR data on neutral kaon decays to \\pi^+\\pi^- and \\pi e\\nu to constrain the CPT--violation parameters appearing in a formulation of the neutral kaon system as an open quantum-mechanical system. The obtained upper limits of the CPT--violation parameters are approaching the range suggested by certain ideas concerning quantum gravity.'],['1995-11-02']
2417,['eng'],"['Derrick, Malcolm']",['Rapidity gaps between jets in photoproduction at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, interaction', 'interaction, photon p', 'jet, photoproduction', 'photoproduction, jet', 'rapidity, gap', 'cross section, rapidity dependence', 'diffraction', 'hard scattering', 'photon, resolved', 'color, singlet', 'exchange, singlet', 'singlet, exchange', 'exchange, color', 'color, exchange', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'positron p --> 2jet positron anything', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510012'],"['Photoproduction events which have two or more jets have been studied in the W_{\\gamma p} range 135~GeV < W_{\\gamma p} < 280~GeV with the ZEUS detector at HERA. A class of events is observed with little hadronic activity between the jets. The jets are separated by pseudorapidity intervals (\\Delta\\eta) of up to four units and have transverse energies greater than 6~GeV. A gap is defined as the absence between the jets of particles with transverse energy greater than 300~MeV. The fraction of events containing a gap is measured as a function of \\deta. It decreases exponentially as expected for processes in which colour is exchanged between the jets, up to a value of \\Delta\\eta \\sim 3, then reaches a constant value of about 0.1. The excess above the exponential fall-off can be interpreted as evidence for hard diffractive scattering via a strongly interacting colour singlet object.']",['1995-10-31']
2418,['eng'],"['Rylko, R']",['On the kinematic reconstruction of e+e- --> W$^{+}$W$^{-}$ --> jj$\\tau\\overline{\\nu}_{\\tau}$ events'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, annihilation', 'annihilation, electron positron', 'W, pair production', 'pair production, W', 'coupling, (3gauge boson)', '(3gauge boson), coupling', 'W, leptonic decay', 'leptonic decay, W', 'W, nonleptonic decay', 'nonleptonic decay, W', 'track data analysis', 'kinematics', 'momentum', 'angular correlation', 'tau, decay', 'decay, tau', 'angular distribution', 'tau, energy', 'conservation law, energy-momentum', 'electron positron --> W+ W-', 'W+ --> 2jet', 'W- --> tau- neutrino/tau']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510011'],"['We show that the kinematic reconstruction of the e^+e^-\\rightarrow W^+W^-\\rightarrow jj\\tau^-\\overline{\\nu}_\\tau\\ events have a one-parameter ambiguity when reconstructed from the momentum of all measured W^-\\ decay products. We propose a {\\em hybrid} method of reconstruction of the e^+e^-\\rightarrow W^+W^-\\rightarrow jj\\tau^-\\overline{\\nu}_\\tau\\ events. This is based on the observation that the difference between the \\tau^-\\ production angles and the production angles of the sum of its visible decay products is small, whilst the \\tau^-\\ energy is poorly reconstructed. This method consists of taking the \\tau^-\\ production angles from those measured for the sum of the visible \\tau^-\\ decay products and reconstructing the \\tau^-\\ energy from energy-momentum conservation constraints. A reconstruction using this method is found to be well-defined and possess a unique solution for the \\tau^-\\ momentum range at LEP II and NLC.']",['1995-10-30']
2419,['eng'],"['Enomoto, R']",['Recent results from TRISTAN'],['Particle Physics - Experimental Results'],"['talk, Stanford 1995/07/10', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'exchange, two-photon', 'two-photon, exchange', 'photon photon, interaction', 'interaction, photon photon', 'vector dominance', 'photon, resolved', 'event shape analysis', 'jet, photoproduction', 'photoproduction, jet', 'transverse momentum, spectra', 'spectra, transverse momentum', 'photon, structure function', 'gluon, momentum spectrum', 'quark, charm', 'quark, pair production', 'pair production, quark', 'D*(2010), hadronic decay', 'hadronic decay, D*(2010)', 'K0(S), photoproduction', 'photoproduction, K0(S)', 'electron, photoproduction', 'photoproduction, electron', 'Lambda, photoproduction', 'photoproduction, Lambda', 'cross section, hadronic', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', 'approx. 58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510010'],"['The TRISTAN results from 1994 to 1995 are reviewed in this report. The physics results dominated the \\gamma \\gamma physics. Therefore, only these are selected in this article. We have systematically investigated jet productions, the \\gamma-structure function, and charm pair productions in \\gamma \\gamma processes. The results, discussions, and future prospects are presented.']",['1995-10-30']
2420,['eng'],"['Derrick, Malcolm']",['Measurement of the proton structure function f$_{2}$ at low x and low q$^{2}$ at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'p, structure function', 'structure function, small-x', 'momentum transfer, low', 'quantum chromodynamics, perturbation theory', 'photon p, interaction', 'interaction, photon p', 'total cross section', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510009'],"['We report on a measurement of the proton structure function F_2 in the range 3.5\\times10^{-5}\\leq x \\leq 4\\times10^{-3} and 1.5 {\\rm GeV^2} \\leq Q^2 \\leq15 {\\rm GeV^2} at the ep collider HERA operating at a centre-of-mass energy of \\sqrt{s} = 300 {\\rm GeV}. The rise of F_2 with decreasing x observed in the previous HERA measurements persists in this lower x and Q^2 range. The Q^2 evolution of F_2, even at the lowest Q^2 and x measured, is consistent with perturbative QCD.']",['1995-10-31']
2421,['eng'],"['Abe, K']",['Measurements of the Q$^{2}$-dependence of the proton and deuteron spin structure functions g$_{1}^{p}$ and g$_{1}^{d}$'],['Particle Physics - Experimental Results'],"['electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'electron deuteron, deep inelastic scattering', 'deep inelastic scattering, electron deuteron', 'electron, polarized beam', 'polarized beam, electron', 'polarized target', 'p, structure function', 'deuteron, structure function', 'structure function, spin', 'spin, structure function', 'structure function, ratio', 'dependence, momentum transfer', 'moment, structure function', 'symmetry, SU(3)', 'sum rule, Bjorken', 'spectrometer, experimental results', 'SLAC Lab', '9.7, 16.2, 29.1 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511015'],"['The ratio g1/F1 has been measured over the range 0.03<x<0.6 and 0.3<Q2<10 (GeV/c)2 using deep-inelastic scattering of polarized electrons from polarized protons and deuterons. We find g1/F1 to be consistent with no Q2-dependence at fixed x in the deep-inelastic region Q^2>1 (GeV/c)2. A trend is observed for g1/F1 to decrease at lower Q2. Fits to world data with and without a possible Q2-dependence in g1/F1 are in agreement with the Bjorken sum rule, but Delta_q is substantially less than the quark-parton model expectation.']",['1995-12-06']
2422,['eng'],"['Abe, K']",['Measurement of the Average $B$ Hadron Lifetime in $Z^{0}$ Decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'beautiful particle, lifetime', 'track data analysis, vertex', 'decay, path length', 'path length, decay', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511005'],"['We report a measurement of the average B-hadron lifetime using data collected with the SLD detector at the SLC in 1993. An inclusive analysis selected three-dimensional vertices with B-hadron lifetime information in a sample of 50k Z^{0} decays. A lifetime of 1.564\\pm0.030\\,(\\rm stat)\\pm 0.037\\,(\\rm syst)~ps was extracted from the decay length distribution of these vertices using a binned maximum-likelihood method.']",['1996-05-07']
2423,['eng'],"['Ootani, W', 'Ito, Y', 'Nishigaki, K', 'Kishimoto, Y', 'Minowa, M', 'Ootuka, Y']",['Sensitive germanium thermistors for cryogenic thermal detector of Tokyo dark matter search programme'],['Particle Physics - Experimental Results'],"['astrophysics, missing-mass', 'missing-mass, astrophysics', 'counters and detectors, cryogenics', 'bolometer', 'semiconductor, fabrication', 'germanium', 'temperature, dependence']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510008'],"['Sensitive n-type and p-type germanium thermistors were fabricated by the melt doping technique and by the neutron transmutation doping (NTD) technique, respectively, aiming at a use for the cryogenic thermal detector, or bolometer of Tokyo dark matter search programme. We report on the measurements of the sensitivities of these thermistors. In particular, the p-type thermistors are sensitive enough to scale up our existing prototype LiF bolometer and realize a multiple array of the bolometers with the total absorber mass of about 1\\,kg.']",['1995-10-30']
2424,['eng'],"['Geer, S']",['Searching for antiproton decay at the Fermilab antiproton accumulator'],['Particle Physics - Experimental Results'],"['talk, Brussels 1995/07/27', 'anti-p, accumulator', 'anti-p, semileptonic decay', 'semileptonic decay, anti-p', 'anti-p, radiative decay', 'radiative decay, anti-p', 'efficiency', 'scintillation counter', 'calorimeter, electromagnetic', 'proportional chamber', 'experimental results', 'Fermilab', 'anti-p --> electron photon', 'anti-p --> pi0 electron', 'anti-p --> eta electron', 'anti-p --> K0 electron', '8.9 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510007'],['This paper describes an experimental search for antiproton decay at the Fermilab Antiproton Accumulator. The E868 (APEX) experimental setup is described. The APEX data is expected to be sensitive to antiproton decay if the antiproton lifetimes is less than a few times 100 000 years.'],['1995-10-20']
2425,['eng'],"['Adler, Stephen Louis', 'Atiya, M S', 'Chiang, I H', 'Frank, J S', 'Haggerty, J S', 'Kycia, T F', 'Li Kai Kong', 'Littenberg, L S', 'Sambamurti, A K', 'Stevens, A', 'Strand, R C', 'Witzig, C', 'Louis, W C', 'Akerib, D S', 'Ardebili, M', 'Convery, M R', 'Ito, M M', 'Marlow, D R', 'McPherson, R A', 'Meyers, P D', 'Selen, M A', 'Shoemaker, F C', 'Smith, A J S', 'Blackmore, E W', 'Bryman, D A', 'Felawka, L', 'Kitching, P', 'Konaka, A', 'Kujala, V A', 'Kuno, Y', 'MacDonald, J A', 'Nakano, T', 'Numao, T', 'Padley, P', 'Poutissou, J M', 'Poutissou, R', 'Roy, J D', 'Soluk, R A', 'Turcot, A S']",['Search for the decay K$^{+}$ --> $\\pi^{+}\\nu\\overline{\\nu}$'],['Particle Physics - Experimental Results'],"['K+, semileptonic decay', 'semileptonic decay, K+', 'neutrino, pair production', 'pair production, neutrino', 'K+, branching ratio', 'upper limit', 'postulated particle, neutral particle', 'postulated particle, weak interaction', 'weak interaction, postulated particle', 'experimental results', 'Brookhaven PS', 'K+ --> pi+ neutrino antineutrino', 'K+ --> pi+ neutral particle']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510006'],"['An upper limit on the branching ratio for the decay K^+ \\! \\rightarrow \\! \\pi^+ \\nu \\overline{\\nu} is set at 2.4 \\times 10^{-9} at the 90\\% C.L. using pions in the kinematic region 214~{\\rm MeV}/c < P_\\pi < 231~{\\rm MeV}/c. An upper limit of 5.2 \\times 10^{-10} is found on the branching ratio for decays K^+ \\! \\rightarrow \\! \\pi^+ X^0, where X^0 is any massless, weakly interacting neutral particle. Limits are also set for cases where M_{X^0}>0.']",['1995-10-19']
2426,['eng'],"['Abe, K']",['First Measurement of the $T$-Odd Correlation between the $Z^{0}$ Spin and the Three-Jet Plane Orientation in Polarized $Z^{0}$ Decays to Three Jets'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'electron, polarized beam', 'polarized beam, electron', 'polarization, longitudinal', 'longitudinal, polarization', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'Z0, spin', 'spin, Z0', 'final state, (3jet)', '(3jet), final state', 'correlation', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'Z0 --> 3jet', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510005'],"['We present the first measurement of the correlation between the Z^0 spin and the three-jet plane orientation in polarized Z^0 decays into three jets in the SLD experiment at SLAC utilizing a longitudinally polarized electron beam. The CP-even and T-odd triple product \\vec{S_Z}\\cdot(\\vec{k_1}\\times \\vec{k_2}) formed from the two fastest jet momenta, \\vec{k_1} and \\vec{k_2}, and the Z^0 polarization vector \\vec{S_Z}, is sensitive to physics beyond the Standard Model. We measure the expectation value of this quantity to be consistent with zero and set 95\\% C.L. limits of -0.022 < \\beta < 0.039 on the correlation between the Z^0-spin and the three-jet plane orientation.']",['1995-10-19']
2427,['eng'],"['LoSecco, J M', 'Adams, T', 'Bishop, J M', 'Cason, N M', 'Manak, J J', 'Sanjari, A H', 'Shephard, W D', 'Stienike, D L', 'Taegar, S A', 'Thompson, D R', 'Chung, S U', 'Hackenburg, R W', 'Olchanski, C', 'Weygand, D P', 'Willutzki, H J', 'Denisov, S P', 'Dushkin, A Yu', 'Kochetkov, V', 'Shein, I V', 'Soldatov, A', 'Brabson, B', 'Crittenden, R R', 'Dzierba, A R', 'Gunter, J', 'Lindenbusch, R', 'Rust, D R', 'Scott, E', 'Smith, P T', 'Sulanke, T', 'Teige, S', 'Bar-Yam, Z', 'Dowd, J P', 'Eugenio, P', 'Hayck, M', 'Kern, W', 'King, E', 'Bodyagin, V A', 'Gribushin, A M', 'Kodolova, O L', 'Kostin, M A', 'Korotkikh, V L', 'Ostrovidov, A I', 'Proskuryakov, A S', 'Sarycheva, L I', 'Sinev, N B', 'Varchenko, Aleksandr Nikolaevich', 'Yershov, A A', 'Brown, D S', 'Pedlar, T K', 'Seth, K K', 'Wise, J', 'Zhao, D', 'Adams, G S', 'Napolitano, J', 'Nozar, M', 'Smith, J A', 'Witkowski, M T']",['Search for exotic mesons in $\\pi_{-}$p interactions at 18 GeV/c'],['Particle Physics - Experimental Results'],"['talk', 'pi- p, exclusive reaction', 'meson, hybrid', 'meson, search for', 'meson, decay', 'decay, meson', 'bound state, (quark antiquark gluon)', 'mass spectrum, ((n)meson)', '((n)meson), mass spectrum', 'decay, asymmetry', 'asymmetry, decay', 'experimental results', 'Brookhaven PS', '18 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510004'],"[""The recent search for non q \\bar{q} mesons in \\pi^{-}p interactions at Brookhaven National Laboratory is summarized. Many final states such as \\eta \\pi, \\eta' \\pi^{-}, a_{0} \\pi, f_{1} \\pi, a_{2} \\pi, b_{1} \\pi, which are favored decay modes of exotics, are under investigation.""]",['1995-10-17']
2428,['eng'],"['Koch, N', 'Kolander, M', 'Kolanoski, H', 'Siegmund, T', 'Bergter, J', 'Eckstein, P', 'Schubert, K R', 'Waldi, R', 'Imhof, M', 'Ressing, D', 'Weiss, U', 'Weseler, S']",['The ARGUS vertex trigger'],['Detectors and Experimental Techniques'],"['electron positron, colliding beam detector', 'colliding beam detector, electron positron', 'drift chamber, vertex', 'semiconductor detector, microstrip', 'trigger, hardware', 'control system', 'programming', 'communications', 'magnetic detector, ARGUS', 'DESY DORIS Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510003'],"['A fast second level trigger has been developed for the ARGUS experiment which recognizes tracks originating from the interaction region. The processor compares the hits in the ARGUS Micro Vertex Drift Chamber to 245760 masks stored in random access memories. The masks which are fully defined in three dimensions are able to reject tracks originating in the wall of the narrow beampipe of 10.5\\,mm radius.']",['1995-10-17']
2429,['eng'],"['Kaplan, D M']","['Production of charm, charmonium, and beauty in 800 GeV proton-nucleon collisions']",['Particle Physics - Experimental Results'],"['talk', 'p nucleon, inclusive reaction', 'quark, charm', 'quark, beauty', 'quark, hadroproduction', 'hadroproduction, quark', 'psi mesons, hadroproduction', 'hadroproduction, psi mesons', 'J/psi(3100), leptonic decay', 'leptonic decay, J/psi(3100)', 'D0, hadroproduction', 'hadroproduction, D0', 'differential cross section, x-dependence', 'x-dependence, differential cross section', 'channel cross section', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'p nucleon --> psi mesons anything', 'p nucleon --> D0 anything', 'p nucleon --> 2beauty anything', 'beauty --> J/psi(3100) anything', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510002'],"['Some recent results from the Fermilab fixed-target experiment E789 on production of charm, charmonium, and beauty are summarized and compared to model predictions. The data indicate that heavy-quark and quarkonium production are not yet entirely understood. The largest discrepancy concerns the rate of \\psi^\\prime production, which is a factor \\approx25 above expectations.']",['1995-10-13']
2430,['eng'],"['Levy, A']",['Measurement of $\\alpha_{s}$ from jet rates in deep inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'positron p, colliding beams', 'colliding beams, positron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'jet, electroproduction', 'electroproduction, jet', 'jet, multiplicity', 'transverse momentum, spectra', 'spectra, transverse momentum', 'quantum chromodynamics, perturbation theory', 'strong interaction, coupling constant', 'coupling constant, strong interaction', 'dependence, momentum transfer', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9510001'],"['Jet production in deep inelastic scattering for 120<Q^2<3600~GeV^2 has been studied using data from an integrated luminosity of 3.2~pb^{-1} collected with the ZEUS detector at HERA. Jets are identified with the JADE algorithm. A cut on the angular distribution of parton emission in the \\gamma^*-parton centre-of-mass system minimises the experimental and theoretical uncertainties in the determination of the jet rates. The jet rates, when compared to {\\cal O}(\\alpha_{s}^2) perturbative QCD calculations, allow a precise determination of \\alpha_{s}(Q) in three Q^2-intervals. The values are consistent with a running of \\alpha_{s}(Q), as expected from QCD. Extrapolating to Q=M_{Z^0} yields \\alpha_{s}(M_{Z^0}) = 0.117~\\pm~0.005~(stat)~^{+0.004}_{-0.005}~(syst_{exp})~ ~{\\pm~0.007}~(syst_{theory}).']",['1995-10-10']
2431,['eng'],"['Bates, R']",['Model of charge transport in semi-insulating undoped GaAs microstrip detectors'],['Detectors and Experimental Techniques'],"['talk, San Miniato 1995/03/19', 'semiconductor detector, microstrip', 'gallium, arsenic', 'semiconductor, electronics', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509011'],"['In this paper we present a method for simulating the response of microstrip detectors to minimum ionizing particles, making use of a program for field calculation, a program for carrier drift and SPICE for circuit response. A knowledge of the electric field is essential for any further improvement of the program. A simple model involving EL2 levels in the metastable state is proposed to explain some measurements of electric field.']",['1995-10-03']
2432,['eng'],"['Bates, R']",['Noise spectra of SIU-GaAs pad detectors with guard rings'],['Detectors and Experimental Techniques'],"['talk, San Miniato 1995/03/19', 'semiconductor detector', 'gallium, arsenic', 'electronics, background']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509012'],"['This paper presents current noise characterization of circular pad Schottky barrier diodes with guard rings. The diodes were fabricated from undopped semi-insulating GaAs, SIU-GaAs, at the University of Glasgow. Current noise spectra were obtained for the detectors for two pad sizes, with reverse bias applied. Three measurements were also made on one of the detectors under forward bias. The noise spectra show an excess noise component, with a low frequency corner at less than 1kHz, and a flat region at higher frequencies. The magnitude of the white noise is approximately half that expected from shot noise theory for the given leakage currents. A fall in the magnitude of the noise was observed at 20kHz which is attributed to the dielectric relaxation time of the material.']",['1995-10-03']
2433,['eng'],"['Abachi, S']",['Jet production via strongly-interacting color-singlet exchange in p$\\overline{p}$ collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'hadroproduction, jet', 'final state, (2jet)', '(2jet), final state', 'charged particle, multiplicity', 'rapidity, gap', 'exchange, two-gluon', 'two-gluon, exchange', 'color, singlet', 'exchange, color', 'color, exchange', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509013'],"['A study of the particle multiplicity between jets with large rapidity separation has been performed using the D\\O\\ detector at the Fermilab Tevatron p\\bar{p} Collider operating at \\sqrt{s}=1.8\\,TeV. A significant excess of low-multiplicity events is observed above the expectation for color-exchange processes. The measured fractional excess is 1.07 \\pm 0.10({\\rm stat})^{ + 0.25}_{- 0.13}({\\rm syst})\\%, which is consistent with a strongly-interacting color-singlet (colorless) exchange process and cannot be explained by electroweak exchange alone. A lower limit of 0.80\\% (95\\% C.L.) is obtained on the fraction of dijet events with color-singlet exchange, independent of the rapidity gap survival probability.']",['1995-10-02']
2434,['eng'],"['Abe, K']",['Measurements of the proton and deuteron spin structure function g$_{2}$ and asymmetry A$_{2}$'],['Particle Physics - Experimental Results'],"['electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'electron deuteron, deep inelastic scattering', 'deep inelastic scattering, electron deuteron', 'electron, polarized beam', 'polarized beam, electron', 'polarized target', 'polarization, longitudinal', 'longitudinal, polarization', 'polarization, transverse', 'transverse, polarization', 'cross section, asymmetry', 'p, structure function', 'deuteron, structure function', 'structure function, spin', 'spin, structure function', 'x-dependence', 'effect, higher-twist', 'spectrometer, experimental results', 'SLAC Lab', '29.1 GeV, 4.5, 7.0 degrees']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511013'],"['We have measured proton and deuteron virtual photon-nucleon asymmetries A2p and A2d and structure functions g2p and g2d over the range 0.03<x<0.8 and 1.3<Q2<10 (GeV/c)2 by inelastically scattering polarized electrons off polarized ammonia targets. Results for A2 are significantly smaller than the positivity limit sqrt(R) for both targets. Within experimental precision, the g2 data are well-described by the twist-2 contribution g2WW. Twist-3 matrix elements have been extracted and are compared to theorectical predictions.']",['1995-12-01']
2435,['eng'],"['Abe, F']",['Measurement of $\\sigma$ x B(W --> e$\\nu$) and $\\sigma$ x B(Z$^{0}$ --> e+e-) in p$\\overline{p}$ collisions at \\Sqrt (s)=1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'intermediate boson, leptonic decay', 'leptonic decay, intermediate boson', 'channel cross section, branching ratio', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509010'],['We present a measurement of \\sigma \\cdot B(W \\rightarrow e \\nu) and \\sigma \\cdot B(Z^0 \\rightarrow e^+e^-) in proton - antiproton collisions at \\sqrt{s} =1.8 TeV using a significantly improved understanding of the integrated luminosity. The data represent an integrated luminosity of 19.7 pb^{-1} from the 1992-1993 run with the Collider Detector at Fermilab (CDF). We find \\sigma \\cdot B(W \\rightarrow e \\nu) = 2.49 \\pm 0.12~nb and \\sigma \\cdot B(Z^0 \\rightarrow e^+e^-) = 0.231 \\pm 0.012~nb.'],['1995-09-26']
2436,['eng'],"['Gowdy, S', 'Brook, N']",['GaAs microstrip test beam results'],['Particle Physics - Experimental Results'],"['talk, San Miniato 1995/03/19', 'semiconductor detector, microstrip', 'gallium, arsenic', 'spatial resolution', 'electronics, background', 'efficiency', 'calibration', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509008'],['A gallium arsenide detector was tested with a beam of 70GeV pions at the {\\sf SPS} at CERN. The detector utilises a novel biasing scheme which has been shown to behave as expected. The detector has a pitch of 50\\mum and therefore an expected resolution of 14.5\\mum. The measured resolution was approximately 14\\mum. By using a non-linear charge division algorithm this can be increased to \\approx 12\\mum. Noise was the limiting factor to the resolution. This was 2000e^- as opposed to the expected 360e^-. This noise is also thought to have reduced the detection efficiency of the detector. The source of the excess noise is currently being investigated.'],['1995-09-15']
2437,['eng'],"['Baum, G']",['The SMC experiment'],['Particle Physics - Experimental Results'],"['talk, Trieste 1995/05/08', 'muon+ p, deep inelastic scattering', 'deep inelastic scattering, muon+ p', 'muon+ deuteron, deep inelastic scattering', 'deep inelastic scattering, muon+ deuteron', 'muon, polarized beam', 'polarized beam, muon', 'deuteron, polarized target', 'polarized target, deuteron', 'hadron, multiple production', 'multiple production, hadron', 'nucleon, structure function', 'structure function, spin', 'spin, structure function', 'moment, structure function', 'sum rule, Bjorken', 'nucleon, spin', 'spin, nucleon', 'quark, spin', 'spin, quark', 'quark, valence', 'polarization, asymmetry', 'asymmetry, polarization', 'x-dependence', 'magnetic spectrometer, experimental results', 'CERN SPS', '100, 190 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509007'],['An overview of the SMC data taking and the polarized deep inelastic scattering experiment is given. The new data on the deuteron extend the kinematic range and have considerably reduced statistical and systematic errors. The evaluation of the first moment of the spin dependent structure function is presented and the result for the Bjorken sum rule from SMC data alone is given. The spin contribution of the quarks to the spin of the nucleon is obtained with information from weak decays of baryons. In a new polarized semi-inclusive analysis the asymmetry of the difference between the number of positive and negative charged hadrons was studied. Preliminary results are shown.'],['1995-09-14']
2438,['eng'],"['McBride, P', 'Stone, S']",['$B_{s}$ mixing via $\\psi$K^{*}$'],['Particle Physics - Experimental Results'],"['talk, Oxford 1995/07/10', 'anti-p p, inclusive reaction', 'B/s0, hadroproduction', 'hadroproduction, B/s0', 'B/s0, hadronic decay', 'hadronic decay, B/s0', 'B/s0, branching ratio', 'B/s0 anti-B/s0, interference', 'time, oscillation', 'J/psi(3100), leptonic decay', 'leptonic decay, J/psi(3100)', 'trigger, dilepton', 'magnetic detector, time resolution', 'rapidity dependence', 'background', 'numerical calculations, Batavia TEVATRON Coll', 'proposed experiment', 'anti-p p --> B/s0 anything', 'B/s0 --> J/psi(3100) K*(892)', 'J/psi(3100) --> lepton+ lepton-', 'K*(892) --> K+ pi-', '1800 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509006', 'http://www-lib.fnal.gov/archive/1995/conf/Conf-95-288.html']","['The decay mode B_s\\to\\psi \\overline{K}^* is suggested as a very good way to measure the B_s mixing parameter x_s. These decays can be gathered using a \\psi\\to\\ell^+\\ell^- trigger. This final state has a well resolved four track decay vertex, useful for good time resolution and background rejection.']",['1995-09-13']
2439,['eng'],"['Abachi, S']",['Studies of topological distributions of the three- and four-jet events in pp collisions at \\Sqrt s = 1800 GeV with the D0 detector'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'hadroproduction, jet', 'final state, (3jet)', '(3jet), final state', 'final state, (4jet)', '(4jet), final state', 'event shape analysis', 'mass spectrum', 'spectra, x-dependence', 'x-dependence, spectra', 'quantum chromodynamics, perturbation theory', 'tree approximation', 'showers, parton', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'tables', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509005'],"['The global topologies of inclusive three-- and four--jet events produced in \\pp interactions are described. The three-- and four--jet events are selected from data recorded by the D\\O\\ detector at the Tevatron Collider operating at a center--of--mass energy of \\sqrt{s} = 1800 GeV. The measured, normalized distributions of various topological variables are compared with parton--level predictions of tree--level QCD calculations. The parton--level QCD calculations are found to be in good agreement with the data. The studies also show that the topological distributions of the different subprocesses involving different numbers of quarks are very similar and reproduce the measured distributions well. The parton shower Monte Carlo generators provide a less satisfactory description of the topologies of the three-- and four--jet events.']",['1995-09-14']
2440,['eng'],"['Sinclair, L E']",['Hard photoproduction by colour singlet exchange at HERA'],['Particle Physics - Experimental Results'],"['talk', 'electron p, colliding beams', 'colliding beams, electron p', 'jet, photoproduction', 'photoproduction, jet', 'final state, (2jet)', '(2jet), final state', 'rapidity, gap', 'gap, width', 'exchange, two-gluon', 'two-gluon, exchange', 'color, singlet', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509004'],"['A search for photoproduction events which contain a rapidity gap between the two highest transverse energy jets has been conducted at HERA using the ZEUS detector. The jets have transverse energies greater than 6~GeV, and are separated by pseudorapidity intervals of up to four units. The fraction of events containing a gap is measured as a function of the gap-width. It is expected that this gap-fraction will fall exponentially with the gap-width, until the dominant gap-production mechanism becomes colour singlet exchange, at which point it will plateau. An indication of a plateau in the measured gap-fraction has been found, at a higher level than that expected from electroweak exchange.']",['1995-09-11']
2441,['eng'],"['Stone, S']","['CLEO III, a dectector to measure rare B decays and CP violation']",['Detectors and Experimental Techniques'],"['talk, Oxford 1995/07/10', 'luminosity, upgrade', 'Cherenkov counter, ring imaging', 'Cherenkov counter, crystal', 'lithium, fluorine', 'semiconductor detector, vertex', 'drift chamber', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509002'],"['The symmetric e^+e^- collider CESR is undergoing a series of upgrades allowing for luminosities in excess of 2\\times 10^{33}cm^{-2}s^{-1}. The most important goals of the upgrade are precision measurement of standard model parameters V_{cb}, V_{ub}, V_{td}/V_{ts}, f_{D_s}, and searching for CP violation and standard model violations in rare B decays. A new detector upgrade, called CLEO III, has started which includes a new silicon-wire drift chamber tracking system and a Ring Imaging Cherenkov Detector, RICH, using a LiF radiator and CH_4-TEA gas based photon detector.']",['1995-09-11']
2442,['eng'],"['Artuso, M']",['The ring imaging detector for CLEO III'],['Detectors and Experimental Techniques'],"['B, particle source', 'luminosity, upgrade', 'particle identification', 'Cherenkov counter, ring imaging', 'lithium, fluorine', 'magnetic detector, CLEO', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509003'],"['The CLEO detector will undergo major improvements in conjunction with a high luminosity upgrade of the CESR electron positron collider, that should increase the luminosity of this machine by a factor of 10. The most innovative feature of the planned CLEO detector is the addition of a state of the art particle identification system, based on a proximity focused Ring Imaging Cherenkov detector. The goal is to achieve good hadron identification at all the momenta relevant to the study of decays of B mesons produced at the upsilon(4S) resonance. This detector design will be discussed, including details of the mechanical design and the readout electronics. The performance of a prototype module will be described.']",['1995-09-11']
2443,['eng'],"['Utley, M L']",['Direct and resolved photoproduction at HERA with virtual and quasi-real photons'],['Particle Physics - Experimental Results'],"['talk, Brussels 1995/07/27', 'positron p, colliding beams', 'colliding beams, positron p', 'exchange, one-photon', 'one-photon, exchange', 'jet, electroproduction', 'electroproduction, jet', 'jet, photoproduction', 'photoproduction, jet', 'final state, (2jet)', '(2jet), final state', 'momentum spectrum', 'yield, ratio', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '27.5 GeV (positron), 820.0 GeV (p)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508016'],"['Preliminary results are presented from a study of dijet photoproduction in ep collisions with both virtual and quasi-real photons at the ZEUS detector. Samples of events with photons of virtuality P^2 in the ranges 0.1 < P^2 < 0.55 GeV^2 and P^2 < 0.02 GeV^2 having two jets of E_T^{jet} > 4 GeV in the final state have been obtained. For both quasi-real and virtual photons, uncorrected distributions of the quantity x_{\\gamma}^{obs}, the fraction of the photon momentum manifest in the two highest E_T jets, are presented. These distributions are sensitive to the relative contributions of the direct and resolved processes. Resolved photon processes are evident in both data sets, with an apparent decrease in the relative contribution from resolved processes as photon virtuality increases.']",['1995-08-31']
2444,['eng'],"['Kaplan, D M']",['High-impact charm physics at the turn of the millennium'],['Particle Physics - Phenomenology'],"['talk', 'charmed particle, photoproduction', 'photoproduction, charmed particle', 'charmed particle, hadroproduction', 'hadroproduction, charmed particle', 'charmed particle, decay modes', 'decay modes, charmed particle', 'violation, CP', 'neutral current, flavor changing', 'lepton number, violation', 'D+', 'D0', 'D0 anti-D0, interference', 'p nucleus, inclusive reaction', 'magnetic spectrometer, proposed', 'trigger', 'numerical calculations', 'experimental results', 'proposed experiment', 'Batavia TEVATRON PS', 'bibliography']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508018'],"['I review the sensitivities achieved by and projected for fixed-target charm experiments in CP violation, flavor-changing neutral-current and lepton-number-violating decays, and mixing, and I describe the Charm2000 experiment intended to run at Fermilab in the Year ~2000. If approved, Charm2000 will in many of these areas exceed the sensitivities projected for a Tau/Charm Factory, but the Tau/Charm Factory retains certain qualitative advantages.']",['1995-09-01']
2445,['eng'],"['Abe, F', 'Albrow, Michael G', 'Amendolia, S R', 'Amidei, D', 'Antos, J', 'Anway-Wiese, C', 'Apollinari, G', 'Areti, H', 'Atac, Muzaffer', 'Auchincloss, P S', 'Azfar, F', 'Azzi, P', 'Bacchetta, N', 'Badgett, W F', 'Bailey, M W', 'Bao, J', 'De Barbaro, P', 'Barbaro-Galtieri, A', 'Barnes, Virgil E', 'Barnett, B A', 'Bartalini, P', 'Bauer, G', 'Baumann, T', 'Bedeschi, F', 'Behrends, S', 'Belforte, S', 'Bellettini, Giorgio', 'Bellinger, J', 'Benjamin, D', 'Benlloch, J M', 'Bensinger, J', 'Benton, D', 'Beretvas, A', 'Berge, J P', 'Bertolucci, S', 'Bhatti, A A', 'Biery, K', 'Binkley, M', 'Bird, F', 'Bisello, D', 'Blair, R', 'Blocker, C A', 'Bodek, Arie', 'Bokhari, W', 'Bolognesi, V', 'Bortoletto, D', 'Boswell, C', 'Boulos, T', 'Brandenburg, G', 'Buckley-Geer, E', 'Budd, H S', 'Burkett, K', 'Busetto, G', 'Byon-Wagner, A', 'Byrum, K L', 'Cammarata, J B', 'Campagnari, C', 'Campbell, M', 'Caner, A', 'Carithers, W C', 'Carlsmith, D', 'Castro, A', 'Cen, Y', 'Cervelli, F', 'Chao, H Y', 'Chapman, J', 'Cheng, M T', 'Chiarelli, G', 'Chikamatsu, T', 'Chiou, C N', 'Christofek, L S', 'Cihangir, S', 'Clark, A G', 'Cobal, M', 'Contreras, M', 'Conway, J', 'Cooper, J', 'Cordelli, M', 'Couyoumtzelis, C', 'Crane, D', 'Cunningham, J D', 'Daniels, T', 'De Jongh, F', 'Delchamps, S W', ""Dell'Agnello, S"", ""Dell'Orso, M"", 'Demortier, L', 'Denby, B', 'Deninno, M M', 'Derwent, P F', 'Devlin, T', 'Dickson, M', 'Dittmann, J R', 'Donati, S', 'Drucker, R B', 'Dunn, A', 'Einsweiler, Kevin F', 'Elias, J E', 'Ely, R P', 'Engels, E', 'Eno, S', 'Errede, D', 'Errede, S', 'Fan, Q', 'Farhat, B', 'Fiori, I', 'Flaugher, B L', 'Foster, G W', 'Franklin, M', 'Frautschi, M A', 'Freeman, J', 'Friedman, J', 'Frisch, H', 'Fry, A', 'Fuess, T A', 'Fukui, Y', 'Funaki, S', 'Gagliardi, G', 'Galeotti, S', 'Gallinaro, M', 'Garfinkel, A F', 'Geer, S', 'Gerdes, D W', 'Giannetti, P', 'Giokaris, N D', 'Giromini, P', 'Gladney, L', 'Glenzinski, D A', 'Gold, M', 'González, J', 'Gordon, A', 'Goshaw, A T', 'Goulianos, K', 'Grassmann, H', 'Grewal, A', 'Groer, L S', 'Grosso-Pilcher, C', 'Haber, C', 'Hahn, S R', 'Hamilton, R', 'Handler, R', 'Hans, R M', 'Hara, K', 'Harral, B D', 'Harris, R M', 'Hauger, S A', 'Hauser, J', 'Hawk, C', 'Heinrich, J', 'Cronin-Hennessy, D', 'Hollebeek, R J', 'Holloway, L', 'Hölscher, A', 'Hong, S', 'Houk, G', 'Hu, P', 'Huffman, B T', 'Hughes, R', 'Hurst, P', 'Huston, J', 'Huth, J E', 'Hylen, J', 'Incagli, M', 'Incandela, J R', 'Iso, H', 'Jensen, H', 'Jessop, C P', 'Joshi, U', 'Kadel, R W', 'Kajfasz, E', 'Kamon, T', 'Kaneko, T', 'Kardelis, D A', 'Kasha, H', 'Kato, Y', 'Keeble, L', 'Kennedy, R D', 'Kephart, R D', 'Kesten, P', 'Kestenbaum, D S', 'Keup, R M', 'Keutelian, H', 'Keyvan, F', 'Kim, D H', 'Kim, H S', 'Kim, S B', 'Kim, S H', 'Kim, Y K', 'Kirsch, L', 'Koehn, P', 'Kondo, K', 'Konigsberg, J', 'Kopp, S E', 'Kordas, K', 'Koska, W', 'Kovacs, E', 'Kowald, W', 'Krasberg, M', 'Kroll, J', 'Kruse, M', 'Kuhlmann, S E', 'Kuns, E W', 'Laasanen, A T', 'Lammel, S', 'Lamoureux, J I', 'LeCompte, T J', 'Leone, S', 'Lewis, J D', 'Limon, P', 'Lindgren, M', 'Liss, T M', 'Lockyer, N', 'Loomis, C', 'Long, O', 'Loreti, M', 'Low, E H', 'Lu, J', 'Lucchesi, D', 'Luchini, C B', 'Lukens, P', 'Lys, j', 'Maas, P', 'Maeshima, K', 'Maghakian, A', 'Maksimovic, P', 'Mangano, Michelangelo L', 'Mansour, J P', 'Mariotti, M', 'Marriner, J P', 'Martin, A', 'Matthews, J A J', 'Mattingly, R', 'McIntyre, P', 'Mélèse, P', 'Menzione, A', 'Meschi, E', 'Michail, G', 'Mikamo, S', 'Miller, M', 'Miller, R', 'Mimashi, T', 'Miscetti, S', 'Mishina, M', 'Mitsushio, H', 'Miyashita, S', 'Morita, Y', 'Moulding, S', 'Müller, J', 'Mukherjee, A', 'Müller, T', 'Musgrave, P', 'Nakae, L F', 'Nakano, I', 'Nelson, C', 'Neuberger, D', 'Newman-Holmes, C', 'Nodulman, L', 'Ogawa, S', 'Oh, S H', 'Ohl, K E', 'Oishi, R', 'Okusawa, T', 'Pagliarone, C', 'Paoletti, R', 'Papadimitriou, V', 'Park, S', 'Patrick, J', 'Pauletta, G', 'Paulini, M', 'Pescara, L', 'Petres, M D', 'Phillips, T J', 'Piacentino, G', 'Pillai, M', 'Plunkett, R K', 'Pondrom, L', 'Produit, N', 'Proudfoot, J', 'Ptohos, F', 'Punzi, G', 'Ragan, K', 'Rimondi, F', 'Ristori, L', 'Roach-Bellino, M', 'Robertson, W J', 'Rodrigo, T', 'Romano, J', 'Rosenson, L', 'Sakumoto, W K', 'Saltzberg, D', 'Sansoni, A', 'Scarpine, V', 'Schindler, A', 'Schlabach, P', 'Schmidt, E E', 'Schmidt, M P', 'Schneider, O', 'Sciacca, G F', 'Scribano, A', 'Segler, S L', 'Seidel, S', 'Seiya, Y', 'Sganos, G', 'Sgolacchia, A', 'Shapiro, M', 'Shaw, N M', 'Shen, Q', 'Shepard, P F', 'Shimojima, M', 'Shochet, M J', 'Siegrist, J', 'Sill, A F', 'Sinervo, P K', 'Singh, P', 'Skarha, J', 'Sliwa, K', 'Smith, D A', 'Snider, F D', 'Song, L', 'Song, T', 'Spalding, J', 'Spiegel, L', 'Sphicas, P', 'Spies, A', 'Stanco, L', 'Steele, J V', 'Stefanini, A', 'Strahl, K', 'Strait, J B', 'Stuart, D', 'Sullivan, G', 'Sumorok, K', 'Swartz, R L', 'Takahashi, T', 'Takikawa, K', 'Tartarelli, F', 'Taylor, W', 'Teramoto, Y', 'Tether, S', 'Theriot, D E', 'Thomas, J', 'Thomas, T L', 'Thun, R', 'Timko, M', 'Tipton, P', 'Titov, A', 'Tkaczyk, S M', 'Tollefson, K', 'Tollestrup, A V', 'Tonnison, J', 'De Trocóniz, J F', 'Tseng, J', 'Turcotte, M', 'Turini, N', 'Uemura, N', 'Ukegawa, F', 'Unal, G', 'Ven den Brink, S', 'Vejcik, S', 'Vidal, R', 'Vondracek, M', 'Vucinic, D', 'Wagner, R G', 'Wagner, R L', 'Wainer, N', 'Walker, R C', 'Wang, G', 'Wang, J', 'Wang, M J', 'Wang, Q F', 'Warburton, A', 'Watts, G', 'Watts, T', 'Webb, R', 'Wei, C', 'Wendt, C', 'Wenzel, H', 'Wester, W C', 'Westhusing, T', 'Wicklund, A B', 'Wicklund, E', 'Wilkinson, R P', 'Williams, H H', 'Wilson, P', 'Winer, B L', 'Wolinski, J', 'Wu, D Y', 'Wu, X', 'Wyss, J', 'Yagil, A', 'Yao, W', 'Yasuoka, K', 'Ye, Y', 'Yeh, G P', 'Yeh, P', 'Yin, M', 'Yoh, J K', 'Yosef, C', 'Yoshida, T', 'Yovanovitch, D D', 'Yu, I', 'Yun, J C', 'Zanetti, A', 'Zetti, F', 'Zhang, L', 'Zhang, S', 'Zhang, W', 'Zucchelli, S', 'Bromberg, C', 'Labanca, N']",['Measurement of correlated $\\mu$-$\\overline{b}$ jet cross sections in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'quark, semileptonic decay', 'semileptonic decay, quark', 'angular distribution, (beauty meson)', '(beauty meson), angular distribution', 'differential cross section, transverse energy', 'transverse energy, differential cross section', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'quantum chromodynamics, perturbation theory', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508017'],"['We report on measurements of differential \\mu - {\\overline b} cross sections, where the muon is from a semi-leptonic b decay and the {\\overline b} is identified using precision track reconstruction in jets. The semi-differential correlated cross sections, d\\sigma/d\\Et^{{\\overline b}}, d\\sigma/d\\pt^{{\\overline b}}, and d\\sigma/d\\delta\\phi(\\mu - {\\overline b}) for \\pt^{\\mu}>~9~GeV/c, |\\eta^{\\mu}|<~0.6, \\Et^{{\\overline b}}>~10~GeV, |\\eta^{{\\overline b}}|<~1.5, are presented and compared to next-to-leading order QCD calculations.']",['1995-08-31']
2446,['eng'],"['Eichler, R']",['Comparison of deep inelastic scattering with photoproduction interactions at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, interaction', 'interaction, photon p', 'hadron, photoproduction', 'photoproduction, hadron', 'transverse energy, energy flow', 'transverse energy, density', 'rapidity dependence', 'energy dependence', 'dependence, momentum transfer', 'diffraction, dissociation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508013'],"['Photon-proton (\\gamma p) interactions with~Q^2<10^{-2}~GeV^2 and deep-inelastic scattering (\\gamma^* p) interactions with photon virtualities Q^2>5~GeV^2 are studied at the high energy electron-proton collider HERA. The transverse energy flow and relative rates of large rapidity gap events are compared in the two event samples. The observed similarity between \\gamma p and \\gamma^* p interactions can be understood in a picture where the photon develops as a hadronic object. The transverse energy density measured in the central region of the collision, at \\eta^*=0 in the \\gsp centre of mass frame, is compared with data from hadron-hadron interactions as function of the CMS energy of the collision.']",['1995-08-29']
2447,['eng'],"['Rosner, Jonathan L']",['Detection of the rf pulse associated with cosmic ray air showers'],['Particle Physics - Experimental Results'],"['cosmic radiation', 'showers, air', 'microwaves', 'background', 'trigger', 'experimental equipment']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508011'],"['A project to detect the radio-frequency pulse associated with extensive air showers of cosmic rays is described briefly. Prototype work is being performed at the CASA/MIA array in Utah, with the intention of designing equipment that can be used in conjunction with the Auger Giant Array proposal.']",['1995-08-10']
2448,['eng'],"['Sugaya, Y', 'Yamaguchi, H', 'Yoshimura, Y', 'Kanda, S', 'Olsen, S', 'Ueno, K', 'Varner, G S', 'Bergfeld, T', 'Bialek, J', 'Lorenc, J', 'Palmer, M', 'Rudnick, G', 'Selen, M', 'Auran, T', 'Boyer, V', 'Honscheid, K', 'Tamura, N', 'Yoshimura, K', 'Lü, C', 'Marlow, D R', 'Mindas, C R', 'Prebys, E J', 'Asai, M', 'Kimura, A', 'Hayashi, S']",['The Cherenkov correlated timing detector'],['Detectors and Experimental Techniques'],"['talk, Uppsala 1995/06/12', 'particle identification', 'Cherenkov counter, angular resolution', 'glass', 'plastics', 'time']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508007'],['Several prototypes of a Cherenkov Correlated Timing (CCT) Detector have been tested at the KEK-PS test beam line. We describe the results for Cherenkov light yields and timing characteristics from quartz and acrylic bar prototypes. A Cherenkov angle resolution is found to be 15 mrad at a propagation distance of 100 cm with a 2 cm thick quartz bar prototype.'],['1995-08-04']
2449,['eng'],"['Aronstein, D', 'Bergfeld, T', 'Horton, D', 'Palmer, M', 'Thayer, G', 'Boyer, V', 'Kichimi, H', 'Sugaya, Y', 'Yamaguchi, H', 'Yoshimura, Y', 'Kanda, S', 'Olsen, S', 'Ueno, K', 'Tamura, N', 'Yoshimura, K', 'Lü, C', 'Marlow, D R', 'Mindas, C R', 'Prebys, E J', 'Pomianowski, P A']",['The Cherenkov correlated timing detector'],['Detectors and Experimental Techniques'],"['talk, Uppsala 1995/06/12', 'particle identification', 'Cherenkov counter', 'optics, absorption', 'absorption, optics', 'photoelectron, amplifier', 'time']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508008'],"['The key parameters of Cherenkov Correlated Timing (CCT) detectors are discussed. Measurements of radiator geometry, optical properties of radiator and coupling materials, and photon detector timing performance are presented.']",['1995-08-04']
2450,['eng'],"['Abachi, S']",['Tests of QCD in W and Z production at Tevatron'],['Particle Physics - Experimental Results'],"['talk, Beijing 1995/07/27', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'intermediate boson, leptonic decay', 'leptonic decay, intermediate boson', 'channel cross section, branching ratio', 'transverse momentum, spectra', 'spectra, transverse momentum', 'charge, asymmetry', 'quantum chromodynamics, validity test', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508002'],['We present measurements of the production cross sections times leptonic branching fractions and the transverse momentum distributions of W and Z bosons in p\\bar{p} collisions at \\sqrt{s}=1.8~TeV using data collected with the D\\O\\ detector at the Fermilab Tevatron p\\bar{p} collider. A preliminary measurement of the W charge asymmetry is also presented.'],['1995-08-02']
2451,['eng'],"['Brandenburg, G']","[""Measurements of the ratios B(D$_{s}^{+}$ --> .eta $\\ell$sup(+)$\\nu$) / B(D$_{s}^{+}$ --> .phi $\\ell$sup(+)$\\nu$) and B(D$_{s}^{+}$ --> $\\eta$'l$^{+}\\nu$) / B(D$_{s}^{+}$ --> .phi $\\ell$sup(+)$\\nu$)""]",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'quark, charm', 'quark, pair production', 'pair production, quark', 'eta', 'eta(958)', 'Phi(1020)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms', 'D/s+, semileptonic decay', 'semileptonic decay, D/s+', 'D/s+, branching ratio', 'D/s+ --> eta positron neutrino', 'D/s+ --> eta(958) positron neutrino', 'D/s+ --> Phi(1020) positron neutrino']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508009'],[],['1995-08-08']
2452,['eng'],"['Gronberg, J B']",['Observation of the isospin-violating decay D$_{s}^{*+}$ --> D$_{s}^{+}\\pi^{0}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'isospin, violation', 'violation, isospin', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.3-10.6 GeV-cms', 'D/s*(2110), electroproduction', 'electroproduction, D/s*(2110)', 'D/s*(2110), hadronic decay', 'hadronic decay, D/s*(2110)', 'D/s*(2110), width', 'mass difference, (D/s*(2110) D/s+)', '(D/s*(2110) D/s+), mass difference', 'D/s*(2110) --> D/s+ pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508001'],[],['1995-08-03']
2453,['eng'],"['Bergfeld, T']","['Observation of the $\\Xi_{c}^{+}$ charmed baryon decays to $\\Sigma^{+}$K$^{-}\\pi^{+}$, $\\Sigma^{+}\\overline{K}^{*0}$, and $\\Lambda$K$^{-}\\pi^{+}\\pi^{+}$']",['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Xi/c+, electroproduction', 'electroproduction, Xi/c+', 'Xi/c+, hadronic decay', 'hadronic decay, Xi/c+', 'K*(892)', 'Xi/c+, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'Xi/c+ --> Sigma+ K- pi+', 'Xi/c+ --> Sigma+ K*(892)', 'Xi/c+ --> Lambda K- 2pi+', 'Xi/c+ --> Xi- 2pi+', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508006'],[],['1995-08-08']
2454,['eng'],"['Avery, P']",['Observation of a narrow state decaying into $\\Xi_{c}^{+}\\pi^{-}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'charmed baryon, electroproduction', 'electroproduction, charmed baryon', 'K*(892)', 'mass spectrum, (Xi 2pi)', '(Xi 2pi), mass spectrum', 'Xi/c+']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508010'],[],['1995-08-08']
2455,['eng'],"['Abachi, S']",['Search for anomalous WW and WZ production at D0'],['Particle Physics - Experimental Results'],"['talk, Brussels 1995/07/27', 'talk, Beijing 1995\\08\\10', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'intermediate boson, pair production', 'pair production, intermediate boson', 'intermediate boson, nonleptonic decay', 'nonleptonic decay, intermediate boson', 'W, leptonic decay', 'leptonic decay, W', 'coupling, (2W photon)', '(2W photon), coupling', 'coupling, (Z0 2W)', '(Z0 2W), coupling', 'final state, (2jet lepton neutrino)', '(2jet lepton neutrino), final state', 'W, transverse momentum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', 'anti-p p --> Z0 W anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507014'],"['We present a preliminary result from a search for anomalous WW and WZ production in p\\bar{p} collisions at \\sqrt{s}=1.8 TeV using p\\bar{p}\\rightarrow e\\nu jj events observed during the 1992--1993 run of the Fermilab Tevatron collider. A fit to the p_T spectrum of W(e\\nu) yields direct limits on the CP--conserving anomalous WW\\gamma and WWZ coupling parameters of -0.89<\\Delta\\kappa<1.07~~(\\lambda=0) and -0.66<\\lambda<0.67~~(\\Delta\\kappa=0) at the 95\\ \\% confidence level, assuming that the WWZ coupling parameters are equal to the WW\\gamma coupling parameters, and a form factor scale \\Lambda=1.5~TeV.']",['1995-07-26']
2456,['eng'],"['Alexander, J']",['Observation of the Cabibbo suppressed charmed baryon decay'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Lambda/c+, electroproduction', 'electroproduction, Lambda/c+', 'Lambda/c+, hadronic decay', 'hadronic decay, Lambda/c+', 'Lambda/c+, branching ratio', 'mass spectrum, (p K+ K-)', '(p K+ K-), mass spectrum', 'Phi(1020)', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Lambda/c+ anything', 'Lambda/c+ --> p K+ K-', 'Lambda/c+ --> Phi(1020) p', 'approx. 10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508005'],[],['1995-08-08']
2457,['eng'],"['Asner, D M']",['Search for exclusive charmless hadronic B decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Upsilon(10570), electroproduction', 'electroproduction, Upsilon(10570)', 'B, pair production', 'pair production, B', 'B0, hadronic decay', 'hadronic decay, B0', 'B+, hadronic decay', 'hadronic decay, B+', 'final state, (0charmed particle)', '(0charmed particle), final state', 'B, branching ratio', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508004'],[],['1995-08-08']
2458,['eng'],"['Reeves, P']",['Measurements of $\\alpha_{s}$ from scaling violations and from R$_{\\tau}$ at LEP'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'electron positron, inclusive reaction', 'momentum spectrum, (charged particle)', 'differential cross section, x-dependence', 'x-dependence, differential cross section', 'scaling, violation', 'tau, semileptonic decay', 'semileptonic decay, tau', 'tau, leptonic decay', 'leptonic decay, tau', 'width, ratio', 'correction, nonperturbative', 'strong interaction, coupling constant', 'coupling constant, strong interaction', 'magnetic detector, OPAL', 'magnetic detector, ALEPH', 'experimental results', 'CERN LEP Stor', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507010'],"['The results of two methods to extract the strong coupling constant, \\alpha_s, are reviewed for the LEP experiments. In the first, scaling violations in the scaled momentum distributions of charged particles at LEP and at lower energy experiments are employed. In the second, QCD corrections to R_\\tau, the ratio of hadronic to leptonic decay rates of the tau lepton, determine \\alpha_s and, using moments of the invariant mass distribution in hadronic tau decays, the non-perturbative corrections to R_\\tau.']",['1995-07-20']
2459,['eng'],"['Spadafora, A L']",['Measurements of the W and Z inclusive cross sections and determination of the W decay width'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'intermediate boson, leptonic decay', 'leptonic decay, intermediate boson', 'channel cross section, branching ratio', 'W, width', 'quantum chromodynamics', 'electroweak interaction, validity test', 'validity test, electroweak interaction', 'mass spectrum', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'anti-p p --> Z0 anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507012'],"['Recent results on the production of W and Z gauge bosons in p\\bar{p} collisions at \\sqrt{s}=1.8~TeV at the Fermilab Tevatron Collider from the \\D0 and CDF experiments are reviewed. Measurements of the inclusive cross sections times leptonic branching ratios in both the electron and muon decay channels are summarized and compared to QCD predictions. Using the ratio R = {\\sigma_W \\cdot B(W\\rightarrow l\\nu)}/ {\\sigma_Z \\cdot B(Z\\rightarrow ll)} and assuming standard model couplings, an indirect determination of the W decay width is obtained. By comparing this measured value with the predicted value for the W width, a limit on the deviation from the standard model is obtained.']",['1995-07-20']
2460,['eng'],"['Levy, A']",['Measurement of elastic $\\varrho^{0}$ photoproduction at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'photon p, interaction', 'interaction, photon p', 'mass spectrum, (pi+ pi-)', '(pi+ pi-), mass spectrum', 'rho(770)0, photoproduction', 'photoproduction, rho(770)0', 'elastic scattering, rho(770) p', 'rho(770) p, elastic scattering', 'differential cross section, energy dependence', 'energy dependence, differential cross section', 'channel cross section', 'rho(770)0, polarization', 'polarization, rho(770)0', 'polarization, transverse', 'transverse, polarization', 'helicity, conservation law', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', '60-80 GeV-cms (photon)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507011'],"['Elastic \\rho^0 photoproduction has been measured using the ZEUS detector at HERA. Untagged photoproduction events from ep interactions were used to measure the reaction \\gamma p \\rightarrow \\rho^0 p (\\rho^0 \\rightarrow \\pi^+ \\pi^-) at photon-proton centre-of-mass energies between 60 and 80~GeV and |t|<0.5~GeV^2, where t is the square of the four-momentum transferred at the proton vertex. The differential cross section d\\sigma/dM_{\\pi\\pi}, where M_{\\pi\\pi} is the invariant mass of the two pions, and the integrated cross section, \\sigma_{\\gamma p\\rightarrow \\rho^0 p}, are presented; the latter was measured to be 14.7\\pm 0.4~(\\mbox{stat.})~\\pm2.4~(\\mbox{syst.})~\\mu\\mbox{b}. The differential cross section d\\sigma/dt has an approximately exponential shape; a fit of the type A^{\\prime}_{t} \\exp{(-b^{\\prime}_{t}|t| + c^{\\prime}_{t} t^2)} yields a t-slope b^{\\prime}_{t}= 9.9~\\pm~1.2~(\\mbox{stat.})~\\pm 1.4~(\\mbox{syst.})~\\mu\\mbox{b}. The results, when compared to low energy data, show a weak energy dependence of both \\sigma_{\\gamma p\\rightarrow \\rho^0 p} and of the t-slope. The \\rho^0 is produced predominantly with transverse polarisation, demonstrating that s-channel helicity conservation holds at these energies.']",['1995-07-20']
2461,['eng'],"['Albrecht, R']",['Production of $\\eta$ mesons in 200 AGeV S+S and S+Au reactions'],['Particle Physics - Experimental Results'],"['nucleus nucleus, nuclear reaction', 'scattering, heavy ion', 'heavy ion, scattering', 'sulfur', 'gold', 'mass spectrum, (2photon)', '(2photon), mass spectrum', 'pi0, hadroproduction', 'hadroproduction, pi0', 'eta, hadroproduction', 'hadroproduction, eta', 'differential cross section', 'spectrometer, lead-glass', 'calorimeter, experimental results', 'CERN SPS', '200 GeV/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507009'],"['Minimum Bias production cross sections of \\eta mesons have been measured in 200~AGeV S+Au and S+S collisions at the CERN SPS by reconstructing the \\eta\\rightarrow\\gamma\\gamma decay. The measurements have been made over the rapidity range 2.1 \\leq y \\leq 2.9 using the leadglass spectrometer of WA80. Within the statistical and systematical uncertainties the spectral shapes of \\pi^0 and \\eta mesons yields are identical when their invariant differential cross section is plotted as a function of the transverse mass. The relative normalization of the \\eta to \\pi^0 transverse mass spectra is found to be 0.53 \\pm 0.07 for S+Au and 0.43 \\pm 0.15 for S+S reactions. Extrapolation to full phase space leads to an integrated cross section ratio of \\eta to \\pi^0 mesons of 0.15 \\pm 0.02 {\\rm (stat.)} \\pm 0.02 {\\rm (syst.)}, and 0.12 \\pm 0.03 {\\rm (stat.)} \\pm 0.02 {\\rm (syst.)} for S+Au and S+S collisions, respectively.']",['1995-07-25']
2462,['eng'],"['Chan, A H']",['Measurables of CP violation in B$_{d}$ --> D$^{0}_{CP}$K$_{S}$ at a B-meson factory'],['Particle Physics - Experimental Results'],"['B0, hadronic decay', 'hadronic decay, B0', 'violation, CP', 'Kobayashi-Maskawa angle', 'B, particle source', 'proposed experiment', 'numerical calculations', 'B0 --> D0 K0(S)', 'B0 --> pi+ pi-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507008'],"['In the context of the standard electroweak model, we emphasize that B_d\\rightarrow D^0_{CP}K_S (D^0_{CP} denotes a CP eigenstate of D^0 or \\bar{D}^0) can compete with B_d\\rightarrow \\pi^+\\pi^- in studying CP violation and probing the Cabibbo-Kobayashi-Maskawa unitarity triangle. We discuss the measurables of direct and indirect CP asymmetries in B^0_d vs \\bar{B}^0_d\\rightarrow D^0_{CP}K_S under the circumstance of an asymmetric B-meson factory running on the \\Upsilon(4S) resonance, and show that both the weak and strong phases are experimentally determinable even in the presence of unknown final-state interactions.']",['1995-07-17']
2463,['eng'],"['Jeon, H', 'Longo, M']",['Search for magnetic monopoles trapped in matter'],['Particle Physics - Experimental Results'],"['postulated particle, magnetic monopole', 'search for, magnetic monopole', 'at rest', 'matter', 'superconducting, interference', 'interference, superconducting', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9508003'],"['There have been many searches for magnetic monopoles in flight, but few for monopoles in matter. We have searched for magnetic monopoles in meteorites, schists, ferromanganese nodules, iron ores and other materials. The detector was a superconducting induction coil connected to a SQUID (Superconducting Quantum Interference Device) with a room temperature bore 15 cm in diameter. We tested a total of more than 331 kg of material including 112 kg of meteorites. We found no monopole and conclude the overall monopole/nucleon ratio in the samples is <1.2 \\times 10^{-29} with a 90\\% confidence level.']",['1995-08-03']
2464,['eng'],"['Müller, U']",['Measurement of the $\\omega_{c}$ lifetime'],['Particle Physics - Experimental Results'],"['Sigma nucleus, nuclear reaction', 'carbon', 'copper', 'Sigma-, secondary beam', 'secondary beam, Sigma-', 'hyperon, production', 'production, hyperon', 'forward spectrometer, experimental results', 'CERN SPS', 'Omega/c0, hadroproduction', 'hadroproduction, Omega/c0', 'Omega/c0, decay modes', 'decay modes, Omega/c0', 'Omega/c0, lifetime', 'Omega/c0 --> Omega- 2pi+ pi-', 'Omega/c0 --> Xi- K- 2pi+', '340 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507004'],"['We present the measurement of the lifetime of the Omega_c we have performed using three independent data samples from two different decay modes. Using a Sigma- beam of 340 GeV/c we have obtained clean signals for the Omega_c decaying into Xi- K- pi+ pi+ and Omega- pi+ pi- pi+, avoiding topological cuts normally used in charm analysis. The short but measurable lifetime of the Omega_c is demonstrated by a clear enhancement of the signals at short but finite decay lengths. Using a continuous maximum likelihood method we determined the lifetime to be tau(Omega_c) = 55 +13-11(stat) +18-23(syst) fs. This makes the Omega_c the shortest living weakly decaying particle observed so far. The short value of the lifetime confirms the predicted pattern of the charmed baryon lifetimes and demonstrates that the strong interaction plays a vital role in the lifetimes of charmed hadrons.']",['1996-05-02']
2465,['eng'],"['Abachi, S']",['Second generation leptoquark search in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'postulated particle, leptoquark', 'search for, leptoquark', 'leptoquark, pair production', 'pair production, leptoquark', 'leptoquark, semileptonic decay', 'semileptonic decay, leptoquark', 'channel cross section, branching ratio', 'mass, leptoquark', 'leptoquark, mass', 'lower limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2leptoquark anything', 'leptoquark --> quark muon', 'leptoquark --> quark neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507002'],['We report on a search for second generation leptoquarks with the D\\O\\ detector at the Fermilab Tevatron p\\overline{p} collider at \\sqrt{s} = 1.8 TeV. This search is based on 12.7 pb^{-1} of data. Second generation leptoquarks are assumed to be produced in pairs and to decay into a muon and quark with branching ratio \\beta or to neutrino and quark with branching ratio (1-\\beta). We obtain cross section times branching ratio limits as a function of leptoquark mass and set a lower limit on the leptoquark mass of 111 GeV/c^{2} for \\beta = 1 and 89 GeV/c^{2} for \\beta = 0.5 at the 95\\%\\ confidence level.'],['1996-05-02']
2466,['eng'],"['Sidwell, R A']",['Search for the flavor-changing neutral-current decays D$^{+}$ --> $\\pi^{+}\\mu^{+}\\mu^{-}$ and D$^{+}$ --> $\\pi^{+}$e+e-'],['Particle Physics - Experimental Results'],"['pi- nucleus, interaction', 'interaction, pi- nucleus', 'D+, hadroproduction', 'hadroproduction, D+', 'D+, semileptonic decay', 'semileptonic decay, D+', 'D+, branching ratio', 'upper limit', 'neutral current, flavor changing', 'mass spectrum', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D+ --> pi+ muon+ muon-', 'D+ --> pi+ positron electron', '500 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507003'],"['We report the results of a search for the flavor-changing neutral-current decays D^+\\rightarrow \\pi^+ \\mu^+ \\mu^- and D^+\\rightarrow \\pi^+ e^+ e^- in data from Fermilab charm hadroproduction experiment E791. No signal above background is found, and we obtain upper limits on branching fractions, B(D^+\\rightarrow \\pi^+ \\mu^+ \\mu^-) < 1.8 \\times 10^{-5} and B(D^+\\rightarrow \\pi^+ e^+ e^-) < 6.6 \\times 10^{-5}, at the 90\\% confidence level.']",['1996-05-02']
2467,['eng'],"['Levy, A']",['Exclusive $\\varrho^{0}$ production in deep inelastic electron-proton scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, exclusive reaction', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'rho(770)0, electroproduction', 'electroproduction, rho(770)0', 'rho(770)0, photoproduction', 'photoproduction, rho(770)0', 'rho(770)0, hadronic decay', 'hadronic decay, rho(770)0', 'mass spectrum, (pi+ pi-)', '(pi+ pi-), mass spectrum', 'gluon, momentum spectrum', 'quantum chromodynamics, perturbation theory', 'channel cross section, momentum transfer', 'channel cross section, energy dependence', 'channel cross section, x-dependence', 'transverse momentum, spectra', 'spectra, transverse momentum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'electron p --> p rho(770)0 electron', 'photon p --> p rho(770)0', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9507001'],"[""The exclusive production of \\rho^0 mesons in deep inelastic electron-proton scattering has been studied using the ZEUS detector. Cross sections have been measured in the range 7 < Q^2 < 25 GeV^2 for \\gamma^*p centre of mass (c.m.) energies from 40 to 130 GeV. The \\gamma^*p \\rightarrow \\rho^0 p cross section exhibits a Q^{-(4.2 \\pm 0.8 ^{+1.4}_{-0.5})} dependence and both longitudinally and transversely polarised \\rho^0's are observed. The \\gamma^*p \\rightarrow \\rho^0 p cross section rises strongly with increasing c.m. energy, when compared with NMC data at lower energy, which cannot be explained by production through soft pomeron exchange. The data are compared with perturbative QCD calculations where the rise in the cross section reflects the increase in the gluon density at low x. the gluon density at low x.""]",['1996-05-02']
2468,['eng'],"['Holzscheiter, M H', 'Feng, X', 'Goldman, T', 'King, N S P', 'Lewis, R A', 'Nieto, Michael Martin', 'Smith, G A']",['Are antiprotons forever?'],['Particle Physics - Experimental Results'],"['anti-p, confinement', 'magnetic field, confinement', 'energy, low', 'anti-p nucleon, annihilation', 'annihilation, anti-p nucleon', 'energy dependence', 'anti-p, energy spectrum', 'energy spectrum, anti-p', 'time dependence', 'scintillation counter, experimental results', 'CERN LEAR']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506015'],"['Up to one million antiprotons from a single LEAR spill have been captured in a large Penning trap. Surprisingly, when the antiprotons are cooled to energies significantly below 1 eV, the annihilation rate falls below background. Thus, very long storage times for antiprotons have been demonstrated in the trap, even at the compromised vacuum conditions imposed by the experimental set up. The significance for future ultra-low energy experiments, including portable antiproton traps, is discussed.']",['1995-06-29']
2469,['eng'],"['Silagadze, Z K']",['A new algorithm for automatic photopeak searches'],['Detectors and Experimental Techniques'],"['semiconductor detector, readout', 'scintillation counter, readout', 'energy spectrum, (photon)', '(photon), energy spectrum', 'statistical analysis']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506013'],"['A new, ""quantum mechanical"" algorithm is proposed for automatic photopeak location in gamma-ray spectra from semiconductor and scintillator detectors.']",['1995-06-20']
2470,['eng'],[],['Measurement of the proton structure function F$_{2}$ and the extraction of the gluon density at small x'],['Particle Physics - Experimental Results'],"['talk', 'electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'p, structure function', 'structure function, small-x', 'gluon, momentum spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506011'],['In the following article we describe our measurement of the proton structure function F_2 and of the gluon momentum density xg in ep collisions with the ZEUS detector at HERA in 1993. The results for F_2 confirm our measurement from the previous year but with much higher statistics and show a strong rise towards small x. The gluon momentum density xg is measured for the first time in a range from 4 \\cdot 10^{-4} < x < 10^{-2} at a value of Q^2 = 20~GeV^2.'],['1995-06-20']
2471,['eng'],[],['Transverse energy and forward jet production in the low x regime at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'transverse energy, energy flow', 'rapidity dependence', 'jet, electroproduction', 'electroproduction, jet', 'production, small-angle', 'small-angle, production', 'x-dependence', 'dependence, momentum transfer', 'Altarelli-Parisi equation', 'Lipatov equation', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506012'],"['The production of transverse energy in deep inelastic scattering is measured as a function of the kinematic variables x and Q^2 using the H1 detector at the ep collider HERA. The results are compared to the different predictions based upon two alternative QCD evolution equations, namely the Dokshitzer-Gribov-Lipatov-Altarelli-Pa risi (DGLAP) and the Balitsky-Fadin-Kuraev-Lipatov (BFKL) equations. In a pseudorapidity interval which is central in the hadronic centre of mass system between the current and the proton remnant fragmentation region the produced transverse energy increases with decreasing x for constant Q^2. Such a behaviour can be explained with a QCD calculation based upon the BFKL ansatz. The rate of forward jets, proposed as a signature for BFKL dynamics, has been measured.']",['1995-06-20']
2472,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Cartiglia, N', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Hultschig, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Kochocki, J A', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Diffractive hard photoproduction at HERA and evidence for the gluon content of the pomeron'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'jet, electroproduction', 'electroproduction, jet', 'rapidity, gap', 'transverse energy, high', 'hard scattering', 'diffraction', 'exchange, pomeron', 'pomeron, exchange', 'structure function, pomeron', 'quantum chromodynamics, perturbation theory', 'Regge poles', 'gluon', 'differential cross section, rapidity dependence', 'rapidity dependence, differential cross section', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'electron p --> jet anything', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506009'],['Inclusive jet cross sections for events with a large rapidity gap with respect to the proton direction from the reaction ep \\rightarrow jet \\; + \\; X with quasi-real photons have been measured with the ZEUS detector. The cross sections refer to jets with transverse energies E_T^{jet}>8~GeV. The data show the characteristics of a diffractive process mediated by pomeron exchange. Assuming that the Wodarczy'],['1995-06-19']
2473,['eng'],[],['A limit on $\\nu_{\\mu}$($\\overline{\\nu}_{\\mu}$) -->$\\nu_{\\tau}$($\\overline{\\nu}_{\\tau}$) oscillations from a precision measurement of neutrino-nucleon neutral current interactions'],['Particle Physics - Experimental Results'],"['neutrino nucleon, interaction', 'interaction, neutrino nucleon', 'neutral current', 'charged current', 'neutrino, oscillation', 'neutrino/e', 'neutrino/mu', 'neutrino/tau', 'neutrino, path length', 'energy', 'neutrino, mass difference', 'mass difference, neutrino', 'neutrino, mixing angle', 'calorimeter, experimental results', 'Batavia TEVATRON PS', '30-500 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506007'],['We present a limit on \\nu_\\mu(\\overline{\\nu}_\\mu)\\to\\nu_\\tau(\\overline{\\nu}_\\tau) oscillations based on a study of inclusive \\nu N interactions performed using the CCFR massive coarse grained detector in the FNAL Tevatron Quadrupole Triplet neutrino beam. The sensitivity to oscillations is from the difference in the longitudinal energy deposition pattern of \\nu_\\mu N versus \\nu_\\tau N charged current interactions. The \\nu_\\mu energies ranged from 30 to 500~GeV with a mean of 140~GeV. The minimum and maximum \\nu_\\mu flight lengths are 0.9~km and 1.4~km respectively. The lowest 90\\% confidence upper limit in \\sin^22\\alpha of 2.7\\times 10^{-3} is obtained at \\Delta m^2\\sim50~eV^2. This result is the most stringent limit to date for 25<\\Delta m^2<90~eV^2.'],['1995-06-16']
2474,['eng'],"['Harris, R M']","['Search for new particles decaying to dijets, bottom quarks, and top quarks at CDF']",['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'new particle, search for', 'postulated particle, nonleptonic decay', 'nonleptonic decay, postulated particle', 'quark, beauty', 'quark, truth', 'quark, pair production', 'pair production, quark', 'mass spectrum, (2jet)', '(2jet), mass spectrum', 'angular distribution', 'postulated particle, axigluon', 'quark, excited state', 'quark, diquark', 'rho(770), technicolor', ""postulated particle, W'"", ""postulated particle, Z'"", 'model, topcolor', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506008'],"[""We present three searches for new particles at CDF. First, using 70 pb^-1 of data we search the dijet mass spectrum for resonances. There is an upward fluctuation near 550 GeV (2.6 sigma) with an angular distribution that is adequately described by either QCD alone or QCD plus 5% signal. There is insufficient evidence to claim a signal, but we set the most stringent mass limits on the hadronic decays of axigluons, excited quarks, technirhos, W', Z', and E6 diquarks. Second, using 19 pb^-1 of data we search the b-tagged dijet mass spectrum for b anti-b resonances. Again, an upward fluctuation near 600 GeV (2 sigma) is not significant enough to claim a signal, so we set the first mass limits on topcolor bosons. Finally, using 67 pb^-1 of data we search the top quark sample for t anti-t resonances like a topcolor Z'. Other than an insignificant shoulder of 6 events on a background of 2.4 in the mass region 475-550 GeV, there is no evidence for new particle production. Mass limits, currently in progress, should be sensitive to a topcolor Z' near 600 GeV. In all three searches there is insufficient evidence to claim new particle production, yet there is an exciting possibility that the upward fluctuations are the first signs of new physics beyond the standard model.""]",['1995-06-16']
2475,['eng'],[],['Study of t$\\overline{t}$ production in p$\\overline{p}$ collisions using total transverse energy'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'final state, (W (n)jet)', '(W (n)jet), final state', 'W, decay modes', 'decay modes, W', 'transverse energy, energy spectrum', 'energy spectrum, transverse energy', 'background', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506006'],"['We analyze a sample of W + jet events collected with the Collider Detector at Fermilab (CDF) in ppbar collisions at sqrt(s) = 1.8 TeV to study ttbar production. We employ a simple kinematical variable ""H"", defined as the scalar sum of the transverse energies of the lepton, neutrino and jets. For events with a W boson and four or more jets, the shape of the ""H"" distribution deviates by 3.8 standard deviations from that expected from known backgrounds to ttbar production. However this distribution agrees well with a linear combination of background and ttbar events, the agreement being best for a top mass of 180 GeV/c^2.']",['1995-06-14']
2476,['eng'],"['Hayashii, H']",['Jet production in $\\gamma\\gamma$ collisions at TRISTAN with the TOPAZ detector'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, inelastic scattering', 'inelastic scattering, electron positron', 'exchange, two-photon', 'two-photon, exchange', 'photon photon, interaction', 'interaction, photon photon', 'jet, photoproduction', 'photoproduction, jet', 'jet, electroproduction', 'electroproduction, jet', 'transverse momentum, spectra', 'spectra, transverse momentum', 'jet, energy flow', 'mass spectrum, (2jet)', '(2jet), mass spectrum', 'angular distribution, correlation', 'correlation, angular distribution', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', '58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506005'],['Jet production in \\gamma \\gamma collisions have been studied with a jet-cone algorithm using a 233 pb^{-1} data taken by the TOPAZ detector at the TRISTAN e^+e^- collider. The transverse momentum dependence of the jet-cross section as well as accompanying activities in the small-angle region show the direct evidence for the resolved photon processes. We also present some properties of the two-jet sample with the emphasis on their correlation with the remnant-jet activity.'],['1995-06-09']
2477,['eng'],"['Aïd, S', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Babaev, A', 'Bähr, J', 'Bán, J', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Brasse, F W', 'Braunschweig, W', 'Brisson, V', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Campbell, A J', 'Carli, T', 'Charles, F', 'Charlet, M', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Colombo, M G', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Coutures, C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'Delcourt, B', 'Del Buono, L', 'de Roeck, A', 'De Wolf, E A', 'Di Nezza, P', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duboc, J', 'Düllmann, D', 'Dünger, O', 'Duhm, H', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Erlichmann, H', 'Eichenberger, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Evrard, E', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Forbush, M', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Görlich, L', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'González-Pineiro, B', 'Gorelov, I V', 'Goritchev, P A', 'Grab, C', 'Grässler, H', 'Grässler, R', 'Greenshaw, T J', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Haack, J', 'Haidt, D', 'Hajduk, L', 'Hamon, O', 'Hampel, M', 'Hapke, M', 'Haynes, W J', 'Heatherington, J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hill, P', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Höppner, M', 'Horisberger, R P', 'Hudgson, V L', 'Huet, Patrick', 'Hütte, M', 'Hufnagel, H', 'Ibbotson, M', 'Itterbeck, H', 'Jabiol, M A', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Jönsson, L B', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Kalmus, Peter I P', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Ko, W', 'Köhler, T', 'Köhne, J H', 'Kolanoski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krämerkämper, T', 'Krasny, M W', 'Krehbiel, H', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Küster, H', 'Kuhlen, M', 'Kurca, T', 'Kurzhöfer, J', 'Kuznik, B', 'Lacour, D', 'Lamarche, F', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Lanius, P', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindström, G', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lohmander, H', 'Lomas, J', 'López, G C', 'Lubimov, V', 'Lüke, D', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Masson, S', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Mercer, D', 'Merz, T', 'Meyer, C A', 'Meyer, H', 'Meyer, J', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Müller, G', 'Müller, K', 'Murín, P', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Peppel, E', 'Pérez, E', 'Phillips, J P', 'Pichler, C', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Rabbertz, K', 'Rädel, G', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Ribarics, P', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riess, S', 'Rietz, M', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rüter, K', 'Rusakov, S V', 'Rybicki, K', 'Rylko, R', 'Sahlmann, N', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'von Schlippe, W', 'Schmidt, D', 'Schmidt, G', 'Schöning, A', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Sciacca, G F', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Stella, B', 'Stephens, K', 'Stier, J', 'Stiewe, J', 'Stösslein, U', 'Stolze, K', 'Strachota, J', 'Straumann, U', 'Struczinski, W', 'Sutton, J P', 'Tapprogge, Stefan', 'Chernyshov, V', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van den Plas, D', 'Van Esch, P', 'Van Mechelen, P', 'Vartapetian, A H', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wellisch, H P', 'West, L R', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wright, A E', 'Wünsch, E', 'Wulff, N', 'Yiou, T P', 'Zácek, J', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zimmermann, W', 'Zomer, F', 'Zuber, K', 'Zur Nedden, M']",['Measurement of the e$^{+}$ and e$^{-}$ induced charged current cross sections at HERA'],['Particle Physics - Experimental Results'],"['positron p, colliding beams', 'colliding beams, positron p', 'electron p, colliding beams', 'colliding beams, electron p', 'hadron, multiple production', 'multiple production, hadron', 'charged current', 'transverse momentum, high', 'channel cross section', 'W, propagator', 'mass, propagator', 'propagator, mass', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms', 'electron p --> (n)hadron neutrino/e', 'positron p --> (n)hadron antineutrino/e']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506002'],"['The cross sections for the charged current processes {e^{-}p}\\rightarrow{\\nu_e+hadrons} and, for the first time, {e^{+}p}\\rightarrow{\\overline{\\nu}_e+hadrons} are measured at HERA for transverse momenta larger than 25 GeV.']",['1995-06-06']
2478,['eng'],[],['Measurement of the $\\tau$ lifetime at SLD'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, leptonic decay', 'leptonic decay, Z0', 'tau, pair production', 'pair production, tau', 'tau, decay modes', 'decay modes, tau', 'tau, lifetime', 'decay, path length', 'path length, decay', 'track data analysis, impact parameter', 'semiconductor detector, vertex', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.2 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506004'],"['A measurement of the lifetime of the tau lepton has been made using a sample of 1671 Z^0\\rightarrow\\tau^+\\tau^- decays collected by the SLD detector at SLC. The measurement benefits from the small and stable collision region at SLC and the precision vertex detector of SLD. Three analysis techniques have been used: decay length, impact parameter, and impact parameter difference methods. The combined result is \\tau_\\tau = 297\\pm 9(stat.)\\pm 5(syst.) fs.']",['1995-06-06']
2479,['eng'],"['Aïd, S', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Babaev, A', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Brasse, F W', 'Braunschweig, W', 'Brisson, V', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Bán, J', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Campbell, A J', 'Carli, T', 'Charles, F', 'Charlet, M', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Colombo, M G', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Coutures, C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'De Wolf, E A', 'Del Buono, L', 'Delcourt, B', 'Di Nezza, P', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duboc, J', 'Duhm, H', 'Düllmann, D', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichenberger, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Erlichmann, H', 'Evrard, E', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Forbush, M', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'González-Pineiro, B', 'Gorelov, I V', 'Goritchev, P A', 'Grab, C', 'Greenshaw, T J', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Haidt, D', 'Hajduk, L', 'Hamon, O', 'Hampel, M', 'Hapke, M', 'Haynes, W J', 'Heatherington, J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hill, P', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Horisberger, R P', 'Hudgson, V L', 'Huet, Patrick', 'Hufnagel, H', 'Höppner, M', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jabiol, M A', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Ko, W', 'Kolanoski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Kuhlen, M', 'Kurca, T', 'Kurzhöfer, J', 'Kuznik, B', 'Köhler, T', 'Köhne, J H', 'Küster, H', 'Lacour, D', 'Lamarche, F', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Lanius, P', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindström, G', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lohmander, H', 'Lomas, J', 'Lubimov, V', 'López, G C', 'Lüke, D', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Masson, S', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Mercer, D', 'Merz, T', 'Meyer, C A', 'Meyer, H', 'Meyer, J', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Peppel, E', 'Phillips, J P', 'Pichler, C', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Pérez, E', 'Rabbertz, K', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Ribarics, P', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riess, S', 'Rietz, M', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rylko, R', 'Rädel, G', 'Rüter, K', 'Sahlmann, N', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schöning, A', 'Sciacca, G F', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Stella, B', 'Stephens, K', 'Stier, J', 'Stiewe, J', 'Stolze, K', 'Strachota, J', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Tapprogge, Stefan', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Van den Plas, D', 'Vartapetian, A H', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wellisch, H P', 'West, L R', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wright, A E', 'Wulff, N', 'Wünsch, E', 'Yiou, T P', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zimmermann, W', 'Zomer, F', 'Zuber, K', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']",['The gluon density of the proton at low x from a QCD analysis of F$_{2}$'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'p, structure function', 'structure function, small-x', 'gluon, momentum spectrum', 'quantum chromodynamics, perturbation theory', 'scaling, violation', 'Altarelli-Parisi equation', 'Lipatov equation', 'differential equations, solution', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506001'],"['We present a QCD analysis of the proton structure function F_2 measured by the H1 experiment at HERA, combined with data from previous fixed target experiments. The gluon density is extracted from the scaling violations of F_2 in the range 2\\cdot 10^{-4}<x<3\\cdot 10^{-2} and compared with an approximate solution of the QCD evolution equations. The gluon density is found to rise steeply with decreasing x.']",['1995-06-05']
2480,['eng'],"['Aïd, S', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Babaev, A', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Brasse, F W', 'Braunschweig, W', 'Brisson, V', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Bán, J', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Campbell, A J', 'Carli, T', 'Charles, F', 'Charlet, M', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Colombo, M G', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Coutures, C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'De Wolf, E A', 'Del Buono, L', 'Delcourt, B', 'Di Nezza, P', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duboc, J', 'Duhm, H', 'Düllmann, D', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichenberger, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Erlichmann, H', 'Evrard, E', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Forbush, M', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'González-Pineiro, B', 'Gorelov, I V', 'Goritchev, P A', 'Grab, C', 'Greenshaw, T J', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Haidt, D', 'Hajduk, L', 'Hamon, O', 'Hampel, M', 'Hapke, M', 'Haynes, W J', 'Heatherington, J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hill, P', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Horisberger, R P', 'Hudgson, V L', 'Huet, Patrick', 'Hufnagel, H', 'Höppner, M', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jabiol, M A', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Ko, W', 'Kolanoski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Kuhlen, M', 'Kurca, T', 'Kurzhöfer, J', 'Kuznik, B', 'Köhler, T', 'Köhne, J H', 'Küster, H', 'Lacour, D', 'Lamarche, F', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Lanius, P', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindström, G', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lohmander, H', 'Lomas, J', 'Lubimov, V', 'López, G C', 'Lüke, D', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Masson, S', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Mercer, D', 'Merz, T', 'Meyer, C A', 'Meyer, H', 'Meyer, J', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Peppel, E', 'Phillips, J P', 'Pichler, C', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Pérez, E', 'Rabbertz, K', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Ribarics, P', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riess, S', 'Rietz, M', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rylko, R', 'Rädel, G', 'Rüter, K', 'Sahlmann, N', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schöning, A', 'Sciacca, G F', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Stella, B', 'Stephens, K', 'Stier, J', 'Stiewe, J', 'Stolze, K', 'Strachota, J', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Tapprogge, Stefan', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Van den Plas, D', 'Vartapetian, A H', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wellisch, H P', 'West, L R', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wright, A E', 'Wulff, N', 'Wünsch, E', 'Yiou, T P', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zimmermann, W', 'Zomer, F', 'Zuber, K', 'Zur Nedden, M', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']",['A direct determination of the gluon density in the proton at low x'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'fusion, photon gluon', 'jet, multiple production', 'multiple production, jet', 'p, structure function', 'gluon, momentum spectrum', 'statistical analysis', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'electron p --> 3jet anything', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505014'],['A leading order determination of the gluon density in the proton has been performed in the fractional momentum range 1.9 \\cdot 10^{-3} < x_{g/p} < 0.18 by measuring multi-jet events from boson-gluon fusion in deep-inelastic scattering with the H1 detector at the electron-proton collider HERA. This direct determination of the gluon density was performed in a kinematic region previously not accessible. The data show a considerable increase of the gluon density with decreasing fractional momenta of the gluons.'],['1995-05-31']
2481,['eng'],"['Kirkby, D']",['A study of hadronic backgrounds to isolated hard photon production with L3'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, annihilation', 'annihilation, electron positron', 'photon, direct production', 'direct production, photon', 'background, hadronic', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'neutral particle, radiative decay', 'radiative decay, neutral particle', 'pi0', 'eta', 'energy, cluster', 'neural network', 'mass spectrum, two-photon', 'two-photon, mass spectrum', 'Higgs particle, hadroproduction', 'hadroproduction, Higgs particle', 'Higgs particle, radiative decay', 'radiative decay, Higgs particle', 'numerical calculations, Monte Carlo', 'experimental methods', 'magnetic detector, L3']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505012'],"['I describe two methods for studying hadronic backgrounds to prompt photon production with L3, and compare the observed background rates with Monte Carlo predictions. I find that the Monte Carlo models JETSET and HERWIG underestimate the production of isolated neutral hadrons in hadronic Z decays at LEP. By extrapolating results obtained with L3, I estimate that the rate of prompt-photon + jet background to a H -> gamma gamma search at the LHC will be larger than Monte Carlo predictions by a factor of 1.5-2.5.']",['1995-05-25']
2482,['eng'],[],['W and Z boson production in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 Tev'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'intermediate boson, leptonic decay', 'leptonic decay, intermediate boson', 'channel cross section, branching ratio', 'W, width', 'mass, transverse', 'transverse, mass', 'mass spectrum, dilepton', 'dilepton, mass spectrum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'anti-p p --> Z0 anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505013'],"['The inclusive cross sections times leptonic branching ratios for W and Z boson production in PbarP collisions at Sqrt(s)=1.8 TeV were measured using the D0 detector at the Fermilab Tevatron collider: Sigma_W*B(W->e, nu) = 2.36 +/- 0.07 +/- 0.13 nb, Sigma_W*B(W->mu,nu) = 2.09 +/- 0.23 +/- 0.11 nb, Sigma_Z*B(Z-> e, e) = 0.218 +/- 0.011 +/- 0.012 nb, Sigma_Z*B(Z->mu,mu) = 0.178 +/- 0.030 +/- 0.009 nb. The first error is the combined statistical and systematic uncertainty, and the second reflects the uncertainty in the luminosity. For the combined electron and muon analyses we find: [Sigma_W*B(W->l,nu)]/[Sigma_Z*B(Z->l,l)] = 10.90 +/- 0.49. Assuming Standard Model couplings, this result is used to determine the width of the W boson: Gamma(W) = 2.044 +/- 0.093 GeV.']",['1995-05-26']
2483,['eng'],"['Skarha, J']",['CDF results on B decays'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 1995/02/20', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'beautiful meson, hadroproduction', 'hadroproduction, beautiful meson', 'beautiful meson, nonleptonic decay', 'nonleptonic decay, beautiful meson', 'beautiful meson, semileptonic decay', 'semileptonic decay, beautiful meson', 'beautiful meson, rare decay', 'rare decay, beautiful meson', 'B+, lifetime', 'B0, lifetime', 'beautiful meson, branching ratio', 'upper limit', 'mass spectrum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B --> psi mesons strange meson', 'B --> charmed meson lepton neutrino', 'beautiful meson --> strange meson muon+ muon-', 'beautiful meson --> muon+ muon-', '1800 GeV-cms', 'B/s, lifetime', 'B/s --> psi mesons Phi(1020) anything', 'B/s --> D/s lepton neutrino anything']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9506003'],"['We present recent CDF results on B lifetimes, B meson mass measurements, ratios of branching ratios, and rare decays. In addition we present the first measurement of time-dependent B_d mixing at CDF. Several results have been updated and a few new ones included since the workshop.']",['1995-06-06']
2484,['eng'],[],['Measurement of the diffractive structure function in deep inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'diffraction', 'rapidity, gap', 'exchange, pomeron', 'pomeron, exchange', 'structure function, pomeron', 'structure function, parametrization', 'momentum dependence', 'dependence, momentum transfer', 'scaling', 'sum rule, momentum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505010'],"['This paper presents an analysis of the inclusive properties of diffractive deep inelastic scattering events produced in ep interactions at HERA. The events are characterised by a rapidity gap between the outgoing proton system and the remaining hadronic system. Inclusive distributions are presented and compared with Monte Carlo models for diffractive processes. The data are consistent with models where the pomeron structure function has a hard and a soft contribution. The diffractive structure function is measured as a function of \\xpom, the momentum fraction lost by the proton, of \\beta, the momentum fraction of the struck quark with respect to \\xpom, and of Q^2. The \\xpom dependence is consistent with the form \\xpoma where a~=~1.30~\\pm~0.08~(stat)~^{+~0.08}_{-~0.14}~(sys) in all bins of \\beta and Q^2. In the measured Q^2 range, the diffractive structure function approximately scales with Q^2 at fixed \\beta. In an Ingelman-Schlein type model, where commonly used pomeron flux factor normalisations are assumed, it is found that the quarks within the pomeron do not saturate the momentum sum rule.']",['1995-05-18']
2485,['eng'],"['Derrick, Malcolm']",['Neutral strange particle production in deep inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'strange particle, electroproduction', 'electroproduction, strange particle', 'strange particle, nonleptonic decay', 'nonleptonic decay, strange particle', 'K0(S), multiplicity', 'Lambda, multiplicity', 'transverse momentum, dependence', 'rapidity dependence', 'rapidity, gap', 'diffraction', 'nondiffractive', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'electron p --> K0(S) anything', 'electron p --> Lambda anything', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505011'],"[""This paper presents measurements of \\k\\ and \\lam\\ production in neutral current, deep inelastic scattering of 26.7 GeV electrons and 820 GeV protons in the kinematic range 10 < Q^{2} < 640 GeV^2, 0.0003 < x < 0.01, and y > 0.04. Average multiplicities for \\k\\ and \\lam\\ production are determined for transverse momenta \\ \\ptr\\ > 0.5 GeV and pseudorapidities \\left| \\eta \\right| < 1.3. The multiplicities favour a stronger strange to light quark suppression in the fragmentation chain than found in e^+ e^- experiments. The production properties of \\k's in events with and without a large rapidity gap with respect to the proton direction are compared. The ratio of neutral \\k's to charged particles per event in the measured kinematic range is, within the present statistics, the same in both samples.""]",['1995-05-19']
2486,['eng'],"['Derwent, P F']",['Charm and beauty results from CDF and D0'],['Particle Physics - Experimental Results'],"['review', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, charm', 'quark, beauty', 'quark, hadroproduction', 'hadroproduction, quark', 'J/psi(3100), leptonic decay', 'leptonic decay, J/psi(3100)', 'chi mesons, charm', 'chi mesons, radiative decay', 'radiative decay, chi mesons', 'B, decay modes', 'decay modes, B', 'B/s, decay modes', 'decay modes, B/s', 'B/s, lifetime', 'B0 anti-B0, interference', 'time dependence', 'transverse momentum, spectra', 'spectra, transverse momentum', 'mass spectrum', 'cross section', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505009'],"['Reporting, for the CDF and D0 collaborations, results from the 1992-93 Fermilab Tevatron Collider run concerning charm and beauty quark production and beauty meson decay properties.']",['1995-05-17']
2487,['eng'],"['Aihara, H']",['W$\\gamma$ and Z$\\gamma$ production at Tevatron'],['Particle Physics - Experimental Results'],"['talk, Los Angeles 1995/02/01', 'anti-p p, colliding beams', 'anti-p p, inclusive reaction', 'intermediate boson, hadroproduction', 'intermediate boson, leptonic decay', 'photon, associated production', 'coupling, (3gauge boson)', 'photon, transverse energy', 'mass spectrum, (lepton+ lepton- photon)', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W photon anything', 'anti-p p --> Z0 photon anything', 'W --> lepton neutrino', 'Z0 --> lepton+ lepton-', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505008'],"['We present results from CDF and D\\O\\ on W\\gamma and Z\\gamma productions in p\\bar{p} collisions at \\sqrt{s}=1.8~{\\rm TeV}. The goal of the analyses is to test the non-abelian self-couplings of the W, Z and photon, one of the most direct consequences of the SU(2)_L\\otimes U(1)_Y gauge symmetry. We present direct measurements of WW\\gamma couplings and limits on ZZ\\gamma and Z\\gamma\\gamma couplings, based on p\\bar{p}\\rightarrow \\ell\\nu\\gamma + X and p\\bar{p}\\rightarrow \\ell\\ell\\gamma+X events, respectively, observed during the 1992--1993 run of the Fermilab Tevatron Collider.']",['1995-05-16']
2488,['eng'],"['Abachi, S']",['Measurement of the WW$\\gamma$ gauge boson couplings in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'W, hadroproduction', 'hadroproduction, W', 'photon, associated production', 'associated production, photon', 'coupling, (2W photon)', '(2W photon), coupling', 'W, leptonic decay', 'leptonic decay, W', 'energy spectrum', 'photon, transverse energy', 'W, magnetic moment', 'magnetic moment, W', 'W, electric moment', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> lepton neutrino photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505007'],"['The WW\\gamma gauge boson couplings were measured using p\\bar{p}\\rightarrow \\ell\\nu\\gamma+X (\\ell=e,\\mu) events at \\sqrt{s}=1.8 TeV observed with the {D\\O} detector at the Fermilab Tevatron Collider. The signal, obtained from the data corresponding to an integrated luminosity of 13.8\\ {\\rm pb}^{-1}, agrees well with the Standard Model prediction. A fit to the photon transverse energy spectrum yields limits at the 95\\% confidence level on the CP--conserving anomalous coupling parameters of -1.6<\\Delta\\kappa<1.8 (\\lambda = 0) and -0.6<\\lambda<0.6 (\\Delta\\kappa = 0).']",['1995-05-15']
2489,['eng'],[],"['Shadowing in inelastic scattering of muons on carbon, calcium and lead at low x$_{Bj}$']",['Particle Physics - Experimental Results'],"['muon+ nucleus, inelastic scattering', 'inelastic scattering, muon+ nucleus', 'carbon', 'calcium', 'lead', 'effect, shadowing', 'small-x', 'cross section, ratio', 'x-dependence', 'dependence, mass number', 'mass number, dependence', 'dependence, momentum transfer', 'energy dependence', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'tables', 'approx. 470 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505006'],"['Nuclear shadowing is observed in the per-nucleon cross-sections of positive muons on carbon, calcium and lead as compared to deuterium. The data were taken by Fermilab experiment E665 using inelastically scattered muons of mean incident momentum 470 GeV/c. Cross-section ratios are presented in the kinematic region 0.0001 < XBj <0.56 and 0.1 < Q**2 < 80 GeVc. The data are consistent with no significant nu or Q**2 dependence at fixed XBj. As XBj decreases, the size of the shadowing effect, as well as its A dependence, are found to approach the corresponding measurements in photoproduction.']",['1995-05-11']
2490,['eng'],"['Rybicki, K', 'Rylko, R']",['Momentum correlations of charmed pairs produced in $\\pi^{-}$-Cu interactions at 230 GeV/c'],['Particle Physics - Experimental Results'],"['pi nucleus, inclusive reaction', 'copper', 'charmed particle, pair production', 'pair production, charmed particle', 'momentum, correlation', 'transverse momentum', 'rapidity, difference', 'mass', 'quantum chromodynamics, perturbation theory', 'semiconductor detector, vertex', 'magnetic spectrometer, experimental results', 'CERN SPS', '230 GeV/c']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505005'],"['We study the production characteristics of 557 pairs of charmed hadrons produced in \\pi^{-}-Cu\\ interactions at 230~GeV/c using a momentum estimator for charmed hadrons with missing decay products. We find, the mean value of the transverse momentum squared of the charmed pairs is <\\pts>=(1.98\\pm 0.11\\pm 0.09)\\; GeV^2/c^2, the mean rapidity difference is <|\\yd|>=0.54\\pm 0.02\\pm 0.24, and the mean effective mass is <\\mef>=(4.45\\pm 0.03\\pm 0.13)\\; GeV/c^2. Comparing these results with the next-to-leading order QCD predictions we find an agreement for the \\yd\\ and \\mef, whilst the measured mean value of \\pts\\ is significantly larger than the predicted value.']",['1995-05-09']
2491,['eng'],[],['A study of the fragmentation of quarks in e$^{-}$p collisions at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'hadron, electroproduction', 'electroproduction, hadron', 'quark, fragmentation function', 'x-dependence', 'dependence, momentum transfer', 'kinematics, Breit frame', 'charged particle, multiplicity', 'electron positron, annihilation', 'annihilation, electron positron', 'quark, pair production', 'pair production, quark', 'showers, parton', 'effect, coherence', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505003'],"['Deep inelastic scattering (DIS) events, selected from 1993 data taken by the H1 experiment at HERA, are studied in the Breit frame of reference. The fragmentation function of the quark is compared with those of \\ee data. It is shown that certain aspects of the quarks emerging from within the proton in \\ep interactions are essentially the same as those of quarks pair-created from the vacuum in \\ee annihilation. The measured area, peak position and widthof the fragmentation function show that the kinematic evolution variable, equivalent to the \\ee squared centre of mass energy, is in the Breit frame the invariant square of the four-momentum transfer. We comment on the extent to which we have evidence for coherence effects in parton showers.']",['1995-05-05']
2492,['eng'],"['Kaplan, D M', 'Papavassiliou, V']",['An ultrahigh-statistics charm experiment for the year $\\sim$ 2000'],['Particle Physics - Experimental Results'],"['talk, Rio de Janeiro 1995/02/20', 'p nucleus, inclusive reaction', 'D, hadroproduction', 'hadroproduction, D', 'D0 anti-D0, interference', 'neutral current, flavor changing', 'violation, CP', 'Kobayashi-Maskawa model', 'quantum chromodynamics, perturbation theory', 'validity test', 'magnetic spectrometer, proposed', 'semiconductor detector, silicon', 'scintillation counter, fibre', 'trigger', 'efficiency', 'yield, (charmed particle)', 'numerical calculations, Monte Carlo', 'proposed experiment, Batavia TEVATRON PS', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505002'],"['After reviewing the motivation for high-statistics charm studies, we describe a fixed-target experiment capable of reconstructing >10^8 charm decays. Such an experiment can test the Standard Model and probe non-Standard physics through sensitive searches for such phenomena as D0 mixing, CP violation, and FCNC decays.']",['1995-05-04']
2493,['eng'],"['Inoue, Y', 'Moriyama, S', 'Hara, H', 'Minowa, M', 'Shimokoshi, F']",['A liquid-helium cooled large-area silicon PIN photodiode x-ray detector'],['Detectors and Experimental Techniques'],"['postulated particle, axion', 'axion, solar', 'photoelectron, surface', 'semiconductor, optical', 'helium, liquid', 'energy resolution', 'energy, threshold']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504010'],['An x-ray detector using a liquid-helium cooled large-area silicon PIN photodiode has been developed along with a tailor-made charge sensitive preamplifier whose first-stage JFET has been cooled. The operating temperature of the JFET has been varied separately and optimized. The x- and \\gamma-ray energy spectra for an \\nuc{241}{Am} source have been measured with the photodiode operated at 13 K. An energy resolution of 1.60 keV (FWHM) has been obtained for 60-keV \\gamma rays and 1.30 keV (FWHM) for the pulser. The energy threshold could be set as low as 3 keV. It has been shown that a silicon PIN photodiode serves as a low-cost excellent x-ray detector which covers large area at 13 K.'],['1995-04-28']
2494,['eng'],"['Hill, J E']",['Results from the LSND neutrino oscillation search'],['Particle Physics - Experimental Results'],"['neutrino, oscillation', 'antineutrino p, interaction', 'interaction, antineutrino p', 'charged current', 'positron, neutrinoproduction', 'neutrinoproduction, positron', 'n nucleus, radiative capture', 'radiative capture, n nucleus', 'correlation, (positron photon)', 'neutrino, mass difference', 'mass difference, neutrino', 'neutrino, mixing angle', 'scintillation counter, liquid', 'experimental results', 'LAMPF Linac', 'antineutrino/mu, beam', 'beam, antineutrino/mu', 'antineutrino/e', 'antineutrino/e p --> n positron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504009'],"['The Liquid Scintillator Neutrino Detector (LSND) at the Los Alamos Meson Physics Facility sets bounds on neutrino oscillations in the appearance channel nu_mu_bar --> nu_e_bar by searching for the signature of the reaction nu_e_bar p --> e^+ n: an e^+ followed by a 2.2MeV gamma ray from neutron capture. Five e^{+/-} -- gamma coincidences are observed in time with the LAMPF beam, with an estimated background of 6.2 events. The 90\\% confidence limits obtained are: Delta (m^2) < 0.07eV^2 for sin^2 (2theta) = 1, and sin^2(2theta) < 6 10^{-3} for Delta (m^2) > 20 eV^2.']",['1995-04-26']
2495,['eng'],"['Anlauf, H', 'Dahmen, H D', 'Himmler, A', 'Manakos, P', 'Ohl, T', 'Mannel, T']","['WOPPER, version 1.3']",['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'annihilation, electron positron', 'W, pair production', 'pair production, W', 'W, decay', 'decay, W', 'W, width', 'fermion, electroproduction', 'electroproduction, fermion', 'photon, multiple production', 'multiple production, photon', 'quantum electrodynamics, radiative correction', 'leading logarithm approximation', 'cross section', 'programming, Monte Carlo', 'programming, manual', 'electron positron --> W+ W-', 'W+ W- --> 4fermion (n)photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504006'],['We describe the Monte Carlo event generator WOPPER for four fermion production through W-pairs including resummed leading logarithmic QED radiative corrections.'],['1995-04-20']
2496,['eng'],"['Ohl, T']","['Hepawk, version 1.6']",['Particle Physics - Experimental Results'],"['programming, Monte Carlo', 'programming, manual']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504007'],"['This manual describes version 1.6 of the programming language hepawk, designed for convenient scanning of data structures arising in the simulation of high energy physics events. The interpreter for this language has been implemented in FORTRAN77, therefore hepawk runs on any machine with a FORTRAN77 compiler.']",['1995-04-20']
2497,['eng'],"['Aïd, S', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Babaev, A', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Barschke, R', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Brasse, F W', 'Braunschweig, W', 'Brisson, V', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Bán, J', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Campbell, A J', 'Carli, T', 'Charles, F', 'Charlet, M', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Colombo, M G', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Coutures, C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'De Wolf, E A', 'Del Buono, L', 'Delcourt, B', 'Di Nezza, P', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duboc, J', 'Duhm, H', 'Düllmann, D', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichenberger, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Erlichmann, H', 'Evrard, E', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Forbush, M', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Glazov, A', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'González-Pineiro, B', 'Gorelov, I V', 'Goritchev, P A', 'Grab, C', 'Greenshaw, T J', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Haidt, D', 'Hajduk, L', 'Hamon, O', 'Hampel, M', 'Hapke, M', 'Haynes, W J', 'Heatherington, J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hill, P', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Horisberger, R P', 'Hudgson, V L', 'Huet, Patrick', 'Hufnagel, H', 'Höppner, M', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jabiol, M A', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Ko, W', 'Kolanoski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Kuhlen, M', 'Kurca, T', 'Kurzhöfer, J', 'Kuznik, B', 'Köhler, T', 'Köhne, J H', 'Küster, H', 'Lacour, D', 'Lamarche, F', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Lanius, P', 'Laporte, J F', 'Lebedev, A', 'Lehner, F', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindström, G', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lohmander, H', 'Lomas, J', 'Lubimov, V', 'López, G C', 'Lüke, D', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, G', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Masson, S', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Mercer, D', 'Merz, T', 'Meyer, C A', 'Meyer, H', 'Meyer, J', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Peppel, E', 'Phillips, J P', 'Pichler, C', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Pérez, E', 'Rabbertz, K', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Ribarics, P', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riess, S', 'Rietz, M', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rylko, R', 'Rädel, G', 'Rüter, K', 'Sahlmann, N', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleif, S', 'Schleper, P', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schöning, A', 'Sciacca, G F', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Stella, B', 'Stephens, K', 'Stier, J', 'Stiewe, J', 'Stolze, K', 'Strachota, J', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Tapprogge, Stefan', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Van den Plas, D', 'Vartapetian, A H', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walther, A', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wellisch, H P', 'West, L R', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wright, A E', 'Wulff, N', 'Wünsch, E', 'Yiou, T P', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zimmermann, W', 'Zomer, F', 'Zuber, K', 'Zur Nedden, M', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']",['Leptoquarks and compositeness scales from a contact interaction analysis of deep inelastic e$^{\\pm}$p scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'positron p, colliding beams', 'colliding beams, positron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'positron p, deep inelastic scattering', 'deep inelastic scattering, positron p', 'hadron, multiple production', 'multiple production, hadron', 'postulated particle, leptoquark', 'coupling, leptoquark', 'leptoquark, coupling', 'model, composite', 'differential cross section, momentum transfer', 'momentum transfer, differential cross section', 'electroweak interaction, validity test', 'validity test, electroweak interaction', 'effective Lagrangian, chiral', 'form factor', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'approx. 300 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504008'],"['A contact interaction analysis is presented to search for new phenomena beyond the Standard Model in deep inelastic e^\\pm p \\rightarrow e^\\pm \\, hadrons scattering. The data are collected with the H1 detector at HERA and correspond to integrated luminosities of 0.909 \\ {\\rm pb}^{-1} and 2.947 \\ {\\rm pb}^{-1} for electron and positron beams, respectively. The differential cross sections d\\sigma / dQ^2 are measured in the Q^2 range bet\\-ween 160 \\ \\GeV^2 and 20, 000 \\ \\GeV^2. The absence of any significant deviation from the Standard Model prediction is used to constrain the couplings and masses of new leptoquarks and to set limits on electron--quark compositeness scales and on the radius of light quarks.']",['1995-04-25']
2498,['eng'],"['Adeva, B']",['Large enhancement of deuteron polarization with frequency modulated microwaves'],['Detectors and Experimental Techniques'],"['deuteron, polarized target', 'polarized target, deuteron', 'polarization, enhancement', 'enhancement, polarization', 'RF system, microwaves', 'resonance, magnetic', 'magnetic, resonance', 'CERN SPS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9509014'],"['We report a large enhancement of 1.7 in deuteron polarization up to values of 0.6 due to frequency modulation of the polarizing microwaves in a two liters polarized target using the method of dynamic nuclear polarization. This target was used during a deep inelastic polarized muon-deuteron scattering experiment at CERN. Measurements of the electron paramagnetic resonance absorption spectra show that frequency modulation gives rise to additional microwave absorption in the spectral wings. Although these results are not understood theoretically, they may provide a useful testing ground for the deeper understanding of dynamic nuclear polarization.']",['1995-10-03']
2499,['eng'],"['Abachi, S']",['Measurement of the ZZ$\\gamma$ and Z$\\gamma\\gamma$ couplings in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'Z0, hadroproduction', 'hadroproduction, Z0', 'coupling, (Z0 2photon)', '(Z0 2photon), coupling', 'coupling, (2Z0 photon)', '(2Z0 photon), coupling', 'energy spectrum, (photon)', '(photon), energy spectrum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2lepton photon anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503010'],"['We have directly measured the ZZ-gamma and Z-gamma-gamma couplings by studying p pbar --> l+ l- gamma + X, (l = e, mu) events at the CM energy of 1.8~TeV with the D0 detector at the Fermilab Tevatron Collider. A fit to the transverse energy spectrum of the photon in the signal events, based on the data set corresponding to an integrated luminosity of 13.9 pb^-1 (13.3 pb^-1) for the electron (muon) channel, yields the following 95% confidence level limits on the anomalous CP-conserving ZZ-gamma couplings: -1.9 < h^Z_30 < 1.8 (h^Z_40 = 0), and -0.5 < h^Z_40 < 0.5 (h^Z_30 = 0), for a form-factor scale Lambda = 500 GeV. Limits for the Z-gamma-gamma couplings and CP-violating couplings are also discussed.']",['1995-03-14']
2500,['eng'],"['Abramowicz, H', 'Caldwell, A', 'Sinkus, R']",['Neural network based electron identification in the ZEUS calorimeter'],['Detectors and Experimental Techniques'],"['particle identification, (electron)', 'neural network', 'calorimeter, sandwich', 'uranium', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505004'],"['We present an electron identification algorithm based on a neural network approach applied to the ZEUS uranium calorimeter. The study is motivated by the need to select deep inelastic, neutral current, electron proton interactions characterized by the presence of a scattered electron in the final state. The performance of the algorithm is compared to an electron identification method based on a classical probabilistic approach. By means of a principle component analysis the improvement in the performance is traced back to the number of variables used in the neural network approach.']",['1995-05-08']
2501,['eng'],"['Piotrzkowski, K']",['Observation of the beam-size effect at HERA'],['Particle Physics - Experimental Results'],"['electron p, storage ring', 'luminosity, beam monitoring', 'beam monitoring, luminosity', 'bremsstrahlung', 'effect, beam profile', 'beam profile, effect', 'beam, width', 'width, beam', 'energy spectrum, (photon)', '(photon), energy spectrum', 'numerical calculations, Monte Carlo', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504003'],"['A precise measurement of the spectrum of the photons from ep bremsstrahlung with the ZEUS luminosity monitor at HERA is reported. The measurement shows a reduced rate compared to the Bethe-Heitler spectrum for photon energies below 5~GeV. This suppression, called the beam-size effect, is explained by the finite transverse size of the beam overlap relative to the typical impact parameter in the process of ep bremsstrahlung at HERA energies.']",['1995-04-12']
2502,['eng'],"['Ahmed, T', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Aïd, S', 'Babaev, A', 'Ban, Y', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bergstein, H', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Biddulph, P', 'Bispham, P', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Brasse, F W', 'Braunschweig, W', 'Brisson, V', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Bán, J', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Campbell, A J', 'Carli, T', 'Charles, F', 'Charlet, M', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Colombo, M G', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Coutures, C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Dau, W D', 'Daum, K', 'David, M', 'De Wolf, E A', 'Del Buono, L', 'Delcourt, B', 'Di Nezza, P', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duboc, J', 'Duhm, H', 'Düllmann, D', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichenberger, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Erlichmann, H', 'Evrard, E', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Forbush, M', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Gamerdinger, K', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'González-Pineiro, B', 'Gorelov, I V', 'Goritchev, P A', 'Grab, C', 'Greenshaw, T J', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Haidt, D', 'Hajduk, L', 'Hamon, O', 'Hampel, M', 'Hanlon, E M', 'Hapke, M', 'Haynes, W J', 'Heatherington, J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hill, P', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Horisberger, R P', 'Hudgson, V L', 'Huet, Patrick', 'Hufnagel, H', 'Höppner, M', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jabiol, M A', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Ko, W', 'Kolanoski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Kubenka, J P', 'Kuhlen, M', 'Kurca, T', 'Kurzhöfer, J', 'Kuznik, B', 'Köhler, T', 'Köhne, J H', 'Küster, H', 'Lacour, D', 'Lamarche, F', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Lanius, P', 'Laporte, J F', 'Lebedev, A', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindner, A', 'Lindström, G', 'Link, J', 'Linsel, F', 'Lipinski, J', 'List, B', 'Lobo, G', 'Loch, P', 'Lohmander, H', 'Lomas, J', 'Lubimov, V', 'López, G C', 'Lüke, D', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Masson, S', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Mercer, D', 'Merz, T', 'Meyer, C A', 'Meyer, H', 'Meyer, J', 'Migliori, A', 'Mikocki, S', 'Milstead, D', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Niedzballa, C', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Ozerov, D', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Peppel, E', 'Phillips, J P', 'Pichler, C', 'Pieuchot, A', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Pérez, E', 'Rabbertz, K', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Ribarics, P', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riess, S', 'Rietz, M', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rylko, R', 'Rädel, G', 'Rüter, K', 'Sahlmann, N', 'Salesch, S G', 'Sankey, D P C', 'Schacht, P', 'Schiek, S', 'Schleper, P', 'Schmidt, C', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schwind, A', 'Schöning, A', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shooshtari, H', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Solochenko, V', 'Soloviev, Yu V', 'Spiekermann, J', 'Spielman, S', 'Spitzer, H', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Stella, B', 'Stephens, K', 'Stier, J', 'Stiewe, J', 'Stolze, K', 'Strachota, J', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Sánchez, E', 'Tapprogge, Stefan', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Vartapetian, A H', 'Vazdik, Ya', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walker, I W', 'Walther, A', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wellisch, H P', 'West, L R', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wittek, C', 'Wright, A E', 'Wulff, N', 'Wünsch, E', 'Yiou, T P', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zimmermann, W', 'Zomer, F', 'Zuber, K', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']",['Inclusive parton cross sections in photoproduction and photon structure'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, interaction', 'interaction, photon p', 'jet, photoproduction', 'photoproduction, jet', 'jet, pair production', 'pair production, jet', 'transverse energy, energy flow', 'photon, resolved', 'momentum spectrum, parton', 'transverse momentum, parton', 'rapidity dependence', 'angular dependence', 'correlation, (jet parton)', 'cross section, transverse momentum', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504004'],['Photoproduction of 2-jet events is studied with the H1 detector at HERA. Parton cross sections are extracted from the data by an unfolding method using leading order parton-jet correlations of a QCD generator. The gluon distribution in the photon is derived in the fractional momentum range 0.04\\le x_\\gamma \\le 1 at the average factorization scale 75 GeV^2.'],['1995-04-12']
2503,['eng'],"['Arneodo, M', 'Arvidson, A', 'Badelek, B', 'Ballintijn, M K', 'Baum, G', 'Beaufays, J', 'Bird, I G', 'Björkholm, P', 'Botje, M', 'Broggini, C', 'Brückner, W', 'Brüll, A', 'Burger, W J', 'Ciborowski, J', 'Van Dantzig, R', 'Dyring, A', 'Engelien, H', 'Ferrero, M I', 'Fluri, L', 'Gaul, U', 'Granier, T', 'Grosse-Perdekamp, M', 'Von Harrach, D', 'Van der Heijden, M', 'Heusch, C A', 'Igo, G', 'Ingram, Q', 'Janson-Prytz, K', 'De Jong, M', 'Kabuss, E M', 'Kaiser, R', 'Kessler, H J', 'Ketel, T J', 'Klein, F', 'Kullander, S', 'Landgraf, U', 'Lindqvist, T', 'Mallot, G K', 'Mariotti, C', 'Van Middelkoop, G', 'Milshtein, A I', 'Mizuno, Y', 'Most, A', 'Mücklich, A', 'Nassalski, J P', 'Nowotny, D', 'Oberski, J', 'Paic, A', 'Peroni, C', 'Povh, B', 'Rieger, R', 'Rith, K', 'Röhrich, K', 'Rondio, E', 'Ropelewski, L', 'Sandacz, A', 'Sanders, D', 'Scholz, C', 'Seitz, R', 'Sever, F', 'Shibata, T A', 'Siebler, M', 'Simon, A', 'Staiano, A', 'Szleper, M', 'Tzamouranis, Yu', 'Virchaux, M', 'Vuilleumier, J L', 'Walcher, T', 'Whitten, C', 'Windmolders, R', 'Witzmann, A', 'Zetsche, F']",['The structure function ratios F$_{2}^{Li}$/F$_{2}^{D}$ and F$_{2}^{C}$/F$_{2}^{D}$ at small x'],['Particle Physics - Experimental Results'],"['muon nucleus, deep inelastic scattering', 'deep inelastic scattering, muon nucleus', 'deuterium', 'lithium', 'carbon', 'structure function, small-x', 'effect, shadowing', 'nuclear physics, effect', 'spectrometer, experimental results', 'CERN SPS', '200 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504002'],['We present the structure function ratios F2(Li)/F2(D) and F2(C)/F2(D) measured in deep inelastic muon-nucleus scattering at a nominal incident muon energy of 200 GeV. The kinematic range 0.0001 < x < 0.7 and 0.01< Q^2 < 70 GeV^2 is covered. For values of x less than 0.002 both ratios indicate saturation of shadowing at values compatible with photoabsorption results.'],['1995-04-05']
2504,['eng'],"['Lü, C', 'Marlow, D R', 'Mindas, C R', 'Prebys, E J']",['First results from the BELLE DIRC prototype'],['Particle Physics - Experimental Results'],"['electron positron, colliding beam detector', 'colliding beam detector, electron positron', 'B, particle source', 'Cherenkov counter, ring imaging', 'optics, reflection', 'radiation, yield', 'angular resolution', 'photoelectron, amplifier', 'numerical calculations, Monte Carlo', 'KEK TRISTAN Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504001'],"[""The DIRC (Detection of Internally Reflected Cerenkov light) is a new type of ring imaging Cerenkov detector, which detects images from Cerenkov light produced in precisely machined quartz bars. The Cerenkov images are transported along several meters of bar to the edge of the detector where they are proximity focussed unto an array of conventional photomultiplier tubes. Results from a prototype device comprising a 2 x 4 x 240 cm**3 quartz bar read by an array of 480 PMT's are presented. Sample images, which are the first observed in this type of detector, are shown. Measurements of the light yield (approximately 20 photoelectrons per image) and the angular resolution are in good agreement with Monte Carlo predictions.""]",['1995-04-05']
2505,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Cartiglia, N', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Hultschig, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Kochocki, J A', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Measurement of charged and neutral current e$^{-}$p deep inelastic scattering cross sections at high Q$^{2}$'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'neutral current', 'charged current', 'transverse momentum, missing-energy', 'cross section, ratio', 'differential cross section, momentum transfer', 'momentum transfer, differential cross section', 'W, mass', 'mass, W', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503016'],"['Deep inelastic e^-p scattering has been studied in both the charged-current (CC) and neutral-current (NC) reactions at momentum transfers squared, Q^2, between 400 GeV^2 and the kinematic limit of 87500 GeV^2 using the ZEUS detector at the HERA ep collider. The CC and NC total cross sections, the NC to CC cross section ratio, and the differential cross sections, d\\sigma/dQ^2 , are presented. For Q^2 \\simeq M_W^2, where M_W is the mass of the W boson, the CC and NC cross sections have comparable magnitudes, demonstrating the equal strengths of the weak and electromagnetic interactions at high Q^2. The Q^2 dependence of the CC cross section determines the mass term in the CC propagator to be M_{W} = 76 \\pm 16 \\pm 13~GeV.']",['1995-04-05']
2506,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Cartiglia, N', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Eskreys, Andrzej', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Monteiro, T', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Measurement of the cross section for the reaction $\\gamma$p --> J/$\\psi$p with the ZEUS detector at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, exclusive reaction', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'channel cross section, energy dependence', 'gluon, momentum spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms', 'J/psi(3100), photoproduction', 'photoproduction, J/psi(3100)', 'J/psi(3100), leptonic decay', 'leptonic decay, J/psi(3100)', 'electron p --> J/psi(3100) p electron', 'J/psi(3100) --> muon+ muon-', 'J/psi(3100) --> positron electron']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503015'],"['This paper reports the cross section measurements for the process ep \\rightarrow e~\\jpsi~p for Q^2 < 4 GeV^2 at \\sqrt s = 296 GeV, based on an integrated luminosity of about 0.5~pb^{-1}, using the ZEUS detector. The \\jpsi~was detected in its \\rm e^{+}e^{-} and \\rm \\mu^{+}\\mu^{-} decay modes. The photoproduction cross section was measured to be 52^{ \\ +7}_{-12}\\pm 10~nb at an average \\gammap centre of mass energy of 67 GeV and 71^{+13}_{-20}\\pm 12~nb at 114 GeV. The significant rise of the cross section compared to lower energy measurements is not in agreement with VDM models, but can be described by QCD inspired models if a rise in the gluon momentum density at low x in the proton is assumed.']",['1995-03-28']
2507,['eng'],"['Spencer, M B']",['A measurement of the branching ratio and form factor of K$_{L}$ --> $\\mu\\mu\\gamma$'],['Particle Physics - Experimental Results'],"['K0(L), radiative decay', 'radiative decay, K0(L)', 'form factor, (K 2photon)', '(K 2photon), form factor', 'K0(L), branching ratio', 'p nucleus, nuclear reaction', 'beryllium', 'experimental results', 'Batavia PS', 'K0(L) --> muon+ muon- photon', '800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9504005'],['We report on a measurement of the decay K_L\\rightarrow\\mu^+\\mu^-\\gam ma from Fermilab experiment E799. We observe 207 candidate signal events with an estimated background of 10.5 \\pm 4.0 events and establish B(K_L\\rightarrow\\mu^+\\mu^-\\gamma) = (3.23\\pm 0.23(stat) \\pm 0.19(sys))\\times 10^{-7}. This provides the first measurement of the K\\gamma\\gamma^* form factor in the muonic Dalitz decay mode of the K_L.'],['1995-04-14']
2508,['eng'],"['Butterworth, J M']",['Photon structure as seen at HERA'],['Particle Physics - Experimental Results'],"['talk', 'electron p, colliding beams', 'colliding beams, electron p', 'electron p, inclusive reaction', 'photon p, interaction', 'interaction, photon p', 'jet, photoproduction', 'photoproduction, jet', 'jet, multiple production', 'multiple production, jet', 'differential cross section, rapidity dependence', 'rapidity dependence, differential cross section', 'differential cross section, transverse energy', 'transverse energy, differential cross section', 'quantum chromodynamics, perturbation theory', 'hard scattering', 'photon, structure function', 'transverse energy, energy flow', 'gluon, momentum spectrum', 'magnetic detector, H1', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503011'],"[""At HERA, the electron-proton collider at DESY, Hamburg, the large flux of almost on-shell photons accompanying the lepton beam is being used to shed new light on the structure of the photon. Recent results are reviewed and discussed, with emphasis on those aspects of the photon's nature which should be understandable using perturbative QCD.""]",['1995-03-20']
2509,['eng'],"['Abe, F']","['Measurement of the B meson differential cross section, d$\\sigma$/dp$_{T}$, in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV']",['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'B, hadroproduction', 'hadroproduction, B', 'B, nonleptonic decay', 'nonleptonic decay, B', 'K*(892)', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'B0, nonleptonic decay', 'nonleptonic decay, B0', 'K*(892)', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> B anything', 'K*(892) --> K+ pi-', '1800 GeV-cms', 'J/psi(3100)', 'J/psi(3100)', 'B+ --> J/psi(3100) K+', 'B0 --> J/psi(3100) K*(892)', 'J/psi(3100) --> muon+ muon-']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503013'],"['This paper presents the first direct measurement of the B meson differential cross section, d\\sigma/dp_T, in p\\overline{p} collisions at \\sqrt{s}=1.8 TeV using a sample of 19.3 \\pm 0.7 pb^{-1} accumulated by the Collider Detector at Fermilab (CDF). The cross section is measured in the central rapidity region |y| < 1 for p_T(B) > 6.0 GeV/c by fully reconstructing the B meson decays B^{+}\\rightarrow J/\\psi K^{+} and B^{0}\\rightarrow J/\\psi K^{*0}(892), where J/\\psi \\rightarrow \\mu^+\\mu^- and K^{*0} \\rightarrow K^+ \\pi^-. A comparison is made to the theoretical QCD prediction calculated at next-to-leading order.']",['1995-03-20']
2510,['eng'],"['Procario, M']",['Charm from hyperons in the future'],['Particle Physics - Experimental Results'],"['talk, Charlottesville 1994/10/07', 'nucleon Sigma, inclusive reaction', 'Sigma-, beam', 'beam, Sigma-', 'charmed baryon, hadroproduction', 'hadroproduction, charmed baryon', 'charmed baryon, decay modes', 'decay modes, charmed baryon', 'yield, (charmed baryon)', 'particle identification, (charmed baryon)', 'forward spectrometer, proposed', 'numerical calculations', 'proposed experiment, Batavia TEVATRON PS', 'Lambda/c+, nonleptonic decay', 'nonleptonic decay, Lambda/c+']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503008'],"['Recent results from CERN experiment WA89 have shown that charmed baryons and particularly charmed-strange baryons have a significant cross section in \\Sigma^- beams. Fermilab experiment 781, which is currently under construction, will utilize this fact to pursue a broad program of high statistics studies of charmed baryons in the next Fermilab fixed target run.']",['1995-03-10']
2511,['eng'],"['Abachi, S']",['Search for W boson pair production in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'W, pair production', 'pair production, W', 'W, leptonic decay', 'leptonic decay, W', 'coupling, (Z0 2W)', '(Z0 2W), coupling', 'coupling, (2W photon)', '(2W photon), coupling', 'final state, dilepton', 'dilepton, final state', 'channel cross section, upper limit', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', 'W --> lepton neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503012'],"['The results of a search for W boson pair production in p\\bar{p} collisions at \\sqrt{s}=1.8 TeV with subsequent decay to dilepton (e\\mu, ee , and \\mu\\mu) channels are presented. One event is observed with an expected background of 0.56\\pm0.13 events with an integrated luminosity of approximately 14 pb^{-1}. %13.9\\pm1.7 pb^{-1}. Assuming equal strengths for the WWZ and WW\\gamma gauge boson coupling parameters \\kappa and \\lambda, limits on the CP-conserving anomalous coupling constants are -2.6<\\Delta\\kappa<2.8 and -2.2<\\lambda<2.2 at the 95\\% confidence level.']",['1995-03-20']
2512,['eng'],"['Debbe, R', 'Gushue, S', 'Moskowitz, B E', 'Norris, J', 'Olness, J', 'Videbaek, F']",['In-beam tests of a ring imaging Cerenkov detector with a multianode photomultiplier readout'],['Detectors and Experimental Techniques'],"['Cherenkov counter, ring imaging', 'carbon, fluorine', 'photoelectron, amplifier', 'photoelectron, yield']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503006'],"['A ring-imaging \\v{C}erenkov counter read out by a 100-channel PMT of active area 10\\times10 cm^2 was operated successfully in a test beam at the BNL AGS with several radiator gases, including the heavy fluorocarbon C_4F_{10}. Ring radii were measured for electrons, muons, pions and kaons over the particle momentum range from 2 to 12 GeV/c, and a best resolution of \\sigma_r/r = 2.3\\% was obtained.']",['1995-03-09']
2513,['eng'],[],['First measurement of the deep-inelastic structure of proton diffraction'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'diffraction', 'p, structure function', 'exchange, pomeron', 'pomeron, exchange', 'structure function, pomeron', 'structure function, factorization', 'rapidity, gap', 'x-dependence', 'dependence, momentum transfer', 'scaling', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', '296 GeV-cms, 8.5 < Q**2 < 50 GeV**2']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503005'],"['A measurement is presented, using data taken with the H1 detector at HERA, of the contribution of diffractive interactions to deep-inelastic electron-proton scattering. The diffractive contribution to the proton structure function is evaluated as a function of the appropriate deep-inelastic scattering variables using a class of deep-inelastic ep scattering events with no hadronic energy flow in an interval of pseudo-rapidity adjacent to the proton beam direction. The dependence of this contribution on x-pomeron is consistent with both a diffractive interpretation and a factorisable ep diffractive cross section. A first measurement of the deep-inelastic structure of the pomeron in the form of a factorised structure function is presented. This structure function is observed to be consistent with scale invariance.']",['1995-03-07']
2514,['eng'],"['Nodulman, L']",['Measurement of the W boson mass'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'W, leptonic decay', 'leptonic decay, W', 'W, mass', 'mass, W', 'mass spectrum, transverse', 'transverse, mass spectrum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> W anything', 'W --> muon neutrino', 'W --> electron neutrino', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503007'],"['We present a measurement of the mass of the W boson using data collected with the CDF detector during the 1992-93 collider run at the Fermilab Tevatron. A fit to the transverse mass spectrum of a sample of 3268 {\\mbox{W \\rightarrow \\mu\\nu}} events recorded in an integrated luminosity of 19.7 pb^{-1} gives a mass M_{W}^{\\mu}=80.310\\pm0.205\\mbox{~(stat.)}\\pm0.130\\mbox{~(syst.)} \\ \\mbox{GeV/c}^{2}. A fit to the transverse mass spectrum of a sample of 5718 {\\mbox{W \\rightarrow e\\nu}} events recorded in 18.2 pb^{-1} gives a mass M_{W}^{e}=80.490\\pm0.145\\mbox{~(stat.)}\\pm0.175\\mbox{~(syst.)} \\ \\mbox{GeV/c}^{2}. Combining the electron and muon results, accounting for correlated uncertainties, yields a mass M_{W}=80.410\\pm0.180 \\ \\mbox{GeV/c}^{2}.']",['1995-03-10']
2515,['eng'],[],['Limits on WWZ and WW$\\gamma$ couplings from WW and WZ production in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'Z0, hadroproduction', 'hadroproduction, Z0', 'intermediate boson, pair production', 'pair production, intermediate boson', 'intermediate boson, leptonic decay', 'leptonic decay, intermediate boson', 'intermediate boson, nonleptonic decay', 'nonleptonic decay, intermediate boson', 'transverse momentum, high', 'coupling, (Z0 W)', '(Z0 W), coupling', 'coupling, (2W photon)', '(2W photon), coupling', 'mass spectrum, (2jet)', '(2jet), mass spectrum', 'transverse momentum, spectra', 'spectra, transverse momentum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2W anything', 'anti-p p --> Z0 W anything', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503009'],"['Direct limits are set on WWZ and WW\\gamma three-boson couplings in a search for WW and WZ production with high transverse momentum in p\\overline{p} collisions at \\sqrt{s} = 1.8 TeV, using the Collider Detector at Fermilab. The results are in agreement with the SU(2) \\times U(1) model of electroweak interactions. Assuming Standard Model WW\\gamma coupling, the the limits are interpreted as direct evidence for a non-zero WWZ coupling at subprocess energies near 500 GeV. Alternatively, assumiong identical WWZ and WW\\gamma couplings, bounds -0.11 < \\kappa < 2.27 and -0.81 < \\lambda < 0.84 are obtained at 95\\% CL for a form factor scale 1000 GeV.']",['1995-03-13']
2516,['eng'],"['Maeno, T', 'Fujikawa, M', 'Kataoka, J', 'Nishihara, Y', 'Orito, S', 'Shigekuni, K', 'Watanabe, Y']",['A search for massive neutral bosons in orthopositronium decay'],['Particle Physics - Experimental Results'],"['positronium, radiative decay', 'radiative decay, positronium', 'energy spectrum, (photon)', '(photon), energy spectrum', 'boson, search for', 'boson, neutral particle', 'positronium, branching ratio', 'upper limit', 'semiconductor detector, germanium', 'experimental results', 'positronium --> boson photon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503004'],"['We have searched for an exotic decay of orthopositronium into a single photon and a short-lived neutral boson in the hitherto unexplored mass region above 900 {\\rm keV}/{\\it c}^{2}, by noting that this decay is one of few remaining candidates which could explain the discrepancy of the orthopositronium decay-rate. A high-resolution measurement of the associated photon energy spectrum was carried out with a germanium detector to search for a sharp peak from this two-body decay. Our negative result provides the upper-limits of\\mbox{ }2.0 \\times 10^{-4} on the branching ratio of such a decay in the mass region from 847 to 1013 {\\rm keV}/{\\it c}^{2}, and excludes the possibility of this decay mode explaining the discrepancy in the orthopositronium decay-rate.']",['1995-03-06']
2517,['eng'],"['Klima, B']",['Observation of the top quark'],"['XX', 'Particle Physics - Experimental Results']","['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'final state, ((n)jet 2lepton)', '((n)jet 2lepton), final state', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'particle identification, beauty', 'transverse energy, missing-energy', 'mass, truth', 'truth, mass', 'channel cross section, mass', 'mass, channel cross section', 'mass spectrum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', '1800 GeV-cms', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'final state, ((n)jet 2lepton)', '((n)jet 2lepton), final state', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'particle identification, beauty', 'transverse energy, missing-energy', 'mass, truth', 'truth, mass', 'channel cross section, mass', 'mass, channel cross section', 'mass spectrum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', '1800 GeV-cms']","['http://www-lib.fnal.gov/archive/1995/conf/Conf-95-102-E.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503003']","['The DO collaboration reports on a search for the Standard Model top quark in pbar-p collisions at Sqrt(s)=1.8TeV at the Fermilab Tevatron, with an integrated luminosity of approximately 50pb-1. We have searched for t-tbar production in the dilepton and single-lepton decay channels, with and without tagging of b-quark jets. We observed 17 events with an expected background of 3.8+/-0.6 events. The probability for an upward fluctuation of the background to produce the observed signal is 2.0E-6 (equivalent to 4.6 standard deviations). The kinematic properties of the excess events are consistent with top quark decay. We conclude that we have observed the top quark and measure its mass to be 199^+19_21 (stat.)+/- 22 (syst.)GeV/c**2 and its production cross section to be 6.4 +/- 2.2 pb.']",['1995-03-06']
2518,['eng'],[],['Observation of top quark production in $\\overline{p}$p collisions'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'mass, truth', 'truth, mass', 'channel cross section', 'particle identification, beauty', 'final state, dilepton', 'dilepton, final state', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'jet, multiplicity', 'mass spectrum', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503002'],"['We establish the existence of the top quark using a 67 pb^-1 data sample of Pbar-P collisions at Sqrt(s) = 1.8 TeV collected with the Collider Detector at Fermilab (CDF). Employing techniques similar to those we previously published, we observe a signal consistent with t-tbar decay to WW b-bbar, but inconsistent with the background prediction by 4.8 sigma. Additional evidence for the top quark is provided by a peak in the reconstructed mass distribution. We measure the top quark mass to be 176 +/-8(stat) +/- 10(sys.) GeV/c^2, and the t-tbar production cross section to be 6.8 +3.6 -2.4 pb.']",['1995-03-03']
2519,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Cartiglia, N', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Eskreys, Andrzej', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Hultschig, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Kochocki, J A', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Dijet cross sections in photoproduction at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, inclusive reaction', 'jet, photoproduction', 'photoproduction, jet', 'jet, pair production', 'pair production, jet', 'gluon, momentum spectrum', 'photon, resolved', 'differential cross section, rapidity dependence', 'rapidity dependence, differential cross section', 'transverse energy, energy flow', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'photon p --> 2jet anything', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9502008'],"['Dijet production by almost real photons has been studied at HERA with the ZEUS detector. Jets have been identified using the cone algorithm. A cut on xg, the fraction of the photon energy participating in the production of the two jets of highest transverse energy, is used to define cross sections sensitive to the parton distributions in the proton and in the photon. The dependence of the dijet cross sections on pseudorapidity has been measured for xg \\ge 0.75 and xg < 0.75. The former is sensitive to the gluon momentum density in the proton. The latter is sensitive to the gluon in the photon. The cross sections are corrected for detector acceptance and compared to leading order QCD calculations.']",['1995-02-24']
2520,['eng'],"['Bishai, M', 'Fast, J', 'Gerndt, E', 'Hinson, J W', 'McIlwain, R L', 'Miao, T', 'Miller, D H', 'Modesitt, M', 'Payne, D', 'Shibata, E I', 'Shipsey, I P J', 'Wang Pei Ning', 'Battle, M', 'Ernst, J', 'Gibbons, L K', 'Kwon, Y', 'Roberts, S', 'Thorndike, E H', 'Wang, C H', 'Dominick, J', 'Lambrecht, M', 'Sanghera, S', 'Shelkov, V', 'Skwarnicki, T', 'Stroynowski, R', 'Volobuev, I', 'Wei, G', 'Artuso, M', 'Gao, M', 'Goldberg, M', 'He, D', 'Horwitz, N', 'Moneti, G C', 'Mountain, R', 'Muheim, F', 'Mukhin, Y', 'Playfer, S', 'Rozen, Y', 'Stone, S', 'Xing, X', 'Zhu, G', 'Bartelt, J', 'Csorna, S E', 'Egyed, Z', 'Jain, V', 'Gibaut, D', 'Kinoshita, K', 'Pomianowski, P A', 'Barish, B C', 'Chadha, M', 'Chan, S', 'Cowen, D F', 'Eigen, G', 'Miller, J S', ""O'Grady, C O"", 'Urheim, J', 'Weinstein, A J', 'Athanas, M', 'Brower, W', 'Masek, G E', 'Paar, H P', 'Gronberg, J B', 'Korte, C M', 'Kutschke, R', 'Menary, S R', 'Morrison, R J', 'Nakanishi, S', 'Nelson, H N', 'Nelson, T K', 'Qiao, C', 'Richman, J D', 'Ryd, A', 'Sperka, D', 'Tajima, H', 'Witherell, M S', 'Procario, M', 'Balest, R', 'Cho, K', 'Ford, W T', 'Johnson, D R', 'Lingel, K', 'Lohner, M', 'Rankin, P', 'Smith, J G', 'Alexander, J P', 'Bebek, C', 'Berkelman, K', 'Bloom, K', 'Browder, T E', 'Cassel, David G', 'Cho, H A', 'Coffman, D M', 'Crowcroft, D S', 'Drell, P S', 'Dumas, D J P', 'Ehrlich, R', 'Gaidarev, P B', 'García-Sciveres, M', 'Geiser, B', 'Gittelman, B', 'Gray, S W', 'Hartill, D L', 'Heltsley, B K', 'Henderson, S', 'Jones, C D', 'Jones, S L', 'Kandaswamy, J', 'Katayama, N', 'Kim, P C', 'Kreinick, D L', 'Ludwig, G S', 'Masui, J', 'Mevissen, J', 'Mistry, N B', 'Ng, C R', 'Nordberg, E', 'Patterson, J R', 'Peterson, D', 'Riley, D', 'Salman, S', 'Sapper, M', 'Würthwein, F', 'Avery, P', 'Freyberger, A P', 'Rodríguez, J', 'Yang, S', 'Yelton, J', 'Cinabro, D', 'Liu, T', 'Saulnier, M', 'Wilson, R', 'Yamamoto, H', 'Bergfeld, T', 'Eisenstein, B I', 'Gollin, G', 'Ong, B', 'Palmer, M', 'Selen, M', 'Thaler, J J', 'Edwards, K W', 'Ogg, M', 'Bellerive, A', 'Britton, D I', 'Hyatt, E R F', 'MacFarlane, D B', 'Patel, P M', 'Spaan, B', 'Sadoff, A J', 'Ammar, R', 'Baringer, P', 'Bean, A', 'Besson, D', 'Coppage, D', 'Copty, N K', 'Davis, R', 'Hancock, N', 'Kelly, M', 'Kotov, S A', 'Kravchenko, I V', 'Kwak, N', 'Lam, H', 'Kubota, Y', 'Lattery, M', 'Momayezi, M', 'Nelson, J K', 'Patton, S', 'Poling, R A', 'Savinov, V', 'Schrenk, S', 'Wang, R', 'Alam, M S', 'Kim, I J', 'Ling, Z', 'Mahmood, A H', ""O'Neill, J J"", 'Severini, H', 'Sun, C R', 'Wappler, F', 'Crawford, G', 'Daubenmier, C M', 'Fulton, R', 'Fujino, D', 'Gan, K K', 'Honscheid, K', 'Kagan, H', 'Kass, R', 'Lee, J', 'Sung, M', 'White, C', 'Wolf, A', 'Zoeller, M M', 'Butler, F', 'Fu, X', 'Nemati, B', 'Ross, W R', 'Skubic, P L', 'Wood, M']",['Measurement of the decay asymmetry parameters in $\\Lambda_{c}^{+ }$ --> $\\Lambda\\pi^{+}$ and $\\Lambda_{c}^{+}$ --> $\\Sigma^{+}\\pi^{0}$'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'decay, asymmetry', 'asymmetry, decay', 'amplitude analysis, parity', 'parity, amplitude analysis', 'helicity, angular distribution', 'angular distribution, helicity', 'mass spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'approx. 10.6 GeV-cms', 'Lambda/c+, electroproduction', 'electroproduction, Lambda/c+', 'Lambda/c+, nonleptonic decay', 'nonleptonic decay, Lambda/c+', 'Lambda/c+, width', 'Lambda/c+ --> Lambda pi+', 'Lambda/c+ --> Sigma+ pi0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9502004'],"['We have measured the weak decay asymmetry parameters (\\aLC ) for two \\LC\\ decay modes. Our measurements are \\aLC = -0.94^{+0.21+0.12}_{-0.0 6-0.06} for the decay mode \\Lambda_c^+ \\rightarrow \\Lambda\\pi^+ and \\aLC = -0.45\\pm 0.31 \\pm 0.06 for the decay mode \\Lambda_c \\rightarrow \\Sigma^+\\pi^0 . By combining these measurements with the previously measured decay rates, we have extracted the parity-violating and parity-conserving amplitudes. These amplitudes are used to test models of nonleptonic charmed baryon decay.']",['1995-02-10']
2521,['eng'],"['Ahmed, T', 'Akhundov, A A', 'Andreev, V', 'Andrieu, B', 'Appuhn, R D', 'Arpagaus, M', 'Aïd, S', 'Babaev, A', 'Baranov, P S', 'Barrelet, E', 'Bartel, W', 'Barth, M', 'Bassler, U', 'Beck, H P', 'Behrend, H J', 'Belousov, A', 'Berger, C', 'Bergstein, H', 'Bernardi, G', 'Bernet, R', 'Bertrand-Coremans, G H', 'Besançon, M', 'Beyer, R', 'Bizot, J C', 'Blobel, Volker', 'Borras, K', 'Botterweck, F', 'Boudry, V', 'Braemer, A', 'Brasse, F W', 'Braunschweig, W', 'Brisson, V', 'Bruncko, D', 'Brune, C R', 'Buchholz, R', 'Buniatian, A Yu', 'Burke, S', 'Burton, M', 'Buschhorn, G W', 'Bán, J', 'Bähr, J', 'Büngener, L', 'Bürger, J', 'Büsser, F W', 'Campbell, A J', 'Carli, T', 'Charles, F', 'Chernyshov, V', 'Clarke, D', 'Clegg, A B', 'Clerbaux, B', 'Colombo, M G', 'Contreras, J G', 'Cormack, C', 'Coughlan, J A', 'Courau, A', 'Coutures, C', 'Cozzika, G', 'Criegee, L', 'Cussans, D G', 'Cvach, J', 'Dagoret, S', 'Dainton, J B', 'Danilov, M V', 'Dau, W D', 'Daum, K', 'David, M', 'De Wolf, E A', 'Deffur, E', 'Del Buono, L', 'Delcourt, B', 'Di Nezza, P', 'Dollfus, C', 'Dowell, John D', 'Dreis, H B', 'Droutskoi, A', 'Duboc, J', 'Duhm, H', 'Düllmann, D', 'Dünger, O', 'Ebert, J', 'Ebert, T R', 'Eckerlin, G', 'Efremenko, V', 'Egli, S', 'Eichenberger, S', 'Eichler, R', 'Eisele, Franz', 'Eisenhandler, Eric F', 'Ellison, R J', 'Elsen, E E', 'Erdmann, M', 'Erdmann, W', 'Erlichmann, H', 'Evrard, E', 'Favart, L', 'Fedotov, A', 'Feeken, D', 'Felst, R', 'Feltesse, Joel', 'Ferencei, J', 'Ferrarotto, F', 'Flamm, K', 'Fleischer, M', 'Flieser, M', 'Flügge, G', 'Fomenko, A', 'Fominykh, B A', 'Forbush, M', 'Formánek, J', 'Foster, J M', 'Franke, G', 'Fretwurst, E', 'Gabathuler, Erwin', 'Gabathuler, K', 'Gamerdinger, K', 'Garvey, J', 'Gayler, J', 'Gebauer, M', 'Gellrich, A', 'Genzel, H', 'Gerhards, R', 'Goerlach, U', 'Gogitidze, N', 'Goldberg, M', 'Goldner, D', 'González-Pineiro, B', 'Gorelov, I V', 'Goritchev, P A', 'Grab, C', 'Greenshaw, T J', 'Grindhammer, G', 'Gruber, A', 'Gruber, C', 'Grässler, H', 'Grässler, R', 'Görlich, L', 'Haack, J', 'Haidt, D', 'Hajduk, L', 'Hamon, O', 'Hampel, M', 'Hanlon, E M', 'Hapke, M', 'Haynes, W J', 'Heatherington, J', 'Heinzelmann, G', 'Henderson, R C W', 'Henschel, H', 'Herynek, I', 'Hess, M F', 'Hildesheim, W', 'Hill, P', 'Hiller, K H', 'Hilton, C D', 'Hladky, J', 'Hoeger, K C', 'Horisberger, R P', 'Hudgson, V L', 'Huet, Patrick', 'Hufnagel, H', 'Höppner, M', 'Hütte, M', 'Ibbotson, M', 'Itterbeck, H', 'Jabiol, M A', 'Jacholkowska, A', 'Jacobsson, C', 'Jaffré, M', 'Janoth, J', 'Jansen, T', 'Johannsen, K', 'Johnson, D P', 'Johnson, L', 'Jung, H', 'Jönsson, L B', 'Kalmus, Peter I P', 'Kant, D', 'Kaschowitz, R', 'Kasselmann, P', 'Kathage, U', 'Katzy, J M', 'Kaufmann, H H', 'Kazarian, S', 'Kenyon, Ian Richard', 'Kermiche, S', 'Keuker, C', 'Kiesling, C', 'Klein, M', 'Kleinwort, C', 'Knies, G', 'Ko, W', 'Kolanoski, H', 'Kole, F', 'Kolya, S D', 'Korbel, V', 'Korn, M', 'Kostka, P', 'Kotelnikov, S K', 'Krasny, M W', 'Krehbiel, H', 'Krämerkämper, T', 'Krücker, D', 'Krüger, U P', 'Krüner-Marquis, U', 'Kubenka, J P', 'Kuhlen, M', 'Kurca, T', 'Kurzhöfer, J', 'Kuznik, B', 'Köhler, T', 'Köhne, J H', 'Küster, H', 'Lacour, D', 'Lamarche, F', 'Lander, R', 'Landon, M P J', 'Lange, W', 'Lanius, P', 'Laporte, J F', 'Lebedev, A', 'Leverenz, C', 'Levonian, S', 'Ley, C', 'Lindner, A', 'Lindström, G', 'Linsel, F', 'Lipinski, J', 'List, B', 'Loch, P', 'Lohmander, H', 'Lubimov, V', 'López, G C', 'Lüke, D', 'Magnussen, N', 'Malinovskii, E I', 'Mani, S', 'Maracek, R', 'Marage, P', 'Marks, J', 'Marshall, R', 'Martens, J', 'Martin, R D', 'Martyn, H U', 'Martyniak, J', 'Masson, S', 'Mavroidis, A', 'Maxfield, S J', 'McMahon, S J', 'Mehta, A', 'Meier, K', 'Mercer, D', 'Merz, T', 'Meyer, C A', 'Meyer, H', 'Meyer, J', 'Mikocki, S', 'Milstead, D', 'Moreau, F', 'Morris, J V', 'Mroczko, E', 'Murín, P', 'Müller, G', 'Müller, K', 'Nagovitsin, V', 'Nahnhauer, R', 'Naroska, B', 'Naumann, T', 'Newman, P R', 'Newton, D', 'Neyret, D', 'Nguyen, H K', 'Nicholls, T C', 'Niebergall, F', 'Niebuhr, C B', 'Nisius, R', 'Nowak, G', 'Noyes, G W', 'Nyberg-Werther, M', 'Oakden, M N', 'Oberlack, H', 'Obrock, U', 'Olsson, J E', 'Panaro, E', 'Panitch, A', 'Pascaud, C', 'Patel, G D', 'Peppel, E', 'Phillips, J P', 'Pichler, C', 'Pitzl, D', 'Pope, G', 'Prell, S', 'Prosi, R', 'Pérez, E', 'Raupach, F', 'Reimer, P', 'Reinshagen, S', 'Ribarics, P', 'Rick, Hartmut', 'Riech, V', 'Riedlberger, J', 'Riess, S', 'Rietz, M', 'Rizvi, E', 'Robertson, S M', 'Robmann, P', 'Roloff, H E', 'Roosen, R', 'Rosenbauer, K', 'Rostovtsev, A A', 'Rouse, F', 'Royon, C', 'Rusakov, S V', 'Rybicki, K', 'Rylko, R', 'Rädel, G', 'Rüter, K', 'Sahlmann, N', 'Sankey, D P C', 'Savitsky, M M', 'Schacht, P', 'Schiek, S', 'Schleper, P', 'Schmidt, C', 'Schmidt, D', 'Schmidt, G', 'Schröder, V', 'Schuhmann, E', 'Schwab, B', 'Schwind, A', 'Schöning, A', 'Seehausen, U', 'Sefkow, F', 'Seidel, M', 'Sell, R', 'Semenov, A A', 'Shekelian, V I', 'Shevyakov, I', 'Shooshtari, H', 'Shtarkov, L N', 'Siegmon, G', 'Siewert, U', 'Sirois, Y', 'Skillicorn, Ian O', 'Smirnov, P', 'Smith, J R', 'Soloviev, Yu V', 'Spiekermann, J', 'Spitzer, H', 'Starosta, R', 'Steenbock, M', 'Steffen, P', 'Steinberg, R', 'Stella, B', 'Stephens, K', 'Stier, J', 'Stiewe, J', 'Strachota, J', 'Straumann, U', 'Struczinski, W', 'Stösslein, U', 'Sutton, J P', 'Sánchez, E', 'Tapprogge, Stefan', 'Taylor, R E', 'Thiebaux, C', 'Thompson, G', 'Truöl, P', 'Turnau, J', 'Tutas, J', 'Uelkes, P', 'Usik, A', 'Valkár, S', 'Valkárová, A', 'Vallée, C', 'Van Esch, P', 'Van Mechelen, P', 'Vartapetian, A H', 'Vazdik, Ya', 'Vecko, M', 'Verrecchia, P', 'Villet, G', 'Wacker, K', 'Wagener, A', 'Wagener, M', 'Walker, I W', 'Walther, A', 'Weber, G', 'Weber, M', 'Wegener, D', 'Wegner, A', 'Wellisch, H P', 'West, L R', 'Willard, S', 'Winde, M', 'Winter, G G', 'Wright, A E', 'Wulff, N', 'Wünsch, E', 'Yiou, T P', 'Zarbock, D', 'Zhang, Z', 'Zhokin, A S', 'Zimmer, M', 'Zimmermann, W', 'Zomer, F', 'Zuber, K', 'Zácek, J', 'de Roeck, A', 'von Schlippe, W']","['A measurement of the proton structure function F$_{2}$(x,Q$^{2}$)']",['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'p, structure function', 'structure function, small-x', 'x-dependence', 'dependence, momentum transfer', 'momentum transfer, high', 'rapidity, gap', 'diffraction', 'magnetic detector, H1', 'experimental results', 'DESY HERA Stor', 'bibliography', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503001'],"['A measurement of the proton structure function F_{\\!2}(x,Q^2) is reported for momentum transfer squared Q^2 between 4.5 GeV^2 and 1600 GeV^2 and for Bjorken x between 1.8\\cdot10^{-4} and 0.13 using data collected by the HERA experiment H1 in 1993. It is observed that F_{\\!2} increases significantly with decreasing x, confirming our previous measurement made with one tenth of the data available in this analysis. The Q^2 dependence is approximately logarithmic over the full kinematic range covered. The subsample of deep inelastic events with a large pseudo-rapidity gap in the hadronic energy flow close to the proton remnant is used to measure the ""diffractive"" contribution to F_{\\!2}.']",['1995-03-02']
2522,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Eskreys, Andrzej', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Hultschig, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Cartiglia, N', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Kochocki, J A', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Jet production in high Q$^{2}$ deep-inelastic ep scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'jet, electroproduction', 'electroproduction, jet', 'jet, pair production', 'pair production, jet', 'quark, jet', 'gluon, jet', 'quantum chromodynamics, perturbation theory', 'transverse energy, energy flow', 'scaling', 'spectra, x-dependence', 'x-dependence, spectra', 'rapidity spectrum', 'mass spectrum, (2jet)', '(2jet), mass spectrum', 'transverse momentum, spectra', 'spectra, transverse momentum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9502003'],"['Two-jet production in deep-inelastic electron-proton scattering has been studied for 160<Q^2<1280~GeV^2, 0.01<x<0.1 and 0.04<y<0.95 with the ZEUS detector at HERA. The kinematic properties of the jets and the jet production rates are presented. The partonic scaling variables of the two-jet system and the rate of two-jet production are compared to perturbative next-to-leading order QCD calculations.']",['1995-02-07']
2523,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Eskreys, Andrzej', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Hultschig, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Cartiglia, N', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Kochocki, J A', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Study of D$*$(2010)$^{\\pm}$ production in ep collisions at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'photon p, inclusive reaction', 'D*(2010), electroproduction', 'electroproduction, D*(2010)', 'D*(2010), hadronic decay', 'hadronic decay, D*(2010)', 'mass difference, (D*(2010) D0)', '(D*(2010) D0), mass difference', 'mass spectrum, (K pi)', '(K pi), mass spectrum', 'quark, charm', 'quark, pair production', 'pair production, quark', 'channel cross section, energy dependence', 'quantum chromodynamics, perturbation theory', 'gluon, momentum spectrum', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'electron p --> D*(2010) anything', 'D*(2010) --> D0 pi+', 'electron p --> 2charm anything', 'photon p --> 2charm anything', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9502002'],"['We report the first observation of charmed mesons with the ZEUS detector at HERA using the decay channel {\\rm D}^{*+}\\rightarrow (\\Do \\rightarrow {\\rm K}^-\\pi^+)\\pi^+ (+ c.c.). Clear signals in the mass difference \\Delta M=M(D^*)--M(D^0) as well as in the M(K\\pi) distribution at the D^0 mass are found. The ep cross section for inclusive \\DSpm\\ production with Q^2<4~\\GeV^2 in the \\gamma p centre-of-mass energy range 115 < W < 275 \\GeV\\ has been determined to be (32 \\pm 7^{+4}_{-7} ) nb in the kinematic region \\mbox{\\{p_T(\\DS)\\geq 1.7 \\,\\GeV, |\\eta(\\DS)| < 1.5 \\}}. Ex\\-tra\\-po\\-la\\-ting outside this region, assuming a mass of the charm quark of 1.5 \\GeV we estimate the ep charm cross section to be \\sigma(e p \\rightarrow c \\bar{c}X ) = (0.45 \\pm 0.11^{+0.37}_{-0.22}) \\, \\mu {\\rm b} at \\mbox{\\sqrt{s} = 296}~\\GeV\\ and \\langle W \\rangle = 198 \\GeV. The average \\gamma p charm cross section \\mbox{\\sigma(\\gamma p \\rightarrow c \\bar{c}X )} is found to be \\mbox{(6.3 \\pm 2.2^{+6.3}_{-3.0}) \\, \\mu {\\rm b} } at \\langle W \\rangle = 163 \\GeV\\ and \\mbox{(16.9 \\pm 5.2^{+13.9}_{-8.5}) \\, \\mu {\\rm b} } at \\langle W \\rangle = 243 \\GeV. The increase of the total charm photoproduction cross section by one order of magnitude with respect to low energy data experiments is well described by QCD NLO calculations using singular gluon distributions in the proton.']",['1995-02-03']
2524,['eng'],"['Nakada, Tatsuya']",['Review of CP violation studies with b-mesons at LHC'],['Particle Physics - Experimental Results'],"['talk', 'p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'violation, CP', 'B, decay modes', 'decay modes, B', 'B0 anti-B0, oscillation', 'counters and detectors, proposed', 'magnetic detector, ATLAS', 'magnetic detector, CMS', 'proposed experiment, CERN LHC Coll', '16000 GeV-cms', 'B/s0 anti-B/s0, oscillation', 'B/s0, mass difference', 'mass difference, B/s0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9502005'],"['The Large Hadron Collider (LHC) proposed at CERN will be the ultimate source of B-mesons. With the large number of B-mesons expected at LHC, a real precision test of CP violation in B-meson decays will become possible. There are already several efforts made to explore this possibility and a summary of those activities is presented.']",['1995-02-14']
2525,['eng'],"['Xing, Z Z']",['Time dependence of coherent P$^{0}\\overline{P}^{0}$ decays and CP violation at asymmetric B factories'],['Particle Physics - Experimental Results'],"['vector meson, decay', 'decay, vector meson', 'K0 anti-K0, interference', 'D0 anti-D0, interference', 'B0 anti-B0, interference', 'B/s0 anti-B/s0, interference', 'decay, coherent interaction', 'coherent interaction, decay', 'violation, CP', 'electron positron, annihilation', 'annihilation, electron positron', 'Upsilon(10570), electroproduction', 'electroproduction, Upsilon(10570)', 'B0, pair production', 'pair production, B0', 'B0, particle source', 'decay, asymmetry', 'asymmetry, decay', 'numerical calculations', 'vector meson --> 2pseudoscalar meson']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9502001'],"['A generic formalism is presented for the time-dependent or time-integrated decays of any coherent P^{0}\\bar{P}^{0} system (P^{0} = K^{0}, D^{0}, B^{0}_{d}, or B^{0}_{s}). To meet various possible measurements at asymmetric B factories, we reanalyze some typical signals of CP violation in the coherent B^{0}_{d}\\bar{B}^ {0}_{d} transitions. The advantage of proper time cuts is illustrated for measuring mixing parameters and CP violation. We show that the direct and indirect CP asymmetries are distinguishable in neutral B decays to CP eigenstates. The possibility to detect the CP- forbidden processes at the \\Upsilon (4S) resonance is explored in some detail.']",['1995-02-02']
2526,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Eskreys, Andrzej', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Hultschig, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Jamieson, V A', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Oh, B Y', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Cartiglia, N', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Kochocki, J A', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Shapira, A', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Measurement of multiplicity and momentum spectra in the current fragmentation region of the Breit frame at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'hadron, electroproduction', 'electroproduction, hadron', 'charged particle, multiplicity', 'momentum spectrum', 'dependence, momentum transfer', 'kinematics, Breit frame', 'scaling, KNO', 'quantum chromodynamics, perturbation theory', 'effect, coherence', 'quark, fragmentation', 'electron p, annihilation', 'annihilation, electron p', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', 'bibliography', '296 GeV-cms, 10 < Q**2 < 1820 GeV**2']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501012'],['Charged particle production has been measured in Deep Inelastic Scattering (DIS) events using the ZEUS detector over a large range of Q^2 from 10 to 1280 {\\rm\\ GeV}^2. The evolution with Q of the charged multiplicity and scaled momentum has been investigated in the current fragmentation region of the Breit frame. The data are used to study QCD \\linebreak coherence effects in DIS and are compared with corresponding \\ee~data in order to test the universality of quark fragmentation.'],['1995-01-31']
2527,['eng'],"['Iwasaki, M', 'Nakano, E', 'Enomoto, R']",['Electron identification using the TOPAZ detector at TRISTAN'],['Particle Physics - Experimental Results'],"['electron positron, colliding beam detector', 'colliding beam detector, electron positron', 'exchange, one-photon', 'one-photon, exchange', 'exchange, two-photon', 'two-photon, exchange', 'particle identification, (electron)', 'efficiency', 'transverse momentum, dependence', 'drift chamber, time projection', 'energy loss', 'velocity, dependence', 'resolution', 'energy, calibration', 'background', 'magnetic detector, TOPAZ', 'KEK TRISTAN Stor', 'approx. 58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501004'],"['We present an electron-identification method using the time-projection chamber and the lead-glass calorimeter in the TOPAZ detector system. Using this method we have achieved good electron identification against hadron backgrounds over a wide momentum range in the hadronic events produced by both single-photon exchange and two-photon processes. Pion-rejection factors and electron efficiencies were 163 and 68.4\\% for high-P_T electrons and 137 and 42.7\\% for low-P_T electrons in the single-photon-exchange process, and 8600 and 36.0\\% for the two-photon process, respectively.']",['1995-01-11']
2528,['eng'],"['Abe, K', 'Abt, I', 'Ahn, C J', 'Akagi, T', 'Allen, N J', 'Ash, William W', 'Aston, D', 'Bacchetta, N', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barakat, M B', 'Baranko, G J', 'Bardon, O', 'Barklow, T L', 'Bazarko, A O', 'Ben-David, R', 'Benvenuti, Alberto C', 'Bienz, T', 'Bilei, G M', 'Bisello, D', 'Blaylock, G', 'Bogart, J R', 'Bolton, T', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Busza, W', 'Calcaterra, A', 'Caldwell, D O', 'Calloway, D H', 'Camanzi, B', 'Carpinelli, M', 'Cassell, R', 'Castaldi, R', 'Castro, A', 'Cavalli-Sforza, M', 'Church, E', 'Cohn, H O', 'Coller, J A', 'Cook, V', 'Cotton, R', 'Cowan, R F', 'Coyne, D G', 'de Oliveira, A', 'Damerell, C J S', 'De Sangro, R', 'De Simone, P', ""Dell'Orso, R"", 'Dima, M', 'Du, P Y C', 'Dubois, R', 'Eisenstein, B I', 'Elia, R', 'Falciai, D', 'Fan, C', 'Fero, M J', 'Frey, R', 'Furuno, K', 'Gillman, T', 'Gladding, G E', 'González, S', 'Hallewell, G D', 'Hart, E L', 'Hasegawa, Y', 'Hedges, S J', 'Hertzbach, S S', 'Hildreth, M D', 'Huber, J', 'Huffer, M E', 'Hughes, E W', 'Hwang, H', 'Iwasaki, Y', 'Jacques, P', 'Jaros, J A', 'Johnson, A S', 'Johnson, J R', 'Johnson, R A', 'Junk, T R', 'Kajikawa, R', 'Kalelkar, M S', 'Karliner, I', 'Kawahara, H', 'Kendall, H W', 'King, M E', 'King, R', 'Kofler, R R', 'Krishna, N M', 'Kroeger, R S', 'Labs, J F', 'Langston, M', 'Lath, A', 'Lauber, J A', 'Leith, D W G S', 'Liu, X', 'Loreti, M', 'Lu, A', 'Lynch, H L', 'Ma, J', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'Massetti, R', 'Masuda, H', 'Mazzucato, E', 'McKemey, A K', 'Meadows, B T', 'Messner, R', 'Mockett, P M', 'Moffeit, K C', 'Mours, B', 'Müller, G', 'Müller, D', 'Nagamine, T', 'Nauenberg, U', 'Neal, H A', 'Nussbaum, M', 'Ohnishi, Y', 'Osborne, L S', 'Panvini, R S', 'Park, H', 'Pavel, T J', 'Peruzzi, I', 'Pescara, L', 'Piccolo, M', 'Piemontese, L', 'Pieroni, E', 'Pitts, K T', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Punkar, G D', 'Quigley, J', 'Ratcliff, B N', 'Reeves, T W', 'Rensing, P E', 'Rochester, L S', 'Rothberg, J E', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schindler, R H', 'Schneekloth, U', 'Schumm, B A', 'Seiden, A', 'Sen, S', 'Serbo, V V', 'Saevitz, M H', 'Shank, J T', 'Shapiro, G', 'Shapiro, S L', 'Sherden, D J', 'Simopoulos, C', 'Sinev, N B', 'Smith, S R', 'Snyder, J A', 'Stamer, P E', 'Steiner, H', 'Steiner, R', 'Strauss, M G', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Szumilo, A', 'Takahashi, T', 'Taylor, F E', 'Torrence, E', 'Turk, J', 'Usher, T', 'Vavra, J', 'Vannini, C', 'Vella, E N', 'Venuti, J P', 'Verdier, R', 'Verdini, P G', 'Wagner, S R', 'Waite, A P', 'Watts, S J', 'Weidemann, A W', 'Whitaker, J S', 'White, S L', 'Wickens, F J', 'Williams, D A', 'Williams, D C', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Woods, M', 'Word, G B', 'Wyss, J', 'Yamamoto, R K', 'Yamartino, J M', 'Yang, X', 'Yellin, S J', 'Young, C C', 'Yuta, H', 'Zapalac, G H', 'Zdarko, R W', 'Zeitlin, C', 'Zhang, Z', 'Zhou, J']",['A test of the flavor independence of strong interactions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, hadronic decay', 'hadronic decay, Z0', 'quark, pair production', 'pair production, quark', 'particle identification, flavor', 'jet, multiplicity', 'strong interaction, coupling constant', 'coupling constant, strong interaction', 'dependence, flavor', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501005'],"['We present a comparison of the strong couplings of light (u, d, and s) c, and b quarks determined from multijet rates in flavor-tagged samples of hadronic Z^0 decays recorded with the SLC Large Detector at the SLAC Linear Collider. Flavor separation on the basis of lifetime and decay multiplicity differences among hadrons containing light, c, and b quarks was made using the SLD precision tracking system. We find: \\alpha_s{_{\\vphantom{y}}}^{uds}/{\\alph a_s{_{\\vphantom{y}}}^{\\rm all}} = 0.987 \\pm 0.027({\\rm stat}) \\pm 0.022({\\rm syst}) \\pm 0.022({\\rm theory}), \\alpha_s{_{\\vphantom{y}} }^c/{\\alpha_s{_{\\vphantom{y}}}^{\\rm all}} = 1.012 \\pm 0.104 \\pm 0.102 \\pm 0.096, and \\alpha_s{_{\\vphantom{y}}}^b/{\\alpha_s{_{\\vphantom{y}}}^{\\rm all}} = 1.026 \\pm 0.041 \\pm 0.041\\pm 0.030.']",['1995-01-13']
2529,['eng'],"['Enomoto, R', 'Abe, K', 'Abe, T', 'Adachi, I', 'Adachi, K', 'Aoki, M', 'Aoki, M', 'Awa, S', 'Emi, K', 'Fujii, H', 'Fujii, K', 'Fujii, T', 'Fujimoto, J', 'Fujita, K', 'Fujiwara, N', 'Hayashii, H', 'Howell, B', 'Iida, N', 'Itoh, R', 'Inoue, Y', 'Iwasaki, H', 'Iwasaki, M', 'Kaneyuki, K', 'Kajikawa, R', 'Kato, S', 'Kawabata, S', 'Kichimi, H', 'Kobayashi, M', 'Koltick, D S', 'Levine, I', 'Minami, S', 'Miyabayashi, K', 'Miyamoto, A', 'Muramatsu, K', 'Nagai, K', 'Nakabayashi, K', 'Nakano, E', 'Nitoh, O', 'Noguchi, S', 'Ochi, A', 'Ochiai, F', 'Ohishi, N', 'Ohnishi, Y', 'Ohshima, Y', 'Okuno, H', 'Okusawa, T', 'Shinohara, T', 'Sugiyama, A', 'Suzuki, S', 'Suzuki, S', 'Takahashi, K', 'Takahashi, T', 'Tanimori, T', 'Tauchi, T', 'Teramoto, Y', 'Toomi, N', 'Tsukamoto, T', 'Tsumura, O', 'Uno, S', 'Watanabe, T', 'Watanabe, Y', 'Yamaguchi, A', 'Yamamoto, A', 'Yamauchi, M']",['Observation of excess $\\lambda\\overline{\\lambda}$ production in two-photon processes at TRISTAN'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'exchange, two-photon', 'two-photon, exchange', 'photon photon, inclusive reaction', 'Lambda, photoproduction', 'photoproduction, Lambda', 'Antilambda, photoproduction', 'photoproduction, Antilambda', 'mass spectrum, (p pi)', '(p pi), mass spectrum', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'channel cross section', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', 'electron positron --> Lambda positron electron', 'approx. 58 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501002'],"['We have carried out inclusive measurements of \\Lambda(\\overline{\\Lamb da}) production in two-photon processes at TRISTAN. The mean \\sqrt{s} was 58 GeV and the integrated luminosity was 265 pb^{-1}. Inclusive \\Lambda (\\overline{\\Lambda}) samples were obtained under such conditions as no-electron, anti-electron, and remnant-jet tags. The data were compared with theoretical calculations. The measured cross sections are two-times larger than the leading-order theoretical predictions, suggesting the necessity of next-to-leading-order Monte-Carlo generator.']",['1995-01-06']
2530,['eng'],"['Azfar, F']",['Measurement of the B$_{s}$ meson lifetime'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'Phi(1020)', 'decay, path length', 'path length, decay', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms', 'B/s, hadroproduction', 'hadroproduction, B/s', 'B/s, semileptonic decay', 'semileptonic decay, B/s', 'B/s, nonleptonic decay', 'nonleptonic decay, B/s', 'J/psi(3100)', 'B/s, lifetime', 'anti-p p --> B/s anything', 'B/s --> D/s- lepton+ neutrino anything', 'B/s --> J/psi(3100) Phi(1020)', 'D/s --> Phi(1020) pi']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412017'],"['The lifetime of the B_s meson is measured using the semileptonic decay B_s \\rightarrow D_s^- \\ell^+ \\nu X. The data sample consists of 19.3 pb^{-1} of p \\bar{p} collisions at \\sqrt{s} = 1.8 TeV collected by the CDF detector at the Fermilab Tevatron collider during 1992-1993. There are 76 \\pm 8 \\ell^{+} D_s^{-} signal events where the D_s is identified via the decay D_s^{-} \\rightarrow \\phi \\pi^{-},~\\phi \\rightarrow K^+ K^-. Using these events, the B_s meson lifetime is determined to be \\tau_{s} = 1.42^{\\ + 0.27}_{\\ - 0.23}\\ {\\rm (stat)} \\pm 0.11 \\ {\\rm (syst)} ps. A measurement of the B_s lifetime in a low statistics sample of exclusive B_s \\rightarrow J/\\psi \\phi decays is also presented in this paper.']",['1995-01-06']
2531,['eng'],"['Abe, F']",['Search for new particles decaying to dijets in p$\\overline{p}$ collisions at \\Sqrt (s) = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'new particle, search for', 'postulated particle, decay', 'decay, postulated particle', 'final state, (2jet)', '(2jet), final state', 'postulated particle, axigluon', 'quark, excited state', 'postulated particle, technirho', 'color, octet', 'channel cross section, branching ratio', 'upper limit', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501001'],"['We have used 19 pb**-1 of data collected with the Collider Detector at Fermilab to search for new particles decaying to dijets. We exclude at 95% confidence level models containing the following new particles: axigluons with mass between 200 and 870 GeV, excited quarks with mass between 80 and 570 GeV, and color octet technirhos with mass between 320 and 480 GeV.']",['1995-01-06']
2532,['eng'],"['Phillips, T J']",['A technique for directly measuring the gravitational acceleration of antihydrogen'],['Particle Physics - Experimental Results'],"['talk', 'antimatter, acceleration', 'gravitation', 'hydrogen, antiparticle', 'hydrogen, beam', 'beam, hydrogen', 'beam, deflection', 'deflection, beam', 'counters and detectors, interference', 'experimental methods, proposed', 'proposed, experimental methods']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412018'],"[""The gravitational force on antimatter has never been directly measured. A method is suggested for measuring the acceleration of antimatter (\\overline g) by measuring the deflection of a beam of neutral antihydrogen atoms in the Earth's gravitational field. While a simple position measurement of the beam could be used, a more efficient measurement can be made using a transmission interferometer. A 1\\% measurement of \\overline g should be possible from a beam of about 100,000 atoms, with the ultimate accuracy being determined largely by the number of antihydrogen atoms that can be produced. A method is suggested for producing an antihydrogen beam appropriate for this experiment.""]",['1995-01-06']
2533,['eng'],"['Abe, F']",['Kinematic evidence for top quark pair production in W + multijet events in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'final state, (W (n)jet)', '(W (n)jet), final state', 'W, hadroproduction', 'hadroproduction, W', 'jet, multiplicity', 'kinematics', 'particle identification, beauty', 'channel cross section', 'energy spectrum, transverse energy', 'transverse energy, energy spectrum', 'angular distribution', 'mass, truth', 'truth, mass', 'numerical calculations, Monte Carlo', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412009'],"['Study of W+multijet events that compares the kinematics of the observed events with expectations from direct QCD W+jet production and from production and decay of top quark pairs. The data were collected in the 1992-93 run with the Collider Detector at Fermilab from 19.3 pb^{-1} of proton-antiproton collisions at \\sqrt{s}=1.8 TeV. From the W+\\geq 3 jet events, a ``signal sample"" with an improved ratio of t \\bar{t} to QCD produced W events is selected by requiring each jet to be emitted centrally in the event center of mass frame. This sample contains 14 events with unusually hard jet E_T distributions not well described by expectations for jets from direct QCD W production and other background processes. Using expected jet E_T distributions, a relative likelihood is defined and used to determine if an event is more consistent with the decay of t \\bar{t} pairs, with M_{top}~=~ 170 GeV/c^2, than with direct QCD W production, while only 1.7 such top--like events are expected in the absence of t \\bar{t}. Good agreement in the jet spectra is obtained if jet production from t \\bar{t} pair decays is included. For those events kinematically more consistent with t \\bar{t} we find evidence for a b-quark content in their jets to the extent expected from top decay, and larger than expected for background processes. For events with four or more jets, the discrepancy with the predicted jet energy distributions from direct QCD W production, and the associated excess of b-quark content is more pronounced.']",['1994-12-14']
2534,['eng'],"['Swartz, M', 'Band, H R', 'Decker, F J', 'Emma, P', 'Fero, M J', 'Frey, R', 'King, R', 'Lath, A', 'Limberg, T', 'Prepost, R', 'Rowson, P C', 'Schumm, B A', 'Woods, M', 'Zolotorev, M S']",['Observation of target electron momentum effects in single-arm Møller polarimetry'],['Particle Physics - Experimental Results'],"['electron electron, elastic scattering', 'elastic scattering, electron electron', 'electron, polarized beam', 'polarized beam, electron', 'target, momentum', 'momentum, target', 'momentum, effect', 'polarization, measurement', 'measurement, polarization', 'polarization, asymmetry', 'asymmetry, polarization', 'angular dependence', 'photon electron, Compton scattering', 'Compton scattering, photon electron', 'beam transport, spin', 'spin, beam transport', 'experimental results', 'SLAC SLC Linac']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412006'],"['In 1992, L.G. Levchuk noted that the asymmetries measured in Møller scattering polarimeters could be significantly affected by the intrinsic momenta of the target electrons. This effect is largest in devices with very small acceptance or very high resolution in laboratory scattering angle. We use a high resolution polarimeter in the linac of the polarized SLAC Linear Collider to study this effect. We observe that the inclusion of the effect alters the measured beam polarization by -14% of itself and produces a result that is consistent with measurements from a Compton polarimeter. Additionally, the inclusion of the effect is necessary to correctly simulate the observed shape of the two-body elastic scattering peak.']",['1994-12-12']
2535,['eng'],"['Bassler, U', 'Bernardi, G']",['On the kinematic reconstruction of deep inelastic scattering at HERA'],['Particle Physics - Experimental Results'],"['electron p, deep inelastic scattering', 'deep inelastic scattering, electron p', 'p, structure function', 'structure function, small-x', 'data analysis method', 'kinematics', 'quantum electrodynamics, radiative correction', 'numerical calculations, DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412004'],"['We review and compare the reconstruction methods of the inclusive deep inelastic scattering variables used at HERA. We introduce a new prescription, the \\Sigma method, which allows to measure the structure function of the proton F_2(x,Q^2) in a large kinematic domain, and in particular in the low x-lowQ^2 region, with small systematic errors and small radiative corrections. A detailed comparison between the \\Sigma method and the other methods is shown. Extensions of the \\Sigma method are presented. The effect of QED radiation on the kinematic reconstruction and on the structure function measurement is discussed.']",['1994-12-07']
2536,['eng'],"['Forden, G E']",['W-jet rapidity correlations in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'hadroproduction, jet', 'transverse momentum, high', 'W, associated production', 'associated production, W', 'W, leptonic decay', 'leptonic decay, W', 'rapidity spectrum', 'correlation', 'angular distribution', 'mass, transverse', 'transverse, mass', 'radiative correction', 'quantum chromodynamics', 'perturbation theory, higher-order', 'color, dipole', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412002'],"['D0 has used W -> e nu events produced in association with a high p_T jet to examine the effects of strong radiative corrections. We have compared the primary jet pseudorapidity distribution, as a function of reconstructed W rapidity to leading order (LO) and next to leading order (NLO) QCD Monte Carlos, as well as a model based on extended color dipoles. Our preliminary analysis finds that the primary jet is more central than either LO or NLO expectations and is in qualitative agreement with the color dipole model.']",['1994-12-06']
2537,['eng'],"['Efimov, A', 'Artuso, M', 'Gao, M', 'Mountain, R', 'Muheim, F', 'Mukhin, Y', 'Playfer, S']",['Monte Carlo studies of a novel LiF radiator for RICH detectors'],['Particle Physics - Experimental Results'],"['Cherenkov counter, ring imaging', 'Cherenkov counter, crystal', 'lithium, fluorine', 'angular resolution', 'radiation, yield', 'magnetic detector, CLEO', 'upgrade', 'numerical calculations, Monte Carlo', 'Cornell CESR Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9502006'],['We show that a multifaceted LiF radiator produces more Cherenkov light and has better resolution per photon than a flat radiator slab when used in a ring imaging Cherenkov counter. Such a system is being considered for the CLEO III upgrade.'],['1995-02-15']
2538,['eng'],[],['Study of the photon remnant in resolved photoproduction at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, interaction', 'interaction, photon p', 'jet, photoproduction', 'photoproduction, jet', 'jet, multiple production', 'multiple production, jet', 'transverse momentum, high', 'event shape analysis, cluster', 'photon, resolved', 'rapidity spectrum', 'transverse energy, energy flow', 'energy flow, longitudinal', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9505001'],"['Photoproduction at HERA is studied in ep collisions, with the ZEUS detector, for \\gamma p centre-of-mass energies ranging from 130-270 GeV. A sample of events with two high-p_T jets (p_T > 6 GeV, \\eta <1.6) and a third cluster in the approximate direction of the electron beam is isolated using a clustering algorithm. These events are mostly due to resolved photoproduction. The third cluster is identified as the photon remnant. Its properties, such as the transverse and longitudinal energy flows around the axis of the cluster, are consistent with those commonly attributed to jets, and in particular with those found for the two jets in these events. The mean value of the photon remnant p_T with respect to the beam axis is measured to be 2.1 \\pm 0.2 GeV, which demonstrates substantial mean transverse momenta for the photon remnant.']",['1995-05-04']
2539,['eng'],"['Derrick, Malcolm', 'Krakauer, D A', 'Magill, S', 'Mikunas, D', 'Musgrave, B', 'Repond, J', 'Stanek, R', 'Talaga, R L', 'Zhang, H', 'Ayad, R', 'Bari, G', 'Basile, M', 'Bellagamba, L', 'Boscherini, D', 'Bruni, A', 'Bruni, G', 'Bruni, P', 'Cara Romeo, G', 'Castellini, G', 'Chiarini, M', 'Cifarelli, Luisa', 'Cindolo, F', 'Contin, A', 'Corradi, M', 'Gialas, I', 'Giusti, P', 'Iacobucci, G', 'Laurenti, G', 'Levi, G', 'Margotti, A', 'Massam, Thomas', 'Nania, R', 'Nemoz, C', 'Palmonari, F', 'Polini, A', 'Sartorelli, G', 'Timellini, R', 'Zamora-Garcia, Yu E', 'Zichichi, Antonino', 'Bargende, A', 'Crittenden, J A', 'Desch, K', 'Diekmann, B', 'Doeker, T', 'Eckert, M', 'Feld, L', 'Frey, A', 'Geerts, M', 'Geitz, G', 'Grothe, M', 'Haas, T', 'Hartmann, H', 'Haun, D', 'Heinloth, K', 'Hilger, E', 'Jakob, H P', 'Katz, U F', 'Mari, S M', 'Mass, A', 'Mengel, S', 'Mollen, J', 'Paul, E', 'Rembser, C', 'Schattevoy, R', 'Schramm, D', 'Stamm, J', 'Wedemeyer, R', 'Campbell-Robson, S', 'Cassidy, A', 'Dyce, N', 'Foster, B', 'George, S', 'Gilmore, R', 'Heath, G P', 'Heath, H F', 'Llewellyn, T J', 'Morgado, C J S', 'Norman, D J P', ""O'Mara, J A"", 'Tapper, R J', 'Wilson, S S', 'Yoshida, R', 'Rau, R R', 'Arneodo, M', 'Iannotti, L', 'Schioppa, M', 'Susinno, G', 'Bernstein, A M', 'Caldwell, A', 'Cartiglia, N', 'Parsons, J A', 'Ritz, S', 'Sciulli, F', 'Straub, P B', 'Wai, L', 'Yang, S', 'Zhu, Q', 'Borzemski, P', 'Chwastowski, J', 'Eskreys, Andrzej', 'Piotrzkowski, K', 'Zachara, M', 'Zawiejski, L', 'Adamczyk, L', 'Bednarek, B', 'Jelen, K', 'Kisielewska, D', 'Kowalski, T', 'Rulikowska-Zarebska, E', 'Suszycki, L', 'Zajac, J', 'Kotanski, Andrzej', 'Przybycien, M B', 'Bauerdick, L A T', 'Behrens, U', 'Beier, H', 'Bienlein, J K', 'Coldewey, C', 'Deppe, O', 'Desler, K', 'Drews, G', 'Flasinski, M', 'Gilkinson, D J', 'Glasman, C', 'Göttlicher, P', 'Grosse-Knetter, J', 'Gutjahr, B', 'Hain, W', 'Hasell, D', 'Hessling, H', 'Iga, Y', 'Joos, P', 'Kasemann, M', 'Klanner, R', 'Koch, W', 'Köpke, L', 'Kötz, U', 'Kowalski, H', 'Labs, J', 'Ladage, A', 'Löhr, B', 'Löwe, M', 'Lüke, D', 'Manczak, O', 'Monteiro, T', 'Ng, J S T', 'Nickel, S', 'Notz, D', 'Ohrenberg, K', 'Roco, M T', 'Rohde, M', 'Roldán, J', 'Schneekloth, U', 'Schulz, W', 'Selonke, F', 'Stiliaris, E', 'Surrow, B', 'Voss, T', 'Westphal, D', 'Wolf, G', 'Youngman, C', 'Zhou, J F', 'Grabosch, H J', 'Kharchilava, A I', 'Leich, A', 'Mattingly, M C K', 'Meyer, A', 'Schlenstedt, S', 'Wulff, N', 'Barbagli, G', 'Pelfer, P G', 'Anzivino, G', 'Maccarrone, G D', 'De Pasquale, S', 'Votano, L', 'Bamberger, Andreas', 'Eisenhardt, S', 'Freidhof, A', 'Söldner-Rembold, S', 'Schröder, J', 'Trefzger, T M', 'Brook, N H', 'Bussey, Peter J', 'Doyle, A T', 'Fleck, I', 'Saxon, D H', 'Utley, M L', 'Wilson, A S', 'Dannemann, A', 'Holm, U', 'Horstmann, D', 'Neumann, T', 'Sinkus, R', 'Wick, K', 'Badura, E', 'Burow, B D', 'Hagge, L', 'Lohrmann, E', 'Mainusch, J', 'Milewski, J', 'Nakahata, M', 'Pavel, N', 'Poelz, G', 'Schott, W', 'Zetsche, F', 'Bacon, T C', 'Butterworth, Ian', 'Gallo, E', 'Harris, V L', 'Hung, B Y H', 'Long, K R', 'Miller, D B', 'Morawitz, P P O', 'Prinias, A', 'Sedgbeer, J K', 'Whitfield, A F', 'Mallik, U', 'McCliment, E', 'Wang, M Z', 'Wang, S M', 'Wu, J T', 'Zhang, Y', 'Cloth, P', 'Filges, D', 'An, S H', 'Hong, S M', 'Nam, S W', 'Park, S K', 'Suh, M H', 'Yon, S H', 'Imlay, R', 'Kartik, S', 'Kim, H J', 'McNeil, R R', 'Metcalf, W', 'Nadendla, V K', 'Barreiro, F', 'Cases, G', 'Graciani, R', 'Hernández, J M', 'Hervás, L', 'Labarga, L', 'Del Peso, J', 'Puga, J', 'Terrón, J', 'De Trocóniz, J F', 'Smith, G R', 'Corriveau, F', 'Hanna, D S', 'Hartmann, J', 'Hung, L W', 'Lim, J N', 'Matthews, C G', 'Patel, P M', 'Sinclair, L E', 'Stairs, D G', 'Saint-Laurent, M G', 'Ullmann, R T', 'Zacek, G', 'Bashkirov, V', 'Dolgoshein, B A', 'Stifutkin, A', 'Bashindzhagian, G L', 'Ermolov, P F', 'Gladilin, L K', 'Golubkov, Yu A', 'Kobrin, V D', 'Kuzmin, V A', 'Proskuryakov, A S', 'Savin, A A', 'Shcheglova, L M', 'Solomin, A N', 'Zotov, N P', 'Botje, M', 'Chlebana, F S', 'Dake, A P', 'Engelen, J', 'De Kamps, M', 'Kooijman, P M', 'Kruse, A', 'Tiecke, H G', 'Verkerke, W', 'Vreeswijk, M', 'Wiggers, L', 'De Wolf, E', 'Van Woudenberg, R', 'Acosta, D', 'Bylsma, B G', 'Durkin, L S', 'Honscheid, K', 'Li Chuan', 'Ling, T Y', 'McLean, K W', 'Murray, W N', 'Park, I H', 'Romanowsky, T A', 'Seidlein, R', 'Bailey, D S', 'Blair, G A', 'Byrne, A', 'Cashmore, Roger J', 'Cooper-Sarkar, A M', 'Daniels, D C', 'Devenish, R C E', 'Harnew, N', 'Lancaster, M', 'Luffman, P', 'Lindemann, L', 'McFall, J D', 'Nath, C', 'Noyes, V A', 'Quadt, A', 'Uijterwaal, H', 'Walczak, R', 'Wilson, F F', 'Yip, T', 'Abbiendi, G', 'Bertolin, A', 'Brugnera, R', 'Carlin, R', 'Dal Corso, F', 'De Giorgi, M', 'Dosselli, U', 'Limentani, S', 'Morandin, M', 'Posocco, M', 'Stanco, L', 'Stroili, R', 'Voci, C', 'Bulmahn, J', 'Butterworth, J M', 'Feild, R G', 'Whitmore, J', ""D'Agostini, G"", 'Marini, G', 'Nigro, A', 'Tassi, E', 'Hart, J C', 'McCubbin, N A', 'Prytz, K', 'Shah, T P', 'Short, T L', 'Barberis, E', 'Dubbs, T', 'Heusch, C A', 'Van Hook, M', 'Hubbard, B', 'Lockman, W', 'Rahn, J T', 'Sadrozinski, H F W', 'Seiden, A', 'Biltzinger, J', 'Seifert, R J', 'Walenta, A H', 'Zech, G', 'Abramowicz, H', 'Briskin, G M', 'Dagan, S', 'Levy, A', 'Hasegawa, T', 'Hazumi, M', 'Ishii, T', 'Kuze, M', 'Mine, S', 'Nagasawa, Y', 'Nakao, M', 'Susuki, I', 'Tokushuku, K', 'Yamada, S', 'Yamazaki, Y', 'Chiba, M', 'Hamatsu, R', 'Hirose, T', 'Homma, K', 'Kitamura, S', 'Nakamitsu, Y', 'Yamauchi, K', 'Cirio, R', 'Costa, M', 'Ferrero, M I', 'Lamberti, L', 'Maselli, S', 'Peroni, C', 'Sacchi, R', 'Solano, A', 'Staiano, A', 'Dardo, M', 'Bailey, D C', 'Bandyopadhyay, D', 'Bénard, F', 'Brkic, M', 'Crombie, M B', 'Gingrich, D M', 'Hartner, G F', 'Joo, K K', 'Levman, G M', 'Martin, J F', 'Orr, R S', 'Sampson, C R', 'Teuscher, R J', 'Catterall, C D', 'Jones, T W', 'Kaziewicz, P B', 'Lane, J B', 'Saunders, R L', 'Shulman, J', 'Blankenship, K', 'Lu, B', 'Mo, L W', 'Bogusz, W', 'Charchula, K', 'Ciborowski, J', 'Gajewski, J', 'Grzelak, G', 'Kasprzak, M', 'Krzyzanowski, M', 'Muchorowski, K', 'Nowak, R J', 'Pawlak, J M', 'Tymieniecka, T', 'Wróblewski, A K', 'Zakrzewski, J A', 'Zarnecki, A F', 'Adamus, M', 'Eisenberg, Y', 'Karshon, U', 'Revel, D', 'Zer-Zion, D', 'Ali, I', 'Badgett, W F', 'Behrens, B H', 'Dasu, S', 'Fordham, C', 'Foudas, C', 'Goussiou, A', 'Loveless, R J', 'Reeder, D D', 'Silverstein, S', 'Smith, W H', 'Vaiciulis, A W', 'Wodarczyk, M', 'Tsurugai, T', 'Bhadra, S', 'Cardy, M L', 'Fagerstroem, C P', 'Frisken, W R', 'Furutani, K M', 'Khakzad, M', 'Schmidke, W B']",['Inclusive transverse momentum distributions of charged particles in diffractive and non-diffractive photoproduction at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'electron p, inclusive reaction', 'charged particle, photoproduction', 'photoproduction, charged particle', 'diffraction', 'nondiffractive', 'transverse momentum, spectra', 'spectra, transverse momentum', 'quantum chromodynamics, perturbation theory', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9503014'],"['Inclusive transverse momentum spectra of charged particles in photoproduction events in the laboratory pseudorapidity range -1.2<\\eta<1.4 have been measured up to p_{T}=8\\GeV using the ZEUS detector. Diffractive and non--diffractive reactions have been selected with an average \\gamma p centre of mass (c.m.) energy of \\langle W \\rangle = 180\\GeV. For diffractive reactions, the p_{T} spectra of the photon dissociation events have been measured in two intervals of the dissociated photon mass with mean values \\langle M_{X} \\rangle = 5 GeV and 10 GeV. The inclusive transverse momentum spectra fall exponentially in the low p_{T} region. The non--diffractive data show a pronounced high p_{T} tail departing from the exponential shape. The p_{T} distributions are compared to lower energy photoproduction data and to hadron--hadron collisions at a similar c.m. energy. The data are also compared to the results of a next--to--leading order QCD calculation.']",['1995-03-28']
2540,['eng'],[],['Observation of hard scattering in photoproduction events with a large rapidity gap at HERA'],['Particle Physics - Experimental Results'],"['electron p, colliding beams', 'colliding beams, electron p', 'exchange, one-photon', 'one-photon, exchange', 'photon p, interaction', 'interaction, photon p', 'jet, photoproduction', 'photoproduction, jet', 'hadron, multiple production', 'multiple production, hadron', 'diffraction', 'rapidity spectrum, gap', 'transverse energy, energy flow', 'transverse energy, high', 'hard scattering', 'magnetic detector, ZEUS', 'experimental results', 'DESY HERA Stor', '296 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501011'],"['Events with a large rapidity gap and total transverse energy greater than 5 GeV have been observed in quasi-real photoproduction at HERA with the ZEUS detector. The distribution of these events as a function of the \\gamma p centre of mass energy is consistent with diffractive scattering. For total transverse energies above 12 GeV, the hadronic final states show predominantly a two-jet structure with each jet having a transverse energy greater than 4 GeV. For the two-jet events, little energy flow is found outside the jets. This observation is consistent with the hard scattering of a quasi-real photon with a colourless object in the proton.']",['1995-01-31']
2541,['eng'],"['Sinkus, R']",['A novel approach to error function minimization for feedforward neural networks'],['Particle Physics - Experimental Results'],"['neural network', 'statistical analysis, error', 'particle identification, (electron)', 'numerical calculations', 'magnetic detector, ZEUS', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501007'],"['Feedforward neural networks with error backpropagation (FFBP) are widely applied to pattern recognition. One general problem encountered with this type of neural networks is the uncertainty, whether the minimization procedure has converged to a global minimum of the cost function. To overcome this problem a novel approach to minimize the error function is presented. It allows to monitor the approach to the global minimum and as an outcome several ambiguities related to the choice of free parameters of the minimization procedure are removed.']",['1995-01-19']
2542,['eng'],"['Abachi, S']",['Search for high mass top quark production in p$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'final state, ((n)jet dilepton)', '((n)jet dilepton), final state', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'mass, truth', 'truth, mass', 'channel cross section, mass', 'mass, channel cross section', 'magnetic detector, CDF', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9411001'],"['We present new results on the search for the top quark in p anti-p collisions at S**(1/2) = 1.8 TeV with an integrated luminosity of 13.5 +- 1.6 pb**(-1). We have considered t anti-t production in the Standard Model using electron and muon dilepton decay channels (t anti-t -> e mu + jets, e e + jets, and mu mu + jets) and single-lepton decay channels (t anti-t -> e + jets and mu + jets) with and without tagging of b quark jets. From all channels, we have 9 events with an expected background of 3.8 +- 0.9. If we assume that the excess is due to t anti-t production, and assuming a top mass of 180 GeV/c**2, we obtain a cross section of 8.2 +- 5.1 pb.']",['1994-11-10']
2543,['eng'],"['Abe, F']",['Charge asymmetry in W-boson decays produced in p-$\\overline{p}$ collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'W, hadroproduction', 'hadroproduction, W', 'W, width', 'W, leptonic decay', 'leptonic decay, W', 'charge, asymmetry', 'rapidity dependence', 'quark, momentum spectrum', 'quark, up', 'quark, down', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501008'],"['The charge asymmetry has been measured using 19,039~W decays recorded by the CDF detector during the 1992-93 run of the Tevatron Collider. The asymmetry is sensitive to the ratio of d and u quark distributions to x<0.01 at Q^2 \\approx M_W^2, where nonperturbative effects are minimal. It is found that of the two current sets of parton distributions, those of Martin, Roberts and Stirling (MRS) are favored over the sets most recently produced by the CTEQ collaboration. The W asymmetry data provide a stronger constraints on d/u ratio than the recent measurements of F_2^{\\mu n}/F_2^{\\mu p} which are limited by uncertainties originating from deutron corrections.']",['1995-01-19']
2544,['eng'],"['Abe, K', 'Abt, I', 'Ahn, C J', 'Akagi, T', 'Ash, William W', 'Aston, D', 'Bacchetta, N', 'Baird, K G', 'Baltay, C', 'Band, H R', 'Barakat, M B', 'Baranko, G J', 'Bardon, O', 'Barklow, T L', 'Bazarko, A O', 'Ben-David, R', 'Benvenuti, Alberto C', 'Bienz, T', 'Bilei, G M', 'Bisello, D', 'Blaylock, G', 'Bogart, J R', 'Bolton, T', 'Bower, G R', 'Brau, J E', 'Breidenbach, M I', 'Bugg, W M', 'Burke, D', 'Burnett, T H', 'Burrows, P N', 'Busza, W', 'Calcaterra, A', 'Caldwell, D O', 'Calloway, D H', 'Camanzi, B', 'Carpinelli, M', 'Cassell, R', 'Castaldi, R', 'Castro, A', 'Cavalli-Sforza, M', 'Church, E', 'Cohn, H O', 'Coller, J A', 'Cook, V', 'Cotton, R', 'Cowan, R F', 'Coyne, D G', 'de Oliveira, A', 'Damerell, C J S', 'Dasu, S', 'De Sangro, R', 'De Simone, P', ""Dell'Orso, R"", 'Dima, M', 'Du, P Y C', 'Dubois, R', 'Eisenstein, B I', 'Elia, R', 'Falciai, D', 'Fan, C', 'Fero, M J', 'Frey, R', 'Furuno, K', 'Gillman, T', 'Gladding, G E', 'González, S', 'Hallewell, G D', 'Hart, E L', 'Hasegawa, Y', 'Hedges, S J', 'Hertzbach, S S', 'Hildreth, M D', 'Huber, J', 'Huffer, M E', 'Hughes, E W', 'Hwang, H', 'Iwasaki, Y', 'Jacques, P', 'Jaros, J A', 'Johnson, A S', 'Johnson, J R', 'Johnson, R A', 'Junk, T R', 'Kajikawa, R', 'Kalelkar, M S', 'Karliner, I', 'Kawahara, H', 'Kendall, H W', 'Kim, Y', 'King, M E', 'King, R', 'Kofler, R R', 'Krishna, N M', 'Kroeger, R S', 'Labs, J F', 'Langston, M', 'Lath, A', 'Lauber, J A', 'Leith, D W G S', 'Liu, X', 'Loreti, M', 'Lu, A', 'Lynch, H L', 'Ma, J', 'Mancinelli, G', 'Manly, S L', 'Mantovani, G C', 'Markiewicz, T W', 'Maruyama, T', 'Massetti, R', 'Masuda, H', 'Mazzucato, E', 'McKemey, A K', 'Meadows, B T', 'Messner, R', 'Mockett, P M', 'Moffeit, K C', 'Mours, B', 'Müller, G', 'Müller, D', 'Nagamine, T', 'Nauenberg, U', 'Neal, H A', 'Nussbaum, M', 'Ohnishi, Y', 'Osborne, L S', 'Panvini, R S', 'Park, H', 'Pavel, T J', 'Peruzzi, I', 'Pescara, L', 'Piccolo, M', 'Piemontese, L', 'Pieroni, E', 'Pitts, K T', 'Plano, R J', 'Prepost, R', 'Prescott, C Y', 'Punkar, G D', 'Quigley, J', 'Ratcliff, B N', 'Reeves, T W', 'Rensing, P E', 'Rochester, L S', 'Rothberg, J E', 'Rowson, P C', 'Russell, J J', 'Saxton, O H', 'Schalk, T L', 'Schindler, R H', 'Schneekloth, U', 'Schumm, B A', 'Seiden, A', 'Sen, S', 'Serbo, V V', 'Shaevitz, M H', 'Shank, J T', 'Shapiro, G', 'Shapiro, S L', 'Sherden, D J', 'Simopoulos, C', 'Sinev, N B', 'Smith, S R', 'Snyder, J A', 'Stamer, P E', 'Steiner, H', 'Steiner, R', 'Strauss, M G', 'Su, D', 'Suekane, F', 'Sugiyama, A', 'Suzuki, S', 'Swartz, M', 'Szumilo, A', 'Takahashi, T', 'Taylor, F E', 'Torrence, E', 'Turk, J', 'Usher, T', 'Vavra, J', 'Vannini, C', 'Vella, E N', 'Venuti, J P', 'Verdini, P G', 'Wagner, S R', 'Waite, A P', 'Watts, S J', 'Weidemann, A W', 'Whitaker, J S', 'White, S L', 'Wickens, F J', 'Williams, D A', 'Williams, D C', 'Williams, S H', 'Willocq, S', 'Wilson, R J', 'Wisniewski, W J', 'Woods, M', 'Word, G B', 'Wyss, J', 'Yamamoto, R K', 'Yamartino, J M', 'Yang, X', 'Yellin, S J', 'Young, C C', 'Yuta, H', 'Zapalac, G H', 'Zdarko, R W', 'Zeitlin, C', 'Zhou, J']",['Measurement of $\\alpha_{s}$(M$_{Z}^{2}$) from hadronic event observables at the $Z^{0}$ resonance'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, nonleptonic decay', 'nonleptonic decay, Z0', 'event shape analysis', 'jet, multiplicity', 'energy, correlation', 'asymmetry', 'energy flow', 'strong interaction, coupling constant', 'coupling constant, strong interaction', 'quantum chromodynamics, perturbation theory', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'bibliography', 'tables', 'approx. 91 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=.&id=SCAN-9412204', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501003']",[],['1994-12-15']
2545,['eng'],"['Park, C H']",['VLPC characterization for the D0 upgrade'],['Particle Physics - Experimental Results'],"['scintillation counter, fibre', 'optics, readout', 'semiconductor, optical', 'efficiency', 'upgrade', 'four-pi-detector, DZERO', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410011'],"['We have studies the performance characteristics of approximately 4000 Visible Light Photon Counters(VLPC) over a range of operating temperatures and biases. We will describe the characterization procedure and present the measured gain, noise and the relative quantum efficiency for the devices. We will also discuss the general operation of the devices and the significant problems during the characterization.']",['1994-10-18']
2546,['eng'],"['Abe, K']",['A search for jet handedness in hadronic Z$^{0}$ decays'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'electron, polarized beam', 'polarized beam, electron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, nonleptonic decay', 'nonleptonic decay, Z0', 'quark, pair production', 'pair production, quark', 'quark, jet', 'antiquark, jet', 'jet, polarization', 'polarization, jet', 'analyzing power, upper limit', 'helicity, amplitude analysis', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501006'],"[""We have searched for signatures of polarization in hadronic jets from Z^0 \\rightarrow q \\bar{q} decays using the ``jet handedness'' method. The polar angle asymmetry induced by the high SLC electron-beam polarization was used to separate quark jets from antiquark jets, expected to be left- and right-polarized, respectively. We find no evidence for jet handedness in our global sample or in a sample of light quark jets and we set upper limits at the 95\\% C.L. of 0.063 and 0.099 respectively on the magnitude of the analyzing power of the method proposed by Efremov {\\it et al.}""]",['1995-01-16']
2547,['eng'],"['Hong, J T']",['Search for slowly moving magnetic monopoles'],['Particle Physics - Experimental Results'],"['talk, Assergi 1993/09/19', 'postulated particle, magnetic monopole', 'postulated particle, dyon', 'grand unified theory', 'cosmic radiation', 'flux, upper limit', 'upper limit, flux', 'dependence, velocity', 'trigger, efficiency', 'deep underground detector, MACRO', 'scintillation counter, experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410006'],['We report a search for slowly moving magnetic monopoles in the cosmic radiation with the first supermodule of the MACRO detector at Gran Sasso. The absence of candidates established an upper limit on the monopole flux of 5.6\\times10^{-15}\\mbox{cm}^{-2}\\mbox{sr}^{-1}\\ mbox{s}^{-1} at 90\\% confidence level for the velocity range of 1.8\\times10^{-4}<\\beta<3\\times10^{-3}.'],['1994-10-17']
2548,['eng'],"['Hagopian, S']",['Search for supersymmetry and leptoquark states at FNAL'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'new particle, search for', 'postulated particle, leptoquark', 'leptoquark, pair production', 'pair production, leptoquark', 'decay, leptoquark', 'leptoquark, decay', 'mass, leptoquark', 'leptoquark, mass', 'lower limit', 'postulated particle, squark', 'postulated particle, gluino', 'final state, ((n)jet missing-energy)', '((n)jet missing-energy), final state', 'sparticle, mass', 'mass, sparticle', 'channel cross section, upper limit', 'four-pi-detector, DZERO', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms,']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410003', 'http://fnalpubs.fnal.gov/archive/1994/conf/Conf-94-331-E.pdf']","['Searches have been made for first generation scalar and vector leptoquarks by the D0 collaboration and for second generation scalar leptoquarks by the CDF collaboration. Lower leptoquark mass limits were set. A search for squarks and gluinos, predicted by Supersymmetric models, was made by D0 in the three or more jets plus missing Et channel. The number of events observed was consistent with background. Squark and gluino mass limits were set.']",['1996-04-03']
2549,['eng'],"['Hong, J T']",['Multiple muon measurements with MACRO'],['Particle Physics - Experimental Results'],"['talk', 'muon, cosmic radiation', 'muon, multiplicity', 'muon, flux', 'flux, muon', 'cosmic radiation, primary', 'cosmic radiation, energy spectrum', 'energy spectrum, cosmic radiation', 'cosmic radiation, mass spectrum', 'mass spectrum, cosmic radiation', 'muon, spatial distribution', 'angular distribution, dimuon', 'dimuon, angular distribution', 'deep underground detector, MACRO', 'experimental results']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410001'],"['The MACRO experiment at Gran Sasso provides means for detailed studies of multiple coincident penetrating cosmic ray muons. In this paper we concentrate on the studies of the ultrahigh energy primary cosmic ray composition using muon bundle multiplicities, muon pair lateral and angular separation distributions.']",['1996-04-03']
2550,['eng'],"['Blessing, S K']",['Search for supersymmetric wino and zino states using the D0 detector'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'sparticle, search for', 'postulated particle, Wino', 'postulated particle, Zino', 'sparticle, pair production', 'pair production, sparticle', 'sparticle, leptonic decay', 'leptonic decay, sparticle', 'final state, (3lepton missing-energy)', '(3lepton missing-energy), final state', 'particle identification, efficiency', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> Wino Zino anything', '1800 GeV-cms,']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410002'],"['The status of a search for the pair production of the lightest chargino and second lightest neutralino states of the minimal supersymmetric model is presented. We have searched for four tri-lepton final states: eee, eemu, emumu, and mumumu, all with missing transverse energy.']",['1994-10-17']
2551,['eng'],"['Enomoto, R', 'Abe, K', 'Abe, T', 'Adachi, I', 'Adachi, K', 'Aoki, M', 'Aoki, M', 'Awa, S', 'Emi, K', 'Fujii, H', 'Fujii, K', 'Fujii, T', 'Fujimoto, J', 'Fujita, K', 'Fujiwara, N', 'Hayashii, H', 'Howell, B', 'Iida, N', 'Itoh, R', 'Inoue, Y', 'Iwasaki, H', 'Iwasaki, M', 'Kaneyuki, K', 'Kajikawa, R', 'Kato, S', 'Kawabata, S', 'Kichimi, H', 'Kobayashi, M', 'Koltick, D S', 'Levine, I', 'Minami, S', 'Miyabayashi, K', 'Miyamoto, A', 'Muramatsu, K', 'Nagai, K', 'Nakabayashi, K', 'Nakano, E', 'Nitoh, O', 'Noguchi, S', 'Ochi, A', 'Ochiai, F', 'Ohishi, N', 'Ohnishi, Y', 'Ohshima, Y', 'Okuno, H', 'Okusawa, T', 'Shinohara, T', 'Sugiyama, A', 'Suzuki, S', 'Suzuki, S', 'Takahashi, K', 'Takahashi, T', 'Tanimori, T', 'Tauchi, T', 'Teramoto, Y', 'Toomi, N', 'Tsukamoto, T', 'Tsumura, O', 'Uno, S', 'Watanabe, T', 'Watanabe, Y', 'Yamaguchi, A', 'Yamamoto, A', 'Yamauchi, M']",['K$^{0}$($\\overline{K}^{0}$) production in two-photon processes at TRISTAN'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'exchange, two-photon', 'two-photon, exchange', 'photon photon, inclusive reaction', 'K0, photoproduction', 'photoproduction, K0', 'photon, resolved', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', 'approx. 58 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=.&id=SCAN-9412224', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412003']","['We have carried out an inclusive measurement of K^0(\\overline{K^0}) production in two-photon processes at TRISTAN. The mean \\sqrt{s} was 58 GeV and the integrated luminosity was 199 pb^{-1}. High-statistics K_s samples were obtained under such conditions as no-, anti-electron, and remnant-jet tags. The remnant-jet tag, in particular, allowed us, for the first time, to measure the cross sections separately for the resolved-photon and direct processes.']",['1994-12-20']
2552,['eng'],"['Raja, R']",['Search for top in D0 using the electron + jets channel with soft $\\mu$ tagging'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'search for, truth', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'final state, ((n)jet muon electron)', '((n)jet muon electron), final state', 'jet, multiplicity', 'background', 'transverse energy, missing-energy', 'channel cross section, mass', 'mass, channel cross section', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9409005'],"['We present preliminary results for the search for the top quark in D-Zero in the electron + jets channel where one of the b quark jets is tagged by means of a soft muon, using 13.5 pb-1 of data. Standard model decay modes for the top quark are assumed. We present the resulting top cross section and error as a function of top mass using this channel combined with the dilepton channel and the untagged lepton + jets channel . At present, no significant signal for top quark production can be established.']",['1994-10-17']
2553,['eng'],"['Adachi, I', 'Sumiyoshi, T', 'Hayashi, K', 'Iida, N', 'Enomoto, R', 'Tsukada, K', 'Suda, R', 'Matsumoto, S', 'Natori, K', 'Yokoyama, M', 'Yokogawa, H']",['Study of a threshold Cherenkov counter based on silica aerogels with low refractive indices'],['Detectors and Experimental Techniques'],"['particle identification, (K pi)', 'Cherenkov counter, threshold', 'Cherenkov counter, aerogel', 'optics, dispersion']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412008'],"['To identify \\pi^{\\pm} and K^{\\pm} in the region of 1.0\\sim 2.5 GeV/c, a threshold Cherenkov counter equipped with silica aerogels has been investigated. Silica aerogels with a low refractive index of 1.013 have been successfully produced using a new technique. By making use of these aerogels as radiators, we have constructed a Cherenkov counter and have checked its properties in a test beam. The obtained results have demonstrated that our aerogel was transparent enough to make up for loss of the Cherenkov photon yield due to a low refractive index. Various configurations for the photon collection system and some types of photomultipliers, such as the fine-mesh type, for a read out were also tested. From these studies, our design of a Cherenkov counter dedicated to \\pi / K separation up to a few GeV/c %in the momentum range of 1.0 \\sim 2.5 GeV/c with an efficiency greater than 90 \\% was considered.']",['1994-12-14']
2554,['eng'],"['Cinabro, D']",['Measurement of the branching fraction for $\\Upsilon$ (1S) --> $\\tau^{+}\\tau^{-}$'],['Particle Physics - Experimental Results'],"['colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Upsilon(9460), electroproduction', 'electroproduction, Upsilon(9460)', 'Upsilon(9460), leptonic decay', 'leptonic decay, Upsilon(9460)', 'tau, pair production', 'pair production, tau', 'final state, (electron)', '(electron), final state', 'lepton, universality', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Upsilon(9460)', 'Upsilon(9460) --> tau+ tau-', 'approx. 9.46 GeV-cms', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Upsilon(9460), electroproduction', 'electroproduction, Upsilon(9460)', 'Upsilon(9460), leptonic decay', 'leptonic decay, Upsilon(9460)', 'Upsilon(9460), branching ratio', 'tau, pair production', 'pair production, tau', 'lepton, universality', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'electron positron --> Upsilon(9460)', 'Upsilon(9460) --> tau+ tau-', '9.46 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9409004'],['We have studied the leptonic decay of the \\Upsilon (1S) resonance into tau pairs using the CLEO II detector. A clean sample of tau pair events is identified via events containing two charged particles where exactly one of the particles is an identified electron. We find B(\\Upsilon(1S) \\rightarrow \\tau^+ \\tau^-) = \\left(2.61~\\pm~0.12~{ +0.09\\atop{-0.13}}\\right)\\%. The result is consistent with expectations from lepton universality.'],['1996-05-02']
2555,['eng'],"['Kreutz, A', 'Holder, M', 'Rost, M', 'Werthenbach, R', 'Siegen, G', 'Peach, Kenneth J', 'Blümer, H', 'Heinz, R', 'Kleinknecht, K', 'Mayer, P', 'Panzer, B', 'Renk, B', 'Rohrer, H', 'Wagner, A', 'Augé, E', 'Fournier, D', 'Iconomidou-Fayard, L', 'Perdereau, O', 'Schaffer, A C', 'Serin, L', 'Bertanza, L', 'Bigi, A', 'Calafiura, P', 'Calvetti, M', 'Carosi, R', 'Casali, R', 'Cerri, C', 'Mannelli, I', 'Marzulli, V M', 'Nappi, A', 'Pierazzini, G M']",['Determination of the branching ratios $\\Gamma(K_{L} \\to 3\\pi^{0}) / \\Gamma(K_{L} \\to \\pi^{+}\\pi^{-}\\pi^{0})$ and $\\Gamma(K_{L} \\to 3\\pi^{0}) / \\Gamma(K_{L} \\to \\pi e\\nu)$'],['Particle Physics - Experimental Results'],"['K0(L), nonleptonic decay', 'nonleptonic decay, K0(L)', 'K0(L), semileptonic decay', 'semileptonic decay, K0(L)', 'K0(L), branching ratio']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9409003'],"['Improved branching ratios were measured for the K_L \\to 3 \\pi^0 decay in a neutral beam at the CERN SPS with the NA31 detector:\\\\ \\Gamma (K_L \\to 3 \\pi^0) / \\Gamma (K_L \\to \\pi^+ \\pi^- \\pi^0) = 1.611 \\pm 0.037 and\\\\ \\Gamma (K_L \\to 3 \\pi^0) / \\Gamma (K_L \\to \\pi e \\nu ) = 0.545 \\pm 0.010.\\\\ {}From the first number an upper limit for \\Delta I =5/2 and \\Delta I = 7/2 transitions in neutral kaon decay is derived. Using older results for the Ke3/K\\mu 3 fraction, the 3\\pi^0 branching ratio is found to be \\Gamma (K_L \\to 3 \\pi^0 )/ \\Gamma_{tot} = (0.211 \\pm 0.003), about a factor three more precise than from previous experiments.\\\\[1ex]']",['1994-10-17']
2556,['eng'],"['Skarha, J']",['B meson lifetimes at CDF'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'beautiful meson, hadroproduction', 'hadroproduction, beautiful meson', 'beautiful meson, nonleptonic decay', 'nonleptonic decay, beautiful meson', 'beautiful meson, semileptonic decay', 'semileptonic decay, beautiful meson', 'K*(892)', 'Phi(1020)', 'D*(2010)', 'psi mesons', 'B+, lifetime', 'B0, lifetime', 'lifetime, ratio', 'charmed meson, nonleptonic decay', 'nonleptonic decay, charmed meson', 'psi(3685), hadronic decay', 'hadronic decay, psi(3685)', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'B+ --> D0 positron neutrino anything', 'B- --> psi mesons K', 'B --> psi mesons K*(892)', 'B0 --> D*(2010) electron neutrino anything', '1800 GeV-cms', 'B/s, lifetime', 'J/psi(3100), leptonic decay', 'leptonic decay, J/psi(3100)', 'B/s --> D/s lepton neutrino anything', 'B/s --> psi mesons Phi(1020)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412014'],"['Measurements of the B_u, B_d, and B_s meson lifetime using semileptonic B_u \\rightarrow e \\nu D^0 X, B_d \\rightarrow e \\nu D^* X, B_s \\rightarrow l \\nu D_s X events and exclusive B_u \\rightarrow \\psi^{(\\prime)} K^{(*)}, B_d \\rightarrow \\psi^{(\\prime)} K^{(*)}_{(s)}, B_s \\rightarrow \\psi \\phi events are presented. These results used the precise position measurements of the CDF SVX silicon vertex detector and were obtained from a 19.3 pb^{-1} sample of 1.8 TeV \\overline{p}p collisions collected in 1992-93 at the Fermilab Tevatron collider. Comparisons with previous measurements will be shown.']",['1995-01-06']
2557,['eng'],"['Grannis, P D']",['Search for the top quark'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'search for, truth', 'quark, truth', 'quark, pair production', 'pair production, quark', 'quark, decay modes', 'decay modes, quark', 'final state, ((n)jet lepton)', '((n)jet lepton), final state', 'final state, ((n)jet dilepton)', '((n)jet dilepton), final state', 'transverse energy, missing-energy', 'channel cross section, mass', 'mass, channel cross section', 'particle identification, beauty', 'vector meson, postulated particle', 'color, octet', 'eta, technicolor', 'postulated particle, decay', 'decay, postulated particle', 'background', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9409006'],"['We review the search for the top quark conducted by the D-Zero collaboration using data from the Fermilab pbar-p collider. Based upon a preliminary analysis of an integrated luminosity of about 13.5 pb-1, we have searched for t-tbar production and decay in the experimental channels involving a pair of dileptons (electron or muon) plus jets, or single leptons plus jets. Summed over all channels, we observe 7 events in our data, to be compared with an expectation from background processes of 3.2 +/- 1.1 events. The t-tbar ~cross-section deduced from the small excess of events is presented as a function of the top quark mass. The statistics are sufficiently limited that no clear evidence for the existence of the top quark can be obtained. We also comment upon contributions to the Parallel session devoted to the top quark at this conference.']",['1994-10-17']
2558,['eng'],"['Skarha, J']",['Mechanical design of the CDF SVX~II silicon vertex detector'],['Particle Physics - Experimental Results'],"['talk', 'semiconductor detector, vertex', 'performance, proposed', 'magnetic detector, CDF', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501009'],"['A next generation silicon vertex detector is planned at CDF for the 1998 Tevatron collider run with the Main Injector. The SVX~II silicon vertex detector will allow high luminosity data-taking, enable online triggering of secondary vertex production, and greatly increase the acceptance for heavy flavor physics at CDF. The design specifications, geometric layout, and early mechanical prototyping work for this detector are discussed.']",['1995-01-24']
2559,['eng'],"['Papadimitriou, V']",['Upsilon production at CDF'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'Upsilon(9460), hadroproduction', 'hadroproduction, Upsilon(9460)', 'Upsilon(10020), hadroproduction', 'hadroproduction, Upsilon(10020)', 'Upsilon(10355), hadroproduction', 'hadroproduction, Upsilon(10355)', 'upsilon mesons, leptonic decay', 'leptonic decay, upsilon mesons', 'mass spectrum, dimuon', 'dimuon, mass spectrum', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'channel cross section', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> upsilon mesons anything', 'upsilon mesons --> muon+ muon-', '1800 GeV-cms']","['http://www-lib.fnal.gov/archive/1995/conf/Conf-95-227-E.html', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9501010']","['We report on measurements of the Upsilon(1S), Upsilon(2S) and Upsilon(3S) differential and integrated cross sections in pp(bar) collisions at sqrt(s)=1.8 TeV. The three resonances were reconstucted through the decay Upsilon-->mu(+)mu(-). The cross section measurements are compared to theoretical models of direct bottomonium production.']",['1995-01-25']
2560,['eng'],"['De Jongh, F']",['$B^{+}$ and $B^{0}$ mean lifetime measurements'],['Particle Physics - Experimental Results'],"['review', 'B+, lifetime', 'B0, lifetime', 'B, branching ratio', 'B, nonleptonic decay', 'nonleptonic decay, B', 'B, semileptonic decay', 'semileptonic decay, B', 'B, electroproduction', 'electroproduction, B', 'B, hadroproduction', 'hadroproduction, B', 'experimental results']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9409002', 'http://fnalpubs.fnal.gov/archive/1994/conf/Conf-94-245.pdf']","['We review B^+ and B^0 mean lifetime measurements, including direct measurements and determination of the lifetime ratio via measurements of the ratio of branching ratios. We present world averages.']",['1996-04-03']
2561,['eng'],"['Norman, D M']",['Search for first and second generation leptoquarks at D0'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'search for, leptoquark', 'leptoquark, pair production', 'pair production, leptoquark', 'scalar particle, leptoquark', 'mass, leptoquark', 'leptoquark, mass', 'lower limit', 'decay, leptoquark', 'leptoquark, decay', 'final state, ((n)jet muon missing-energy)', '((n)jet muon missing-energy), final state', 'final state, ((n)jet dimuon)', '((n)jet dimuon), final state', 'transverse energy, missing-energy', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9409008'],"[""A search for first and second generation leptoquarks has been done with the D\\O \\ detector at Fermilab's p\\={p} collider with \\sqrt{s}=1.8 TeV. 95\\% C.L. mass limits for first generation scalar leptoquarks have been recently published. The number for the total integrated luminosity used in the first generation leptoquark analysis has changed (via a change in the total inelastic cross section) since the publication. The new limits are 130 GeV/c^{2} and 116 GeV/c^{2} for a respective 100\\% and 50\\% decay branching ratio of the leptoquark to electron. The preliminary upper limit on the cross section from the search for second generation scalar leptoquarks has set limits on the mass of the second generation leptoquark of 97 GeV/c^{2} for 100\\% branching to muons and 80 GeV/c^{2} for 50\\% branching. In contrast with leptoquark detection thresholds at e^{+}e^{-} and e-p machines, these limits are independent of the unknown coupling of the leptoquark to leptons and quarks.""]",['1994-10-17']
2562,['eng'],"['Pitts, K T']",['Polarized Bhabha scattering and a precision measurement of the electron neutral current couplings'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, elastic scattering', 'elastic scattering, electron positron', 'electron, polarized beam', 'polarized beam, electron', 'polarization, asymmetry', 'asymmetry, polarization', 'Weinberg angle', 'electron, coupling constant', 'coupling constant, electron', 'coupling constant, vector', 'vector, coupling constant', 'coupling constant, axial-vector', 'axial-vector, coupling constant', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410009'],['We present the first measurement of the left-right asymmetry in Bhabha scattering with a polarized electron beam. The effective electron vector and axial vector couplings to the Z.sup.(0) are extracted from a combined analysis of the polarized Bhabha scattering data and the left-right asymmetry previously published by this collaboration.'],['1994-10-18']
2563,['eng'],"['Piekarz, H']",['A study of events with large total transverse energy produced in proton-antiproton collisions at \\Sqrt s = 1.8 TeV'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'jet, hadroproduction', 'hadroproduction, jet', 'jet, multiplicity', 'event shape analysis, cluster', 'transverse energy, spectra', 'spectra, transverse energy', 'rapidity spectrum', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON PS', '1800 GeV-cms']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410008', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=.&id=SCAN-9409100']","['Properties of events originating from proton--antiproton interactions in which the total transverse energy of the event exceeded 400 GeV are presented. Based on a data sample of 5.45 pb-1, the topology of these hard scattering events as well as preliminary results for the cross--section versus total transverse energy are presented and discussed.']",['1994-10-18']
2564,['eng'],"['Amidei, D', 'Baden, A', 'Foster, G', 'Jackson, G', 'Kamon, T', 'López, J', 'McIntyre, P', 'Strait, J B', 'White, J']",['Tevatron energy and luminosity upgrades beyond the main injector'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, storage ring', 'energy, upgrade', 'luminosity, upgrade', 'anti-p, particle source', 'magnet, superconducting', 'superconducting, magnet', 'beam optics', 'Batavia TEVATRON PS', 'Batavia TEVATRON Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9408005'],"[""The Fermilab Tevatron will be the world's highest energy hadron collider until the LHC is commissioned, it has the world's highest energy fixed target beams, and Fermilab will be the leading high energy physics laboratory in the US for the foreseeable future. Following the demise of the SSC, a number of possible upgrades to the Tevatron complex, beyond construction of the Main Injector, are being discussed. Using existing technology, it appears possible to increase the luminosity of the \\bar{p}p Collider to at least 10^{33}cm^{-2}sec^{-1} (Tevatron-Star) and to increase the beam energy to 2 TeV (DiTevatron). Fixed target beam of energy about 1.5 TeV could also be delivered. Leaving the existing Tevatron in the tunnel and constructing bypasses around the collider halls would allow simultaneous 800 GeV fixed target and \\sqrt{s} = 4 TeV collider operation. These upgrades would give Fermilab an exciting physics program which would be complementary to the LHC, and they would lay the groundwork for the construction of a possible post-LHC ultra-high energy hadron collider. (Presented at the Eighth Meeting of the Division of Particles and Fields Albuquerque, New Mexico, August 2-6, 1994.)""]",['1996-04-03']
2565,['eng'],"['Daniels, T']",['J/$\\psi\\psi$(2S) --> $\\mu^{+}\\mu^{-}$ and B --> J/$\\psi\\psi$(2S) cross sections'],['Particle Physics - Experimental Results'],"['talk, Glasgow 1994/07/20', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'psi(3685), hadroproduction', 'hadroproduction, psi(3685)', 'quark, beauty', 'quark, hadroproduction', 'hadroproduction, quark', 'central region', 'B, decay', 'decay, B', 'psi mesons, leptonic decay', 'leptonic decay, psi mesons', 'mass spectrum, dimuon', 'dimuon, mass spectrum', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'anti-p p --> psi mesons anything', 'B --> psi mesons anything', 'psi mesons --> muon+ muon-', '1800 GeV-cms,', 'J/psi(3100), hadroproduction', 'hadroproduction, J/psi(3100)']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412013'],"['This paper presents a measurement of J/psi,psi(2S) differential cross sections in p-pbar collisions at square root s = 1.8 TeV. The cross sections are measured above 4 GeV/c in the central region (|eta| < 0.6) using the dimuon decay channel. The fraction of events from B decays is measured, and used to calculate b quark cross sections and direct J/psi,psi(2S) cross sections. The direct cross sections are found to be more than an order of magnitude above theoretical expectations.']",['1995-01-06']
2566,['eng'],"['Forden, G E']",['Probing color coherency using high pT W events at the Tevatron'],['Particle Physics - Experimental Results'],"['talk', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'jet, hadroproduction', 'hadroproduction, jet', 'W, associated production', 'associated production, W', 'transverse momentum, high', 'color, coherence', 'rapidity spectrum, correlation', 'jet, energy flow', 'four-pi-detector, DZERO', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9408004'],"['\\D0 has used W --> e nu events associated with a high pT jet to probe for the effects of extended source color dipole radiation in W-jet rapidity correlations. We have also studied the low energy flow in these events and shown an enhancement between the jet and the beam directions, indicating the effects of color coherency.']",['1996-05-02']
2567,['eng'],"['Enomoto, R']",['New tagging method of B flavor of neutral B meson in CP violation measurement in asymmetric b-factory experiment'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'annihilation, electron positron', 'energy, asymmetry', 'B0, electroproduction', 'electroproduction, B0', 'B0, decay modes', 'decay modes, B0', 'violation, CP', 'particle identification, (B0 anti-B0)', 'efficiency', 'data analysis method', 'neural network']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412005'],"['In CP violation measurements in asymmetric B-factory experiments, a determination of the B flavor of the neutral B mesons is necessary. A new method to this purpose using only three vectors of charged particles has been developed. This method (weighted charge method) does not require either lepton identification or charged-kaon identification. The tagging efficiency, probability for incorrect tagging, and effective tagging efficiency of this method are 43.1, 18.3, and 17.3\\%, respectively.']",['1994-12-08']
2568,['eng'],"['Urheim, J']",['New results from CLEO-II on hadronic decays of the $\\tau$ lepton'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'tau, electroproduction', 'electroproduction, tau', 'tau, pair production', 'pair production, tau', 'tau, semileptonic decay', 'semileptonic decay, tau', 'tau, decay modes', 'decay modes, tau', 'tau, branching ratio', 'mass spectrum', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'tau- --> pi- pi0 neutrino/tau', 'tau- --> K- pi0 neutrino/tau', 'tau- --> 3charged particle neutrino/tau', 'tau- --> 3charged particle pi0 neutrino/tau', 'approx. 10.6 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9408003'],"['Results on semi-hadronic decays of the \\tau lepton are presented, from studies of e^+e^- annihilation data obtained at the Cornell Electron Storage Ring with the CLEO-II detector. Branching fractions have been measured for decays to two, three and four hadrons, namely \\tau ^-\\!\\!\\rightarrow\\! \\nu_\\tau h^-\\pi^0, \\tau^-\\!\\!\\rightarrow\\! \\nu_\\tau h^-h^+h^-, and \\tau^-\\!\\!\\rightarrow\\! \\nu_\\tau h^-h^+h^-\\pi^0, where h^\\pm represents a charged pion or kaon. CLEO-II has also observed decays with charged and/or neutral kaons; preliminary results for branching ratios and structure arising from the decay dynamics are given. Connections are made with predictions derived from theoretical models, the Conserved Vector Current theorem, isospin constraints and sum rules.']",['1996-04-03']
2569,['eng'],"['Gollin, G D', 'Hogan, W P']",['New measurements of CP violation parameters as tests of CPT in K meson decay'],['Particle Physics - Experimental Results'],"['talk', 'K0(L), decay modes', 'decay modes, K0(L)', 'K0(S), decay modes', 'decay modes, K0(S)', 'violation, CP', 'K0, nonleptonic decay', 'nonleptonic decay, K0', 'K0, radiative decay', 'radiative decay, K0']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9408002'],"['Using a technique which employs a pair of solid scintillator regenerators, the E773 collaboration has measured several CP violation parameters in K meson decay at Fermilab. We report new results for the phase of eta_+-, the K_L-K_S mass difference, the K_S lifetime, and the phase difference Arg(eta_00)-Arg(eta_+-) in K ->pi pi decay. In addition, we report a measurement of the magnitude and phase of eta_+-gamma in K ->pi+ pi- gamma decay. Our preliminary results are compared with theoretical expectations based on CPT symmetry. (Glasgow ICHEP94 paper Ref. gls0167, set with REVTeX)']",['1994-08-10']
2570,['eng'],"['Eggers, H C', 'Lipa, P']",['Unbiased estimators for correlation measurements'],['Particle Physics - Experimental Results'],"['multiple production', 'correlation function', 'statistical analysis', 'correction, higher-order', 'numerical calculations']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9407003'],"['Higher order correlation measurements involve multiple event averages which must run over unequal events to avoid statistical bias. We derive correction formulas for small event samples, where the bias is largest, and utilize the results to achieve savings in CPU time consumption for the star integral. Results from a simple model of correlations illustrate the utility and importance of these corrections. Single-event correlation measurements such as in galaxy distributions and envisaged at RHIC must take great care to avoid this unnecessary pitfall.']",['1994-08-02']
2571,['eng'],[],['Measurement of the B -> D^* l nu Branching Fractions and |Vcb|'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Upsilon(10570), electroproduction', 'electroproduction, Upsilon(10570)', 'B, pair production', 'pair production, B', 'B, semileptonic decay', 'semileptonic decay, B', 'B-, branching ratio', 'anti-B0, branching ratio', 'D*(2010)', 'isospin, invariance', 'invariance, isospin', 'lifetime, ratio', 'Kobayashi-Maskawa angle', 'magnetic detector, CLEO', 'experimental results', 'Cornell CESR Stor', 'bibliography', 'B --> D*(2010) lepton antineutrino', '10.57 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9406005'],"['We study the exclusive semileptonic B meson decays B- -> D*0 l- nu and B0 -> D*+ l- nu using data collected with the CLEO II detector at CESR. We present measurements of the branching fractions B(B0 -> D*+ l-nu) = 0.5/f00* [4.49+/-0.32+/-0.39]% and B(B- -> D*0 l-nu) = 0.5/f+-*[5.13+/-0.54+/-0.64]%, where f00 and f+- are the neutral and charged B meson production fractions at the Upsilon(4s) resonance. Assuming isospion invariance and taking the charged to neutral B meson lifetimes measured at higher energy machines, we determine the ratio f+-/f00=1.04+/-0.14+/-0.13+-/-0.10; further assuming f+- + f00 = 1 we also determine the partial width G(B->D* l nu) = 29.9+/-1.9+/-2.7+/-2.0 ns-1 (independent of f+-/f00). From this partial width we calculate B -> D* l nu branching fractions that do not depend on f+-/f00, nor the individual B lifetimes, but only on the charged to neutral lifetime ratio. The product of the CKM matrix element |Vcb| times the normalization of the decay form factor at the point of zero recoil of the D* meson, F(y=1), is determined from a linear fit to the combined differential decay rate of the exclusive B->D* l nu decays: |Vcb|F(y) = 0.0351 +/- 0.0019 +/- 0.0018 +/- 0.0008. Using theoretical calculations of the form factor normalization we extract a value for |Vcb|. LATEX (REVTEX style) file with uuencoded figures attached (uses PSBOX). Available on WWW http://w4.lns.cornell.edu/public/CLNS/']",['1994-06-27']
2572,['eng'],"['Kantowski, R', 'Marzban, C']",['A neural network for locating the primary vertex in a pixel detector'],['Nonlinear Systems'],"['p p, colliding beam detector', 'colliding beam detector, p p', 'jet, hadroproduction', 'hadroproduction, jet', 'track data analysis, vertex', 'spatial resolution, vertex', 'neural network', 'numerical calculations, Monte Carlo', 'magnetic detector, SDC', 'SSC Coll']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9406003'],"['Using simulated collider data for p+p\\rightarrow 2{\\rm Jets}\\ interactions in a 2-barrel pixel detector, a neural network is trained to construct the coordinate of the primary vertex to a high degree of accuracy. Three other estimates of this coordinate are also considered and compared to that of the neural network. It is shown that the network can match the best of the traditional estimates.']",['1994-06-22']
2573,['eng'],"['Derwent, P F']",['Measurement of correlated b quark cross sections at CDF'],['Particle Physics - Experimental Results'],"['talk, Glasgow 1994/07/21', 'anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'quark, semileptonic decay', 'semileptonic decay, quark', 'particle identification, beauty', 'channel cross section, momentum dependence', 'angular correlation, (jet muon)', 'jet, transverse energy', 'quantum chromodynamics, perturbation theory', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', '1800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9410007'],"['Using data collected during the 1992-1993 collider run at Fermilab, CDF has made measurements of correlated b quark cross sections where one b is detected from the lepton from semileptonic decay and the second b is detected with secondary vertex techniques. We report on measurements of the cross section as a function of the momentum of the second b and as a function of the azimuthal separation of the two b quarks, for transverse momentum of the initial b quark greater than 15 GeV. The vertex reconstruction techniques are valid over a large range in transverse momentum, starting at a minimum of 10 GeV. Results are compared to QCD predictions.']",['1994-10-17']
2574,['eng'],"['Pietrzyk, B']",['LEP asymmetries and fits of the Standard Model'],['Particle Physics - Experimental Results'],"['talk', 'electron positron, annihilation', 'annihilation, electron positron', 'lepton, electroproduction', 'electroproduction, lepton', 'quark, electroproduction', 'electroproduction, quark', 'angular distribution, asymmetry', 'asymmetry, angular distribution', 'electroweak interaction, validity test', 'validity test, electroweak interaction', 'tau, electroproduction', 'electroproduction, tau', 'tau, polarization', 'polarization, tau', 'quark, charm', 'quark, beauty', 'quark, truth', 'mass, truth', 'truth, mass', 'numerical calculations, interpretation of experiments', 'CERN LEP Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9406001'],"['The lepton and quark asymmetries measured at LEP are presented. The results of the Standard Model fits to the electoweak data presented at this conference are given. The top mass obtained from the fit to the LEP data is 172^{+13+18}_{-14-20} GeV; it is 177^{+11+18}_{-11-19} when also the collider, \\nu and A_{LR} data are included.']",['1994-06-06']
2575,['eng'],"['Abplanalp, M', 'Berger, C', 'Czapek, G', 'Diggelmann, U', 'Furlan, M', 'Gabutti, A', 'Janos, S', 'Moser, U', 'Pozzi, R', 'Pretzl, Klaus P', 'Schmiemann, K', 'Perret-Gallix, D', 'Van den Brandt, B', 'Konter, J A', 'Mango, S']",['Phase transition time delays in irradiated superheated superconducting granules'],['Particle Physics - Experimental Results'],"['talk', 'cosmic radiation', 'counters and detectors, superconducting', 'superconducting, counters and detectors', 'superconducting, droplet', 'droplet, superconducting', 'n nucleus, elastic scattering', 'elastic scattering, n nucleus', 'nucleus, recoil', 'p, beam', 'beam, p', 'zinc', 'tin']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405009'],"['The time difference between a particle interaction in a Superheated Superconducting Granule (SSG) and the resulting phase transition signal has been explored. Detectors containing Zn and Sn SSG were irradiated with neutrons and protons to study the heating mechanism taking place in nuclear recoil and ionizing events. Scattered neutrons have been detected by a scintillator hodoscope behind the SSG with a recoil energy measurement resolution of 10\\% and an interaction time resolution of 1ns. The fast transition of the metastable granules allowed to determine the elapsed time between an energy deposition and the phase transition signal. In the case of Sn granules, the results show that the time distributions are narrow and independent of the deposited energy in nuclear recoil and ionizing events. In Zn, however, the time distributions are much broader and depend on the energy deposition in the granule.']",['1994-05-25']
2576,['eng'],"['Wislicki, W']",['Polarization of valence and sea quarks in the proton'],['Particle Physics - Experimental Results'],"['talk', 'muon+ nucleon, deep inelastic scattering', 'deep inelastic scattering, muon+ nucleon', 'deuterium, polarized target', 'polarized target, deuterium', 'hydrogen, polarized target', 'polarized target, hydrogen', 'nucleon, structure function', 'dependence, mass number', 'mass number, dependence', 'muon+, polarized beam', 'polarized beam, muon+', 'quark, valence', 'quark, sea', 'quark, spin', 'spin, quark', 'cross section, asymmetry', 'spin, dependence', 'dependence, spin', 'quark, polarization', 'polarization, quark', 'spectrometer, experimental results', 'CERN Lab', '100, 190 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405012'],"['Analysis was performed of semi-inclusive and inclusive spin asymmetries determined from the polarized deep inelastic scattering by the Spin Muon Collaboration. Combined analysis of data for polarized deuterium and hydrogen targets allows for separate determination of spin carried by valence {\\it u} and {\\it d} quarks and non-strange sea quarks as a function of x_{Bj} in the range 0.006<x_{Bj}<0.6. It was found that polarization of valence {\\it u} quarks is positive and of valence {\\it d} quarks is negative, whereas the sea polarization is small and consistent with zero within errors.']",['1994-05-31']
2577,['eng'],"['Gabutti, A']",['Quasiparticle and phonon propagation in superheated superconducting granules after nuclear recoils'],['Particle Physics - Experimental Results'],"['talk', 'counters and detectors, superconducting', 'superconducting, counters and detectors', 'superconducting, droplet', 'droplet, superconducting', 'n nucleus, elastic scattering', 'elastic scattering, n nucleus', 'nucleus, recoil', 'zinc', 'tin', 'thermodynamics, diffusion', 'time']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405010'],['The propagation of the excess of quasiparticles and phonons produced by a nuclear recoil inside Sn and Zn superheated superconducting granules will be discussed. The decay towards equilibrium of the initial disturbance is assumed to be a thermal diffusion process described by a set of coupled heat flow equations for the effective quasiparticle and phonon temperatures. The solution is carried out analytically for a point source located anywhere inside the superconducting granule with the initial energy distributed in both quasiparticle and phonon systems. The calculated time delay between the neutron interaction and the nucleation of the phase transition will be compared to the time delay distributions obtained by irradiating Zn and Sn SSG detectors with a 70Me\\!V neutron beam.'],['1994-05-25']
2578,['eng'],"['Dremin, I M', 'Arena, V', 'Boca, G', 'Giannini, G', 'Malvezzi, S', 'Merlo, M', 'Ratti, S P', 'Riccardi, C', 'Salvadori, G', 'Viola, L', 'Vitulo, P']",['Cumulant to factorial moment ratio and multiplicity data'],['Particle Physics - Experimental Results'],"['p p, inclusive reaction', 'anti-p p, inclusive reaction', 'electron positron, annihilation', 'annihilation, electron positron', 'multiple production', 'multiplicity, spectra', 'spectra, multiplicity', 'moment', 'quantum chromodynamics, perturbation theory', 'numerical calculations, interpretation of experiments']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405007'],['The ratio of cumulant to factorial moments of experimental multiplicity distributions has been calculated for e^{+}e^{-} and hh interactions in a wide range of energies. As a function of the rank it exhibits an initial steep decrease and a series of oscillations around zero. Those features cannot be reproduced by the Negative Binomial Distribution. A comparable behaviour is instead predicted in high-energy perturbative QCD. The presence of a qualitatively similar behaviour for different processes and in wide energy intervals suggests speaking of an approximate scaling of the cumulant to factorial moment ratio.'],['1994-05-19']
2579,['eng'],"['Abe, F']",['Evidence for top quark production in $\\overline{p}$p collisions at \\Sqrt s. = 1.8 TeV'],['Particle Physics - Experimental Results'],"['anti-p p, colliding beams', 'colliding beams, anti-p p', 'anti-p p, inclusive reaction', 'quark, truth', 'quark, hadroproduction', 'hadroproduction, quark', 'quark, pair production', 'pair production, quark', 'quark, decay', 'decay, quark', 'W, leptonic decay', 'leptonic decay, W', 'W, nonleptonic decay', 'nonleptonic decay, W', 'particle identification, beauty', 'jet, multiplicity', 'mass, truth', 'truth, mass', 'channel cross section', 'magnetic detector, CDF', 'experimental results', 'Batavia TEVATRON Coll', 'anti-p p --> 2truth anything', 'truth --> W beauty', 'W --> lepton neutrino', 'W --> quark antiquark', '1800 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405005'],"['We summarize a search for the top quark with the Collider Detector at Fermilab (CDF) in a sample of \\bar{p}p collisions at \\sqrt{s}= 1.8 TeV with an integrated luminosity of 19.3~pb^{-1}. We find 12 events consistent with either two W bosons, or a W boson and at least one b jet. The probability that the measured yield is consistent with the background is 0.26\\%. Though the statistics are too limited to establish firmly the existence of the top quark, a natural interpretation of the excess is that it is due to t\\bar{t} production. Under this assumption, constrained fits to individual events yield a top quark mass of 174 \\pm 10^{+13}_{-12} GeV/c^2. The t\\bar{t} production cross section is measured to be 13.9^{+6.1}_{-4.8}~pb. (Submitted to Physical Review Letters on May 16 1994).']",['1996-05-02']
2580,['eng'],"['Barrette, J']",['Observation of anisotropic event shapes and transverse flow in Au+Au collisions at AGS energy'],['Particle Physics - Experimental Results'],"['nucleus nucleus, nuclear reaction', 'gold', 'scattering, heavy ion', 'heavy ion, scattering', 'event shape analysis, anisotropy', 'transverse energy, angular distribution', 'angular distribution, transverse energy', 'rapidity dependence', 'calorimeter, experimental results', 'Brookhaven PS', '11.4 GeV/c/nucleon']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405003'],['Event shapes for Au + Au collisions at 11.4 GeV/c per nucleon were studied over nearly the full solid angle with the E877 apparatus. The analysis was performed by Fourier expansion of azimuthal distributions of the transverse energy (E_T) measured in different pseudorapidity intervals. For semicentral collisions a pronounced event anisotropy is identified beyond that expected due to fluctuations in particle multiplicity. The signal decreases for peripheral and very central collisions. The amplitude of the flow signal reaches up to 7% of the mean E_T.'],['1996-05-02']
2581,['eng'],"['Brümmer, N']",['Experimental momentum spectra of identified hadrons in jets and the predictions from LPHD + MLLA'],"['Particle Physics - Phenomenology', 'Particle Physics - Experimental Results']","['electron positron, annihilation', 'annihilation, electron positron', 'hadron, multiple production', 'multiple production, hadron', 'jet, hadronization', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, nonleptonic decay', 'nonleptonic decay, Z0', 'leading logarithm approximation, correction', 'duality, hadron parton', 'showers, parton', 'quantum chromodynamics, perturbation theory', 'momentum spectrum, (hadron)', 'parametrization', 'energy dependence', 'mass, dependence', 'dependence, mass', 'strong interaction, coupling constant', 'coupling constant, strong interaction', 'numerical calculations, interpretation of experiments', 'electron positron, annihilation', 'annihilation, electron positron', 'hadron, multiple production', 'multiple production, hadron', 'jet, hadronization', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, nonleptonic decay', 'nonleptonic decay, Z0', 'leading logarithm approximation, correction', 'duality, hadron parton', 'showers, parton', 'quantum chromodynamics, perturbation theory', 'momentum spectrum, (hadron)', 'parametrization', 'energy dependence', 'mass, dependence', 'dependence, mass', 'strong interaction, coupling constant', 'coupling constant, strong interaction', 'numerical calculations, interpretation of experiments']","['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=scan&id=P00023409', 'http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405001']","['Experimental data on the shape of hadronic momentum spectra are compared with theoretical predictions in the context of calculations in the Modified Leading Log Approximation (MLLA), under the assumption of Local Parton Hadron Duality (LPHD). Considered are experimental measurements at e^+e^--colliders of \\xi_p^*, the position of the maximum in the distribution of \\xi_p=\\log(1/x_p), where x_p=p/p_{beam}. The parameter \\xi_p^* is determined for various hadrons at various centre of mass energies. It is interesting to look at the dependence of \\xi^*_p on the hadron type. This is used to study the influence of the hadron type on the cut-off scale Q_0 in the parton shower development. The dependence of \\xi^*_p on the centre of mass energy is seen to be described adequately by perturbation theory. The approach is made quantitative by extracting a value of \\alpha_s(m_Z) from an overall fit to the scaling behaviour of \\xi^*_p.']",['1996-04-03']
2582,['eng'],"['Swartz, M']",['Precise measurement of the left-right cross section asymmetry in Z boson production by e+e- collisions'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'electron positron, annihilation', 'Z0, electroproduction', 'electron, polarized beam', 'polarization, longitudinal', 'Z0, nonleptonic decay', 'Z0, leptonic decay', 'tau, pair production', 'polarization, asymmetry', 'Weinberg angle', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', '91.28 GeV-cms']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9404001'],"['We present a precise measurement of the left-right cross section asymmetry (A_{LR}) for Z boson production by \\ee collisions. The measurement was performed at a center-of-mass energy of 91.26~GeV with the SLD detector at the SLAC Linear Collider (SLC). The luminosity-weighted average polarization of the SLC electron beam was (63.0\\pm1.1)\\%. Using a sample of 49,392 \\z0 decays, we measure A_{LR} to be 0.1628\\pm0.0071(stat.)\\pm0.0028(syst.) which determines the effective weak mixing angle to be \\swein=0.2292\\pm0.0009({\\rm stat.})\\pm0.0004({\\rm syst.}).}']",['1996-05-02']
2583,['eng'],"['Abe, K']",['Measurement of alpha-s from energy-energy correlations at the Z0 resonance'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, nonleptonic decay', 'nonleptonic decay, Z0', 'angular correlation, two-particle', 'energy, correlation', 'asymmetry', 'coupling constant, strong interaction', 'strong interaction, coupling constant', 'quantum chromodynamics, perturbation theory', 'renormalization', 'plastics, stability', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV-cms']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405006'],"['We have determined the strong coupling alpha-s from a comprehensive study of energy-energy correlations (EEC) and their asymmetry (AEEC) in hadronic decays of Z0 bosons collected by the SLD experiment at SLAC. The data were compared with all four available predictions of QCD calculated up to O(alpha-s**2) in perturbation theory, and also with a resummed calculation matched to all four of these calculations. We find large discrepancies between alpha-s values extracted from the different O(alpha-s**2) calculations. We also find a large renormalization scale ambiguity in alpha-s determined from the EEC using the O(alpha-s**2) calculations; this ambiguity is reduced in the case of the AEEC, and is very small when the matched calculations are used. Averaging over all calculations, and over the EEC and AEEC results, we obtain alpha-s(MZ)=0.124+0.003-0.004(exp.) +-0.009(theory).']",['2003-12-11']
2584,['eng'],"['Bracker, S B', 'Gounder, K', 'Hendrix, K', 'Summers, D J']",['A simple multiprocessor management system for event-parallel computing'],['Particle Physics - Experimental Results'],"['microprocessor, multiprocessor', 'microprocessor, vector', 'programming, off-line', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9511009'],"['Offline software using TCP/IP sockets to distribute particle physics events to multiple UNIX/RISC workstations is described. A modular, building block approach was taken, which allowed tailoring to solve specific tasks efficiently and simply as they arose. The modest, initial cost was having to learn about sockets for interprocess communication. This multiprocessor management software has been used to control the reconstruction of eight billion raw data events from Fermilab Experiment E791.']",['1995-11-24']
2585,['eng'],"['Brümmer, N']",['An optimal method of moments to measure the charge asymmetry at the Z$^{0}$'],['Particle Physics - Experimental Results'],"['electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'Z0, decay', 'decay, Z0', 'angular distribution, asymmetry', 'asymmetry, angular distribution', 'charge, asymmetry', 'violation, CP', 'moment', 'statistical analysis', 'acceptance', 'efficiency', 'numerical calculations, Monte Carlo']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405002'],"['Parity violation at LEP or SLC can be measured through the charge asymmetry. An optimal method of moments is developed here to measure this asymmetry, as well as similar asymmetries. This method is equivalent to the likelihood fit. It is simpler in use, as it gives analytical formulas for both the asymmetry and its statistical error. These formulas give the dependence of the accuracy on the experimental angular acceptance explicitly.']",['1996-04-03']
2586,['eng'],"['Dremin, I M', 'Nechitailo, V A']",['Average multiplicities in gluon and quark jets in higher-order perturbative QCD'],['Particle Physics - Experimental Results'],"['gluon, jet', 'quark, jet', 'multiplicity, energy dependence', 'quantum chromodynamics', 'perturbation theory, higher-order', 'dimension, anomaly', 'numerical calculations']","['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9406002', 'http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=scan&id=P00021938']",['The ratio of average multiplicities in gluon and quark jets is shown to become noticeably smaller in higher-order QCD compared to its lowest order value what improves agreement with experiment. QCD anomalous dimension has been calculated. It has been used to get energy dependence of mean multiplicities.'],['1994-06-07']
2587,['eng'],"['Enomoto, R']",['Measurement of the D$*^{\\pm}$ cross section using a soft-pion analysis in two-photon processes'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'exchange, two-photon', 'two-photon, exchange', 'photon photon, interaction', 'interaction, photon photon', 'D*(2010), photoproduction', 'photoproduction, D*(2010)', 'D*(2010), hadronic decay', 'hadronic decay, D*(2010)', 'pi, transverse momentum', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'mass, charm', 'charm, mass', 'squark, truth', 'mass, squark', 'squark, mass', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', 'electron positron --> D*(2010) positron electron anything', 'D*(2010) --> D0 pi', 'approx. 58.1 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412001'],"['The differential cross section of d\\sigma(e^+e^-\\rightarrow e^+e^-D^{*\\pm}X)/dP_T was measured using a soft-pion analysis of D^{*\\pm}\\rightarrow \\pi_s^\\pm D^0(\\overline{D^0}) at TRISTAN. The average \\sqrt{s} was 58.1 GeV and the integrated luminosity used in this analysis was 198 pb^{-1}, respectively.']",['1994-12-05']
2588,['eng'],[],['A precise measurement of the weak mixing angle in neutrino-nucleon scattering'],['Particle Physics - Experimental Results'],"['neutrino nucleon, deep inelastic scattering', 'deep inelastic scattering, neutrino nucleon', 'neutrino nucleon, inclusive reaction', 'neutral current', 'charged current', 'channel cross section, ratio', 'Weinberg angle', 'mass, truth', 'truth, mass', 'Higgs particle, mass', 'mass, Higgs particle', 'calorimeter, experimental results', 'Batavia TEVATRON PS', '< 660']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405008'],"['We report a precise measurement of the weak mixing angle from the ratio of neutral current to charged current inclusive cross-sections in deep-inelastic neutrino-nucleon scattering. The data were gathered at the CCFR neutrino detector in the Fermilab quadrupole-triplet neutrino beam, with neutrino energies up to 600 GeV. Using the on-shell definition, {\\rm sin ^2\\theta_W} \\equiv 1 - \\frac{{\\rm M_W} ^2}{{\\rm M_Z} ^2}, we obtain {\\rm sin ^2\\theta_W} = 0.2218 \\pm 0.0025 ({\\rm stat.}) \\pm 0.0036 ({\\rm exp.\\: syst.}) \\pm 0.0040 ({\\rm model}).']",['1994-05-19']
2589,['eng'],"['Abe, K']",['Measurement of the charged multiplicity of Z --> b$\\overline{b}$ events'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, annihilation', 'annihilation, electron positron', 'Z0, electroproduction', 'electroproduction, Z0', 'quark, beauty', 'quark, pair production', 'pair production, quark', 'hadron, multiple production', 'multiple production, hadron', 'charged particle, multiplicity', 'quantum chromodynamics, perturbation theory', 'asymptotic freedom', 'magnetic detector, SLD', 'experimental results', 'SLAC SLC Linac', 'approx. 91 GeV']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9405004'],"['Using an impact parameter tag to select an enriched sample of Z \\rightarrow b \\overline{b} events, we have measured the difference between the average charged multiplicity of Z \\rightarrow b \\overline{b} and Z^0 \\rightarrow hadrons to be \\overline{n}_{b} - \\overline{n}_{had} = 2.24\\pm 0.30(\\rm{stat.}) \\pm 0.33(\\rm{syst.}) tracks per event. {}From this, we have derived \\overline{n}_{b} - \\overline{n}_{uds} = 3.31 \\pm 0.41 \\pm 0.79. Comparing this measurement with those at lower center-of-mass energies, we find no evidence that \\overline{n}_{b} - \\overline{n}_{uds} depends on energy. This result is in agreement with a precise prediction of perturbative QCD, and supports the notion that QCD remains asymptotically free down to the scale M_b^2.']",['1996-05-07']
2590,['eng'],"['Enomoto, R']",['A measurement of the D$^{*\\pm}$ cross section in two-photon processes'],['Particle Physics - Experimental Results'],"['electron positron, colliding beams', 'colliding beams, electron positron', 'electron positron, inelastic scattering', 'inelastic scattering, electron positron', 'exchange, two-photon', 'two-photon, exchange', 'photon photon, interaction', 'interaction, photon photon', 'D*(2010), photoproduction', 'photoproduction, D*(2010)', 'D*(2010), decay modes', 'decay modes, D*(2010)', 'mass difference, spectra', 'spectra, mass difference', 'differential cross section, transverse momentum', 'transverse momentum, differential cross section', 'magnetic detector, TOPAZ', 'experimental results', 'KEK TRISTAN Stor', 'electron positron --> D*(2010) positron electron anything', 'D*(2010) --> D0 pi', 'D0 --> K pi anything', '57.16 GeV-cms,']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9411002'],"['We have measured the inclusive D^{*\\pm} production cross section in a two-photon collision at the TRISTAN e^+e^- collider. The mean \\sqrt{s} of the collider was 57.16 GeV and the integrated luminosity was 150 pb^{-1}. The differential cross section (d\\sigma(D^{*\\pm})/dP_T) was obtained in the P_T range between 1.6 and 6.6 GeV and compared with theoretical predictions, such as those involving direct and resolved photon processes.']",['1994-11-30']
2591,['eng'],"['Enomoto, R', 'Sumiyoshi, T', 'Fujita, Y']",['Test of various photocathodes'],['Detectors and Experimental Techniques'],"['talk, Bari 1993/06/02', 'photoelectron, surface', 'cesium, iodine', 'cesium, tellurium', 'efficiency']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412007'],"['A test of various photocathodes was carried out. The tested materials were CsI, CsTe, their multi-layers and so on. The quantum efficiencies of the various materials were measured under a vacuum and/or after exposure to several kinds of gases.']",['1994-12-13']
2592,['eng'],"['Enomoto, R']",['Feasibility study of single-photon counting using a fine-mesh phototube for an aerogel readout'],['Detectors and Experimental Techniques'],"['Cherenkov counter, aerogel', 'Cherenkov counter, readout', 'photoelectron, surface', 'photoelectron, amplifier', 'efficiency', 'magnetic field']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=9412010'],"['The fine-mesh phototube is one type of photodetector which can be used under a strong magnetic field. For an aerogel readout, the single-photon detection efficiency should be close to 100\\% in order to identify particle species. We carried out a feasibility study of single-photon counting using fine-mesh phototubes, and obtained a possible solution.']",['1994-12-14']
2593,['eng'],"['Grindhammer, G', 'Peters, S']",['The Parameterized Simulation of Electromagnetic Showers in Homogeneous and Sampling Calorimeters'],['Detectors and Experimental Techniques'],"['talk, Tallahassee 1993/02/22', 'calorimeter, showers', 'showers, electromagnetic', 'parametrization', 'showers, spatial distribution', 'calorimeter, liquid argon', 'magnetic detector, H1', 'DESY HERA Stor']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001020'],['A general approach to a fast simulation of electromagnetic showers using parameterizations of the longitudinal and radial profiles in homogeneous and sampling calorimeters is described. The dependence of the shower development on the materials used and the sampling geometry is taken into account explicitly. Comparisons with detailed simulations of various calorimeters and with data from the liquid argon calorimeter of the H1 experiment are made.'],['2000-01-11']
2594,['eng'],"['Cremaldi, L M', 'Aitala, E M', ""D'Almeida, F"", 'Amato, S', 'Anjos, J C', 'Appel, J A', 'Ashery, D', 'Astorga, J', 'Todorova-Nová, S', 'Beck, S', 'Bediaga, I', 'Blaylock, G', 'Bracker, S B', 'Burchat, P R', 'Burnstein, R A', 'Carter, T', 'Costa, I', 'Denisenko, K', 'Darling, C L', 'Gagnon, P', 'Gerzon, S', 'Gounder, K', 'Granite, D', 'Halling, M', 'James, C', 'Kasper, P A', 'Kwan, S', 'Lichtenstadt, J', 'Lundberg, B', 'De Mello-Neto, J R T', 'Milburn, R H', 'De Miranda, J M', 'Napier, A', 'Nguyen, A', 'De Oliveira, A B', 'Peng, K C', 'Purohit, M V', 'Quinn, B', 'Radeztsky, S', 'Rafatian, A', 'Ramalho, A J', 'Reay, N W', 'Reibel, K', 'Reidy, J J', 'Rubin, H A', 'Santha, A K S', 'Santoro, A F S', 'Schwartz, A', 'Sheaff, M', 'Sidwell, R A', 'Da Silva-Carvalho, H', 'Slaughter, J', 'Sokoloff, M D', 'Souza, M', 'Stanton, N', 'Sugano, K', 'Summers, D J', 'Takach, S', 'Thorne, K', 'Tripathi, A K', 'Trumer, D', 'Watanabe, S', 'Wiener, J', 'Witchey, N', 'Wolin, E', 'Yi, D']",['Fermilab E791'],['Particle Physics - Experimental Results'],"['talk, Dallas 1992/08/06', 'pi- nucleus, inclusive reaction', 'carbon, platinum', 'charmed meson, hadroproduction', 'hadroproduction, charmed meson', 'charmed meson, decay modes', 'decay modes, charmed meson', 'transverse energy, trigger', 'computer', 'D0 anti-D0, interference', 'semiconductor detector, microstrip', 'Cherenkov counter', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0010027'],"[""Fermilab E791, a very high statistics charm particle experiment, recently completed its data taking at Fermilab's Tagged Photon Laboratory. Over 20 billion events were recorded through a loose transverse energy trigger and written to 8mm tape in the the 1991-92 fixed target run at Fermilab. This unprecedented data sample containing charm is being analysed on many-thousand MIP RISC computing farms set up at sites in the collaboration. A glimpse of the data taking and analysis effort is presented. We also show some preliminary results for common charm decay modes. Our present analysis indicates a very rich yield of over 200K reconstructed charm decays.""]",['2000-10-13']
2595,['eng'],"['Amato, S', 'De Mello-Neto, J R T', 'De Miranda, J M', 'James, C', 'Summers, D J', 'Bracker, S B']",['The E791 Parallel Architecture Data Acquisition System'],['Detectors and Experimental Techniques'],"['talk', 'data acquisition', 'programming', 'magnetic spectrometer', 'charmed particle, hadroproduction', 'hadroproduction, charmed particle', 'Batavia TEVATRON PS']",['http://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0001003'],"['To collect data for the study of charm particle decays, we built a high speed data acquisition system for use with the E791 magnetic spectrometer at Fermilab. The DA system read out 24000 channels in 50 uS. Events were accepted at the rate of 9000 per second. Eight large FIFOs were used to buffer event segments, which were then compressed and formatted by 54 processors housed in 6 VME crates. Data was written continuously to 42 Exabyte tape drives at the rate of 9.6 Mb/s. During the 1991 fixed target run at Fermilab, 20 billion physics events were recorded on 24000 8 mm tapes; this 50 Tb (Terabyte) data set is now being analyzed.']",['2000-01-04']
2596,['eng'],"['Summers, D J']",['Charm Physics at Fermilab E791'],['Particle Physics - Experimental Results'],"['talk', 'pi- nucleus, inclusive reaction', 'beryllium', 'aluminum', 'copper', 'tungsten', 'D, hadroproduction', 'hadroproduction, D', 'D0, nonleptonic decay', 'nonleptonic decay, D0', 'D+, nonleptonic decay', 'nonleptonic decay, D+', 'mass spectrum, (K- pi+)', '(K- pi+), mass spectrum', 'mass spectrum, (K- 2pi+)', '(K- 2pi+), mass spectrum', 'data acquisition', 'semiconductor detector, vertex', 'magnetic spectrometer, experimental results', 'Batavia TEVATRON PS', 'D0 --> K- pi+', 'D+ --> K- 2pi+', '500 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0009015'],"[""Experiment 791 at Fermilab's Tagged Photon Laboratory has just accumulated a high statistics charm sample by recording 20 billion events on 24000 8mm tapes. A 500 GeV/c pi- beam was used with a fixed target and a magnetic spectrometer which now includes 23 silicon fixed target and a magnetic spectrometer which now includes 23 silicon microstrip planes for vertex reconstruction. A new data acquisition system read out 9000 events/sec during the part of the Tevatron cycle that delivered beam. Digitization and readout took 50 uS per event. Data was buffered in eight large FIFO memories to allow continuous event building and continuous tape writing to a wall of 42 Exabytes at 9.6 MB/sec. The 50 terabytes of data buffered to tape is now being filtered on RISC CPUs. Preliminary results show D0 --> K- pi+ and D+ --> K- pi+ pi+ decays. Rarer decays will be pursued.""]",['2000-09-07']
2597,['eng'],"['Stoughton, C', 'Summers, D J']",['Using Multiple RISC CPUs in Parallel to Study Charm Quarks'],['Particle Physics - Experimental Results'],"['hadron nucleus, inclusive reaction', 'charmed particle, hadroproduction', 'hadroproduction, charmed particle', 'magnetic spectrometer', 'data management', 'microprocessor, multiprocessor', 'communications', 'Fermilab']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0007002'],"['We have integrated a system of 16 RISC CPUs to help reconstruct and analyze a 1.3 Terabyte data set of 400 million high energy physics interactions. These new CPUs provided an affordable means of processing a very large data set. The data was generated using a hadron beam and a fixed target at Fermilab Experiment 769. Signals were recorded on tape from particles created in or decaying near the target and passing though a magnetic spectrometer. Because all the interactions were independent, each CPU could completely reconstruct any interaction without reference to other CPUs. Problems of this sort are ideal for multiple processors. In the offline reconstuction system, we used Exabyte 8mm video tape drives with an I/O capacity of 7 Terabytes per year and a storage capacity of 2.3 Gigabytes per tape. This reduced tape mounts to one or two per day rather than one or two per hour as would be the case with 9-track tapes. The ETHERNET network used to link the CPUs and has an I/O capacity of 15 Terabytes per year. The RISC CPUs came in the form of commercially supported workstations with little memory and no graphics to minimize cost. Each 25 MHz MIPS R3000 RISC CPU processed data 20 times faster than 16MHz Motorola 68020 CPUs that were also used. About 8000 hours of processing was needed to reconstruct the data set. A sample of thousands of fully reconstructed particles containing a charm quark has been produced.']",['2000-07-04']
2598,['eng'],"['Summers, D J']",['Charm Hadroproduction at Fermilab E791'],['Particle Physics - Experimental Results'],"['talk', 'pi nucleus, inclusive reaction', 'K nucleus, inclusive reaction', 'p nucleus, inclusive reaction', 'hadron, tagged beam', 'tagged beam, hadron', 'beryllium', 'aluminum', 'copper', 'tungsten', 'D0, hadroproduction', 'hadroproduction, D0', 'D+, hadroproduction', 'hadroproduction, D+', 'D0, nonleptonic decay', 'nonleptonic decay, D0', 'D+, nonleptonic decay', 'nonleptonic decay, D+', 'mass spectrum, (K- pi+)', '(K- pi+), mass spectrum', 'mass spectrum, (K- 2pi+)', '(K- 2pi+), mass spectrum', 'spectrometer, experimental results', 'Batavia PS', '250 GeV/c']",['http://documents.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ex&id=0011020'],"['E769 has just recorded on tape the interactions of 500 million pions, kaons, and protons. A Cerenkov counter and a TRD were used to tag beam particle types in both positive and negative 250 GeV/c hadron beams. Thin foil Be, Al, Cu, and W targets were used with a spectrometer including silicon microstrips to look for charm decay vertices. Preliminary results show D0 --> K- pi+ and D+ --> K- pi+ pi+ mass peaks. As the event reconstruction progresses on numerous parallel microprocessors, we intend to explore the pT, xF, A, and flavor dependence of the production of charmed mesons and baryons.']",['2000-11-07']