id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
706.3914 | Asymptotic behavior of the entropy of chains placed on stripes | By using the transfer matrix approach, we investigate the asymptotic behavior
of the entropy of flexible chains with $M$ monomers each placed on stripes. In
the limit of high density of monomers, we study the behavior of the entropy as
a function of the density of monomers and the width of the stripe, inspired by
rec... | cond-mat.stat-mech | by using the transfer matrix approach we investigate the asymptotic behavior of the entropy of flexible chains with m monomers each placed on stripes in the limit of high density of monomers we study the behavior of the entropy as a function of the density of monomers and the width of the stripe inspired by recent anal... | [['by', 'using', 'the', 'transfer', 'matrix', 'approach', 'we', 'investigate', 'the', 'asymptotic', 'behavior', 'of', 'the', 'entropy', 'of', 'flexible', 'chains', 'with', 'm', 'monomers', 'each', 'placed', 'on', 'stripes', 'in', 'the', 'limit', 'of', 'high', 'density', 'of', 'monomers', 'we', 'study', 'the', 'behavior... | [-0.10127685184467256, 0.11348564322928295, -0.05302146987934761, 0.03591222679653369, 0.06579735251622931, -0.09534879885476959, 0.06506845120833639, 0.32879178690285804, -0.20644291575231097, -0.25742189114338115, 0.09071850888379712, -0.30490869426541717, -0.14854013694532434, 0.14331495992305196, 0.0237969871103654... |
706.3915 | Do unbounded bubbles ultimately become fenced inside a black hole? | We examine the dynamical behavior of recently introduced bubbles in
asymptotically flat, five-dimensional spacetimes. Using numerical methods, we
find that even bubbles that initially start expanding eventually collapse to a
Schwarzschild-Tangherlini black hole.
| hep-th gr-qc | we examine the dynamical behavior of recently introduced bubbles in asymptotically flat fivedimensional spacetimes using numerical methods we find that even bubbles that initially start expanding eventually collapse to a schwarzschildtangherlini black hole | [['we', 'examine', 'the', 'dynamical', 'behavior', 'of', 'recently', 'introduced', 'bubbles', 'in', 'asymptotically', 'flat', 'fivedimensional', 'spacetimes', 'using', 'numerical', 'methods', 'we', 'find', 'that', 'even', 'bubbles', 'that', 'initially', 'start', 'expanding', 'eventually', 'collapse', 'to', 'a', 'schwar... | [-0.15231622766816255, 0.1459545227840091, -0.12891998630242818, 0.15412593071320743, -0.04305136175543973, -0.14440796509117002, 0.003546414671070648, 0.3338209217357816, -0.11533861246072885, -0.2018225804168844, 0.12146880391237298, -0.2971857838106878, -0.17022685379241453, 0.1289450411656589, -0.0396436769233057, ... |
706.3916 | Effects of solute concentrations on kinetic pathways in Ni-Al-Cr alloys | The kinetic pathways resulting from the formation of coherent L12-ordered
y'-precipitates in the g-matrix (f.c.c.) of Ni-7.5 Al-8.5 Cr at.% and Ni-5.2
Al-14.2 Cr at.% alloys, aged at 873 K, are investigated by atom-probe
tomography (APT) over a range of aging times from 1/6 to 1024 hours; these
alloys have approximat... | cond-mat.mtrl-sci | the kinetic pathways resulting from the formation of coherent l12ordered yprecipitates in the gmatrix fcc of ni75 al85 cr at and ni52 al142 cr at alloys aged at 873 k are investigated by atomprobe tomography apt over a range of aging times from 16 to 1024 hours these alloys have approximately the same volume fraction o... | [['the', 'kinetic', 'pathways', 'resulting', 'from', 'the', 'formation', 'of', 'coherent', 'l12ordered', 'yprecipitates', 'in', 'the', 'gmatrix', 'fcc', 'of', 'ni75', 'al85', 'cr', 'at', 'and', 'ni52', 'al142', 'cr', 'at', 'alloys', 'aged', 'at', '873', 'k', 'are', 'investigated', 'by', 'atomprobe', 'tomography', 'apt'... | [-0.06361513953461141, 0.17415287867695295, -0.08764034261781291, 0.03783378702252596, 0.0644905267181952, -0.06615699823552958, 0.06090908164877546, 0.36065064949699405, -0.23749612725092745, -0.32862234181490074, 0.045467592807499325, -0.28636022100263103, -0.07168270793242924, 0.14942063806740072, 0.0640290873806264... |
706.3917 | Holomorphic curves in Exploded Torus Fibrations: Compactness | The category of exploded torus fibrations is an extension of the category of
smooth manifolds in which some adiabatic limits look smooth. (For example, the
limits considered in tropical geometry appear smooth, also degenerations
corresponding to an algebraic family with normal crossing singularities are
smooth.) In t... | math.SG math.AP | the category of exploded torus fibrations is an extension of the category of smooth manifolds in which some adiabatic limits look smooth for example the limits considered in tropical geometry appear smooth also degenerations corresponding to an algebraic family with normal crossing singularities are smooth in this pape... | [['the', 'category', 'of', 'exploded', 'torus', 'fibrations', 'is', 'an', 'extension', 'of', 'the', 'category', 'of', 'smooth', 'manifolds', 'in', 'which', 'some', 'adiabatic', 'limits', 'look', 'smooth', 'for', 'example', 'the', 'limits', 'considered', 'in', 'tropical', 'geometry', 'appear', 'smooth', 'also', 'degener... | [-0.2080548422141786, -0.01840432922752765, -0.149535937750914, 0.17189409911453005, -0.112361077370728, -0.13118828695648946, -0.03228397782841495, 0.3374188084559268, -0.30534654384456483, -0.18918245955067406, 0.15392610724420702, -0.2009101042254682, -0.13122787832630328, 0.23292008374469825, -0.2656899350498949, -... |
706.3918 | A Linearization of Connes' Embedding Problem | We show that Connes' embedding problem for II_1-factors is equivalent to a
statement about distributions of sums of self-adjoint operators with matrix
coefficients. This is an application of a linearization result for finite von
Neumann algebras, which is proved using asymptotic second order freeness of
Gaussian rand... | math.OA | we show that connes embedding problem for ii_1factors is equivalent to a statement about distributions of sums of selfadjoint operators with matrix coefficients this is an application of a linearization result for finite von neumann algebras which is proved using asymptotic second order freeness of gaussian random matr... | [['we', 'show', 'that', 'connes', 'embedding', 'problem', 'for', 'ii_1factors', 'is', 'equivalent', 'to', 'a', 'statement', 'about', 'distributions', 'of', 'sums', 'of', 'selfadjoint', 'operators', 'with', 'matrix', 'coefficients', 'this', 'is', 'an', 'application', 'of', 'a', 'linearization', 'result', 'for', 'finite'... | [-0.10370727131764094, 0.06969025685763579, -0.12010540249563444, 0.06552471432466216, -0.09193298991400904, -0.1500372471443067, -0.04285453929333016, 0.3356267516646767, -0.3264841490114729, -0.13883458654163405, 0.1489070401682208, -0.3001713800864915, -0.14362083616045615, 0.15801747787433365, -0.17618874087929726,... |
706.3919 | Neutron electric polarizability from unquenched lattice QCD using the
background field approach | A calculational scheme for obtaining the electric polarizability of the
neutron in lattice QCD with dynamical quarks is developed, using the background
field approach. The scheme differs substantially from methods previously used
in the quenched approximation, the physical reason being that the QCD ensemble
is no lon... | hep-lat | a calculational scheme for obtaining the electric polarizability of the neutron in lattice qcd with dynamical quarks is developed using the background field approach the scheme differs substantially from methods previously used in the quenched approximation the physical reason being that the qcd ensemble is no longer i... | [['a', 'calculational', 'scheme', 'for', 'obtaining', 'the', 'electric', 'polarizability', 'of', 'the', 'neutron', 'in', 'lattice', 'qcd', 'with', 'dynamical', 'quarks', 'is', 'developed', 'using', 'the', 'background', 'field', 'approach', 'the', 'scheme', 'differs', 'substantially', 'from', 'methods', 'previously', 'u... | [-0.11790163963265281, 0.22823386282687622, -0.10134434343087784, 0.09564106109269717, -0.0632933088464655, -0.07519724823539442, 0.07045092145810795, 0.36113748718251254, -0.14128270636416695, -0.2871927600576879, 0.01350999049386604, -0.2663106618379738, -0.06281018872408474, 0.16218548484562717, 0.029531005188510654... |
706.392 | Molecular dynamics simulations of the dipolar-induced formation of
magnetic nanochains and nanorings | Iron, cobalt and nickel nanoparticles, grown in the gas phase, are known to
arrange in chains and bracelet-like rings due to the long-range dipolar
interaction between the ferromagnetic (or super-paramagnetic) particles. We
investigate the dynamics and thermodynamics of such magnetic dipolar
nanoparticles for low den... | cond-mat.mtrl-sci cond-mat.stat-mech | iron cobalt and nickel nanoparticles grown in the gas phase are known to arrange in chains and braceletlike rings due to the longrange dipolar interaction between the ferromagnetic or superparamagnetic particles we investigate the dynamics and thermodynamics of such magnetic dipolar nanoparticles for low densities usin... | [['iron', 'cobalt', 'and', 'nickel', 'nanoparticles', 'grown', 'in', 'the', 'gas', 'phase', 'are', 'known', 'to', 'arrange', 'in', 'chains', 'and', 'braceletlike', 'rings', 'due', 'to', 'the', 'longrange', 'dipolar', 'interaction', 'between', 'the', 'ferromagnetic', 'or', 'superparamagnetic', 'particles', 'we', 'invest... | [-0.1610877745047522, 0.2483083178723852, -0.006537068697313467, 0.0918076366558671, 0.02307810368326803, -0.09992515180259944, 0.03510863130291303, 0.43762623141209284, -0.24834732389155154, -0.3501321281989416, 0.024243601098035774, -0.29463972700138885, -0.08778880590262512, 0.13833228988184904, 0.10015471071625749,... |
706.3921 | The neutrino self-energy in a magnetized medium | In this work we calculate the neutrino self-energy in presence of a
magnetized medium. The magnetized medium consists of electrons, positrons,
neutrinos and a uniform classical magnetic field. The calculation is done
assuming the background magnetic field is weak compared to the $W$-Boson mass
squared, as a consequen... | hep-ph | in this work we calculate the neutrino selfenergy in presence of a magnetized medium the magnetized medium consists of electrons positrons neutrinos and a uniform classical magnetic field the calculation is done assuming the background magnetic field is weak compared to the wboson mass squared as a consequence of which... | [['in', 'this', 'work', 'we', 'calculate', 'the', 'neutrino', 'selfenergy', 'in', 'presence', 'of', 'a', 'magnetized', 'medium', 'the', 'magnetized', 'medium', 'consists', 'of', 'electrons', 'positrons', 'neutrinos', 'and', 'a', 'uniform', 'classical', 'magnetic', 'field', 'the', 'calculation', 'is', 'done', 'assuming'... | [-0.1368461779339064, 0.2055720979310322, -0.02723816302354954, 0.13877826312872513, -0.04064142143341319, -0.05087517612557483, -0.011282743461080045, 0.32746802217908355, -0.1723558747079911, -0.2748646413823027, -0.01365286721957335, -0.28501080035625787, -0.0509489460554499, 0.14042987497820325, 0.03530131578570444... |
706.3922 | CDF Central Preshower and Crack Detector Upgrade | The CDF Central Preshower and Crack Detector Upgrade consist of scintillator
tiles with embedded wavelength-shifting fibers, clear-fiber optical cables, and
multi-anode photomultiplier readout. A description of the detector design, test
results from R&D studies, and construction phase are reported. The upgrade was
in... | physics.ins-det | the cdf central preshower and crack detector upgrade consist of scintillator tiles with embedded wavelengthshifting fibers clearfiber optical cables and multianode photomultiplier readout a description of the detector design test results from rd studies and construction phase are reported the upgrade was installed late... | [['the', 'cdf', 'central', 'preshower', 'and', 'crack', 'detector', 'upgrade', 'consist', 'of', 'scintillator', 'tiles', 'with', 'embedded', 'wavelengthshifting', 'fibers', 'clearfiber', 'optical', 'cables', 'and', 'multianode', 'photomultiplier', 'readout', 'a', 'description', 'of', 'the', 'detector', 'design', 'test'... | [-0.06965916433061163, 0.14109923159280283, -0.08328434679600777, -0.059341965186776535, -0.04305602628455469, -0.20040762861908384, -0.08871529527206087, 0.39286481510763144, -0.07930709820268958, -0.35405570413973747, 0.1657580476532916, -0.43128255211437744, -0.006282366586453987, 0.214775190536977, -0.0599251166973... |
706.3923 | Nonparametric estimation for dependent data with an application to panel
time series | In this paper we consider nonparametric estimation for dependent data, where
the observations do not necessarily come from a linear process. We study
density estimation and also discuss associated problems in nonparametric
regression using the 2-mixing dependence measure. We compare the results under
2-mixing with th... | math.ST stat.TH | in this paper we consider nonparametric estimation for dependent data where the observations do not necessarily come from a linear process we study density estimation and also discuss associated problems in nonparametric regression using the 2mixing dependence measure we compare the results under 2mixing with those der... | [['in', 'this', 'paper', 'we', 'consider', 'nonparametric', 'estimation', 'for', 'dependent', 'data', 'where', 'the', 'observations', 'do', 'not', 'necessarily', 'come', 'from', 'a', 'linear', 'process', 'we', 'study', 'density', 'estimation', 'and', 'also', 'discuss', 'associated', 'problems', 'in', 'nonparametric', '... | [-0.04920933892990046, 0.043920358951002894, -0.1115774145442332, 0.04683822811121829, -0.0714693682727318, -0.11551455463157266, 0.056076514622170136, 0.38458713075370654, -0.2867355653223522, -0.2792837826389793, 0.14631549351442447, -0.2401347446028541, -0.14539832274775444, 0.19608517193337838, -0.11142327975323225... |
706.3924 | Total quadruple photoionization cross section of Beryllium in a
quasiclassical framework | In a quasiclassical framework, we formulate the quadruple ionization by
single photon absorption of the Coulomb five-body problem. We present the
quadruple photoionization total cross section of the ground state of Beryllium
for energies up to 620 eV. Our quasiclassical results for energies close to
threshold are in ... | physics.atom-ph | in a quasiclassical framework we formulate the quadruple ionization by single photon absorption of the coulomb fivebody problem we present the quadruple photoionization total cross section of the ground state of beryllium for energies up to 620 ev our quasiclassical results for energies close to threshold are in agreem... | [['in', 'a', 'quasiclassical', 'framework', 'we', 'formulate', 'the', 'quadruple', 'ionization', 'by', 'single', 'photon', 'absorption', 'of', 'the', 'coulomb', 'fivebody', 'problem', 'we', 'present', 'the', 'quadruple', 'photoionization', 'total', 'cross', 'section', 'of', 'the', 'ground', 'state', 'of', 'beryllium', ... | [-0.05666656081037697, 0.09891552184961101, -0.020597738524278004, 0.07827238630243512, 0.03293840859677325, -0.09618911711325825, 0.09221881260380668, 0.37797915474186805, -0.18440002335105524, -0.3498282245858464, -0.08272053508806339, -0.3097850935779108, -0.013740085682636776, 0.1988839311814008, 0.0393212609220469... |
706.3925 | Influence of second-order corrections to the energy-dependence of
neutrino flavor conversion formulae | We discuss the {\em intermediate} wave-packet formalism for analytically
quantifying the energy dependence of the two-flavor conversion formula that is
usually considered for analyzing neutrino oscillations and adjusting the
focusing horn, target position and/or detector location of some flavor
conversion experiments... | hep-ph | we discuss the em intermediate wavepacket formalism for analytically quantifying the energy dependence of the twoflavor conversion formula that is usually considered for analyzing neutrino oscillations and adjusting the focusing horn target position andor detector location of some flavor conversion experiments followin... | [['we', 'discuss', 'the', 'em', 'intermediate', 'wavepacket', 'formalism', 'for', 'analytically', 'quantifying', 'the', 'energy', 'dependence', 'of', 'the', 'twoflavor', 'conversion', 'formula', 'that', 'is', 'usually', 'considered', 'for', 'analyzing', 'neutrino', 'oscillations', 'and', 'adjusting', 'the', 'focusing',... | [-0.12105501249839529, 0.1953174749151691, -0.06640833091116001, 0.15457022364325665, -0.07173742567963835, -0.10745033368217845, 0.09499386177464787, 0.32052854641082407, -0.22722931988850362, -0.3082144858879076, 0.08212543615754381, -0.27796575565873294, -0.09514584761707723, 0.18525985502999887, 0.03125273541570837... |
706.3926 | Theoretical correlation between possible evidences of neutrino chiral
oscillations and polarization measurements | Reporting about the formalism with the Dirac equation we describe the
dynamics of chiral oscillations for a fermionic particle non-minimally coupling
with an external magnetic field. For massive particles, the chirality and
helicity quantum numbers represent different physical quantities of
representative importance ... | hep-ph | reporting about the formalism with the dirac equation we describe the dynamics of chiral oscillations for a fermionic particle nonminimally coupling with an external magnetic field for massive particles the chirality and helicity quantum numbers represent different physical quantities of representative importance in th... | [['reporting', 'about', 'the', 'formalism', 'with', 'the', 'dirac', 'equation', 'we', 'describe', 'the', 'dynamics', 'of', 'chiral', 'oscillations', 'for', 'a', 'fermionic', 'particle', 'nonminimally', 'coupling', 'with', 'an', 'external', 'magnetic', 'field', 'for', 'massive', 'particles', 'the', 'chirality', 'and', '... | [-0.19617313195736436, 0.28292700156157297, -0.014941794131939277, 0.08622249467222672, -0.08077546523702217, -0.10395398715177809, 0.0017584746502854718, 0.3162243159608991, -0.21634253751244245, -0.31449271603752443, -0.019245805699620547, -0.2648395821224989, -0.12384358365505146, 0.15592946009085765, 0.092721927668... |
706.3927 | The X-ray binary population in M33: II. X-ray spectra and variability | In this paper we investigate the X-ray spectra and X-ray spectral variability
of compact X-ray sources for 3 Chandra observations of the Local Group galaxy
M33. The observations are centered on the nucleus and the star forming region
NGC 604. In the observations 261 sources have been detected. For a total of 43
sourc... | astro-ph | in this paper we investigate the xray spectra and xray spectral variability of compact xray sources for 3 chandra observations of the local group galaxy m33 the observations are centered on the nucleus and the star forming region ngc 604 in the observations 261 sources have been detected for a total of 43 sources the n... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'xray', 'spectra', 'and', 'xray', 'spectral', 'variability', 'of', 'compact', 'xray', 'sources', 'for', '3', 'chandra', 'observations', 'of', 'the', 'local', 'group', 'galaxy', 'm33', 'the', 'observations', 'are', 'centered', 'on', 'the', 'nucleus', 'and', 'the', 'st... | [-0.07183396060330173, 0.09459210930702587, -0.04495408845499956, 0.11918124902738436, -0.07864187023203288, -0.07668891111832289, 0.0879757121632186, 0.4959076944029047, -0.11240305632319568, -0.38531435162183786, 0.11392159961895751, -0.3908201352648792, 0.003239580470004252, 0.24688475118683917, -0.01095624796926997... |
706.3928 | Small Corrections to the Tunneling Phase Time Formulation | After reexamining the above barrier diffusion problem where we notice that
the wave packet collision implies the existence of {\em multiple} reflected and
transmitted wave packets, we analyze the way of obtaining phase times for
tunneling/reflecting particles in a particular colliding configuration where
the idea of ... | hep-ph | after reexamining the above barrier diffusion problem where we notice that the wave packet collision implies the existence of em multiple reflected and transmitted wave packets we analyze the way of obtaining phase times for tunnelingreflecting particles in a particular colliding configuration where the idea of multipl... | [['after', 'reexamining', 'the', 'above', 'barrier', 'diffusion', 'problem', 'where', 'we', 'notice', 'that', 'the', 'wave', 'packet', 'collision', 'implies', 'the', 'existence', 'of', 'em', 'multiple', 'reflected', 'and', 'transmitted', 'wave', 'packets', 'we', 'analyze', 'the', 'way', 'of', 'obtaining', 'phase', 'tim... | [-0.1738067226302572, 0.17832341688527067, -0.10189152617061878, 0.05871918302600401, -0.03141299865113394, -0.12135916243368475, 0.07148821481646303, 0.3569391063230969, -0.28752246610208476, -0.24296022478463877, 0.08768542394310536, -0.2626406488562832, -0.14946885397453813, 0.16731933967964926, 0.02058699912643128,... |
706.3929 | The Exact Correspondence between Phase Times and Dwell Times in a
Symmetrical Quantum Tunneling Configuration | The general and explicit relation between the phase time and the dwell time
for quantum tunneling or scattering is investigated. Considering a symmetrical
collision of two identical wave packets with an one-dimensional barrier, here
we demonstrate that these two distinct transit time definitions give connected
result... | quant-ph | the general and explicit relation between the phase time and the dwell time for quantum tunneling or scattering is investigated considering a symmetrical collision of two identical wave packets with an onedimensional barrier here we demonstrate that these two distinct transit time definitions give connected results whe... | [['the', 'general', 'and', 'explicit', 'relation', 'between', 'the', 'phase', 'time', 'and', 'the', 'dwell', 'time', 'for', 'quantum', 'tunneling', 'or', 'scattering', 'is', 'investigated', 'considering', 'a', 'symmetrical', 'collision', 'of', 'two', 'identical', 'wave', 'packets', 'with', 'an', 'onedimensional', 'barr... | [-0.18696080349036492, 0.15435302205798962, -0.09227026980079245, 0.05565264681536064, -0.04666745220856683, -0.13262148641297244, 0.07223329140015267, 0.3868438837816939, -0.2784917959579616, -0.2852485261973925, 0.07209070980934484, -0.2551912091931854, -0.132456464221832, 0.17601544137687597, 0.013271114232338732, 0... |
706.393 | Relativistic tunneling and accelerated transmission | We obtain the solutions for the tunneling zone of a one-dimensional
electrostatic potential in the relativistic (Dirac to Klein-Gordon) wave
equation regime when the incoming wave packet exhibits the possibility of being
almost totally transmitted through the potential barrier. The conditions for
the occurrence of ac... | quant-ph | we obtain the solutions for the tunneling zone of a onedimensional electrostatic potential in the relativistic dirac to kleingordon wave equation regime when the incoming wave packet exhibits the possibility of being almost totally transmitted through the potential barrier the conditions for the occurrence of accelerat... | [['we', 'obtain', 'the', 'solutions', 'for', 'the', 'tunneling', 'zone', 'of', 'a', 'onedimensional', 'electrostatic', 'potential', 'in', 'the', 'relativistic', 'dirac', 'to', 'kleingordon', 'wave', 'equation', 'regime', 'when', 'the', 'incoming', 'wave', 'packet', 'exhibits', 'the', 'possibility', 'of', 'being', 'almo... | [-0.19166716772894027, 0.1431609108957334, -0.09319861288931147, 0.08181499135246792, -0.06296402633454942, -0.1755118678031745, 0.07476117506388726, 0.3259571421453181, -0.26692165177790267, -0.25248228284808827, -0.008828182647680389, -0.2909314449986114, -0.1479461083517355, 0.23028333222164826, 0.04754986390745377,... |
706.3931 | The coupling constants for an electroweak model with a $SU(4)_{PS}
\otimes SU(4)_{EW}$ unification symmetry | We introduce the sequence of spontaneous symmetry breaking of a coupling
between Pati-Salam and electroweak symmetries $SU(4)_{PS} \otimes SU(4)_{EW}$
in order to establish a mathematically consistent relation among the coupling
constants at grand unification energy scale. With the values of baryon minus
lepton quant... | hep-ph | we introduce the sequence of spontaneous symmetry breaking of a coupling between patisalam and electroweak symmetries su4_ps otimes su4_ew in order to establish a mathematically consistent relation among the coupling constants at grand unification energy scale with the values of baryon minus lepton quantum numbers of k... | [['we', 'introduce', 'the', 'sequence', 'of', 'spontaneous', 'symmetry', 'breaking', 'of', 'a', 'coupling', 'between', 'patisalam', 'and', 'electroweak', 'symmetries', 'su4_ps', 'otimes', 'su4_ew', 'in', 'order', 'to', 'establish', 'a', 'mathematically', 'consistent', 'relation', 'among', 'the', 'coupling', 'constants'... | [-0.15686084448492954, 0.3530323950839894, 0.013152553526950734, 0.17506299673446588, -0.07396410115595375, -0.12633541523745018, 0.06414028475826074, 0.32521372511982916, -0.2607219574706895, -0.3547277586002435, -0.021353770022480085, -0.2514595004862973, 0.010062176468116897, 0.03995594132159438, 0.07781720706926924... |
706.3932 | Dirac neutrino mass from the beta decay end-point modified by the
dynamics of a Lorentz-violating equation of motion | Using a generalized procedure for obtaining the equation of motion of a
propagating fermionic particle, we examine previous claims for a lightlike
preferred axis embedded in the framework of Lorentz-invariance violation with
preserved algebra. In a high energy scale, the corresponding equation of motion
is reduced to... | hep-ph | using a generalized procedure for obtaining the equation of motion of a propagating fermionic particle we examine previous claims for a lightlike preferred axis embedded in the framework of lorentzinvariance violation with preserved algebra in a high energy scale the corresponding equation of motion is reduced to a con... | [['using', 'a', 'generalized', 'procedure', 'for', 'obtaining', 'the', 'equation', 'of', 'motion', 'of', 'a', 'propagating', 'fermionic', 'particle', 'we', 'examine', 'previous', 'claims', 'for', 'a', 'lightlike', 'preferred', 'axis', 'embedded', 'in', 'the', 'framework', 'of', 'lorentzinvariance', 'violation', 'with',... | [-0.15211789266757625, 0.19561859591055833, -0.08487163732984457, 0.10330306166172798, -0.09647278228357177, -0.14470860666338484, -0.0019150228057613317, 0.2668740698618108, -0.26061202825485974, -0.27814958717716837, 0.022553032953238607, -0.2604604775043226, -0.04370610854299418, 0.13674847295791467, 0.0080876275074... |
706.3933 | Negative capacitance in organic semiconductor devices: bipolar injection
and charge recombination mechanism | We report negative capacitance at low frequencies in organic semiconductor
based diodes and show that it appears only under bipolar injection conditions.
We account quantitatively for this phenomenon by the recombination current due
to electron-hole annihilation. Simple addition of the recombination current to
the we... | physics.chem-ph | we report negative capacitance at low frequencies in organic semiconductor based diodes and show that it appears only under bipolar injection conditions we account quantitatively for this phenomenon by the recombination current due to electronhole annihilation simple addition of the recombination current to the well es... | [['we', 'report', 'negative', 'capacitance', 'at', 'low', 'frequencies', 'in', 'organic', 'semiconductor', 'based', 'diodes', 'and', 'show', 'that', 'it', 'appears', 'only', 'under', 'bipolar', 'injection', 'conditions', 'we', 'account', 'quantitatively', 'for', 'this', 'phenomenon', 'by', 'the', 'recombination', 'curr... | [-0.12146791927775161, 0.13045787300086684, -0.011425355014054932, 0.059624259638985676, -0.00012157055445843273, -0.15536476004765265, 0.07106984521572789, 0.39622002132236955, -0.24304259271464415, -0.29714543430341617, 0.010505762921335796, -0.23890954089454478, -0.09005477963429358, 0.21505354886305414, -0.00173153... |
706.3934 | Foundations of Relational Particle Dynamics | Relational particle dynamics include the dynamics of pure shape and cases in
which absolute scale or absolute rotation are additionally meaningful. These
are interesting as regards the absolute versus relative motion debate as well
as discussion of conceptual issues connected with the problem of time in
quantum gravi... | gr-qc | relational particle dynamics include the dynamics of pure shape and cases in which absolute scale or absolute rotation are additionally meaningful these are interesting as regards the absolute versus relative motion debate as well as discussion of conceptual issues connected with the problem of time in quantum gravity ... | [['relational', 'particle', 'dynamics', 'include', 'the', 'dynamics', 'of', 'pure', 'shape', 'and', 'cases', 'in', 'which', 'absolute', 'scale', 'or', 'absolute', 'rotation', 'are', 'additionally', 'meaningful', 'these', 'are', 'interesting', 'as', 'regards', 'the', 'absolute', 'versus', 'relative', 'motion', 'debate',... | [-0.0659203297608266, 0.1153599363106468, -0.07015961835897722, 0.10666056596840333, -0.06944463307877163, -0.12292601641364764, -0.03481987305753097, 0.36980306083889125, -0.27399972700360387, -0.31101350661797017, 0.1281149226220345, -0.21848549945331128, -0.14005682609238468, 0.1837809274790573, -0.08344142938257901... |
706.3935 | Feedback in the Antennae Galaxies (NGC 4038/9): I. High-Resolution
Infrared Spectroscopy of Winds from Super Star Clusters | We present high-resolution (R ~ 24,600) near-IR spectroscopy of the youngest
super star clusters (SSCs) in the prototypical starburst merger, the Antennae
Galaxies. These SSCs are young (3-7 Myr old) and massive (10^5 - 10^7 M_sun for
a Kroupa IMF) and their spectra are characterized by broad, extended Br-gamma
emiss... | astro-ph | we present highresolution r 24600 nearir spectroscopy of the youngest super star clusters sscs in the prototypical starburst merger the antennae galaxies these sscs are young 37 myr old and massive 105 107 m_sun for a kroupa imf and their spectra are characterized by broad extended brgamma emission so we refer to them ... | [['we', 'present', 'highresolution', 'r', '24600', 'nearir', 'spectroscopy', 'of', 'the', 'youngest', 'super', 'star', 'clusters', 'sscs', 'in', 'the', 'prototypical', 'starburst', 'merger', 'the', 'antennae', 'galaxies', 'these', 'sscs', 'are', 'young', '37', 'myr', 'old', 'and', 'massive', '105', '107', 'm_sun', 'for... | [-0.049234857682798366, 0.18684731996876913, -0.04179830770525667, 0.12981749974100643, -0.0700539544185934, -0.09428288789672984, 0.03403841750760977, 0.4599558185372088, -0.13741527656998692, -0.3393287285282794, 0.025599151380204906, -0.27120697659298054, 0.03128092101154228, 0.19793973967381234, -0.0442432773428865... |
706.3936 | On the commuting charges for the highest dimension SU(2) operators in
planar ${\cal N}=4$ SYM | We consider the highest anomalous dimension operator in the SU(2) sector of
planar ${\cal N}=4$ SYM at all-loop, though neglecting wrapping contributions.
In any case, the latter enter the loop expansion only after a precise
length-depending order. In the thermodynamic limit we write both a linear
integral equation f... | hep-th | we consider the highest anomalous dimension operator in the su2 sector of planar cal n4 sym at allloop though neglecting wrapping contributions in any case the latter enter the loop expansion only after a precise lengthdepending order in the thermodynamic limit we write both a linear integral equation for the bethe roo... | [['we', 'consider', 'the', 'highest', 'anomalous', 'dimension', 'operator', 'in', 'the', 'su2', 'sector', 'of', 'planar', 'cal', 'n4', 'sym', 'at', 'allloop', 'though', 'neglecting', 'wrapping', 'contributions', 'in', 'any', 'case', 'the', 'latter', 'enter', 'the', 'loop', 'expansion', 'only', 'after', 'a', 'precise', ... | [-0.14495868619414978, 0.16764490232756846, -0.06978742252103984, 0.08612085800947776, -0.06274791515703934, -0.08379428741754964, 0.020851193531416356, 0.26189400561755366, -0.2326157043183533, -0.22469245241954922, 0.08476743834326043, -0.3244798485073261, -0.12084045427230497, 0.10545615351293236, 0.0248558831129533... |
706.3937 | Rips complexes and covers in the uniform category | James \cite{Jam} introduced uniform covering maps as an analog of covering
maps in the topological category. Subsequently Berestovskii and Plaut
\cite{BP3} introduced a theory of covers for uniform spaces generalizing their
results for topological groups \cite{BP1}-\cite{BP2}. Their main concepts are
discrete actions... | math.MG math.GN | james citejam introduced uniform covering maps as an analog of covering maps in the topological category subsequently berestovskii and plaut citebp3 introduced a theory of covers for uniform spaces generalizing their results for topological groups citebp1citebp2 their main concepts are discrete actions and prodiscrete ... | [['james', 'citejam', 'introduced', 'uniform', 'covering', 'maps', 'as', 'an', 'analog', 'of', 'covering', 'maps', 'in', 'the', 'topological', 'category', 'subsequently', 'berestovskii', 'and', 'plaut', 'citebp3', 'introduced', 'a', 'theory', 'of', 'covers', 'for', 'uniform', 'spaces', 'generalizing', 'their', 'results... | [-0.11344163383667667, 0.14431688916940605, -0.06925732516018408, 0.09706304153882056, -0.06930073558737243, -0.05877060776886841, 0.05197022036216887, 0.38994083987800254, -0.30191453201474533, -0.22526953505936065, 0.1473587270898168, -0.22124684356626065, -0.16020299257000997, 0.2073648638269376, -0.2015048898165188... |
706.3938 | The UV-optical Galaxy Color-Magnitude Diagram I: Basic Properties | We have analyzed the bivariate distribution of galaxies as a function of
ultraviolet-optical colors and absolute magnitudes in the local universe. The
sample consists of galaxies with redshifts and optical photometry from the
Sloan Digital Sky Survey (SDSS) main galaxy sample matched with detections in
the near-ultra... | astro-ph | we have analyzed the bivariate distribution of galaxies as a function of ultravioletoptical colors and absolute magnitudes in the local universe the sample consists of galaxies with redshifts and optical photometry from the sloan digital sky survey sdss main galaxy sample matched with detections in the nearultraviolet ... | [['we', 'have', 'analyzed', 'the', 'bivariate', 'distribution', 'of', 'galaxies', 'as', 'a', 'function', 'of', 'ultravioletoptical', 'colors', 'and', 'absolute', 'magnitudes', 'in', 'the', 'local', 'universe', 'the', 'sample', 'consists', 'of', 'galaxies', 'with', 'redshifts', 'and', 'optical', 'photometry', 'from', 't... | [-0.0011795214219605338, 0.11108416828727002, -0.07242639755336071, 0.08542111178749874, -0.08564480847209557, -0.02372169578585681, 0.0441901583152553, 0.4938652677504161, -0.12939105500673292, -0.34842023898612795, 0.040223645102339334, -0.31969624173024114, -0.01436229367146823, 0.1663497564878727, -0.06757779889082... |
706.3939 | Future Directions in Parity Violation: From Quarks to the Cosmos | I discuss the prospects for future studies of parity-violating (PV)
interactions at low energies and the insights they might provide about open
questions in the Standard Model as well as physics that lies beyond it. I cover
four types of parity-violating observables: PV electron scattering; PV hadronic
interactions; ... | nucl-th | i discuss the prospects for future studies of parityviolating pv interactions at low energies and the insights they might provide about open questions in the standard model as well as physics that lies beyond it i cover four types of parityviolating observables pv electron scattering pv hadronic interactions pv correla... | [['i', 'discuss', 'the', 'prospects', 'for', 'future', 'studies', 'of', 'parityviolating', 'pv', 'interactions', 'at', 'low', 'energies', 'and', 'the', 'insights', 'they', 'might', 'provide', 'about', 'open', 'questions', 'in', 'the', 'standard', 'model', 'as', 'well', 'as', 'physics', 'that', 'lies', 'beyond', 'it', '... | [-0.12251316261244938, 0.20445672384812497, 0.012592340337505448, 0.16477793766534887, 0.0193775816114794, -0.17341828260396142, 0.014138823715256876, 0.2697918257326819, -0.2644901628009393, -0.2836716389792855, 0.015552698849205626, -0.37795692958752625, -0.06064106280973647, 0.21330743874932523, 0.09304608777165413,... |
706.394 | The Northern Site of the Pierre Auger Observatory | The Pierre Auger Observatory is a multi-national project for research on
ultra-high energy cosmic rays. The Southern Auger Observatory in Mendoza
province, Argentina, is approaching completion in 2007 with an instrumented
area of 3,000 km^2. It will accurately measure the spectrum and composition of
ultra-high energy... | astro-ph | the pierre auger observatory is a multinational project for research on ultrahigh energy cosmic rays the southern auger observatory in mendoza province argentina is approaching completion in 2007 with an instrumented area of 3000 km2 it will accurately measure the spectrum and composition of ultrahigh energy cosmic ray... | [['the', 'pierre', 'auger', 'observatory', 'is', 'a', 'multinational', 'project', 'for', 'research', 'on', 'ultrahigh', 'energy', 'cosmic', 'rays', 'the', 'southern', 'auger', 'observatory', 'in', 'mendoza', 'province', 'argentina', 'is', 'approaching', 'completion', 'in', '2007', 'with', 'an', 'instrumented', 'area', ... | [-0.0799800834247435, 0.18387888580294506, -0.04391278790717479, 0.11729657347495959, -0.07796884989753987, 0.009779683323965097, -0.008806876410744735, 0.378378932082948, -0.19793456932529807, -0.39603839688546333, 0.08010201828619756, -0.3874790310467991, -0.025675460322114912, 0.2277799970106571, -0.0072364906081929... |
706.3941 | Intrinsic alignments of galaxies and their effects on weak lensing
detections of mass concentrations | In this paper we investigate the influence of the intrinsic alignment of
background galaxies on weak lensing detections of mass concentrations.
Specifically, we analyze the number counts of false peaks resulting from
intrinsic ellipticities in lensing convergence maps. Including the alignment of
source galaxies, the ... | astro-ph | in this paper we investigate the influence of the intrinsic alignment of background galaxies on weak lensing detections of mass concentrations specifically we analyze the number counts of false peaks resulting from intrinsic ellipticities in lensing convergence maps including the alignment of source galaxies the full n... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'influence', 'of', 'the', 'intrinsic', 'alignment', 'of', 'background', 'galaxies', 'on', 'weak', 'lensing', 'detections', 'of', 'mass', 'concentrations', 'specifically', 'we', 'analyze', 'the', 'number', 'counts', 'of', 'false', 'peaks', 'resulting', 'from', 'intrin... | [-0.11818814687380243, 0.08410153837631577, -0.019114247614355838, 0.09517457186365905, -0.04786890538272691, -0.07934499519077413, 0.05486484783139768, 0.3468968725520308, -0.21532322673390256, -0.3793954128673447, 0.07568106225453844, -0.29828442159139185, -0.08508938511722194, 0.18744572077665236, -0.075963128970571... |
706.3942 | Chiral Symmetries and Low Energy Searches for New Physics | I discuss low energy searches for new physics beyond the Standard Model,
identifying the role played by chiral symmetries in these searches and in
various new physics scenarios. I focus in particular on electric dipole moment
searches; precision studies of weak decays and electron scattering; and
neutrino properties ... | nucl-th | i discuss low energy searches for new physics beyond the standard model identifying the role played by chiral symmetries in these searches and in various new physics scenarios i focus in particular on electric dipole moment searches precision studies of weak decays and electron scattering and neutrino properties and in... | [['i', 'discuss', 'low', 'energy', 'searches', 'for', 'new', 'physics', 'beyond', 'the', 'standard', 'model', 'identifying', 'the', 'role', 'played', 'by', 'chiral', 'symmetries', 'in', 'these', 'searches', 'and', 'in', 'various', 'new', 'physics', 'scenarios', 'i', 'focus', 'in', 'particular', 'on', 'electric', 'dipol... | [-0.09942870790138841, 0.23937792912125588, 0.011553476493572816, 0.15691763563081623, -0.06876342615578324, -0.1583896913379431, 0.012219514864264057, 0.295606792345643, -0.228876324146986, -0.33817052640020845, 0.04346098805079237, -0.30898845767602323, -0.07468699442222715, 0.16685890113469212, 0.11277539749629796, ... |
706.3943 | The globular cluster system in NGC5866: optical observations from HST
Advanced Camera for Surveys | We perform a detailed study of the Globular Cluster (GC) system in the galaxy
NGC5866 based on F435W, F555W, and F625W (~ B, V, and R) HST Advanced Camera
for Surveys images.
Adopting color, size and shape selection criteria, the final list of GC
candidates comprises 109 objects, with small estimated contamination ... | astro-ph | we perform a detailed study of the globular cluster gc system in the galaxy ngc5866 based on f435w f555w and f625w b v and r hst advanced camera for surveys images adopting color size and shape selection criteria the final list of gc candidates comprises 109 objects with small estimated contamination from background ga... | [['we', 'perform', 'a', 'detailed', 'study', 'of', 'the', 'globular', 'cluster', 'gc', 'system', 'in', 'the', 'galaxy', 'ngc5866', 'based', 'on', 'f435w', 'f555w', 'and', 'f625w', 'b', 'v', 'and', 'r', 'hst', 'advanced', 'camera', 'for', 'surveys', 'images', 'adopting', 'color', 'size', 'and', 'shape', 'selection', 'cr... | [-0.016609370170044713, 0.05927378407588029, -0.11445818222377316, 0.10901716246787276, -0.06886537278809815, -0.0569249127880929, 0.07964001163600187, 0.45324649911240805, -0.14031749057591827, -0.3832103809067381, 0.0037668339895649944, -0.3133481708895748, -0.025363673572558452, 0.19400029277572425, -0.0791693954607... |
706.3944 | A new tetra-quark interpretation of X(3872) | A new tetra-quark interpretation of X(3872) is presented. In this model,
X(3872) consists of two degenerate tetra-quark mesons, {[cn](cbar nbar) +-
(cn)[cbar nbar]}_{I=0}, and, therefore, it is naturally understood that X(3872)
decays into two different eigenstates of G-parity.
| hep-ph hep-ex nucl-th | a new tetraquark interpretation of x3872 is presented in this model x3872 consists of two degenerate tetraquark mesons cncbar nbar cncbar nbar_i0 and therefore it is naturally understood that x3872 decays into two different eigenstates of gparity | [['a', 'new', 'tetraquark', 'interpretation', 'of', 'x3872', 'is', 'presented', 'in', 'this', 'model', 'x3872', 'consists', 'of', 'two', 'degenerate', 'tetraquark', 'mesons', 'cncbar', 'nbar', 'cncbar', 'nbar_i0', 'and', 'therefore', 'it', 'is', 'naturally', 'understood', 'that', 'x3872', 'decays', 'into', 'two', 'diff... | [-0.1319083909449332, 0.3087815114242189, -0.11478419782703414, 0.24716638600083946, -0.10135174153701347, -0.225145752692376, 0.08475380211808335, 0.2713591927073567, -0.16055127392139504, -0.12385624729316025, -0.1646429458667305, -0.2471209363464047, -0.051925781347295814, 0.004935384705758598, 0.10736208022846018, ... |
706.3945 | Slow light with integrated gain and large pulse delay | We demonstrate slow and stored light in Rb vapor with a combination of
desirable features: minimal loss and distortion of the pulse shape, and large
fractional delay (> 10). This behavior is enabled by: (i) a group index that
can be controllably varied during light pulse propagation; and (ii)
controllable gain integr... | physics.optics physics.atom-ph quant-ph | we demonstrate slow and stored light in rb vapor with a combination of desirable features minimal loss and distortion of the pulse shape and large fractional delay 10 this behavior is enabled by i a group index that can be controllably varied during light pulse propagation and ii controllable gain integrated into the m... | [['we', 'demonstrate', 'slow', 'and', 'stored', 'light', 'in', 'rb', 'vapor', 'with', 'a', 'combination', 'of', 'desirable', 'features', 'minimal', 'loss', 'and', 'distortion', 'of', 'the', 'pulse', 'shape', 'and', 'large', 'fractional', 'delay', '10', 'this', 'behavior', 'is', 'enabled', 'by', 'i', 'a', 'group', 'inde... | [-0.09035868868930265, 0.2076485364511609, -0.07456134659548601, 0.016570126687486968, -0.07649358506004016, -0.19673460621386765, 0.056404845577975114, 0.49979779465124013, -0.32849343694746497, -0.3376155454913775, 0.07484653077243517, -0.24403234034466248, -0.09575851170967023, 0.19818859604497752, -0.08814760152250... |
706.3946 | Phase diagram for a Bose-Einstein condensate moving in an optical
lattice | The stability of superfluid currents in a system of ultracold bosons was
studied using a moving optical lattice. Superfluid currents in a very weak
lattice become unstable when their momentum exceeds 0.5 recoil momentum.
Superfluidity vanishes already for zero momentum as the lattice deep reaches
the Mott insulator(M... | cond-mat.other | the stability of superfluid currents in a system of ultracold bosons was studied using a moving optical lattice superfluid currents in a very weak lattice become unstable when their momentum exceeds 05 recoil momentum superfluidity vanishes already for zero momentum as the lattice deep reaches the mott insulatormi phas... | [['the', 'stability', 'of', 'superfluid', 'currents', 'in', 'a', 'system', 'of', 'ultracold', 'bosons', 'was', 'studied', 'using', 'a', 'moving', 'optical', 'lattice', 'superfluid', 'currents', 'in', 'a', 'very', 'weak', 'lattice', 'become', 'unstable', 'when', 'their', 'momentum', 'exceeds', '05', 'recoil', 'momentum'... | [-0.1773068680735263, 0.3168840923908729, -0.07809809410969752, 0.02625477677714583, 0.0032992741755872696, -0.158584770171794, 0.12031388316913885, 0.3787098508663811, -0.23964974943649126, -0.19159288044079198, 0.07215079884799952, -0.30115919983064804, -0.03212058774052976, 0.1260095744368595, 0.07641286149553887, 0... |
706.3947 | Transient Lunar Phenomena: Regularity and Reality | Transient lunar phenomena (TLPs) have been reported for centuries, but their
nature is largely unsettled. A review of TLP reports shows regularities in the
observations; a key question is whether this structure is imposed by human
observer effects, terrestrial atmospheric effects or processes tied to the
lunar surfac... | astro-ph | transient lunar phenomena tlps have been reported for centuries but their nature is largely unsettled a review of tlp reports shows regularities in the observations a key question is whether this structure is imposed by human observer effects terrestrial atmospheric effects or processes tied to the lunar surface i inte... | [['transient', 'lunar', 'phenomena', 'tlps', 'have', 'been', 'reported', 'for', 'centuries', 'but', 'their', 'nature', 'is', 'largely', 'unsettled', 'a', 'review', 'of', 'tlp', 'reports', 'shows', 'regularities', 'in', 'the', 'observations', 'a', 'key', 'question', 'is', 'whether', 'this', 'structure', 'is', 'imposed',... | [-0.08605037781074089, 0.14824548321804223, -0.07806813014415007, 0.08172699817232129, -0.0848743229646575, -0.11468082184636737, 0.07310574387198446, 0.3676368291957172, -0.20669464216841088, -0.35638606470929923, 0.12208469024708765, -0.32381111327351025, -0.12821564463150711, 0.2022231030347151, -0.11883651654384891... |
706.3948 | Metal-insulator transition in the two-orbital Hubbard model at
fractional band fillings: Self-energy functional approach | We investigate the infinite-dimensional two-orbital Hubbard model at
arbitrary band fillings. By means of the self-energy functional approach, we
discuss the stability of the metallic state in the systems with same and
different bandwidths. It is found that the Mott insulating phases are realized
at commensurate band... | cond-mat.str-el | we investigate the infinitedimensional twoorbital hubbard model at arbitrary band fillings by means of the selfenergy functional approach we discuss the stability of the metallic state in the systems with same and different bandwidths it is found that the mott insulating phases are realized at commensurate band filling... | [['we', 'investigate', 'the', 'infinitedimensional', 'twoorbital', 'hubbard', 'model', 'at', 'arbitrary', 'band', 'fillings', 'by', 'means', 'of', 'the', 'selfenergy', 'functional', 'approach', 'we', 'discuss', 'the', 'stability', 'of', 'the', 'metallic', 'state', 'in', 'the', 'systems', 'with', 'same', 'and', 'differe... | [-0.224388282898227, 0.21352547463736957, -0.028103538096257593, 0.09423115895913702, 0.009074910982995283, -0.20541569816915295, 0.1031031741943399, 0.4356408211626584, -0.2685915577001398, -0.25964735726578325, 0.05433467955658613, -0.28702561204805027, -0.13854437686290733, 0.11224356555096994, 0.044051883954413326,... |
706.3949 | Lunar Outgassing, Transient Phenomena and The Return to The Moon, I:
Existing Data | Herein the transient lunar phenomena (TLP) report database is subjected to a
discriminating statistical filter robust against sites of spurious reports, and
produces a restricted sample that may be largely reliable. This subset is
highly correlated geographically with the catalog of outgassing events seen by
the Apol... | astro-ph | herein the transient lunar phenomena tlp report database is subjected to a discriminating statistical filter robust against sites of spurious reports and produces a restricted sample that may be largely reliable this subset is highly correlated geographically with the catalog of outgassing events seen by the apollo 15 ... | [['herein', 'the', 'transient', 'lunar', 'phenomena', 'tlp', 'report', 'database', 'is', 'subjected', 'to', 'a', 'discriminating', 'statistical', 'filter', 'robust', 'against', 'sites', 'of', 'spurious', 'reports', 'and', 'produces', 'a', 'restricted', 'sample', 'that', 'may', 'be', 'largely', 'reliable', 'this', 'subs... | [-0.05697864740402914, 0.18861303740079272, -0.054180178841419624, 0.07066672392139367, -0.06958861134472187, -0.09402084329342265, 0.05669221915597823, 0.3791997425638846, -0.22190837514413397, -0.35183051645663993, 0.1451156389250345, -0.32133271970724975, -0.11658236021889767, 0.21409245780720138, -0.116981841195510... |
706.395 | Thorn independence in the field of real numbers with a small
multiplicative group | We characterize thorn-independence in a variety of structures, focusing on
the field of real numbers expanded by predicate defining a dense multiplicative
subgroup, G, satisfying the Mann property and whose pth powers are of finite
index in G. We also show such structures are super-rosy and eliminate
imaginaries up t... | math.LO | we characterize thornindependence in a variety of structures focusing on the field of real numbers expanded by predicate defining a dense multiplicative subgroup g satisfying the mann property and whose pth powers are of finite index in g we also show such structures are superrosy and eliminate imaginaries up to codes ... | [['we', 'characterize', 'thornindependence', 'in', 'a', 'variety', 'of', 'structures', 'focusing', 'on', 'the', 'field', 'of', 'real', 'numbers', 'expanded', 'by', 'predicate', 'defining', 'a', 'dense', 'multiplicative', 'subgroup', 'g', 'satisfying', 'the', 'mann', 'property', 'and', 'whose', 'pth', 'powers', 'are', '... | [-0.20631412844415065, 0.1290366658595977, -0.03919640345567906, 0.05160263908544072, -0.08896900230104586, -0.06941956868697027, 0.0228599169209634, 0.37701656317545307, -0.34178506641614215, -0.26559911895094923, 0.09844385857987045, -0.23004095011425238, -0.13487263496413274, 0.22266927463243957, -0.0953626162113828... |
706.3951 | Extending SU(2) to SU(N) QCD | Abelian dominance is used to reformulate the QCD Lagrangian as a sum over the
roots of Lie group representation theory. This greatly facilitates extending
the SU(2) magnetic ground state energy spectrum, several arguments for the
stability of the magnetic ground state, and the Faddeev-Skyrme model to
arbitrary SU(N) ... | hep-th | abelian dominance is used to reformulate the qcd lagrangian as a sum over the roots of lie group representation theory this greatly facilitates extending the su2 magnetic ground state energy spectrum several arguments for the stability of the magnetic ground state and the faddeevskyrme model to arbitrary sun qcd | [['abelian', 'dominance', 'is', 'used', 'to', 'reformulate', 'the', 'qcd', 'lagrangian', 'as', 'a', 'sum', 'over', 'the', 'roots', 'of', 'lie', 'group', 'representation', 'theory', 'this', 'greatly', 'facilitates', 'extending', 'the', 'su2', 'magnetic', 'ground', 'state', 'energy', 'spectrum', 'several', 'arguments', '... | [-0.1642021759679275, 0.16563777484912046, -0.10772849279081649, 0.10149971848087651, -0.12161652192625465, -0.0252473944018842, 0.05208651387674392, 0.30457833243001786, -0.2509960119365429, -0.277161786902924, 0.08923861646682632, -0.20799946060822327, -0.06256296853439844, 0.0887699426218335, 0.04697776329228465, 0.... |
706.3952 | Lunar Outgassing, Transient Phenomena and The Return to The Moon, II:
Predictions for Interactions between Outgassing and Regolith | We consider the implications from Paper I on how gas leaking through the
lunar surface might interact with the regolith, and in what respects this might
affect or cause the appearance of optical Transient Lunar Phenomena (TLPs). We
consider briefly a range of phenomena, but concentrate at the extremes of high
and low... | astro-ph | we consider the implications from paper i on how gas leaking through the lunar surface might interact with the regolith and in what respects this might affect or cause the appearance of optical transient lunar phenomena tlps we consider briefly a range of phenomena but concentrate at the extremes of high and low gas fl... | [['we', 'consider', 'the', 'implications', 'from', 'paper', 'i', 'on', 'how', 'gas', 'leaking', 'through', 'the', 'lunar', 'surface', 'might', 'interact', 'with', 'the', 'regolith', 'and', 'in', 'what', 'respects', 'this', 'might', 'affect', 'or', 'cause', 'the', 'appearance', 'of', 'optical', 'transient', 'lunar', 'ph... | [-0.08137814153153482, 0.21981717990307056, -0.06436163581550569, 0.05779752015603433, -0.04800315233545041, -0.06600272078496172, 0.06278624111244538, 0.3351706009971633, -0.2914764486736405, -0.31874052542198206, 0.12585502873896381, -0.28266527110300704, -0.10880878910266575, 0.1964741813173079, -0.08911490433336054... |
706.3953 | Maps between moduli spaces of vector bundles and the base locus of the
theta divisor | Given a vector bundle $E$ of rank $r$ and degree $d$ on a curve $C$ of genus
$g$, one can associate to $E$ in a natural way several other vector bundles.
For example, one can take wedge powers of $E$. If $E$ is generated by global
sections, the kernel of the evaluation map of sections is again a vector
bundle. Also, ... | math.AG | given a vector bundle e of rank r and degree d on a curve c of genus g one can associate to e in a natural way several other vector bundles for example one can take wedge powers of e if e is generated by global sections the kernel of the evaluation map of sections is again a vector bundle also new vector bundles can be... | [['given', 'a', 'vector', 'bundle', 'e', 'of', 'rank', 'r', 'and', 'degree', 'd', 'on', 'a', 'curve', 'c', 'of', 'genus', 'g', 'one', 'can', 'associate', 'to', 'e', 'in', 'a', 'natural', 'way', 'several', 'other', 'vector', 'bundles', 'for', 'example', 'one', 'can', 'take', 'wedge', 'powers', 'of', 'e', 'if', 'e', 'is'... | [-0.1703411219300349, 0.10997693004600446, -0.09353854773357383, 0.04710618355652671, -0.07709667183346404, -0.1642488502046286, 0.03171174966525447, 0.40085125746655054, -0.3023314023197725, -0.22844787936452937, 0.08976535881861467, -0.24266358553873504, -0.12480388323330835, 0.19435922121869978, -0.06124982855218495... |
706.3954 | Lunar Outgassing, Transient Phenomena and The Return to The Moon, III:
Observational and Experimental Techniques | In Papers II and III we show that Transient Lunar Phenomena (TLPs) are likely
related to lunar outgassing, albeit in ways not fully understood. Here we
propose a path forward, in which current and forthcoming technologies provide a
more controlled, sensitive probe of lunar outgassing. Many of these techniques
are bei... | astro-ph | in papers ii and iii we show that transient lunar phenomena tlps are likely related to lunar outgassing albeit in ways not fully understood here we propose a path forward in which current and forthcoming technologies provide a more controlled sensitive probe of lunar outgassing many of these techniques are being realiz... | [['in', 'papers', 'ii', 'and', 'iii', 'we', 'show', 'that', 'transient', 'lunar', 'phenomena', 'tlps', 'are', 'likely', 'related', 'to', 'lunar', 'outgassing', 'albeit', 'in', 'ways', 'not', 'fully', 'understood', 'here', 'we', 'propose', 'a', 'path', 'forward', 'in', 'which', 'current', 'and', 'forthcoming', 'technolo... | [-0.08193337065946778, 0.16483377443223496, -0.08553191227749868, 0.06317473288263396, -0.08540856500511224, -0.10580618731932495, 0.05030479920167519, 0.3944271441492404, -0.2580293946697628, -0.3185877890030397, 0.15119621464840982, -0.26703810024857805, -0.18829241752298725, 0.2434602519778354, -0.14929218186411397,... |
706.3955 | Study of charmonia in four-meson final states produced in two-photon
collisions | We report measurements of charmonia produced in two-photon collisions and
decaying to four-meson final states, where the meson is either a charged pion
or a charged kaon. The analysis is based on a 395fb^{-1} data sample
accumulated with the Belle detector at the KEKB electron-positron collider. We
observe signals fo... | hep-ex | we report measurements of charmonia produced in twophoton collisions and decaying to fourmeson final states where the meson is either a charged pion or a charged kaon the analysis is based on a 395fb1 data sample accumulated with the belle detector at the kekb electronpositron collider we observe signals for the three ... | [['we', 'report', 'measurements', 'of', 'charmonia', 'produced', 'in', 'twophoton', 'collisions', 'and', 'decaying', 'to', 'fourmeson', 'final', 'states', 'where', 'the', 'meson', 'is', 'either', 'a', 'charged', 'pion', 'or', 'a', 'charged', 'kaon', 'the', 'analysis', 'is', 'based', 'on', 'a', '395fb1', 'data', 'sample... | [-0.08457277918153393, 0.30211596817077535, -0.10619841837407355, 0.13199889032694045, -0.005360029288567603, -0.14405976320683425, 0.06143470174720278, 0.33503072149220053, -0.12765659020364442, -0.1593396659674389, -0.05868593616261413, -0.4435287265971835, 0.0643729110743152, 0.10792007705978383, 0.17900881622751644... |
706.3956 | Long-time tails in freely cooling granular gases | The long-time behavior of the current auto-correlation functions for the
velocity, the shear stress and the heat flux is investigated in freely cooling
granular gases. It is found that the correlation functions for the velocity and
the shear stress have the long-time tails obeying $\tau^{-d/2}$, while the
correlation... | cond-mat.stat-mech cond-mat.soft | the longtime behavior of the current autocorrelation functions for the velocity the shear stress and the heat flux is investigated in freely cooling granular gases it is found that the correlation functions for the velocity and the shear stress have the longtime tails obeying taud2 while the correlation function of hea... | [['the', 'longtime', 'behavior', 'of', 'the', 'current', 'autocorrelation', 'functions', 'for', 'the', 'velocity', 'the', 'shear', 'stress', 'and', 'the', 'heat', 'flux', 'is', 'investigated', 'in', 'freely', 'cooling', 'granular', 'gases', 'it', 'is', 'found', 'that', 'the', 'correlation', 'functions', 'for', 'the', '... | [-0.13894277055978135, 0.20360323966991517, -0.0958474792429917, 0.030365619827212104, 0.035089191274657365, -0.07185004597469684, -0.013962219536845242, 0.3262317208272795, -0.2892412259694069, -0.2329464305733, 0.06281858749477373, -0.28913296098189967, -0.02772794562762463, 0.23242727780504333, 0.09019555467911945, ... |
706.3957 | Notes on $\pi_1$ of Smooth Loci of Log Del Pezzo Surfaces | It is known that the fundamental groups of smooth loci of Log del Pezzo
Surfaces are finite groups. The aim of this note is to study these finite
groups. A short table containing these groups is given. And lots of groups on
the table are proved to be fundamental groups.
| math.AG | it is known that the fundamental groups of smooth loci of log del pezzo surfaces are finite groups the aim of this note is to study these finite groups a short table containing these groups is given and lots of groups on the table are proved to be fundamental groups | [['it', 'is', 'known', 'that', 'the', 'fundamental', 'groups', 'of', 'smooth', 'loci', 'of', 'log', 'del', 'pezzo', 'surfaces', 'are', 'finite', 'groups', 'the', 'aim', 'of', 'this', 'note', 'is', 'to', 'study', 'these', 'finite', 'groups', 'a', 'short', 'table', 'containing', 'these', 'groups', 'is', 'given', 'and', '... | [-0.22462055526673794, 0.1093189174681902, -0.12705335136502982, 0.11121564040426164, -0.06954239007551223, -0.13786272614262998, 0.04297654449939728, 0.39528542906045916, -0.28828772431239486, -0.2968080861121416, 0.1403576902952045, -0.27524465769529344, -0.12328362717293202, 0.25099247198551894, -0.18977345338091253... |
706.3958 | Di-jet hadron pair correlation in a hydrodynamical model with a
quenching jet | In jet quenching, a hard QCD parton, before fragmenting into a jet of
hadrons, deposits a fraction of its energy in the medium, leading to suppressed
production of high-$p_T$ hadrons. Assuming that the deposited energy quickly
thermalizes, we simulate the subsequent hydrodynamic evolution of the QGP
fluid. Hydrodynam... | nucl-th | in jet quenching a hard qcd parton before fragmenting into a jet of hadrons deposits a fraction of its energy in the medium leading to suppressed production of highp_t hadrons assuming that the deposited energy quickly thermalizes we simulate the subsequent hydrodynamic evolution of the qgp fluid hydrodynamic evolution... | [['in', 'jet', 'quenching', 'a', 'hard', 'qcd', 'parton', 'before', 'fragmenting', 'into', 'a', 'jet', 'of', 'hadrons', 'deposits', 'a', 'fraction', 'of', 'its', 'energy', 'in', 'the', 'medium', 'leading', 'to', 'suppressed', 'production', 'of', 'highp_t', 'hadrons', 'assuming', 'that', 'the', 'deposited', 'energy', 'q... | [-0.05707590356819652, 0.25921232682923157, -0.23894734205978532, 0.15479238959209574, 0.004570543305367552, -0.011034114586730157, -0.08158639419863942, 0.3764324116130029, -0.22174281014069433, -0.27233545889236754, -0.07265528416140907, -0.32828349443853544, 0.14615085668715094, 0.08613789717101002, 0.09105163454128... |
706.3959 | Self-Similar Dynamics of a Magnetized Polytropic Gas | In broad astrophysical contexts of large-scale gravitational collapses and
outflows and as a basis for various further astrophysical applications, we
formulate and investigate a theoretical problem of self-similar MHD for a
non-rotating polytropic gas of quasi-spherical symmetry permeated by a
completely random magne... | astro-ph | in broad astrophysical contexts of largescale gravitational collapses and outflows and as a basis for various further astrophysical applications we formulate and investigate a theoretical problem of selfsimilar mhd for a nonrotating polytropic gas of quasispherical symmetry permeated by a completely random magnetic fie... | [['in', 'broad', 'astrophysical', 'contexts', 'of', 'largescale', 'gravitational', 'collapses', 'and', 'outflows', 'and', 'as', 'a', 'basis', 'for', 'various', 'further', 'astrophysical', 'applications', 'we', 'formulate', 'and', 'investigate', 'a', 'theoretical', 'problem', 'of', 'selfsimilar', 'mhd', 'for', 'a', 'non... | [-0.19496012386796926, 0.08645575214476792, -0.06722144558335896, 0.11564966008534709, -0.0729206486790989, -0.11484766562388819, -0.005077120395992411, 0.31918867010960483, -0.23801620802822918, -0.2481253265231702, 0.10549760250642477, -0.248557036942582, -0.06466033423813865, 0.2046897262344405, 0.04740314397097458,... |
706.396 | Kaluza-Klein Gluons as a Diagnostic of Warped Models | We study the properties of $g^{1}$, the first excited state of the gluon in
representative variants of the Randall Sundrum model with the Standard Model
fields in the bulk. We find that measurements of the coupling to light quarks
(from the inclusive cross-section for $pp\to g^{1} \to t\bar t$), the coupling
to botto... | hep-ph | we study the properties of g1 the first excited state of the gluon in representative variants of the randall sundrum model with the standard model fields in the bulk we find that measurements of the coupling to light quarks from the inclusive crosssection for ppto g1 to tbar t the coupling to bottom quarks from the rat... | [['we', 'study', 'the', 'properties', 'of', 'g1', 'the', 'first', 'excited', 'state', 'of', 'the', 'gluon', 'in', 'representative', 'variants', 'of', 'the', 'randall', 'sundrum', 'model', 'with', 'the', 'standard', 'model', 'fields', 'in', 'the', 'bulk', 'we', 'find', 'that', 'measurements', 'of', 'the', 'coupling', 't... | [-0.09015951706932332, 0.201377212830658, -0.07456068450537248, 0.1170355720863415, -0.04178144184466547, -0.14193956196212615, 0.042427323706066, 0.31354255333829384, -0.23638194811721452, -0.29739463419581835, 0.0028876681024065385, -0.31490393007795014, -0.02045111579175752, 0.1621312400433593, 0.043597794610720414,... |
706.3961 | Extra dimensions and atomic transition frequencies | New unification theories predict Large Extra Dimensions (LEDs). If that is
the case, gravity would be stronger at short ranges than what Newtonian gravity
predicts. LEDs could also have effects at atomic level. In this paper we
propose a new method to constrain the size of gravity-only LEDs by analyzing
how these LED... | gr-qc | new unification theories predict large extra dimensions leds if that is the case gravity would be stronger at short ranges than what newtonian gravity predicts leds could also have effects at atomic level in this paper we propose a new method to constrain the size of gravityonly leds by analyzing how these leds modify ... | [['new', 'unification', 'theories', 'predict', 'large', 'extra', 'dimensions', 'leds', 'if', 'that', 'is', 'the', 'case', 'gravity', 'would', 'be', 'stronger', 'at', 'short', 'ranges', 'than', 'what', 'newtonian', 'gravity', 'predicts', 'leds', 'could', 'also', 'have', 'effects', 'at', 'atomic', 'level', 'in', 'this', ... | [-0.05566154659697504, 0.20213655508264447, -0.04810037637750308, 0.09823433867034813, -0.061666707180891976, -0.16886448102128326, 0.06942124010670478, 0.3493838518745068, -0.18121993220340687, -0.3722715955848495, 0.046560855298726396, -0.2724097253274963, -0.06804262284986731, 0.18745842991241565, -0.050539731561686... |
706.3962 | Quantum measurement, detection and locality | According to Bell's theorem, local realism is incompatible with quantum
theory. However, it depends on an implied assumption about quantum measurement.
We suggest that the assumption might be removed by a detailed quantum analysis
of the interaction between the measured system and measuring apparatus using
Born's sta... | quant-ph | according to bells theorem local realism is incompatible with quantum theory however it depends on an implied assumption about quantum measurement we suggest that the assumption might be removed by a detailed quantum analysis of the interaction between the measured system and measuring apparatus using borns statistical... | [['according', 'to', 'bells', 'theorem', 'local', 'realism', 'is', 'incompatible', 'with', 'quantum', 'theory', 'however', 'it', 'depends', 'on', 'an', 'implied', 'assumption', 'about', 'quantum', 'measurement', 'we', 'suggest', 'that', 'the', 'assumption', 'might', 'be', 'removed', 'by', 'a', 'detailed', 'quantum', 'a... | [-0.08491716685091864, 0.11784533246975139, -0.1602168060687026, 0.1011769039279345, -0.07669525570530869, -0.19356828755286487, 0.06159694158159715, 0.2933001469915049, -0.2476466815189062, -0.3449180598453253, 0.05833360940052927, -0.27854115761156323, -0.1515170763588593, 0.2086252702659444, -0.05582177747170665, 0.... |
706.3963 | Carbonates in space - The challenge of low temperature data | Carbonates have repeatedly been discussed as possible carriers of stardust
emission bands. However, the band assignments proposed so far were mainly based
on room temperature powder transmission spectra of the respective minerals.
Since very cold calcite grains have been claimed to be present in protostars
and in Pla... | astro-ph | carbonates have repeatedly been discussed as possible carriers of stardust emission bands however the band assignments proposed so far were mainly based on room temperature powder transmission spectra of the respective minerals since very cold calcite grains have been claimed to be present in protostars and in planetar... | [['carbonates', 'have', 'repeatedly', 'been', 'discussed', 'as', 'possible', 'carriers', 'of', 'stardust', 'emission', 'bands', 'however', 'the', 'band', 'assignments', 'proposed', 'so', 'far', 'were', 'mainly', 'based', 'on', 'room', 'temperature', 'powder', 'transmission', 'spectra', 'of', 'the', 'respective', 'miner... | [-0.025336933400819207, 0.14500379831887783, -0.02161019841887425, 0.010923700856999207, -0.0245569520112541, -0.09913221991394834, 0.07444376150460401, 0.4667093429883076, -0.21785159515592542, -0.34864545048601586, 0.0895192646871823, -0.3313548125656237, -0.05332008712166161, 0.1846937922072892, -0.00533652827411951... |
706.3964 | Coxeter polytopes with a unique pair of non-intersecting facets | We consider compact hyperbolic Coxeter polytopes whose Coxeter diagram
contains a unique dotted edge. We prove that such a polytope in d-dimensional
hyperbolic space has at most d+3 facets. In view of results of Lann\'er,
Kaplinskaja, Esselmann, and the second author, this implies that compact
hyperbolic Coxeter poly... | math.MG math.CO math.GR | we consider compact hyperbolic coxeter polytopes whose coxeter diagram contains a unique dotted edge we prove that such a polytope in ddimensional hyperbolic space has at most d3 facets in view of results of lanner kaplinskaja esselmann and the second author this implies that compact hyperbolic coxeter polytopes with a... | [['we', 'consider', 'compact', 'hyperbolic', 'coxeter', 'polytopes', 'whose', 'coxeter', 'diagram', 'contains', 'a', 'unique', 'dotted', 'edge', 'we', 'prove', 'that', 'such', 'a', 'polytope', 'in', 'ddimensional', 'hyperbolic', 'space', 'has', 'at', 'most', 'd3', 'facets', 'in', 'view', 'of', 'results', 'of', 'lanner'... | [-0.1611525094246163, 0.15421078398888793, -0.05207812159513945, 0.018707025979357937, -0.11217318103059798, -0.17177252154386438, 0.0028378936164218057, 0.36021200364099487, -0.2776529985045165, -0.19950762119911172, 0.1059165062958046, -0.3565643355113399, -0.16026104052605875, 0.13336449420689056, -0.187611738394480... |
706.3965 | Unambiguous symmetry assignment for the top valence band of ZnO by
magneto-optical studies of the free A-exciton state | We studied the circular polarization and angular dependences of the
magneto-photoluminescence spectra of the free A-exciton 1S state in wurtzite
ZnO at T = 5 K. The circular polarization properties of the spectra clearly
indicate that the top valence band has Gamma_7 symmetry. The out-of-plane
component of the magnet... | cond-mat.mtrl-sci | we studied the circular polarization and angular dependences of the magnetophotoluminescence spectra of the free aexciton 1s state in wurtzite zno at t 5 k the circular polarization properties of the spectra clearly indicate that the top valence band has gamma_7 symmetry the outofplane component of the magnetic field w... | [['we', 'studied', 'the', 'circular', 'polarization', 'and', 'angular', 'dependences', 'of', 'the', 'magnetophotoluminescence', 'spectra', 'of', 'the', 'free', 'aexciton', '1s', 'state', 'in', 'wurtzite', 'zno', 'at', 't', '5', 'k', 'the', 'circular', 'polarization', 'properties', 'of', 'the', 'spectra', 'clearly', 'in... | [-0.1894491413368447, 0.24255613963313327, -0.013414646510385198, -0.009599944468274122, -0.023925020995706616, -0.13832732727105665, 0.04756575924837685, 0.43810175750220176, -0.27855272325548797, -0.27384262722870795, -0.046992198463833644, -0.28990060825011515, 0.02289581117174118, 0.11188417718293939, 0.14015946650... |
706.3966 | A double-slit `which-way' experiment on the complementarity--uncertainty
debate | A which-way measurement in Young's double-slit will destroy the interference
pattern. Bohr claimed this complementarity between wave- and particle behaviour
is enforced by Heisenberg's uncertainty principle: distinguishing two positions
a distance s apart transfers a random momentum q \sim \hbar/s to the particle.
Th... | quant-ph | a whichway measurement in youngs doubleslit will destroy the interference pattern bohr claimed this complementarity between wave and particle behaviour is enforced by heisenbergs uncertainty principle distinguishing two positions a distance s apart transfers a random momentum q sim hbars to the particle this claim has ... | [['a', 'whichway', 'measurement', 'in', 'youngs', 'doubleslit', 'will', 'destroy', 'the', 'interference', 'pattern', 'bohr', 'claimed', 'this', 'complementarity', 'between', 'wave', 'and', 'particle', 'behaviour', 'is', 'enforced', 'by', 'heisenbergs', 'uncertainty', 'principle', 'distinguishing', 'two', 'positions', '... | [-0.15014223338832625, 0.1649104388540282, -0.12813720887354693, 0.10070127166784172, -0.09640521685271955, -0.17097341669566868, 0.09336267264086377, 0.35203574031215756, -0.25443153329068374, -0.30555667555225746, -0.0006512176155449212, -0.2991108478461744, -0.07805440400750573, 0.1282538480825816, -0.12183126300072... |
706.3967 | Revisiting Rotational Perturbations and the Microwave Background | We consider general-relativistic rotational perturbations in homogeneous and
isotropic Friedman - Robertson - Walker (FRW) cosmologies. Taking linear
perturbations of FRW models, the general solution of the field equations
contains tensorial, vectorial and scalar functions. The vectorial terms are in
connection with ... | astro-ph | we consider generalrelativistic rotational perturbations in homogeneous and isotropic friedman robertson walker frw cosmologies taking linear perturbations of frw models the general solution of the field equations contains tensorial vectorial and scalar functions the vectorial terms are in connection with rotations in ... | [['we', 'consider', 'generalrelativistic', 'rotational', 'perturbations', 'in', 'homogeneous', 'and', 'isotropic', 'friedman', 'robertson', 'walker', 'frw', 'cosmologies', 'taking', 'linear', 'perturbations', 'of', 'frw', 'models', 'the', 'general', 'solution', 'of', 'the', 'field', 'equations', 'contains', 'tensorial'... | [-0.1582451283150623, 0.12406553481076468, -0.08082574450020348, 0.058672954769234266, -0.08149021277204156, -0.07191899467499986, -0.09919580753457041, 0.3082303830572674, -0.2304151709281629, -0.2822093201703542, 0.07285862033060121, -0.2854778865923084, -0.0978146591062297, 0.12747607709118916, 0.011673012790420363,... |
706.3968 | Multiscale inference about a density | We introduce a multiscale test statistic based on local order statistics and
spacings that provides simultaneous confidence statements for the existence and
location of local increases and decreases of a density or a failure rate. The
procedure provides guaranteed finite-sample significance levels, is easy to
impleme... | math.ST stat.TH | we introduce a multiscale test statistic based on local order statistics and spacings that provides simultaneous confidence statements for the existence and location of local increases and decreases of a density or a failure rate the procedure provides guaranteed finitesample significance levels is easy to implement an... | [['we', 'introduce', 'a', 'multiscale', 'test', 'statistic', 'based', 'on', 'local', 'order', 'statistics', 'and', 'spacings', 'that', 'provides', 'simultaneous', 'confidence', 'statements', 'for', 'the', 'existence', 'and', 'location', 'of', 'local', 'increases', 'and', 'decreases', 'of', 'a', 'density', 'or', 'a', 'f... | [-0.1589031915559813, 0.008264898559664962, -0.14808962060380038, 0.13556638002369759, -0.07090165100439831, -0.13997258817673558, 0.15616478625236563, 0.3653157741452257, -0.1907356562161887, -0.31092427196671013, 0.12404778250924277, -0.20734334681872968, -0.12084375377485736, 0.13081619788081972, -0.0701138356321111... |
706.3969 | Passage Times for Polymer Translocation Pulled through a Narrow Pore | We study the passage times of a translocating polymer of length $N$ in three
dimensions, while it is pulled through a narrow pore with a constant force $F$
applied to one end of the polymer. At small to moderate forces, satisfying the
condition $FN^{\nu}/k_BT\lesssim1$, where $\nu\approx0.588$ is the Flory
exponent f... | cond-mat.soft cond-mat.stat-mech physics.bio-ph q-bio.BM | we study the passage times of a translocating polymer of length n in three dimensions while it is pulled through a narrow pore with a constant force f applied to one end of the polymer at small to moderate forces satisfying the condition fnnuk_btlesssim1 where nuapprox0588 is the flory exponent for the polymer we find ... | [['we', 'study', 'the', 'passage', 'times', 'of', 'a', 'translocating', 'polymer', 'of', 'length', 'n', 'in', 'three', 'dimensions', 'while', 'it', 'is', 'pulled', 'through', 'a', 'narrow', 'pore', 'with', 'a', 'constant', 'force', 'f', 'applied', 'to', 'one', 'end', 'of', 'the', 'polymer', 'at', 'small', 'to', 'modera... | [-0.13727007032930852, 0.20160884853452443, -0.08123164631798864, -0.02887035652063787, 0.026426452187355606, -0.13871450963616372, 0.03022493689879775, 0.3760370825845748, -0.300056220293045, -0.2545863189264201, 0.04724089628085494, -0.2561748072654009, -0.09289176713116468, 0.15376952271908523, 0.023131900881417096,... |
706.397 | Raynaud vector bundles | We construct vector bundles $R^r_\mu$ on a smooth projective curve $X$ having
the property that for all sheaves $E$ of slope $\mu$ and rank $r$ on $X$ we
have an equivalence: $E$ is a semistable vector bundle $\iff$
$Hom(R^r_\mu,E)=0$.
As a byproduct of our construction we obtain effective bounds on $r$ such
that t... | math.AG | we construct vector bundles rr_mu on a smooth projective curve x having the property that for all sheaves e of slope mu and rank r on x we have an equivalence e is a semistable vector bundle iff homrr_mue0 as a byproduct of our construction we obtain effective bounds on r such that the linear system r cdot theta has ba... | [['we', 'construct', 'vector', 'bundles', 'rr_mu', 'on', 'a', 'smooth', 'projective', 'curve', 'x', 'having', 'the', 'property', 'that', 'for', 'all', 'sheaves', 'e', 'of', 'slope', 'mu', 'and', 'rank', 'r', 'on', 'x', 'we', 'have', 'an', 'equivalence', 'e', 'is', 'a', 'semistable', 'vector', 'bundle', 'iff', 'homrr_mu... | [-0.2435337446804624, 0.046334027724924454, -0.11583106065518223, 0.000641600485323579, -0.08187484041263815, -0.1690998674966977, 0.041974258550908417, 0.3835666411323473, -0.2927014186279848, -0.15232820974779315, 0.08912231166323181, -0.26119314960669726, -0.13060845088330097, 0.20602820441126823, -0.101957674145523... |
706.3971 | On the L^p-distorsion of finite quotients of amenable groups | We study the L^p-distortion of finite quotients of amenable groups. In
particular, for every number p larger or equal than 2, we prove that the
l^p-distortion of the finite lamplighter group grows like (\log n)^{1/p}. We
also give the asymptotic behavior of the l^p-distortion of finite quotients of
certain metabelian... | math.MG | we study the lpdistortion of finite quotients of amenable groups in particular for every number p larger or equal than 2 we prove that the lpdistortion of the finite lamplighter group grows like log n1p we also give the asymptotic behavior of the lpdistortion of finite quotients of certain metabelian polycyclic groups ... | [['we', 'study', 'the', 'lpdistortion', 'of', 'finite', 'quotients', 'of', 'amenable', 'groups', 'in', 'particular', 'for', 'every', 'number', 'p', 'larger', 'or', 'equal', 'than', '2', 'we', 'prove', 'that', 'the', 'lpdistortion', 'of', 'the', 'finite', 'lamplighter', 'group', 'grows', 'like', 'log', 'n1p', 'we', 'als... | [-0.17488578267057164, 0.19521340962091926, -0.10942618941771798, 0.10246592815383337, -0.07567334780469537, -0.14082137077639345, 0.03254508193640504, 0.365836646000389, -0.28866437503893394, -0.20620954854530282, 0.13674537306178536, -0.2992188321222784, -0.08880624003813864, 0.21945654865339748, -0.08772452203265857... |
706.3972 | XMM-Newton observation of the persistent Be/neutron-star system X Persei
at a high-luminosity level | We report on the XMM-Newton observation of the HMXRB X Persei, the prototype
of the persistent and low-luminosity Be/neutron star pulsars, which was
performed on February 2003. The source was detected at a luminosity level of ~
1.4x10^35 erg/s, which is the highest level of the latest three decades. The
pulsation per... | astro-ph | we report on the xmmnewton observation of the hmxrb x persei the prototype of the persistent and lowluminosity beneutron star pulsars which was performed on february 2003 the source was detected at a luminosity level of 14x1035 ergs which is the highest level of the latest three decades the pulsation period has increas... | [['we', 'report', 'on', 'the', 'xmmnewton', 'observation', 'of', 'the', 'hmxrb', 'x', 'persei', 'the', 'prototype', 'of', 'the', 'persistent', 'and', 'lowluminosity', 'beneutron', 'star', 'pulsars', 'which', 'was', 'performed', 'on', 'february', '2003', 'the', 'source', 'was', 'detected', 'at', 'a', 'luminosity', 'leve... | [-0.10517294234539057, 0.1325562506359916, -0.08864112914699855, 0.05548626576347471, -0.07907137014200351, -0.10462734967390178, 0.06556227270433782, 0.4271943345437386, -0.18787529777758327, -0.37603288078737773, 0.08905470053496788, -0.32165329745810683, 0.013477976355370295, 0.22028832053594247, -0.0149788695308622... |
706.3973 | Whitehead-Torsion und Faserungen | This work treats on the question whether a given map f: M -> B of smooth
closed manifolds is homotopic to a smooth fiber bundle. We define a first
obstruction in H^1(B;Wh(\pi_1(E))) and, provided that this obstruction vanishes
and one additional condition is verified, a second obstruction in Wh(\pi_1(E))
>. Both elem... | math.GT | this work treats on the question whether a given map f m b of smooth closed manifolds is homotopic to a smooth fiber bundle we define a first obstruction in h1bwhpi_1e and provided that this obstruction vanishes and one additional condition is verified a second obstruction in whpi_1e both elements vanish if the answer ... | [['this', 'work', 'treats', 'on', 'the', 'question', 'whether', 'a', 'given', 'map', 'f', 'm', 'b', 'of', 'smooth', 'closed', 'manifolds', 'is', 'homotopic', 'to', 'a', 'smooth', 'fiber', 'bundle', 'we', 'define', 'a', 'first', 'obstruction', 'in', 'h1bwhpi_1e', 'and', 'provided', 'that', 'this', 'obstruction', 'vanish... | [-0.20283967017770765, 0.07903467355286108, -0.052708429849131946, 0.07469483241785635, -0.07319847241717767, -0.1845658036256011, 0.026041827595574742, 0.3291383971697948, -0.28000756713284297, -0.23203864355789536, 0.09449882246058514, -0.2456705536138504, -0.20868660948496867, 0.1581630920087225, -0.1322877467709018... |
706.3974 | Kinetic and hydrodynamic models of chemotactic aggregation | We derive general kinetic and hydrodynamic models of chemotactic aggregation
that describe certain features of the morphogenesis of biological colonies
(like bacteria, amoebae, endothelial cells or social insects). Starting from a
stochastic model defined in terms of N coupled Langevin equations, we derive a
nonlinea... | physics.bio-ph | we derive general kinetic and hydrodynamic models of chemotactic aggregation that describe certain features of the morphogenesis of biological colonies like bacteria amoebae endothelial cells or social insects starting from a stochastic model defined in terms of n coupled langevin equations we derive a nonlinear mean f... | [['we', 'derive', 'general', 'kinetic', 'and', 'hydrodynamic', 'models', 'of', 'chemotactic', 'aggregation', 'that', 'describe', 'certain', 'features', 'of', 'the', 'morphogenesis', 'of', 'biological', 'colonies', 'like', 'bacteria', 'amoebae', 'endothelial', 'cells', 'or', 'social', 'insects', 'starting', 'from', 'a',... | [-0.13135801148959078, 0.11150230919010937, -0.09754723587001746, 0.08714615567945518, -0.05381962593812018, -0.10010898807205451, -0.006429474850973257, 0.25115299987582823, -0.27801328213909304, -0.25579125358758925, 0.02488471973203839, -0.251612578633313, -0.2263162471473408, 0.12864394321416814, -0.014111306210263... |
706.3975 | Hierarchical Spatial Organization of Geographical Networks | In this work we propose the use of a hirarchical extension of the
polygonality index as a means to characterize and model geographical networks:
each node is associated with the spatial position of the nodes, while the edges
of the network are defined by progressive connectivity adjacencies. Through the
analysis of s... | physics.soc-ph | in this work we propose the use of a hirarchical extension of the polygonality index as a means to characterize and model geographical networks each node is associated with the spatial position of the nodes while the edges of the network are defined by progressive connectivity adjacencies through the analysis of such n... | [['in', 'this', 'work', 'we', 'propose', 'the', 'use', 'of', 'a', 'hirarchical', 'extension', 'of', 'the', 'polygonality', 'index', 'as', 'a', 'means', 'to', 'characterize', 'and', 'model', 'geographical', 'networks', 'each', 'node', 'is', 'associated', 'with', 'the', 'spatial', 'position', 'of', 'the', 'nodes', 'while... | [-0.13464872799291203, 0.03283262777734886, -0.050747692987153474, 0.03933777579963631, -0.05122051146728071, -0.11598611551612108, 0.05522929137739332, 0.3890550479462201, -0.28007046337006614, -0.31056357712540456, 0.11628322540755934, -0.27377087478949264, -0.24341643225422807, 0.13097012734876692, -0.06292977766398... |
706.3976 | Towards an Experimental Test of Gravity-induced Quantum State Reduction | According to the hypothesis of Penrose and Diosi, quantum state reduction is
a manifestation of the incompatibilty of general relativity and the unitary
time evolution of quantum physics. Dimensional analysis suggests that
Schrodinger cat type states should collapse on measurable time scales when
masses and lengths o... | cond-mat.str-el cond-mat.other quant-ph | according to the hypothesis of penrose and diosi quantum state reduction is a manifestation of the incompatibilty of general relativity and the unitary time evolution of quantum physics dimensional analysis suggests that schrodinger cat type states should collapse on measurable time scales when masses and lengths of th... | [['according', 'to', 'the', 'hypothesis', 'of', 'penrose', 'and', 'diosi', 'quantum', 'state', 'reduction', 'is', 'a', 'manifestation', 'of', 'the', 'incompatibilty', 'of', 'general', 'relativity', 'and', 'the', 'unitary', 'time', 'evolution', 'of', 'quantum', 'physics', 'dimensional', 'analysis', 'suggests', 'that', '... | [-0.13538202236763983, 0.21918618224505065, -0.06776457697604642, 0.08224844973330912, -0.02433872538985628, -0.1321573486890305, 0.03818884018468765, 0.32946127051290014, -0.24878158550615412, -0.3064417474305803, 0.057008689588683686, -0.2583821423991461, -0.08181003529244488, 0.1869132228470831, -0.01044092352756045... |
706.3977 | Multipolar expansion of the electrostatic interaction between charged
colloids at interfaces | The general form of the electrostatic potential around an arbitrarily charged
colloid at an interface between a dielectric and a screening phase (such as air
and water, respectively) is analyzed in terms of a multipole expansion. The
leading term is isotropic in the interfacial plane and varies with $d^{-3}$
where $d... | cond-mat.soft | the general form of the electrostatic potential around an arbitrarily charged colloid at an interface between a dielectric and a screening phase such as air and water respectively is analyzed in terms of a multipole expansion the leading term is isotropic in the interfacial plane and varies with d3 where d is the inpla... | [['the', 'general', 'form', 'of', 'the', 'electrostatic', 'potential', 'around', 'an', 'arbitrarily', 'charged', 'colloid', 'at', 'an', 'interface', 'between', 'a', 'dielectric', 'and', 'a', 'screening', 'phase', 'such', 'as', 'air', 'and', 'water', 'respectively', 'is', 'analyzed', 'in', 'terms', 'of', 'a', 'multipole... | [-0.17331483540115783, 0.20443817399909034, -0.004197534926310934, 0.028938664316265572, 0.02595685545656115, -0.1686123602910701, -0.043913516874490965, 0.3573806602131538, -0.24522197488319092, -0.2968836981953696, -0.009506628916815224, -0.3609430491924286, -0.12506949980837304, 0.11709174327787501, 0.09206974174653... |
706.3978 | Holographic heavy-light mesons from non-Abelian DBI | In the context of gauge/gravity duals with flavor, we examine heavy-light
mesons which involve a heavy and a light quark. For this purpose we embed two
D7 brane probes at different positions into the gravity background. We
establish the non-Abelian Dirac-Born-Infeld (DBI) action for these probes, in
which the U(2) ma... | hep-th | in the context of gaugegravity duals with flavor we examine heavylight mesons which involve a heavy and a light quark for this purpose we embed two d7 brane probes at different positions into the gravity background we establish the nonabelian diracborninfeld dbi action for these probes in which the u2 matrix describing... | [['in', 'the', 'context', 'of', 'gaugegravity', 'duals', 'with', 'flavor', 'we', 'examine', 'heavylight', 'mesons', 'which', 'involve', 'a', 'heavy', 'and', 'a', 'light', 'quark', 'for', 'this', 'purpose', 'we', 'embed', 'two', 'd7', 'brane', 'probes', 'at', 'different', 'positions', 'into', 'the', 'gravity', 'backgrou... | [-0.09658244794905733, 0.2998797803405015, -0.05397351741489461, 0.1468855161630713, -0.03434810384094496, -0.1643815639117212, -0.0159300661933444, 0.29764225472257855, -0.15147984926314914, -0.184681277598857, -0.02686754809024826, -0.345105801243335, -0.019100192496005225, 0.02784184387522092, 0.055931935319676995, ... |
706.3979 | The informational model - possible tests | In our previous arXiv papers (more systematically the informational
conception is presented in the paper "The Information as Absolute", 2010) it
was rigorously shown that Matter in our Universe - and Universe as a whole -
are some informational systems (structures), which exist as uninterruptedly
transforming [practi... | physics.gen-ph | in our previous arxiv papers more systematically the informational conception is presented in the paper the information as absolute 2010 it was rigorously shown that matter in our universe and universe as a whole are some informational systems structures which exist as uninterruptedly transforming practically infinites... | [['in', 'our', 'previous', 'arxiv', 'papers', 'more', 'systematically', 'the', 'informational', 'conception', 'is', 'presented', 'in', 'the', 'paper', 'the', 'information', 'as', 'absolute', '2010', 'it', 'was', 'rigorously', 'shown', 'that', 'matter', 'in', 'our', 'universe', 'and', 'universe', 'as', 'a', 'whole', 'ar... | [-0.11344225914668171, 0.12797534153346093, -0.1316241642955931, 0.10077077260451212, -0.08455198993605952, -0.11801166539531081, 0.036310814278981376, 0.31751664603850055, -0.2490623951842633, -0.3143915298665243, 0.075099214958027, -0.2466009128059546, -0.17285117251618254, 0.2023845329820629, -0.08294525717520305, 0... |
706.398 | Fluctuation Propagator and Heavy Quark Diffusion | The quark fluctuation propagator is evaluated. It defines the diffusion
coefficient in the vicinity of the phase transition and the gradient term in
the Ginzburg-Landau functional.
| hep-ph | the quark fluctuation propagator is evaluated it defines the diffusion coefficient in the vicinity of the phase transition and the gradient term in the ginzburglandau functional | [['the', 'quark', 'fluctuation', 'propagator', 'is', 'evaluated', 'it', 'defines', 'the', 'diffusion', 'coefficient', 'in', 'the', 'vicinity', 'of', 'the', 'phase', 'transition', 'and', 'the', 'gradient', 'term', 'in', 'the', 'ginzburglandau', 'functional']] | [-0.17730477217656487, 0.16824028139504102, -0.14084264858124348, 0.0831834751029069, -0.03375540616420599, -0.02461715801977194, 0.05543701035472063, 0.2795684084009666, -0.2893876556593638, -0.19599689872792134, 0.03719619202176826, -0.34587634813327056, -0.16874859181161111, 0.05400085305938354, 0.07380349497095896,... |
706.3981 | On the Greenfield-Wallach and Katok conjectures | We survey recent progress on the Greenfield-Wallach and Katok conjectures on
globally hypoelliptic and cohomology free vector fields and derive a proof of
the conjectures in dimension three. The argument is primarily based on recent
work of F. and J. Rodriguez Hertz which allows us to reduce the question to the
case ... | math.DS | we survey recent progress on the greenfieldwallach and katok conjectures on globally hypoelliptic and cohomology free vector fields and derive a proof of the conjectures in dimension three the argument is primarily based on recent work of f and j rodriguez hertz which allows us to reduce the question to the case of a r... | [['we', 'survey', 'recent', 'progress', 'on', 'the', 'greenfieldwallach', 'and', 'katok', 'conjectures', 'on', 'globally', 'hypoelliptic', 'and', 'cohomology', 'free', 'vector', 'fields', 'and', 'derive', 'a', 'proof', 'of', 'the', 'conjectures', 'in', 'dimension', 'three', 'the', 'argument', 'is', 'primarily', 'based'... | [-0.17172016837186627, 0.04713425861199858, -0.10677342864914567, 0.00841092207323905, -0.1274132101264383, -0.14954466772471348, 0.02735136998681255, 0.2659060319571139, -0.21382310574378383, -0.31228527267064365, 0.12038556131830608, -0.23945998748807484, -0.1626891727716505, 0.2240594746696146, -0.11561518703139835,... |
706.3982 | Lorentz anomaly in the semi-light-cone gauge superstrings | We study the Lorentz invariance of D=4 and 6 superstrings in the
double-spinor formalism, which are equivalent to the D=4 and 6 superstrings in
the pure-spinor formalism in the sense of the BRST cohomology. We first
re-examine how the conformal and Lorentz anomalies appear in the D=4 and 6
Green-Schwarz superstrings ... | hep-th | we study the lorentz invariance of d4 and 6 superstrings in the doublespinor formalism which are equivalent to the d4 and 6 superstrings in the purespinor formalism in the sense of the brst cohomology we first reexamine how the conformal and lorentz anomalies appear in the d4 and 6 greenschwarz superstrings in the semi... | [['we', 'study', 'the', 'lorentz', 'invariance', 'of', 'd4', 'and', '6', 'superstrings', 'in', 'the', 'doublespinor', 'formalism', 'which', 'are', 'equivalent', 'to', 'the', 'd4', 'and', '6', 'superstrings', 'in', 'the', 'purespinor', 'formalism', 'in', 'the', 'sense', 'of', 'the', 'brst', 'cohomology', 'we', 'first', ... | [-0.16202731419616612, 0.18130628819926642, -0.04502037509519141, 0.12549315067735733, -0.07308823711355217, -0.10719033360146568, -0.020255498361620994, 0.3437407702076598, -0.19044018838030752, -0.24724525137935416, 0.053907711934698455, -0.22484089284444053, -0.2187150851059414, 0.07946552720477484, -0.0950389818754... |
706.3983 | Social applications of two-dimensional Ising models | I review three socio-economic models of economic opinions, urban segregation,
and language change and show that the well known two-dimensional Ising model
gives about the same results in each case.
| physics.soc-ph | i review three socioeconomic models of economic opinions urban segregation and language change and show that the well known twodimensional ising model gives about the same results in each case | [['i', 'review', 'three', 'socioeconomic', 'models', 'of', 'economic', 'opinions', 'urban', 'segregation', 'and', 'language', 'change', 'and', 'show', 'that', 'the', 'well', 'known', 'twodimensional', 'ising', 'model', 'gives', 'about', 'the', 'same', 'results', 'in', 'each', 'case']] | [-0.054060543219869334, 0.09388747548994919, -0.027171549449364344, 0.11603644561643402, -0.05897875148802996, -0.16915021582196157, -0.0008813345591382434, 0.3631414600958427, -0.19905446854730446, -0.3036147547264894, 0.05711790988765036, -0.30040603975454966, -0.2420379767815272, 0.13552699268329887, -0.077291174729... |
706.3984 | A Comparison of Push and Pull Techniques for Ajax | Ajax applications are designed to have high user interactivity and low
user-perceived latency. Real-time dynamic web data such as news headlines,
stock tickers, and auction updates need to be propagated to the users as soon
as possible. However, Ajax still suffers from the limitations of the Web's
request/response ar... | cs.SE cs.PF | ajax applications are designed to have high user interactivity and low userperceived latency realtime dynamic web data such as news headlines stock tickers and auction updates need to be propagated to the users as soon as possible however ajax still suffers from the limitations of the webs requestresponse architecture ... | [['ajax', 'applications', 'are', 'designed', 'to', 'have', 'high', 'user', 'interactivity', 'and', 'low', 'userperceived', 'latency', 'realtime', 'dynamic', 'web', 'data', 'such', 'as', 'news', 'headlines', 'stock', 'tickers', 'and', 'auction', 'updates', 'need', 'to', 'be', 'propagated', 'to', 'the', 'users', 'as', 's... | [-0.11732904364827038, 0.017904241041530138, -0.04278205699584861, 0.06942281112990006, -0.17399682433622526, -0.20428552457209057, 0.16872765960821803, 0.38924233072126907, -0.3399891930425333, -0.33590595121495426, 0.1717752224325927, -0.31375357930503217, -0.10913095265601037, 0.18975820251216646, -0.133290809992710... |
706.3985 | Distributions associated with general runs and patterns in hidden Markov
models | This paper gives a method for computing distributions associated with
patterns in the state sequence of a hidden Markov model, conditional on
observing all or part of the observation sequence. Probabilities are computed
for very general classes of patterns (competing patterns and generalized later
patterns), and thus... | stat.ME stat.AP stat.CO | this paper gives a method for computing distributions associated with patterns in the state sequence of a hidden markov model conditional on observing all or part of the observation sequence probabilities are computed for very general classes of patterns competing patterns and generalized later patterns and thus the th... | [['this', 'paper', 'gives', 'a', 'method', 'for', 'computing', 'distributions', 'associated', 'with', 'patterns', 'in', 'the', 'state', 'sequence', 'of', 'a', 'hidden', 'markov', 'model', 'conditional', 'on', 'observing', 'all', 'or', 'part', 'of', 'the', 'observation', 'sequence', 'probabilities', 'are', 'computed', '... | [-0.06252350902254535, 0.10453453397809537, -0.0723432999256314, 0.08875165873390882, -0.0924502532568057, -0.10762200550157197, 0.025689432599429726, 0.3741698386907882, -0.2860487141697129, -0.3042568549336422, 0.13507910560322356, -0.2410914660415606, -0.1688836008242211, 0.23085996040561219, -0.060825250342767055, ... |
706.3986 | Positivity of Some Integral Transforms, and Generalization of Bochner's
Theorem on Functions of Positive Type | Using the integral representations of the solutions of Schr\"odinger
equation, which are the essential ingredients of the Gel'fand-Levitan and
Marchenko integral equations of inverse scattering theory, we obtain a general
theorem on the positivity of some integral transforms, and extend the theorem
of Bochner on Four... | math-ph math.MP | using the integral representations of the solutions of schrodinger equation which are the essential ingredients of the gelfandlevitan and marchenko integral equations of inverse scattering theory we obtain a general theorem on the positivity of some integral transforms and extend the theorem of bochner on fourier trans... | [['using', 'the', 'integral', 'representations', 'of', 'the', 'solutions', 'of', 'schrodinger', 'equation', 'which', 'are', 'the', 'essential', 'ingredients', 'of', 'the', 'gelfandlevitan', 'and', 'marchenko', 'integral', 'equations', 'of', 'inverse', 'scattering', 'theory', 'we', 'obtain', 'a', 'general', 'theorem', '... | [-0.1063159492900013, 0.024680286913644524, -0.1772241927916184, 0.12261215537582756, -0.13383296206593515, -0.07782457423163577, -0.011137628472351935, 0.2783334319712594, -0.3092207921203226, -0.16323696303879842, 0.16058792251860723, -0.2863656686153263, -0.16711034530308097, 0.22861637736205012, -0.0282884785439819... |
706.3987 | Exciting the quark-gluon plasma with a relativistic jet | We discuss the properties of a system composed by a static plasma traversed
by a jet of particles. Assuming that both the jet and the plasma can be
described using a hydrodynamical approach, and in the conformal limit, we find
that unstable modes arise when the velocity of the jet is larger than the speed
of the soun... | hep-ph | we discuss the properties of a system composed by a static plasma traversed by a jet of particles assuming that both the jet and the plasma can be described using a hydrodynamical approach and in the conformal limit we find that unstable modes arise when the velocity of the jet is larger than the speed of the sound of ... | [['we', 'discuss', 'the', 'properties', 'of', 'a', 'system', 'composed', 'by', 'a', 'static', 'plasma', 'traversed', 'by', 'a', 'jet', 'of', 'particles', 'assuming', 'that', 'both', 'the', 'jet', 'and', 'the', 'plasma', 'can', 'be', 'described', 'using', 'a', 'hydrodynamical', 'approach', 'and', 'in', 'the', 'conformal... | [-0.1521805831270486, 0.25736103936075083, -0.12613018589735323, 0.05963165316633977, -0.04966998182829808, -0.08627487353484642, -0.023959334782481967, 0.3519185432172441, -0.23358764421488099, -0.2623669813665283, 0.03566271395727919, -0.24847707401525665, 0.0001262534778661929, 0.2059251893208836, 0.0369261846145881... |
706.3988 | 5-dimensional solution with acceleration and small variation of G | A 5-dimensional cosmological solution in the model with two 2-forms and two
``phantom'' scalar fields is considered. The model contains two dilatonic
coupling vectors obeying certain restrictions. It is shown that there exists a
time interval where accelerating expansion of ``our'' 3-dimensional space is
compatible w... | gr-qc astro-ph | a 5dimensional cosmological solution in the model with two 2forms and two phantom scalar fields is considered the model contains two dilatonic coupling vectors obeying certain restrictions it is shown that there exists a time interval where accelerating expansion of our 3dimensional space is compatible with a small val... | [['a', '5dimensional', 'cosmological', 'solution', 'in', 'the', 'model', 'with', 'two', '2forms', 'and', 'two', 'phantom', 'scalar', 'fields', 'is', 'considered', 'the', 'model', 'contains', 'two', 'dilatonic', 'coupling', 'vectors', 'obeying', 'certain', 'restrictions', 'it', 'is', 'shown', 'that', 'there', 'exists', ... | [-0.24757489327263707, 0.1746548452377923, -0.03764325219930874, 0.0528133329008361, -0.1245520177245554, -0.19575226438098103, -0.09000875972452815, 0.3335568652729745, -0.19309891643071617, -0.26003248610154345, 0.07571549085615617, -0.2633649282398875, -0.13934551217351798, 0.15883578940863824, 0.03251433681213745, ... |
706.3989 | Hans-Juergen Treder and the discovery of confinement in Einstein's
unified field theory | In the year 1957, when interest in Einstein's unified field theory was fading
away for lack of understanding of its physical content, Treder performed a
momentous critical analysis of the possible definitions of the electric
four-current in the theory. As an outcome of this scrutiny he was able to prove
by the E.I.H.... | physics.hist-ph gr-qc | in the year 1957 when interest in einsteins unified field theory was fading away for lack of understanding of its physical content treder performed a momentous critical analysis of the possible definitions of the electric fourcurrent in the theory as an outcome of this scrutiny he was able to prove by the eih method th... | [['in', 'the', 'year', '1957', 'when', 'interest', 'in', 'einsteins', 'unified', 'field', 'theory', 'was', 'fading', 'away', 'for', 'lack', 'of', 'understanding', 'of', 'its', 'physical', 'content', 'treder', 'performed', 'a', 'momentous', 'critical', 'analysis', 'of', 'the', 'possible', 'definitions', 'of', 'the', 'el... | [-0.09728481378961662, 0.11602465677991725, -0.13862347153523819, 0.0746100450259283, -0.08404765771958259, -0.15063867365744887, 0.045973259464884605, 0.3038132492187988, -0.19685763411582746, -0.31376655767201833, 0.05749772952008702, -0.25421686019158896, -0.13312388832441643, 0.1464568469630674, -0.0834758654834890... |
706.399 | The order completion method for systems of nonlinear PDEs:
Pseudo-topological perspectives | By setting up appropriate uniform convergence structures, we are able to
reformulate the Order Completion Method of Oberguggenberger and Rosinger in a
setting that more closely resembles the usual topological constructions for
solving PDEs. As an application, we obtain existence and uniqueness results for
the solutio... | math.GM | by setting up appropriate uniform convergence structures we are able to reformulate the order completion method of oberguggenberger and rosinger in a setting that more closely resembles the usual topological constructions for solving pdes as an application we obtain existence and uniqueness results for the solutions of... | [['by', 'setting', 'up', 'appropriate', 'uniform', 'convergence', 'structures', 'we', 'are', 'able', 'to', 'reformulate', 'the', 'order', 'completion', 'method', 'of', 'oberguggenberger', 'and', 'rosinger', 'in', 'a', 'setting', 'that', 'more', 'closely', 'resembles', 'the', 'usual', 'topological', 'constructions', 'fo... | [-0.08425521624041721, 0.03069981011823984, -0.07217428409698186, 0.10684819294605404, -0.10599878627806902, -0.11919497604481875, -0.01955069401767105, 0.33693145053461193, -0.2867966336311656, -0.27250451330561193, 0.17708244026405737, -0.24493495620787142, -0.19682657848112284, 0.22023596230894327, -0.08967994883656... |
706.3991 | A Quiver of Many Runaways | We study the quantum corrections to the moduli space of the quiver gauge
theory corresponding to regular and fractional D3-branes at the dP_1
singularity. We find that besides the known runaway behavior at the lowest step
of the duality cascade, there is a runaway direction along a mesonic branch at
every higher step... | hep-th | we study the quantum corrections to the moduli space of the quiver gauge theory corresponding to regular and fractional d3branes at the dp_1 singularity we find that besides the known runaway behavior at the lowest step of the duality cascade there is a runaway direction along a mesonic branch at every higher step of t... | [['we', 'study', 'the', 'quantum', 'corrections', 'to', 'the', 'moduli', 'space', 'of', 'the', 'quiver', 'gauge', 'theory', 'corresponding', 'to', 'regular', 'and', 'fractional', 'd3branes', 'at', 'the', 'dp_1', 'singularity', 'we', 'find', 'that', 'besides', 'the', 'known', 'runaway', 'behavior', 'at', 'the', 'lowest'... | [-0.13461692276537235, 0.1492887296653525, -0.10996112242387032, 0.08815340692303891, -0.0661447315827518, -0.0903178415387685, 0.004229208076499218, 0.306969077107899, -0.2782296253588154, -0.21176107503749705, 0.08397940536788492, -0.28486490386457725, -0.1470318258863789, 0.10549626977723321, -0.01739714895432562, 0... |
706.3992 | Wedge-Local Quantum Fields and Noncommutative Minkowski Space | Within the setting of a recently proposed model of quantum fields on
noncommutative Minkowski spacetime, the consequences of the consistent
application of the proper, untwisted Poincare group as the symmetry group are
investigated. The emergent model contains an infinite family of fields which
are labelled by differe... | hep-th math-ph math.MP | within the setting of a recently proposed model of quantum fields on noncommutative minkowski spacetime the consequences of the consistent application of the proper untwisted poincare group as the symmetry group are investigated the emergent model contains an infinite family of fields which are labelled by different no... | [['within', 'the', 'setting', 'of', 'a', 'recently', 'proposed', 'model', 'of', 'quantum', 'fields', 'on', 'noncommutative', 'minkowski', 'spacetime', 'the', 'consequences', 'of', 'the', 'consistent', 'application', 'of', 'the', 'proper', 'untwisted', 'poincare', 'group', 'as', 'the', 'symmetry', 'group', 'are', 'inves... | [-0.14095752243805776, 0.1644974969779243, -0.0862582655711062, 0.08521862188979183, -0.0851689281579632, -0.13957544571513797, -0.03893186206126198, 0.35541876660497396, -0.25703146030513835, -0.2492905117058814, 0.08711752085087059, -0.2569031811791203, -0.13989290525049172, 0.1636561265655937, -0.05704032042436458, ... |
706.3993 | Quantum Resonances and Ratchets in Free-Falling Frames | Quantum resonance (QR) is defined in the free-falling frame of the quantum
kicked particle subjected to gravity. The general QR conditions are derived.
They imply the rationality of the gravity parameter $\eta$, the kicking-period
parameter $\tau /(2\pi)$, and the quasimomentum $\beta$. Exact results are
obtained con... | nlin.CD | quantum resonance qr is defined in the freefalling frame of the quantum kicked particle subjected to gravity the general qr conditions are derived they imply the rationality of the gravity parameter eta the kickingperiod parameter tau 2pi and the quasimomentum beta exact results are obtained concerning wavepacket evolu... | [['quantum', 'resonance', 'qr', 'is', 'defined', 'in', 'the', 'freefalling', 'frame', 'of', 'the', 'quantum', 'kicked', 'particle', 'subjected', 'to', 'gravity', 'the', 'general', 'qr', 'conditions', 'are', 'derived', 'they', 'imply', 'the', 'rationality', 'of', 'the', 'gravity', 'parameter', 'eta', 'the', 'kickingperi... | [-0.19401967085432262, 0.2094841642341075, -0.08667418517154427, 0.07798460565973073, -0.029391591184629272, -0.20069878042245715, -0.002236690726847603, 0.3428515990766195, -0.2721305294965322, -0.2426969680791864, 0.020954418374010575, -0.22080253320387921, -0.1473836379376455, 0.2076289201558281, -0.0308719528838992... |
706.3994 | Attractor scenarios and superluminal signals in k-essence cosmology | Cosmological scenarios with k-essence are invoked in order to explain the
observed late-time acceleration of the universe. These scenarios avoid the need
for fine-tuned initial conditions (the "coincidence problem") because of the
attractor-like dynamics of the k-essence field \phi. It was recently shown that
all k-e... | gr-qc astro-ph hep-ph hep-th | cosmological scenarios with kessence are invoked in order to explain the observed latetime acceleration of the universe these scenarios avoid the need for finetuned initial conditions the coincidence problem because of the attractorlike dynamics of the kessence field phi it was recently shown that all kessence scenario... | [['cosmological', 'scenarios', 'with', 'kessence', 'are', 'invoked', 'in', 'order', 'to', 'explain', 'the', 'observed', 'latetime', 'acceleration', 'of', 'the', 'universe', 'these', 'scenarios', 'avoid', 'the', 'need', 'for', 'finetuned', 'initial', 'conditions', 'the', 'coincidence', 'problem', 'because', 'of', 'the',... | [-0.1696644978802291, 0.10568499478954663, -0.11813445864193842, 0.13315847725350183, -0.13961593432285055, -0.18586616856123203, -0.044578645535005394, 0.3114007358228304, -0.19559902079321073, -0.2855377184299145, 0.04372155772411465, -0.22351238156735734, -0.12151221145273737, 0.15830038979910674, -0.042839095315468... |
706.3995 | Dynamical instability and dispersion management of an attractive
condensate in an optical lattice | We investigate the stability of an attractive Bose-Einstein condensate in a
moving 1D optical lattice in the presence of transverse confinement. By means
of a Bogoliubov linear stability analysis we find that the system is
dynamically unstable for low quasimomenta and becomes stable near the band
edge, in a specular ... | cond-mat.other | we investigate the stability of an attractive boseeinstein condensate in a moving 1d optical lattice in the presence of transverse confinement by means of a bogoliubov linear stability analysis we find that the system is dynamically unstable for low quasimomenta and becomes stable near the band edge in a specular fashi... | [['we', 'investigate', 'the', 'stability', 'of', 'an', 'attractive', 'boseeinstein', 'condensate', 'in', 'a', 'moving', '1d', 'optical', 'lattice', 'in', 'the', 'presence', 'of', 'transverse', 'confinement', 'by', 'means', 'of', 'a', 'bogoliubov', 'linear', 'stability', 'analysis', 'we', 'find', 'that', 'the', 'system'... | [-0.2112717980940383, 0.2228976468079334, -0.09354949699851343, 0.0565596448510545, 0.004973857838194817, -0.11490980590371272, 0.01818834256566613, 0.3851375134411053, -0.24727607513957012, -0.21465226345473917, 0.0930742522591922, -0.2644599550851406, -0.08945037272552817, 0.1301165734140131, 0.030838894163025543, 0.... |
706.3996 | Phase transitions in higher derivative gravity and gauge theory:
R-charged black holes | This is a continuation of our earlier work where we constructed a
phenomenologically motivated effective action of the boundary gauge theory at
finite temperature and finite gauge coupling on $S^3 \times S^1$. In this
paper, we argue that this effective action qualitatively reproduces the gauge
theory representing va... | hep-th | this is a continuation of our earlier work where we constructed a phenomenologically motivated effective action of the boundary gauge theory at finite temperature and finite gauge coupling on s3 times s1 in this paper we argue that this effective action qualitatively reproduces the gauge theory representing various bul... | [['this', 'is', 'a', 'continuation', 'of', 'our', 'earlier', 'work', 'where', 'we', 'constructed', 'a', 'phenomenologically', 'motivated', 'effective', 'action', 'of', 'the', 'boundary', 'gauge', 'theory', 'at', 'finite', 'temperature', 'and', 'finite', 'gauge', 'coupling', 'on', 's3', 'times', 's1', 'in', 'this', 'pap... | [-0.17085511723588057, 0.17687516949851723, -0.1080503716640284, 0.08577020461876493, -0.026956419508411166, -0.12482671802589561, 0.008245808214483345, 0.32599383304991264, -0.14768713657223784, -0.2748004296411048, 0.03879626396947595, -0.2574990733855349, -0.18572008162257536, 0.10538297654677402, -0.065342010526150... |
706.3997 | Kondo quantum dot coupled to ferromagnetic leads: Numerical
renormalization group study | We systematically study the influence of ferromagnetic leads on the Kondo
resonance in a quantum dot tuned to the local moment regime. We employ Wilson's
numerical renormalization group method, extended to handle leads with a spin
asymmetric density of states, to identify the effects of (i) a finite spin
polarization... | cond-mat.mes-hall cond-mat.str-el | we systematically study the influence of ferromagnetic leads on the kondo resonance in a quantum dot tuned to the local moment regime we employ wilsons numerical renormalization group method extended to handle leads with a spin asymmetric density of states to identify the effects of i a finite spin polarization in the ... | [['we', 'systematically', 'study', 'the', 'influence', 'of', 'ferromagnetic', 'leads', 'on', 'the', 'kondo', 'resonance', 'in', 'a', 'quantum', 'dot', 'tuned', 'to', 'the', 'local', 'moment', 'regime', 'we', 'employ', 'wilsons', 'numerical', 'renormalization', 'group', 'method', 'extended', 'to', 'handle', 'leads', 'wi... | [-0.17776780231475928, 0.1723071912591031, -0.05745894708180506, 0.04601239511005891, -0.018764128767591166, -0.1580298008262425, 0.08348707245890533, 0.3572967269829589, -0.2644855248570246, -0.3104597087576781, 0.006133731094642395, -0.23986076157981237, -0.09868885313258752, 0.15619667134198703, 0.016874491717380966... |
706.3998 | Fluctuation Effects on R_pA at High Energy | We discuss a new physical phenomenon for R_pA in the fixed coupling case, the
total gluon shadowing, which arises due to the effect of gluon number
fluctuations.
| hep-ph | we discuss a new physical phenomenon for r_pa in the fixed coupling case the total gluon shadowing which arises due to the effect of gluon number fluctuations | [['we', 'discuss', 'a', 'new', 'physical', 'phenomenon', 'for', 'r_pa', 'in', 'the', 'fixed', 'coupling', 'case', 'the', 'total', 'gluon', 'shadowing', 'which', 'arises', 'due', 'to', 'the', 'effect', 'of', 'gluon', 'number', 'fluctuations']] | [-0.17070100290907753, 0.2423387666888259, -0.126325653107078, 0.15518436146279177, -0.0573807444371697, -0.030130138189566356, 0.029735240947317193, 0.2763796261063329, -0.2649918104763384, -0.23757488211547886, -0.015211050316725892, -0.24629101415889132, -0.10811026242596132, 0.10784325479633278, -0.0496793486591842... |
706.3999 | On Matrix Superpotential and Three-Component Normal Modes | We consider the supersymmetric quantum mechanics (SUSY QM) with three-
component normal modes for the Bogomol'nyi-Prasad-Sommerfield (BPS) states. An
explicit form of the SUSY QM matrix superpotential is presented and the
corresponding three-component bosonic zero-mode eigenfunction is investigated.
| hep-th | we consider the supersymmetric quantum mechanics susy qm with three component normal modes for the bogomolnyiprasadsommerfield bps states an explicit form of the susy qm matrix superpotential is presented and the corresponding threecomponent bosonic zeromode eigenfunction is investigated | [['we', 'consider', 'the', 'supersymmetric', 'quantum', 'mechanics', 'susy', 'qm', 'with', 'three', 'component', 'normal', 'modes', 'for', 'the', 'bogomolnyiprasadsommerfield', 'bps', 'states', 'an', 'explicit', 'form', 'of', 'the', 'susy', 'qm', 'matrix', 'superpotential', 'is', 'presented', 'and', 'the', 'correspondi... | [-0.1292585378855859, 0.22021113578145896, -0.015506539175188854, 0.14295349581975883, -0.03608355140558591, -0.2157781580217967, -0.07767373435566888, 0.2693929106095119, -0.1212191137877342, -0.1901255017636638, 0.01762097379756405, -0.2989925213378707, -0.1400518449219434, 0.03898357800943287, 0.00011806890956665341... |
706.4 | Effective field theory and cold Fermi gases near unitary limit | We study a dynamics of ultracold Fermi-gases near the unitary limit in the
framework of Effective Field Theory. It is shown that, while one can obtain a
reasonable description of the universal proportionality constant both in the
narrow and the broad Feshbach resonance limits, the reguirement of the
reparametrisation... | cond-mat.supr-con nucl-th | we study a dynamics of ultracold fermigases near the unitary limit in the framework of effective field theory it is shown that while one can obtain a reasonable description of the universal proportionality constant both in the narrow and the broad feshbach resonance limits the reguirement of the reparametrisation invar... | [['we', 'study', 'a', 'dynamics', 'of', 'ultracold', 'fermigases', 'near', 'the', 'unitary', 'limit', 'in', 'the', 'framework', 'of', 'effective', 'field', 'theory', 'it', 'is', 'shown', 'that', 'while', 'one', 'can', 'obtain', 'a', 'reasonable', 'description', 'of', 'the', 'universal', 'proportionality', 'constant', '... | [-0.14977478854272935, 0.15349340946479162, -0.09323553800462397, 0.07424749694043167, -0.03293140967127303, -0.1147355766127437, 0.03177139883808477, 0.31802589984112223, -0.25371996232662614, -0.28784127623944633, 0.05195103426673778, -0.24177715586314738, -0.0990788486563194, 0.14761431037750042, -0.0177857380976874... |
706.4001 | Pseudo-Quantum Criticality in Electron Liquids Exhibited in Expanded
Alkali Metals | With paying special attention to the divergence in the compressibility
$\kappa$, we study the Coulombic screening in alkali metals to find singular
long-range fluctuations in the electronic polarization originating from this
divergence. As a consequence of this singularity, we predict the decrease of
the equilibratio... | cond-mat.other cond-mat.mtrl-sci | with paying special attention to the divergence in the compressibility kappa we study the coulombic screening in alkali metals to find singular longrange fluctuations in the electronic polarization originating from this divergence as a consequence of this singularity we predict the decrease of the equilibration distanc... | [['with', 'paying', 'special', 'attention', 'to', 'the', 'divergence', 'in', 'the', 'compressibility', 'kappa', 'we', 'study', 'the', 'coulombic', 'screening', 'in', 'alkali', 'metals', 'to', 'find', 'singular', 'longrange', 'fluctuations', 'in', 'the', 'electronic', 'polarization', 'originating', 'from', 'this', 'dive... | [-0.11220387244415095, 0.14936097533624063, -0.06478442438482039, 0.059226062061832466, 0.021564145133584397, -0.12721413212839042, 0.05989287642697836, 0.3183937795545863, -0.22791213791110906, -0.25586764927653743, -0.013047662087255853, -0.39403150826103817, -0.06643851022450147, 0.10508744835040007, -0.026553276594... |
706.4002 | Local results for flows whose speed or height satisfies a bound of the
form $\frac c t$ | In this paper we prove local results for solutions to the Ricci flow (heat
flow) whose speed (height) is bounded by $\frac c t$ for some time interval $ t
\in (0,T)$. These results are contained in chapter 7 of the author's
habilitation thesis, University of Freiburg, Germany, 2006.
| math.DG | in this paper we prove local results for solutions to the ricci flow heat flow whose speed height is bounded by frac c t for some time interval t in 0t these results are contained in chapter 7 of the authors habilitation thesis university of freiburg germany 2006 | [['in', 'this', 'paper', 'we', 'prove', 'local', 'results', 'for', 'solutions', 'to', 'the', 'ricci', 'flow', 'heat', 'flow', 'whose', 'speed', 'height', 'is', 'bounded', 'by', 'frac', 'c', 't', 'for', 'some', 'time', 'interval', 't', 'in', '0t', 'these', 'results', 'are', 'contained', 'in', 'chapter', '7', 'of', 'the'... | [-0.16001184137227634, 0.12094283910604038, -0.04094193460574994, -0.03899380730096406, -0.04374908873190483, -0.1118080024801505, -0.029367487475004356, 0.3257304336875677, -0.2642978302634826, -0.26424929751859355, 0.150671714739777, -0.3324297823613354, -0.056875460354300834, 0.1892276767078632, -0.13046700262930244... |
706.4003 | Shot noise in the interacting resonance level model | The shot noise power and the Fano factor of a spinless resonant level model
is calculated. The Coulomb interaction which in this model acts between the
lead electron and the impurity is considered in the first order approximation.
The logarithmic divergencies which appeared in the expressions for shot noise
and the t... | cond-mat.str-el | the shot noise power and the fano factor of a spinless resonant level model is calculated the coulomb interaction which in this model acts between the lead electron and the impurity is considered in the first order approximation the logarithmic divergencies which appeared in the expressions for shot noise and the trans... | [['the', 'shot', 'noise', 'power', 'and', 'the', 'fano', 'factor', 'of', 'a', 'spinless', 'resonant', 'level', 'model', 'is', 'calculated', 'the', 'coulomb', 'interaction', 'which', 'in', 'this', 'model', 'acts', 'between', 'the', 'lead', 'electron', 'and', 'the', 'impurity', 'is', 'considered', 'in', 'the', 'first', '... | [-0.1510041923849007, 0.12237567213326526, -0.09764442679814386, 0.10301285649397962, 0.004888512422235644, -0.15619230067015302, 0.03011137224069787, 0.3149335541553339, -0.2532397813106678, -0.28484089218308123, -0.00035248494859100606, -0.32590628632021196, -0.1745939358536686, 0.15242233591353788, 0.001642781124469... |
706.4004 | End-to-End Available Bandwidth Measurement Tools : A Comparative
Evaluation of Performances | In recent years, there has been a strong interest in measuring the available
bandwidth of network paths. Several methods and techniques have been proposed
and various measurement tools have been developed and evaluated. However, there
have been few comparative studies with regards to the actual performance of
these t... | cs.NI | in recent years there has been a strong interest in measuring the available bandwidth of network paths several methods and techniques have been proposed and various measurement tools have been developed and evaluated however there have been few comparative studies with regards to the actual performance of these tools t... | [['in', 'recent', 'years', 'there', 'has', 'been', 'a', 'strong', 'interest', 'in', 'measuring', 'the', 'available', 'bandwidth', 'of', 'network', 'paths', 'several', 'methods', 'and', 'techniques', 'have', 'been', 'proposed', 'and', 'various', 'measurement', 'tools', 'have', 'been', 'developed', 'and', 'evaluated', 'h... | [-0.0966845308891037, 0.004898647900547955, -0.08723610799227442, 0.023912822287836737, -0.02615984315359658, -0.12075256243614214, 0.05815947656187096, 0.4406517626574406, -0.18091513176069973, -0.3660715298911372, 0.17514822221806292, -0.28773322877484364, -0.12080191191449598, 0.24936095940378997, -0.074296459701464... |
706.4005 | Absolute frequency measurements for hyperfine structure determination of
the R(26) 62-0 transition at 501.7 nm in molecular iodine | The absolute frequencies of the hyperfine components of the R(26) 62-0
transition in molecular iodine at 501.7 nm are measured for the first time with
an optical clockwork based on a femtosecond laser frequency comb generator. The
set-up is composed of an Ar+ laser locked to a hyperfine component of the R(26)
62-0 tr... | physics.atom-ph | the absolute frequencies of the hyperfine components of the r26 620 transition in molecular iodine at 5017 nm are measured for the first time with an optical clockwork based on a femtosecond laser frequency comb generator the setup is composed of an ar laser locked to a hyperfine component of the r26 620 transition det... | [['the', 'absolute', 'frequencies', 'of', 'the', 'hyperfine', 'components', 'of', 'the', 'r26', '620', 'transition', 'in', 'molecular', 'iodine', 'at', '5017', 'nm', 'are', 'measured', 'for', 'the', 'first', 'time', 'with', 'an', 'optical', 'clockwork', 'based', 'on', 'a', 'femtosecond', 'laser', 'frequency', 'comb', '... | [-0.11396634349085648, 0.23538260654868803, 0.015997337129223962, -0.07790406060876089, 0.020825906110734774, -0.11065463590082424, 0.0767733814387486, 0.48782508220823334, -0.201691114233978, -0.3021203927246147, 0.053627004640862, -0.2761579044377324, 0.07429584926101325, 0.20628026490843715, 0.042579841800034046, -0... |
706.4006 | Gutzwiller's Trace Formula and Vacuum Pair Production | We propose a new application of the Gutzwiller trace formula formalism, to
give a compact expression for the semiclassical vacuum pair production rate in
quantum electrodynamics, for general inhomogeneous electromagnetic background
fields.
| hep-th | we propose a new application of the gutzwiller trace formula formalism to give a compact expression for the semiclassical vacuum pair production rate in quantum electrodynamics for general inhomogeneous electromagnetic background fields | [['we', 'propose', 'a', 'new', 'application', 'of', 'the', 'gutzwiller', 'trace', 'formula', 'formalism', 'to', 'give', 'a', 'compact', 'expression', 'for', 'the', 'semiclassical', 'vacuum', 'pair', 'production', 'rate', 'in', 'quantum', 'electrodynamics', 'for', 'general', 'inhomogeneous', 'electromagnetic', 'backgrou... | [-0.14822921447193949, 0.13052243980928324, -0.0895132583391387, 0.1642975331051275, -0.09788223566283705, -0.11475619037810247, 0.006973051196837332, 0.31378307996783406, -0.14747237879782915, -0.21861110406462103, -0.04770298360745073, -0.20660111506003886, -0.1268828399049653, 0.21818909235298634, 0.0219232427480164... |
706.4007 | Transmission des forces dans un milieu compos\'e de grains non
sph\'eriques | We perform a detailed analysis of the contact force network in a dense
confined packing of pentagonal particles simulated by means of the contact
dynamics method. The effect of particle shape is evidenced by comparing the
data from pentagon packing and from a packing with identical characteristics
except for the circ... | physics.class-ph | we perform a detailed analysis of the contact force network in a dense confined packing of pentagonal particles simulated by means of the contact dynamics method the effect of particle shape is evidenced by comparing the data from pentagon packing and from a packing with identical characteristics except for the circula... | [['we', 'perform', 'a', 'detailed', 'analysis', 'of', 'the', 'contact', 'force', 'network', 'in', 'a', 'dense', 'confined', 'packing', 'of', 'pentagonal', 'particles', 'simulated', 'by', 'means', 'of', 'the', 'contact', 'dynamics', 'method', 'the', 'effect', 'of', 'particle', 'shape', 'is', 'evidenced', 'by', 'comparin... | [-0.17875179171415737, 0.14372279176698818, -0.09694742649913796, 0.03767918011008371, -0.01989374152467316, -0.11349511207231591, 0.06940397285075198, 0.36573363389940033, -0.25564641743718136, -0.2947841891418061, 0.04038689723914309, -0.2878022563072943, -0.15390861771640277, 0.14300235944064033, 0.00568980753662124... |
706.4008 | Conserved Matter Superenergy Currents for Orthogonally Transitive
Abelian G2 Isometry Groups | In a previous paper we showed that the electromagnetic superenergy tensor,
the Chevreton tensor, gives rise to a conserved current when there is a
hypersurface orthogonal Killing vector present. In addition, the current is
proportional to the Killing vector. The aim of this paper is to extend this
result to the case ... | gr-qc | in a previous paper we showed that the electromagnetic superenergy tensor the chevreton tensor gives rise to a conserved current when there is a hypersurface orthogonal killing vector present in addition the current is proportional to the killing vector the aim of this paper is to extend this result to the case when we... | [['in', 'a', 'previous', 'paper', 'we', 'showed', 'that', 'the', 'electromagnetic', 'superenergy', 'tensor', 'the', 'chevreton', 'tensor', 'gives', 'rise', 'to', 'a', 'conserved', 'current', 'when', 'there', 'is', 'a', 'hypersurface', 'orthogonal', 'killing', 'vector', 'present', 'in', 'addition', 'the', 'current', 'is... | [-0.17484208977593763, 0.15204824069620704, -0.05824006778224335, 0.028005375105028898, -0.12759180560816902, -0.07493287066372668, -0.07510369087043278, 0.3377096342624395, -0.2206859205268904, -0.23068318857702536, 0.06713527831507472, -0.25282979864844835, -0.1922701014517262, 0.13945682658571992, -0.036976017838029... |
706.4009 | Multi-criteria scheduling of pipeline workflows | Mapping workflow applications onto parallel platforms is a challenging
problem, even for simple application patterns such as pipeline graphs. Several
antagonist criteria should be optimized, such as throughput and latency (or a
combination). In this paper, we study the complexity of the bi-criteria mapping
problem fo... | cs.DC | mapping workflow applications onto parallel platforms is a challenging problem even for simple application patterns such as pipeline graphs several antagonist criteria should be optimized such as throughput and latency or a combination in this paper we study the complexity of the bicriteria mapping problem for pipeline... | [['mapping', 'workflow', 'applications', 'onto', 'parallel', 'platforms', 'is', 'a', 'challenging', 'problem', 'even', 'for', 'simple', 'application', 'patterns', 'such', 'as', 'pipeline', 'graphs', 'several', 'antagonist', 'criteria', 'should', 'be', 'optimized', 'such', 'as', 'throughput', 'and', 'latency', 'or', 'a'... | [-0.16017231349982214, -0.030449947721303203, -0.04876099012488889, 0.09126776239840141, -0.10060916420852029, -0.15112443591013205, 0.08280535664024957, 0.47184599459517834, -0.31770553416031044, -0.34221595520868375, 0.15356050700566537, -0.2203135533518223, -0.20005514142699107, 0.2684220398077741, -0.08498880122030... |
706.401 | Quantum toy model for black-hole back-reaction | We propose a simple quantum field theoretical toy model for black hole
evaporation and study the back-reaction of Hawking radiation onto the classical
background. It turns out that the horizon is also ``pushed back'' in this
situation (i.e., the interior region shrinks) but this back-reaction is not
caused by energy ... | gr-qc | we propose a simple quantum field theoretical toy model for black hole evaporation and study the backreaction of hawking radiation onto the classical background it turns out that the horizon is also pushed back in this situation ie the interior region shrinks but this backreaction is not caused by energy conservation b... | [['we', 'propose', 'a', 'simple', 'quantum', 'field', 'theoretical', 'toy', 'model', 'for', 'black', 'hole', 'evaporation', 'and', 'study', 'the', 'backreaction', 'of', 'hawking', 'radiation', 'onto', 'the', 'classical', 'background', 'it', 'turns', 'out', 'that', 'the', 'horizon', 'is', 'also', 'pushed', 'back', 'in',... | [-0.11090358379535759, 0.16730875643835857, -0.09467175608285917, 0.11507466225287853, -0.08826952623442197, -0.12396945018106355, 0.06426289977016261, 0.2925405086089785, -0.2399674770064079, -0.28790162133578306, 0.08856927894820006, -0.30307522998788416, -0.08269936841828987, 0.17059255734635279, -0.0681243898389556... |
706.4011 | Determination of density and concentration from fluorescent images of a
gas flow | A fluorescent image analysis procedure to determine the distribution of
species concentration and density in a gas flow is proposed. The fluorescent
emission is due to the excitation of atoms/molecules of a gas that is
intercepted by an electron blade. The intensity of the fluorescent light is
proportional to the loc... | physics.flu-dyn | a fluorescent image analysis procedure to determine the distribution of species concentration and density in a gas flow is proposed the fluorescent emission is due to the excitation of atomsmolecules of a gas that is intercepted by an electron blade the intensity of the fluorescent light is proportional to the local nu... | [['a', 'fluorescent', 'image', 'analysis', 'procedure', 'to', 'determine', 'the', 'distribution', 'of', 'species', 'concentration', 'and', 'density', 'in', 'a', 'gas', 'flow', 'is', 'proposed', 'the', 'fluorescent', 'emission', 'is', 'due', 'to', 'the', 'excitation', 'of', 'atomsmolecules', 'of', 'a', 'gas', 'that', 'i... | [-0.05761566908542056, 0.16936719708618547, -0.12257318211835151, 0.021916138242382956, 0.013792197330523346, -0.09423950230597523, 0.0101709134171659, 0.3858631981568316, -0.2473980859132473, -0.3184531602882228, 0.04474040306512645, -0.28627718727256957, 0.006620606599575551, 0.14999309288979756, -0.00325718137440876... |
706.4012 | Existence of mesons after deconfinement | We investigate the possibility for a quark-antiquark pair to form a bound
state at temperatures higher than the critical one ($T>T_c$), thus after
deconfinement. Our main goal is to find analytical criteria constraining the
existence of such mesons. Our formalism relies on a Schr\"{o}dinger equation
for which we stud... | hep-ph | we investigate the possibility for a quarkantiquark pair to form a bound state at temperatures higher than the critical one tt_c thus after deconfinement our main goal is to find analytical criteria constraining the existence of such mesons our formalism relies on a schrodinger equation for which we study the physical ... | [['we', 'investigate', 'the', 'possibility', 'for', 'a', 'quarkantiquark', 'pair', 'to', 'form', 'a', 'bound', 'state', 'at', 'temperatures', 'higher', 'than', 'the', 'critical', 'one', 'tt_c', 'thus', 'after', 'deconfinement', 'our', 'main', 'goal', 'is', 'to', 'find', 'analytical', 'criteria', 'constraining', 'the', ... | [-0.09431345828595293, 0.1978886702311504, -0.09739678151086922, 0.10132721613478628, -0.017860050320589713, -0.11604108432141744, 0.0843866975832683, 0.3238181784321928, -0.1843166656697252, -0.29701477919177266, 0.029414870287588307, -0.2811792355734643, -0.06626782165306389, 0.1775073540058865, 0.05739678072618546, ... |
706.4013 | A Chandra Study of the Lobe/ISM Interactions Around the Inner Radio
Lobes of Centaurus A: Constraints on the Temperature Structure and Transport
Processes | We present results from deeper {\em Chandra} observations of the southwest
radio lobe of Centaurus A, first described by Kraft et al. (2003). We find that
the sharp X-ray surface brightness discontinuity extends around $\sim$75% of
the periphery of the radio lobe, and detect significant temperature jumps in
the brigh... | astro-ph | we present results from deeper em chandra observations of the southwest radio lobe of centaurus a first described by kraft et al 2003 we find that the sharp xray surface brightness discontinuity extends around sim75 of the periphery of the radio lobe and detect significant temperature jumps in the brightest regions of ... | [['we', 'present', 'results', 'from', 'deeper', 'em', 'chandra', 'observations', 'of', 'the', 'southwest', 'radio', 'lobe', 'of', 'centaurus', 'a', 'first', 'described', 'by', 'kraft', 'et', 'al', '2003', 'we', 'find', 'that', 'the', 'sharp', 'xray', 'surface', 'brightness', 'discontinuity', 'extends', 'around', 'sim75... | [-0.05760554808734494, 0.16806540624200111, -0.06449435881585024, 0.07916190710208677, -0.06072813167043452, -0.06889896089022206, 0.05737834574637126, 0.4024976404629788, -0.22557529284144348, -0.29368306398040284, 0.037832383584354146, -0.27965523712337015, -0.0196067013004619, 0.201334756981353, 0.003798597325342444... |
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