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 |
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709.1335 | Interference of Spontaneous Emission of Light from two Solid-State
Atomic Ensembles | We report an interference experiment of spontaneous emission of light from
two distant solid-state ensembles of atoms that are coherently excited by a
short laser pulse. The ensembles are Erbium ions doped into two LiNbO3 crystals
with channel waveguides, which are placed in the two arms of a Mach-Zehnder
interferome... | quant-ph | we report an interference experiment of spontaneous emission of light from two distant solidstate ensembles of atoms that are coherently excited by a short laser pulse the ensembles are erbium ions doped into two linbo3 crystals with channel waveguides which are placed in the two arms of a machzehnder interferometer th... | [['we', 'report', 'an', 'interference', 'experiment', 'of', 'spontaneous', 'emission', 'of', 'light', 'from', 'two', 'distant', 'solidstate', 'ensembles', 'of', 'atoms', 'that', 'are', 'coherently', 'excited', 'by', 'a', 'short', 'laser', 'pulse', 'the', 'ensembles', 'are', 'erbium', 'ions', 'doped', 'into', 'two', 'li... | [-0.16541721926491082, 0.2910953267093437, -0.055016709120729854, 0.019184573616088673, 0.042707556673218454, -0.18650636369922916, 0.03686211614836568, 0.4894549073898687, -0.20412821194107553, -0.2567465544010686, -0.01720251089716083, -0.34870592126029387, -0.06067603745341169, 0.17350036479054695, 0.030031289109976... |
709.1336 | X-ray active galactic nuclei in the core of the Perseus cluster | We present a study of the X-ray emission from the nuclei of galaxies observed
in the core of the Perseus cluster in a deep exposure with Chandra. Point
sources are found coincident with the nuclei of 13 early-type galaxies, as well
as the central galaxy NGC1275. This corresponds to all galaxies brighter than
M_B = -1... | astro-ph | we present a study of the xray emission from the nuclei of galaxies observed in the core of the perseus cluster in a deep exposure with chandra point sources are found coincident with the nuclei of 13 earlytype galaxies as well as the central galaxy ngc1275 this corresponds to all galaxies brighter than m_b 18 in the c... | [['we', 'present', 'a', 'study', 'of', 'the', 'xray', 'emission', 'from', 'the', 'nuclei', 'of', 'galaxies', 'observed', 'in', 'the', 'core', 'of', 'the', 'perseus', 'cluster', 'in', 'a', 'deep', 'exposure', 'with', 'chandra', 'point', 'sources', 'are', 'found', 'coincident', 'with', 'the', 'nuclei', 'of', '13', 'early... | [-0.02227026697046141, 0.08843630357323662, -0.06486376395460756, 0.16768919512755442, -0.059943818472583524, -0.04809224116762385, 0.04792253360366039, 0.5079079278914621, -0.08368741669369943, -0.3707476325813423, 0.020277025683273404, -0.39372821048241835, 0.025222524268400368, 0.19531721634104898, 0.034331352760394... |
709.1337 | Phenomenology of Gamma-Ray Jets | We discuss some phenomenological aspects of $\gamma$-ray emitting jets. In
particular, we present calculations of the $\gamma$-sphere and $\pi$-sphere for
various target photon fields, and employ them to demonstrate how $\gamma$-ray
observations at very high energies can be used to constraint the Doppler factor
of th... | astro-ph | we discuss some phenomenological aspects of gammaray emitting jets in particular we present calculations of the gammasphere and pisphere for various target photon fields and employ them to demonstrate how gammaray observations at very high energies can be used to constraint the doppler factor of the emitting plasma and... | [['we', 'discuss', 'some', 'phenomenological', 'aspects', 'of', 'gammaray', 'emitting', 'jets', 'in', 'particular', 'we', 'present', 'calculations', 'of', 'the', 'gammasphere', 'and', 'pisphere', 'for', 'various', 'target', 'photon', 'fields', 'and', 'employ', 'them', 'to', 'demonstrate', 'how', 'gammaray', 'observatio... | [-0.04883994588797742, 0.22807693645696747, -0.02325137052261694, 0.22533463155427438, -0.10064406775530767, -0.12477188482880593, 0.03529262911232019, 0.4605282981626012, -0.17891119854440066, -0.3640993574634194, 0.0183846056048589, -0.2746073604984717, -0.007459827614101497, 0.24028433514335615, 0.012432838187404824... |
709.1338 | Spin-gap behaviour in the 2-leg spin-ladder BiCu2PO6 | We present magnetic suscceptibility and heat capacity data on a new S=1/2
two-leg spin ladder compound BiCu2PO6. From our susceptibility analysis, we
find that the leg coupling J1/k_B is ~ 80 K and the ratio of the rung to leg
coupling J2/J1 ~ 0.9. We present the magnetic contribution to the heat capacity
of a two-le... | cond-mat.str-el | we present magnetic suscceptibility and heat capacity data on a new s12 twoleg spin ladder compound bicu2po6 from our susceptibility analysis we find that the leg coupling j1k_b is 80 k and the ratio of the rung to leg coupling j2j1 09 we present the magnetic contribution to the heat capacity of a twoleg ladder the spi... | [['we', 'present', 'magnetic', 'suscceptibility', 'and', 'heat', 'capacity', 'data', 'on', 'a', 'new', 's12', 'twoleg', 'spin', 'ladder', 'compound', 'bicu2po6', 'from', 'our', 'susceptibility', 'analysis', 'we', 'find', 'that', 'the', 'leg', 'coupling', 'j1k_b', 'is', '80', 'k', 'and', 'the', 'ratio', 'of', 'the', 'ru... | [-0.2108219427873205, 0.14498240636675147, 0.015285764216863807, 0.013913011881927758, -0.05866209532984573, -0.1292653017596382, 0.1424354642437285, 0.36906501162203326, -0.2231664573436306, -0.2914988566594927, 0.0364286808239674, -0.3840000691783169, -0.08365307498784007, 0.18545389058831, 0.1139416585345685, -0.018... |
709.1339 | Control of Quantum Systems Despite Feedback Delay | Feedback control (based on the quantum continuous measurement) of quantum
systems inevitably suffers from estimation delays. In this paper we give a
delay-dependent stability criterion for a wide class of nonlinear stochastic
systems including quantum spin systems. We utilize a semi-algebraic problem
approach to inco... | quant-ph | feedback control based on the quantum continuous measurement of quantum systems inevitably suffers from estimation delays in this paper we give a delaydependent stability criterion for a wide class of nonlinear stochastic systems including quantum spin systems we utilize a semialgebraic problem approach to incorporate ... | [['feedback', 'control', 'based', 'on', 'the', 'quantum', 'continuous', 'measurement', 'of', 'quantum', 'systems', 'inevitably', 'suffers', 'from', 'estimation', 'delays', 'in', 'this', 'paper', 'we', 'give', 'a', 'delaydependent', 'stability', 'criterion', 'for', 'a', 'wide', 'class', 'of', 'nonlinear', 'stochastic', ... | [-0.1868436224386096, 0.06344476087697937, -0.07438127909476558, 0.02492041778440277, -0.030652480088174342, -0.15523066414520145, 0.04925304750756671, 0.3171553108965357, -0.3016772437437127, -0.2626468462900569, 0.1155535757758965, -0.21790645079066356, -0.1953597381711006, 0.2403348293931534, -0.09728182752927145, 0... |
709.134 | Measurement of B(Ds -> munu) | We present a measurement of the branching fraction $B(D_s^+\to\mu^+\nu_\mu)$
using a 548 fb$^{-1}$ data sample collected by the Belle experiment at the KEKB
$e^+e^-$ collider. The $D_s$ momentum is determined by reconstruction of the
system recoiling against $DK\gamma X$ in events of the type $e^+e^-\to D_s^\ast
DKX,... | hep-ex | we present a measurement of the branching fraction bd_stomunu_mu using a 548 fb1 data sample collected by the belle experiment at the kekb ee collider the d_s momentum is determined by reconstruction of the system recoiling against dkgamma x in events of the type eeto d_sast dkx d_sast to d_sgamma where x represents ad... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'branching', 'fraction', 'bd_stomunu_mu', 'using', 'a', '548', 'fb1', 'data', 'sample', 'collected', 'by', 'the', 'belle', 'experiment', 'at', 'the', 'kekb', 'ee', 'collider', 'the', 'd_s', 'momentum', 'is', 'determined', 'by', 'reconstruction', 'of', 'the', 'system',... | [-0.09287396994186566, 0.1862864518114789, -0.06113107217877934, 0.057709128846710714, 0.024759833405418746, -0.12492982442490756, 0.10362814960535616, 0.29263844845647163, -0.14364789651854978, -0.3322671901476993, -0.04097936430268667, -0.43106694812463087, 0.1360494445734234, 0.15046836313664574, 0.03871970690617507... |
709.1341 | Coincidence rotations of the root lattice $A_4$ | The coincidence site lattices of the root lattice $A_4$ are considered, and
the statistics of the corresponding coincidence rotations according to their
indices is expressed in terms of a Dirichlet series generating function. This
is possible via an embedding of $A_4$ into the icosian ring with its rich
arithmetic st... | math.MG math.CO | the coincidence site lattices of the root lattice a_4 are considered and the statistics of the corresponding coincidence rotations according to their indices is expressed in terms of a dirichlet series generating function this is possible via an embedding of a_4 into the icosian ring with its rich arithmetic structure ... | [['the', 'coincidence', 'site', 'lattices', 'of', 'the', 'root', 'lattice', 'a_4', 'are', 'considered', 'and', 'the', 'statistics', 'of', 'the', 'corresponding', 'coincidence', 'rotations', 'according', 'to', 'their', 'indices', 'is', 'expressed', 'in', 'terms', 'of', 'a', 'dirichlet', 'series', 'generating', 'function... | [-0.1203660526643357, 0.10694591788177926, -0.06876890721069949, 0.08282049443955804, -0.08582970661471688, -0.08637932559565431, 0.012698904340786318, 0.3871636084851719, -0.3206985746960967, -0.24273111102651926, 0.11027427111384308, -0.25596991055194407, -0.10028205914122443, 0.11597201055302585, -0.0366029292269940... |
709.1342 | Electro-optic control of atom-light interactions using Rydberg
dark-state polaritons | We demonstrate a multiphoton Rydberg dark resonance where a Lambda-system is
coupled to a Rydberg state. This N-type level scheme combines the ability to
slow and store light pulses associated with long lived ground state
superpositions, with the strongly interacting character of Rydberg states. For
the nd_{5/2} Rydb... | quant-ph | we demonstrate a multiphoton rydberg dark resonance where a lambdasystem is coupled to a rydberg state this ntype level scheme combines the ability to slow and store light pulses associated with long lived ground state superpositions with the strongly interacting character of rydberg states for the nd_52 rydberg state ... | [['we', 'demonstrate', 'a', 'multiphoton', 'rydberg', 'dark', 'resonance', 'where', 'a', 'lambdasystem', 'is', 'coupled', 'to', 'a', 'rydberg', 'state', 'this', 'ntype', 'level', 'scheme', 'combines', 'the', 'ability', 'to', 'slow', 'and', 'store', 'light', 'pulses', 'associated', 'with', 'long', 'lived', 'ground', 'st... | [-0.14149295992478983, 0.30404471760181573, 0.0008012619451619685, -0.008516751244314946, 0.010300385629913459, -0.19650784369635707, 0.05549051137447047, 0.467720988431635, -0.21248109020137537, -0.29913890052897235, 0.004260807644459419, -0.27912364590447397, -0.02133970701834187, 0.19222163784434088, 0.0376811685661... |
709.1343 | Observation of an in-plane magnetic-field-driven phase transition in a
quantum Hall system with SU(4) symmetry | In condensed matter physics, the study of electronic states with SU(N)
symmetry has attracted considerable and growing attention in recent years, as
systems with such a symmetry can often have a spontaneous symmetry-breaking
effect giving rise to a novel ground state. For example, pseudospin quantum
Hall ferromagnet ... | cond-mat.mes-hall cond-mat.str-el | in condensed matter physics the study of electronic states with sun symmetry has attracted considerable and growing attention in recent years as systems with such a symmetry can often have a spontaneous symmetrybreaking effect giving rise to a novel ground state for example pseudospin quantum hall ferromagnet of broken... | [['in', 'condensed', 'matter', 'physics', 'the', 'study', 'of', 'electronic', 'states', 'with', 'sun', 'symmetry', 'has', 'attracted', 'considerable', 'and', 'growing', 'attention', 'in', 'recent', 'years', 'as', 'systems', 'with', 'such', 'a', 'symmetry', 'can', 'often', 'have', 'a', 'spontaneous', 'symmetrybreaking',... | [-0.20049762257977444, 0.2652338928564431, -0.05096793786925606, 0.015769045818460118, -0.04772551348706817, -0.18657670926357456, 0.03502564084140913, 0.35216642900982953, -0.25184208298759425, -0.33356395888635343, 0.023839219169937732, -0.26895733837257413, -0.10781748456031304, 0.12841681634034852, 0.01930398285690... |
709.1344 | 3-5 micron spectroscopy of obscured AGNs in ULIRGs | We present the results of infrared L-band (3-4 micron) and M-band (4-5
micron) VLT-ISAAC spectroscopy of five bright Ultraluminous InfraRed Galaxies
(ULIRGs) hosting an AGN. From our analysis we distinguish two types of sources:
ULIRGs where the AGN is unobscured (with a flat continuum and no absorption
features at 3... | astro-ph | we present the results of infrared lband 34 micron and mband 45 micron vltisaac spectroscopy of five bright ultraluminous infrared galaxies ulirgs hosting an agn from our analysis we distinguish two types of sources ulirgs where the agn is unobscured with a flat continuum and no absorption features at 34 micron and 46 ... | [['we', 'present', 'the', 'results', 'of', 'infrared', 'lband', '34', 'micron', 'and', 'mband', '45', 'micron', 'vltisaac', 'spectroscopy', 'of', 'five', 'bright', 'ultraluminous', 'infrared', 'galaxies', 'ulirgs', 'hosting', 'an', 'agn', 'from', 'our', 'analysis', 'we', 'distinguish', 'two', 'types', 'of', 'sources', ... | [0.03279332644207046, 0.03471973718316146, -0.018543484780924224, 0.09269620593928679, -0.04568240681253638, -0.12635809381274468, 0.05684603190260893, 0.5475105927292759, -0.10481244078606156, -0.2890493048194809, 0.030542193019452196, -0.3784167706860718, -0.03897044168956948, 0.12478141627086207, -0.0103418107973477... |
709.1345 | The Gonihedric Ising Model and Glassiness | The Gonihedric 3D Ising model is a lattice spin model in which planar Peierls
boundaries between + and - spins can be created at zero energy cost. Instead of
weighting the area of Peierls boundaries as the case for the usual 3D Ising
model with nearest neighbour interactions, the edges, or "bends" in an
interface are... | cond-mat.stat-mech | the gonihedric 3d ising model is a lattice spin model in which planar peierls boundaries between and spins can be created at zero energy cost instead of weighting the area of peierls boundaries as the case for the usual 3d ising model with nearest neighbour interactions the edges or bends in an interface are weighted a... | [['the', 'gonihedric', '3d', 'ising', 'model', 'is', 'a', 'lattice', 'spin', 'model', 'in', 'which', 'planar', 'peierls', 'boundaries', 'between', 'and', 'spins', 'can', 'be', 'created', 'at', 'zero', 'energy', 'cost', 'instead', 'of', 'weighting', 'the', 'area', 'of', 'peierls', 'boundaries', 'as', 'the', 'case', 'for... | [-0.09849595024721126, 0.16316981358839508, -0.05821249692084605, 0.052075480474239405, -0.049128774320706725, -0.10878927736334375, 0.04622713471276099, 0.38295652736620656, -0.2783359016165346, -0.30643466330968355, 0.08005590676049028, -0.2997729581768689, -0.1385683679636086, 0.09140666803858917, 0.0080727001186460... |
709.1346 | A MAPS-based Digital Electromagnetic Calorimeter for the ILC | A novel design for a silicon-tungsten electromagnetic calorimeter is
described, based on Monolithic Active Pixel Sensors (MAPS). A test sensor with
a pixel size of 50x50 um2 has been fabricated in July 2007. The simulation of
the physical sensor is done using a detailed three-dimensional charge spread
algorithm. Phys... | physics.ins-det | a novel design for a silicontungsten electromagnetic calorimeter is described based on monolithic active pixel sensors maps a test sensor with a pixel size of 50x50 um2 has been fabricated in july 2007 the simulation of the physical sensor is done using a detailed threedimensional charge spread algorithm physics studie... | [['a', 'novel', 'design', 'for', 'a', 'silicontungsten', 'electromagnetic', 'calorimeter', 'is', 'described', 'based', 'on', 'monolithic', 'active', 'pixel', 'sensors', 'maps', 'a', 'test', 'sensor', 'with', 'a', 'pixel', 'size', 'of', '50x50', 'um2', 'has', 'been', 'fabricated', 'in', 'july', '2007', 'the', 'simulatio... | [-0.09507149759332066, 0.11378570288870034, -0.06732827134348535, -0.015022501923850032, -0.037664365847236835, -0.1472934069787408, 0.0027866600373002526, 0.40332892479804844, -0.1932046503483594, -0.3780196855602029, 0.08273641365211826, -0.2922986650450544, -0.08318809929539214, 0.1842445544182108, -0.08755203628155... |
709.1347 | Rigid rotators and diatomic molecules via Tsallis statistics | We obtain an analytic expression for the specific heat of a system of N rigid
rotators exactly in the high temperature limit, and via a pertubative approach
in the low temperature limit. We then evaluate the specific heat of a diatomic
gas with both translational and rotational degrees of freedom, and conclude
that t... | cond-mat.stat-mech | we obtain an analytic expression for the specific heat of a system of n rigid rotators exactly in the high temperature limit and via a pertubative approach in the low temperature limit we then evaluate the specific heat of a diatomic gas with both translational and rotational degrees of freedom and conclude that there ... | [['we', 'obtain', 'an', 'analytic', 'expression', 'for', 'the', 'specific', 'heat', 'of', 'a', 'system', 'of', 'n', 'rigid', 'rotators', 'exactly', 'in', 'the', 'high', 'temperature', 'limit', 'and', 'via', 'a', 'pertubative', 'approach', 'in', 'the', 'low', 'temperature', 'limit', 'we', 'then', 'evaluate', 'the', 'spe... | [-0.14293050127162132, 0.19809802358149148, -0.06774928800159079, -0.0033814895415322527, 0.0007306562346296714, -0.11334081285852282, 0.09617009893854093, 0.3244575551327537, -0.22899866164388025, -0.2768590524107875, 0.056604598876540825, -0.26974755470805306, -0.08567564528065678, 0.15125585304956665, -0.01009311898... |
709.1348 | Exclusive processes in position space and the pion distribution
amplitude | We suggest to carry out lattice calculations of current correlators in
position space, sandwiched between the vacuum and a hadron state (e.g. pion),
in order to access hadronic light-cone distribution amplitudes (DAs). In this
way the renormalization problem for composite lattice operators is avoided
altogether, and ... | hep-ph hep-lat | we suggest to carry out lattice calculations of current correlators in position space sandwiched between the vacuum and a hadron state eg pion in order to access hadronic lightcone distribution amplitudes das in this way the renormalization problem for composite lattice operators is avoided altogether and the connectio... | [['we', 'suggest', 'to', 'carry', 'out', 'lattice', 'calculations', 'of', 'current', 'correlators', 'in', 'position', 'space', 'sandwiched', 'between', 'the', 'vacuum', 'and', 'a', 'hadron', 'state', 'eg', 'pion', 'in', 'order', 'to', 'access', 'hadronic', 'lightcone', 'distribution', 'amplitudes', 'das', 'in', 'this',... | [-0.12735294728455218, 0.13779859581670229, -0.12410275418742382, 0.09122170300284509, -0.03658290343235963, -0.04896003170677823, 0.06840624063745264, 0.37647771488967513, -0.23248611041921968, -0.23508987116265642, 0.016638910388266127, -0.31455505633926834, -0.09999086807120192, 0.0844407906459475, 0.040336708638293... |
709.1349 | Knot localization in adsorbing polymer rings | We study by Monte Carlo simulations a model of knotted polymer ring adsorbing
onto an impenetrable, attractive wall. The polymer is described by a
self-avoiding polygon (SAP) on the cubic lattice. We find that the adsorption
transition temperature, the crossover exponent $\phi$ and the metric exponent
$\nu$, are the ... | cond-mat.soft | we study by monte carlo simulations a model of knotted polymer ring adsorbing onto an impenetrable attractive wall the polymer is described by a selfavoiding polygon sap on the cubic lattice we find that the adsorption transition temperature the crossover exponent phi and the metric exponent nu are the same as in the m... | [['we', 'study', 'by', 'monte', 'carlo', 'simulations', 'a', 'model', 'of', 'knotted', 'polymer', 'ring', 'adsorbing', 'onto', 'an', 'impenetrable', 'attractive', 'wall', 'the', 'polymer', 'is', 'described', 'by', 'a', 'selfavoiding', 'polygon', 'sap', 'on', 'the', 'cubic', 'lattice', 'we', 'find', 'that', 'the', 'adso... | [-0.16048340495819083, 0.1915381214043569, -0.0802513780982759, 0.040312494699789495, -0.016287479169057824, -0.1855471724889074, 0.04110371747698922, 0.4031337107149645, -0.27629724161651653, -0.24701728667237033, 0.06203866973877526, -0.2863136478580343, -0.15246542658394155, 0.13473744744894645, 0.005553687874896404... |
709.135 | Conical square function estimates in UMD Banach spaces and applications
to H-infinity functional calculi | We study conical square function estimates for Banach-valued functions, and
introduce a vector-valued analogue of the Coifman-Meyer-Stein tent spaces.
Following recent work of Auscher-McIntosh-Russ, the tent spaces in turn are
used to construct a scale of vector-valued Hardy spaces associated with a given
bisectorial... | math.FA math.SP | we study conical square function estimates for banachvalued functions and introduce a vectorvalued analogue of the coifmanmeyerstein tent spaces following recent work of auschermcintoshruss the tent spaces in turn are used to construct a scale of vectorvalued hardy spaces associated with a given bisectorial operator a ... | [['we', 'study', 'conical', 'square', 'function', 'estimates', 'for', 'banachvalued', 'functions', 'and', 'introduce', 'a', 'vectorvalued', 'analogue', 'of', 'the', 'coifmanmeyerstein', 'tent', 'spaces', 'following', 'recent', 'work', 'of', 'auschermcintoshruss', 'the', 'tent', 'spaces', 'in', 'turn', 'are', 'used', 't... | [-0.10062433986670592, 0.04815871132622388, -0.1212929127399217, 0.17220065396342596, -0.0958741598222828, -0.08539531561757692, 0.0028874717345884577, 0.33017229431054806, -0.28704517676325686, -0.17611738250336864, 0.16788969810268925, -0.24389511195477098, -0.19412793707187204, 0.23462446243925528, -0.13502212575086... |
709.1351 | Temperature Inversion Symmetry in Gauge-Higgs Unification Models | The temperature inversion symmetry $R\to \frac{1}{T}$ is studied for the
finite temperature effective potential of the N=1, $d=5$, supersymmetric
$SU(3)_{c}{\times}SU(3)_{w}$ model, on the orbifold $S^{1}/Z_{2}$. For the
value of the Wilson line parameter $\alpha=1$ ($SU(2)_{L}$ breaks to a
$U'(1)$), it is found that... | hep-ph math-ph math.MP | the temperature inversion symmetry rto frac1t is studied for the finite temperature effective potential of the n1 d5 supersymmetric su3_ctimessu3_w model on the orbifold s1z_2 for the value of the wilson line parameter alpha1 su2_l breaks to a u1 it is found that the effective potential contains a symmetric part and an... | [['the', 'temperature', 'inversion', 'symmetry', 'rto', 'frac1t', 'is', 'studied', 'for', 'the', 'finite', 'temperature', 'effective', 'potential', 'of', 'the', 'n1', 'd5', 'supersymmetric', 'su3_ctimessu3_w', 'model', 'on', 'the', 'orbifold', 's1z_2', 'for', 'the', 'value', 'of', 'the', 'wilson', 'line', 'parameter', ... | [-0.15355044922034722, 0.2036836958592403, -0.06051177334302338, 0.06846315845814388, -0.07590565218379197, -0.20842012972570956, 0.016436118785350118, 0.3503550838504452, -0.1863511919582379, -0.2485375663782179, 0.11276610268851073, -0.27614358565188013, -0.11815283217765682, 0.06150206749953213, 0.009997492459660862... |
709.1352 | Quantum Phase Transitions of Light in the Dicke-Bose-Hubbard model | We extend the idea of quantum phase transitions of light in atom-photon
system with Dicke-Bose-Hubbard model for arbitrary number of two-level atoms.
The formulations of eigenenergies, effective Rabi frequencies, and critical
chemical potentials for two atoms are derived. With a self-consistent method,
we obtain a co... | quant-ph | we extend the idea of quantum phase transitions of light in atomphoton system with dickebosehubbard model for arbitrary number of twolevel atoms the formulations of eigenenergies effective rabi frequencies and critical chemical potentials for two atoms are derived with a selfconsistent method we obtain a complete phase... | [['we', 'extend', 'the', 'idea', 'of', 'quantum', 'phase', 'transitions', 'of', 'light', 'in', 'atomphoton', 'system', 'with', 'dickebosehubbard', 'model', 'for', 'arbitrary', 'number', 'of', 'twolevel', 'atoms', 'the', 'formulations', 'of', 'eigenenergies', 'effective', 'rabi', 'frequencies', 'and', 'critical', 'chemi... | [-0.12075237201417993, 0.19594367105092336, -0.04788444574963111, 0.03111130301925578, 0.014162600135607441, -0.1669477450960472, 0.11880997644846131, 0.37988324853571226, -0.18636212276675515, -0.28566918690709303, -0.020345972482978373, -0.29212311070657127, -0.127453213819323, 0.1804987086598374, 0.03957575178929489... |
709.1353 | Dynamics of Linear and Affine Maps | The well-known theory of "rational canonical form of an operator" describes
the invariant factors, or elementary divisors, as a complete set of invariants
of a similarity class of an operator on a finite-dimensional vector space $\V$
over a given field $\F$. A finer part of the theory is the contribution by
Frobenius... | math.DS math.GR | the wellknown theory of rational canonical form of an operator describes the invariant factors or elementary divisors as a complete set of invariants of a similarity class of an operator on a finitedimensional vector space v over a given field f a finer part of the theory is the contribution by frobenius dealing with t... | [['the', 'wellknown', 'theory', 'of', 'rational', 'canonical', 'form', 'of', 'an', 'operator', 'describes', 'the', 'invariant', 'factors', 'or', 'elementary', 'divisors', 'as', 'a', 'complete', 'set', 'of', 'invariants', 'of', 'a', 'similarity', 'class', 'of', 'an', 'operator', 'on', 'a', 'finitedimensional', 'vector',... | [-0.1558054855038216, 0.07056547736848236, -0.09157364926987181, 0.026169784674206505, -0.0588184074700908, -0.09004374774552784, 0.013997415950717894, 0.32223292487967564, -0.35413049665696333, -0.20031752100361414, 0.08689433280884068, -0.2583839579816221, -0.1911136683901484, 0.1952124832559524, -0.10460081037231966... |
709.1354 | The stellar mass assembly of galaxies from z=0 to z=4. Analysis of a
sample selected in the rest-frame near-infrared with Spitzer | Using a sample of ~28,000 sources selected at 3.6-4.5 microns with Spitzer
observations of the HDF-N, the CDF-S, and the Lockman Hole (surveyed area: ~664
arcmin^2), we study the evolution of the stellar mass content of the Universe
at 0<z<4. We calculate stellar masses and photometric redshifts, based on
~2,000 temp... | astro-ph | using a sample of 28000 sources selected at 3645 microns with spitzer observations of the hdfn the cdfs and the lockman hole surveyed area 664 arcmin2 we study the evolution of the stellar mass content of the universe at 0z4 we calculate stellar masses and photometric redshifts based on 2000 templates built with stella... | [['using', 'a', 'sample', 'of', '28000', 'sources', 'selected', 'at', '3645', 'microns', 'with', 'spitzer', 'observations', 'of', 'the', 'hdfn', 'the', 'cdfs', 'and', 'the', 'lockman', 'hole', 'surveyed', 'area', '664', 'arcmin2', 'we', 'study', 'the', 'evolution', 'of', 'the', 'stellar', 'mass', 'content', 'of', 'the'... | [-0.015114284298522058, 0.15002246148354054, -0.034048065569516894, 0.16126506362173257, -0.07636932713186953, -0.02260469912677106, 0.05320135052791749, 0.45865379704883064, -0.00821388607086736, -0.4215038171476501, 0.02050493548099074, -0.33008707420098304, 0.08497996386170326, 0.18641262285090154, -0.00414074510743... |
709.1355 | Enhancement of localization in one-dimensional random potentials with
long-range correlations | We experimentally study the effect of enhancement of localization in weak
one-dimensional random potentials. Our experimental setup is a single mode
waveguide with 100 tuneable scatterers periodically inserted into the
waveguide. By measuring the amplitudes of transmitted and reflected waves in
the spacing between ea... | cond-mat.dis-nn | we experimentally study the effect of enhancement of localization in weak onedimensional random potentials our experimental setup is a single mode waveguide with 100 tuneable scatterers periodically inserted into the waveguide by measuring the amplitudes of transmitted and reflected waves in the spacing between each pa... | [['we', 'experimentally', 'study', 'the', 'effect', 'of', 'enhancement', 'of', 'localization', 'in', 'weak', 'onedimensional', 'random', 'potentials', 'our', 'experimental', 'setup', 'is', 'a', 'single', 'mode', 'waveguide', 'with', '100', 'tuneable', 'scatterers', 'periodically', 'inserted', 'into', 'the', 'waveguide'... | [-0.2315395810874179, 0.25016198231263415, 0.0016227578607333057, -0.005213448036503156, 0.023396207810626093, -0.1954323453897172, 0.04820756766575334, 0.45148398661438155, -0.26492273851352577, -0.24178453111637602, -0.008206189764143132, -0.3337138953673489, -0.14120240627294955, 0.1608508550835883, 0.03572278957375... |
709.1356 | Iron lines from transient and persisting hot spots on AGN accretion
disks | [abridged] We model the X-ray reprocessing from a strong co-rotating flare
above an accretion disk in active galactic nuclei. We explore the horizontal
structure and evolution of the underlying hot spot. To obtain the spectral
evolution seen by a distant observer, we apply a general relativity ray-tracing
technique. ... | astro-ph | abridged we model the xray reprocessing from a strong corotating flare above an accretion disk in active galactic nuclei we explore the horizontal structure and evolution of the underlying hot spot to obtain the spectral evolution seen by a distant observer we apply a general relativity raytracing technique we concentr... | [['abridged', 'we', 'model', 'the', 'xray', 'reprocessing', 'from', 'a', 'strong', 'corotating', 'flare', 'above', 'an', 'accretion', 'disk', 'in', 'active', 'galactic', 'nuclei', 'we', 'explore', 'the', 'horizontal', 'structure', 'and', 'evolution', 'of', 'the', 'underlying', 'hot', 'spot', 'to', 'obtain', 'the', 'spe... | [-0.08935591063081202, 0.1655467391543789, -0.08064063650301911, 0.14833717832003127, -0.09061394121836533, -0.09807064828166569, 0.03859246530443091, 0.4356770021586933, -0.23278721077409997, -0.3319777063968253, 0.08167662099384787, -0.322089735056189, -0.021940030435269528, 0.2374357830885459, -0.026896721667124604,... |
709.1357 | The Millennium Galaxy Catalogue: The severe attenuation of bulge flux by
dusty spiral discs | Using the Millennium Galaxy Catalogue we quantify the dependency of the disc
and bulge luminosity functions on galaxy inclination. Using a contemporary dust
model we show that our results are consistent with galaxy discs being optically
thick in their central regions (tau_B^f=3.8+/-0.7). As a consequence the
measured... | astro-ph | using the millennium galaxy catalogue we quantify the dependency of the disc and bulge luminosity functions on galaxy inclination using a contemporary dust model we show that our results are consistent with galaxy discs being optically thick in their central regions tau_bf3807 as a consequence the measured bband fluxes... | [['using', 'the', 'millennium', 'galaxy', 'catalogue', 'we', 'quantify', 'the', 'dependency', 'of', 'the', 'disc', 'and', 'bulge', 'luminosity', 'functions', 'on', 'galaxy', 'inclination', 'using', 'a', 'contemporary', 'dust', 'model', 'we', 'show', 'that', 'our', 'results', 'are', 'consistent', 'with', 'galaxy', 'disc... | [0.015240952630205463, 0.0961537741994321, -0.07630079866776013, 0.09665855747709215, -0.08015912863672436, -0.02435732874266036, 0.01920293247060138, 0.4736362294814385, -0.1523579402042635, -0.35814535106970546, 0.04141849622572087, -0.2921308410655269, -0.010867298241732094, 0.20876015642692008, -0.07168183336205616... |
709.1358 | Mori-Zwanzig Equations With Time-Dependent Liouvillian | We extend the Mori-Zwanzig equations to the case where the Liouvillian is
time-dependent by way of a Dyson identity due to Holian and Evans. This
extension makes it possible to treat, for example, more general cases of
continuous-wave (cw) or pulsed irradiation in NMR and coherent optics. The
formalism immediately al... | physics.chem-ph physics.atom-ph | we extend the morizwanzig equations to the case where the liouvillian is timedependent by way of a dyson identity due to holian and evans this extension makes it possible to treat for example more general cases of continuouswave cw or pulsed irradiation in nmr and coherent optics the formalism immediately allows for re... | [['we', 'extend', 'the', 'morizwanzig', 'equations', 'to', 'the', 'case', 'where', 'the', 'liouvillian', 'is', 'timedependent', 'by', 'way', 'of', 'a', 'dyson', 'identity', 'due', 'to', 'holian', 'and', 'evans', 'this', 'extension', 'makes', 'it', 'possible', 'to', 'treat', 'for', 'example', 'more', 'general', 'cases',... | [-0.05563255499388712, 0.08967314177813629, -0.11094315341033507, 0.07653628699481488, -0.09420502330952635, -0.15977534452298034, 0.06612996364322801, 0.39070491325110196, -0.2615993260794009, -0.25770721489874027, 0.05620430987134265, -0.21959094964380105, -0.1451909411426944, 0.25682484802867594, -0.0618562610470689... |
709.1359 | A robust morphological classification of high-redshift galaxies using
support vector machines on seeing limited images. I Method description | We present a new non-parametric method to quantify morphologies of galaxies
based on a particular family of learning machines called support vector
machines. The method, that can be seen as a generalization of the classical CAS
classification but with an unlimited number of dimensions and non-linear
boundaries betwee... | astro-ph | we present a new nonparametric method to quantify morphologies of galaxies based on a particular family of learning machines called support vector machines the method that can be seen as a generalization of the classical cas classification but with an unlimited number of dimensions and nonlinear boundaries between deci... | [['we', 'present', 'a', 'new', 'nonparametric', 'method', 'to', 'quantify', 'morphologies', 'of', 'galaxies', 'based', 'on', 'a', 'particular', 'family', 'of', 'learning', 'machines', 'called', 'support', 'vector', 'machines', 'the', 'method', 'that', 'can', 'be', 'seen', 'as', 'a', 'generalization', 'of', 'the', 'clas... | [-0.021541493451916315, 0.04643937871423599, -0.09337608224533973, 0.08876122613288859, -0.11635223898660153, -0.13558712194257594, 0.0641606389614258, 0.43089311487497167, -0.2095086579785702, -0.35612969025375046, 0.11017987891793884, -0.2688474006376209, -0.06473532898495211, 0.23839516288382892, -0.0620547443192372... |
709.136 | Progress with Particle Flow Calorimetry | One of the most important requirements for a detector at the ILC is good jet
energy resolution. It is widely believed that the particle flow approach to
calorimetry is the key to achieving the ILC goal of a di-jet invariant mass
resolution sigma_m/m < Gamma_Z/m_Z. This paper describes the current
performance of the P... | physics.ins-det physics.data-an | one of the most important requirements for a detector at the ilc is good jet energy resolution it is widely believed that the particle flow approach to calorimetry is the key to achieving the ilc goal of a dijet invariant mass resolution sigma_mm gamma_zm_z this paper describes the current performance of the pandorapfa... | [['one', 'of', 'the', 'most', 'important', 'requirements', 'for', 'a', 'detector', 'at', 'the', 'ilc', 'is', 'good', 'jet', 'energy', 'resolution', 'it', 'is', 'widely', 'believed', 'that', 'the', 'particle', 'flow', 'approach', 'to', 'calorimetry', 'is', 'the', 'key', 'to', 'achieving', 'the', 'ilc', 'goal', 'of', 'a'... | [-0.06648663996376705, 0.11564980950016453, -0.10330008242127238, 0.10450645649035899, -0.050224370750769666, -0.12058836965802677, -0.08848432714608973, 0.3944811860897711, -0.2148091837310004, -0.35934175906835925, 0.02803740130347789, -0.26618691829356306, 0.06261667038066959, 0.23067771705052798, -0.008663882406390... |
709.1361 | Relaxation times of unstable states in systems with long range
interactions | We consider several models with long-range interactions evolving via
Hamiltonian dynamics. The microcanonical dynamics of the basic Hamiltonian Mean
Field (HMF) model and perturbed HMF models with either global anisotropy or an
on-site potential are studied both analytically and numerically. We find that
in the magne... | cond-mat.stat-mech | we consider several models with longrange interactions evolving via hamiltonian dynamics the microcanonical dynamics of the basic hamiltonian mean field hmf model and perturbed hmf models with either global anisotropy or an onsite potential are studied both analytically and numerically we find that in the magnetic phas... | [['we', 'consider', 'several', 'models', 'with', 'longrange', 'interactions', 'evolving', 'via', 'hamiltonian', 'dynamics', 'the', 'microcanonical', 'dynamics', 'of', 'the', 'basic', 'hamiltonian', 'mean', 'field', 'hmf', 'model', 'and', 'perturbed', 'hmf', 'models', 'with', 'either', 'global', 'anisotropy', 'or', 'an'... | [-0.19895382311616866, 0.26311970887859987, -0.07017658684975994, 0.08715639504678722, 0.04988777923468008, -0.14391218928207275, -0.007284255812542056, 0.3637188065726802, -0.2911698832802633, -0.30970013297145377, 0.06437871230322481, -0.2681530673696027, -0.10043770300426502, 0.12991043757471554, 0.09352822730071703... |
709.1362 | Quantum-field dynamics of expanding and contracting Bose-Einstein
condensates | We analyze the dynamics of quantum statistics in a harmonically trapped
Bose-Einstein condensate, whose two-body interaction strength is controlled via
a Feshbach resonance. From an initially non-interacting coherent state, the
quantum field undergoes Kerr squeezing, which can be qualitatively described
with a single... | cond-mat.other | we analyze the dynamics of quantum statistics in a harmonically trapped boseeinstein condensate whose twobody interaction strength is controlled via a feshbach resonance from an initially noninteracting coherent state the quantum field undergoes kerr squeezing which can be qualitatively described with a single mode mod... | [['we', 'analyze', 'the', 'dynamics', 'of', 'quantum', 'statistics', 'in', 'a', 'harmonically', 'trapped', 'boseeinstein', 'condensate', 'whose', 'twobody', 'interaction', 'strength', 'is', 'controlled', 'via', 'a', 'feshbach', 'resonance', 'from', 'an', 'initially', 'noninteracting', 'coherent', 'state', 'the', 'quant... | [-0.17475840261889786, 0.2754268232820323, -0.11798303015677471, 0.019601855441762864, -0.0005934695842899853, -0.21932723083757336, 0.032995380321222866, 0.36771613647100293, -0.23625971570233756, -0.20520297265788423, -0.05416798618286141, -0.21748145471645308, -0.10243395414745694, 0.2121875787984957, 0.067301897878... |
709.1363 | Electron-ion recombination of Si IV forming Si III: Storage-ring
measurement and multiconfiguration Dirac-Fock calculations | The electron-ion recombination rate coefficient for Si IV forming Si III was
measured at the heavy-ion storage-ring TSR. The experimental electron-ion
collision energy range of 0-186 eV encompassed the 2p(6) nl n'l' dielectronic
recombination (DR) resonances associated with 3s to nl core excitations, 2s
2p(6) 3s nl n... | physics.atom-ph astro-ph | the electronion recombination rate coefficient for si iv forming si iii was measured at the heavyion storagering tsr the experimental electronion collision energy range of 0186 ev encompassed the 2p6 nl nl dielectronic recombination dr resonances associated with 3s to nl core excitations 2s 2p6 3s nl nl resonances asso... | [['the', 'electronion', 'recombination', 'rate', 'coefficient', 'for', 'si', 'iv', 'forming', 'si', 'iii', 'was', 'measured', 'at', 'the', 'heavyion', 'storagering', 'tsr', 'the', 'experimental', 'electronion', 'collision', 'energy', 'range', 'of', '0186', 'ev', 'encompassed', 'the', '2p6', 'nl', 'nl', 'dielectronic', ... | [-0.04320637987507152, 0.13350208137070632, 0.15561410808893106, 0.10170726919944846, 0.03460524892007918, -0.2416660665456234, 0.03371933830736688, 0.3510558559125616, -0.1737332081391995, -0.30268379646346316, -0.09142853840048076, -0.38779102337639065, 0.04318195736286309, 0.129480415011422, 0.18828233533880126, 0.0... |
709.1364 | The process gg->WW as a probe into the EWSB mechanism | We present the first estimate of the gluon-gluon fusion process, gg->4f, in
the high energy domain as a probe of the electroweak symmetry breaking
mechanism (EWSB). We consider the exact matrix element at
$O(\alpha_s\alpha_{em}^2)$, and we include all irreducible background coming
from qq->4f. Purely leptonic final s... | hep-ph | we present the first estimate of the gluongluon fusion process gg4f in the high energy domain as a probe of the electroweak symmetry breaking mechanism ewsb we consider the exact matrix element at oalpha_salpha_em2 and we include all irreducible background coming from qq4f purely leptonic final states ppllvv are numeri... | [['we', 'present', 'the', 'first', 'estimate', 'of', 'the', 'gluongluon', 'fusion', 'process', 'gg4f', 'in', 'the', 'high', 'energy', 'domain', 'as', 'a', 'probe', 'of', 'the', 'electroweak', 'symmetry', 'breaking', 'mechanism', 'ewsb', 'we', 'consider', 'the', 'exact', 'matrix', 'element', 'at', 'oalpha_salpha_em2', '... | [-0.09034678195329274, 0.21355070241124313, -0.07677610752117985, 0.14593992445094472, -0.08411500383825864, -0.13272075100308833, 0.03856080978670541, 0.35899378061294557, -0.2973316267132759, -0.2492078400490915, 0.09504587661666686, -0.2538313814164961, -0.07437427952022785, 0.08597288017763811, 0.06763932706021211,... |
709.1365 | Four-point functions of different-weight operators in the AdS/CFT
correspondence | We calculate four-point correlation functions of two weight-2 and two
weight-3 1/2-BPS operators in \mathcal{N}=4 SYM in the large N limit in
supergravity approximation. By the AdS/CFT conjecture, these operators are dual
to AdS supergravity scalar fields s_2 and s_3 with mass m^2 = -4 and m^2 = -3
respectively. This... | hep-th | we calculate fourpoint correlation functions of two weight2 and two weight3 12bps operators in mathcaln4 sym in the large n limit in supergravity approximation by the adscft conjecture these operators are dual to ads supergravity scalar fields s_2 and s_3 with mass m2 4 and m2 3 respectively this is the first nontrivia... | [['we', 'calculate', 'fourpoint', 'correlation', 'functions', 'of', 'two', 'weight2', 'and', 'two', 'weight3', '12bps', 'operators', 'in', 'mathcaln4', 'sym', 'in', 'the', 'large', 'n', 'limit', 'in', 'supergravity', 'approximation', 'by', 'the', 'adscft', 'conjecture', 'these', 'operators', 'are', 'dual', 'to', 'ads',... | [-0.1576489899718367, 0.20521370891262503, -0.032350515129555966, 0.09616024746541299, -0.023729489917647752, -0.13018566612884694, -0.04620397101982734, 0.2841325996023621, -0.1495767488217383, -0.2337589535916991, 0.07025174745792231, -0.34020748719636934, -0.2034012692291107, 0.11252222760060035, 0.02043505491889721... |
709.1366 | Multiwavelength modeling of TeV AGN observed by HESS | The High Energy Stereoscopic System (H.E.S.S.) experiment, a ground-based
gamma-ray Cherenkov telescope array located in Namibia, has now detected many
extragalactic objects, which redshifts range from z=0.00183 up to z=0.2,
possibly more. With the increasing performances of Cherenkov telescopes, it now
becomes possi... | astro-ph | the high energy stereoscopic system hess experiment a groundbased gammaray cherenkov telescope array located in namibia has now detected many extragalactic objects which redshifts range from z000183 up to z02 possibly more with the increasing performances of cherenkov telescopes it now becomes possible to probe these o... | [['the', 'high', 'energy', 'stereoscopic', 'system', 'hess', 'experiment', 'a', 'groundbased', 'gammaray', 'cherenkov', 'telescope', 'array', 'located', 'in', 'namibia', 'has', 'now', 'detected', 'many', 'extragalactic', 'objects', 'which', 'redshifts', 'range', 'from', 'z000183', 'up', 'to', 'z02', 'possibly', 'more',... | [-0.05362220635527412, 0.1558031201079164, -0.06087819965115348, 0.191147155080616, -0.1635909048378679, -0.11785105813591593, 0.005192541708530867, 0.4517988906655874, -0.1780319183841033, -0.41158224600434734, 0.023376753364221736, -0.3393745871085296, -0.0019314430995983779, 0.2760639017968605, -0.006796208110183549... |
709.1367 | Feedback from the first stars and galaxies and its influence on
structure formation | Once the first sources have formed, their mass deposition, energy injection
and emitted radiation can deeply affect the subsequent galaxy formation process
and influence the evolution of the IGM via a number of so-called feedback
effects. The word 'feedback' is by far one of the most used in modern
cosmology, where i... | astro-ph | once the first sources have formed their mass deposition energy injection and emitted radiation can deeply affect the subsequent galaxy formation process and influence the evolution of the igm via a number of socalled feedback effects the word feedback is by far one of the most used in modern cosmology where it is appl... | [['once', 'the', 'first', 'sources', 'have', 'formed', 'their', 'mass', 'deposition', 'energy', 'injection', 'and', 'emitted', 'radiation', 'can', 'deeply', 'affect', 'the', 'subsequent', 'galaxy', 'formation', 'process', 'and', 'influence', 'the', 'evolution', 'of', 'the', 'igm', 'via', 'a', 'number', 'of', 'socalled'... | [-0.0685546506560691, 0.1690313611422544, -0.08483349001262863, 0.0704812440736809, -0.10530018174980321, -0.057174614505113464, 0.05345991847267293, 0.3374032276439602, -0.25752627037809755, -0.30711206788116174, 0.10550510798601191, -0.2766947434243301, -0.094351019633367, 0.21660784288188037, -0.008275788937411878, ... |
709.1368 | Diffractive Excitation in DIS and pp Collisions | We have in earlier papers presented an extension of Mueller's dipole cascade
model, which includes subleading effects from energy conservation and running
coupling as well as colour suppressed effects from pomeron loops via a ``dipole
swing''. The model was applied to describe the total cross sections in pp and
gamma... | hep-ph | we have in earlier papers presented an extension of muellers dipole cascade model which includes subleading effects from energy conservation and running coupling as well as colour suppressed effects from pomeron loops via a dipole swing the model was applied to describe the total cross sections in pp and gammap collisi... | [['we', 'have', 'in', 'earlier', 'papers', 'presented', 'an', 'extension', 'of', 'muellers', 'dipole', 'cascade', 'model', 'which', 'includes', 'subleading', 'effects', 'from', 'energy', 'conservation', 'and', 'running', 'coupling', 'as', 'well', 'as', 'colour', 'suppressed', 'effects', 'from', 'pomeron', 'loops', 'via... | [-0.04570159610011615, 0.15340055202324782, -0.11240483906592337, 0.10762752793710785, -0.02371645306596871, -0.06983429379265131, 0.010949893679274035, 0.3538685520536753, -0.22187980652796052, -0.30056285035574215, -0.015362395500811876, -0.3302994714242893, -0.0935795335046185, 0.15675403587705328, 0.054529051541149... |
709.1369 | On the Wu metric in unbounded domains | We discuss the properties of the Wu pseudometric and present counterexamples
for its upper semicontinuity that answers the question posed by Jarnicki and
Pflug. We also give formulae for the Wu pseudometric in elementary Reinhardt
domains.
| math.CV | we discuss the properties of the wu pseudometric and present counterexamples for its upper semicontinuity that answers the question posed by jarnicki and pflug we also give formulae for the wu pseudometric in elementary reinhardt domains | [['we', 'discuss', 'the', 'properties', 'of', 'the', 'wu', 'pseudometric', 'and', 'present', 'counterexamples', 'for', 'its', 'upper', 'semicontinuity', 'that', 'answers', 'the', 'question', 'posed', 'by', 'jarnicki', 'and', 'pflug', 'we', 'also', 'give', 'formulae', 'for', 'the', 'wu', 'pseudometric', 'in', 'elementar... | [-0.13902718563460642, 0.0454596354953133, -0.059009108575992286, 0.14357710054092523, -0.11242494980494182, -0.13959387476400784, 0.11687342915037233, 0.3313799637318071, -0.25117540711330044, -0.2662525205459032, 0.119989420167662, -0.2685962511588716, -0.18770207899473867, 0.23299558833241463, -0.20996248939385018, ... |
709.137 | Self-interacting polynomials | We introduce a class of dynamical systems of algebraic origin, consisting of
self-interacting irreducible polynomials over a field. A polynomial f is made
to act on a polynomial g by mapping the roots of g. This action identifies a
new polynomial h, as the minimal polynomial of the displaced roots. By allowing
severa... | math.DS | we introduce a class of dynamical systems of algebraic origin consisting of selfinteracting irreducible polynomials over a field a polynomial f is made to act on a polynomial g by mapping the roots of g this action identifies a new polynomial h as the minimal polynomial of the displaced roots by allowing several polyno... | [['we', 'introduce', 'a', 'class', 'of', 'dynamical', 'systems', 'of', 'algebraic', 'origin', 'consisting', 'of', 'selfinteracting', 'irreducible', 'polynomials', 'over', 'a', 'field', 'a', 'polynomial', 'f', 'is', 'made', 'to', 'act', 'on', 'a', 'polynomial', 'g', 'by', 'mapping', 'the', 'roots', 'of', 'g', 'this', 'a... | [-0.22668802675504524, 0.09406767680775374, -0.12581011396832764, 0.03110599908261345, -0.13862941352328143, -0.12629113161193134, 0.005301172791335445, 0.29123897920810404, -0.31111933239914763, -0.21176986994060615, 0.0757117834795141, -0.24030399351165846, -0.17692870344035327, 0.2210878534332061, -0.029219597143730... |
709.1371 | On the Dipole Swing and the Search for Frame Independence in the Dipole
Model | Small-x evolution in QCD is conveniently described by Mueller's dipole model
which, however, does not include saturation effects in a way consistent with
boost invariance. In this paper we first show that the recently studied zero
and one dimensional toy models exhibiting saturation and explicit boost
invariance can ... | hep-ph | smallx evolution in qcd is conveniently described by muellers dipole model which however does not include saturation effects in a way consistent with boost invariance in this paper we first show that the recently studied zero and one dimensional toy models exhibiting saturation and explicit boost invariance can be inte... | [['smallx', 'evolution', 'in', 'qcd', 'is', 'conveniently', 'described', 'by', 'muellers', 'dipole', 'model', 'which', 'however', 'does', 'not', 'include', 'saturation', 'effects', 'in', 'a', 'way', 'consistent', 'with', 'boost', 'invariance', 'in', 'this', 'paper', 'we', 'first', 'show', 'that', 'the', 'recently', 'st... | [-0.13778758333225188, 0.17127105018830505, -0.04728451363013752, 0.049820087155616234, -0.0689210283112359, -0.13706619532554057, -0.027746936473955305, 0.3868815978218255, -0.22013617180546763, -0.3093467006331374, 0.008837545665928388, -0.2779185570945064, -0.11132587075377975, 0.09731219555973879, 0.012057974304329... |
709.1372 | The reflecting surface of the MAGIC-II Telescope | The MAGIC Collaboration is building a second telescope, MAGIC II, improving
the design of the current MAGIC Telescope. MAGIC II is being built at 85 m of
distance from MAGIC I, and will also feature a huge reflecting surface of ~240
m$^2$ of area. One of the improvement is the design for the mirror of MAGIC II,
that ... | astro-ph | the magic collaboration is building a second telescope magic ii improving the design of the current magic telescope magic ii is being built at 85 m of distance from magic i and will also feature a huge reflecting surface of 240 m2 of area one of the improvement is the design for the mirror of magic ii that are lighter ... | [['the', 'magic', 'collaboration', 'is', 'building', 'a', 'second', 'telescope', 'magic', 'ii', 'improving', 'the', 'design', 'of', 'the', 'current', 'magic', 'telescope', 'magic', 'ii', 'is', 'being', 'built', 'at', '85', 'm', 'of', 'distance', 'from', 'magic', 'i', 'and', 'will', 'also', 'feature', 'a', 'huge', 'refl... | [-0.0610465739077578, 0.17765880992153177, -0.028611177119805858, 0.027101499762998343, -0.04880428142431709, -0.16888163069401074, 0.04152722501333941, 0.39740734710185616, -0.17920955125311458, -0.374775162504779, 0.1776960487882779, -0.3136042086062608, -0.054509332148289236, 0.21719922207778802, -0.0465996556880849... |
709.1373 | Parallax and Luminosity Measurements of an L Subdwarf | We present the first parallax and luminosity measurements for an L subdwarf,
the sdL7 2MASS J05325346+8246465. Observations conducted over three years by
the USNO infrared astrometry program yield an astrometric distance of
26.7+/-1.2 pc and a proper motion of 2.6241+/-0.0018"/yr. Combined with
broadband spectral and... | astro-ph | we present the first parallax and luminosity measurements for an l subdwarf the sdl7 2mass j053253468246465 observations conducted over three years by the usno infrared astrometry program yield an astrometric distance of 26712 pc and a proper motion of 2624100018yr combined with broadband spectral and photometric measu... | [['we', 'present', 'the', 'first', 'parallax', 'and', 'luminosity', 'measurements', 'for', 'an', 'l', 'subdwarf', 'the', 'sdl7', '2mass', 'j053253468246465', 'observations', 'conducted', 'over', 'three', 'years', 'by', 'the', 'usno', 'infrared', 'astrometry', 'program', 'yield', 'an', 'astrometric', 'distance', 'of', '... | [-0.051224213917004435, 0.10741858148026757, -0.08746191932770767, 0.08476801728569339, -0.1316300335095117, -0.07805094169514058, 0.11222221120260656, 0.4119433262434445, -0.15129354484379293, -0.3736002128620289, 0.0649085587680977, -0.2741105718146029, 0.03718347725654511, 0.2075975323151062, -0.08673787879111172, -... |
709.1374 | Lithium abundances in the old open cluster NGC 3960 from VLT/FLAMES
observations | Old open clusters are very useful targets to investigate mechanisms
responsible for lithium (Li) depletion during the main sequence. Comparison of
the Li abundances in clusters of different age allows us to understand the
efficiency of the Li destruction process. Our goal is the determination of
membership and Li abu... | astro-ph | old open clusters are very useful targets to investigate mechanisms responsible for lithium li depletion during the main sequence comparison of the li abundances in clusters of different age allows us to understand the efficiency of the li destruction process our goal is the determination of membership and li abundance... | [['old', 'open', 'clusters', 'are', 'very', 'useful', 'targets', 'to', 'investigate', 'mechanisms', 'responsible', 'for', 'lithium', 'li', 'depletion', 'during', 'the', 'main', 'sequence', 'comparison', 'of', 'the', 'li', 'abundances', 'in', 'clusters', 'of', 'different', 'age', 'allows', 'us', 'to', 'understand', 'the... | [-0.032776186419381396, 0.13589623750497584, -0.05733779123744709, 0.0714587227539362, -0.07141552697657533, -0.06129015176302463, 0.15328438163523853, 0.3973133388584423, -0.1459755325394943, -0.42230547524365775, -0.000544157483722787, -0.31038455814359917, 0.0274191433354206, 0.17678120461969346, -0.0917159135639068... |
709.1375 | Toward a Deterministic Model of Planetary Formation IV: Effects of
Type-I Migration | In a further development of a deterministic planet-formation model (Ida & Lin
2004), we consider the effect of type-I migration of protoplanetary embryos due
to their tidal interaction with their nascent disks. During the early embedded
phase of protostellar disks, although embryos rapidly emerge in regions
interior ... | astro-ph | in a further development of a deterministic planetformation model ida lin 2004 we consider the effect of typei migration of protoplanetary embryos due to their tidal interaction with their nascent disks during the early embedded phase of protostellar disks although embryos rapidly emerge in regions interior to the ice ... | [['in', 'a', 'further', 'development', 'of', 'a', 'deterministic', 'planetformation', 'model', 'ida', 'lin', '2004', 'we', 'consider', 'the', 'effect', 'of', 'typei', 'migration', 'of', 'protoplanetary', 'embryos', 'due', 'to', 'their', 'tidal', 'interaction', 'with', 'their', 'nascent', 'disks', 'during', 'the', 'earl... | [-0.11313511173838102, 0.187297320851887, -0.037429823888395324, 0.06892614518849018, -0.0659001756415608, -0.04858647175200716, 0.06869768957561895, 0.3443973443725659, -0.21301549520896937, -0.3398180781505948, 0.08642246501024245, -0.23449227036368372, -0.04719272622099632, 0.1496189100392824, -0.045769826578232795,... |
709.1376 | Time-reversal properties in the coupling of quantum angular momenta | After a synoptic panorama about some still unsolved foundational problems
involving time-reversal, we show that the \emph{double time-reversal
superselection rule} of Nonrelativistic Quantum Mechanics is redundant. We then
analyze which, among the symmetries of the Clebsch-Gordan coefficients, may be
inferred through... | quant-ph math-ph math.MP | after a synoptic panorama about some still unsolved foundational problems involving timereversal we show that the emphdouble timereversal superselection rule of nonrelativistic quantum mechanics is redundant we then analyze which among the symmetries of the clebschgordan coefficients may be inferred through timereversa... | [['after', 'a', 'synoptic', 'panorama', 'about', 'some', 'still', 'unsolved', 'foundational', 'problems', 'involving', 'timereversal', 'we', 'show', 'that', 'the', 'emphdouble', 'timereversal', 'superselection', 'rule', 'of', 'nonrelativistic', 'quantum', 'mechanics', 'is', 'redundant', 'we', 'then', 'analyze', 'which'... | [-0.1635325563869341, 0.22509254822139874, -0.0792030813141824, 0.07042434075265191, -0.09392680011469086, -0.1419192478949155, 0.027107689674410625, 0.3135810089726491, -0.282418323956479, -0.27007498883176595, 0.06215456609022926, -0.2505557144476801, -0.1288680690095613, 0.1363064645005292, -0.02827546117508686, 0.0... |
709.1377 | Confinement of the Sun's interior magnetic field: some exact
boundary-layer solutions | High-latitude laminar confinement of the Sun's interior magnetic field is
shown to be possible, as originally proposed by Gough and McIntyre (1998) but
contrary to a recent claim by Brun and Zahn (A&A 2006). Mean downwelling as
weak as 2x10^-6cm/s -- gyroscopically pumped by turbulent stresses in the
overlying convec... | astro-ph | highlatitude laminar confinement of the suns interior magnetic field is shown to be possible as originally proposed by gough and mcintyre 1998 but contrary to a recent claim by brun and zahn aa 2006 mean downwelling as weak as 2x106cms gyroscopically pumped by turbulent stresses in the overlying convection zone andor t... | [['highlatitude', 'laminar', 'confinement', 'of', 'the', 'suns', 'interior', 'magnetic', 'field', 'is', 'shown', 'to', 'be', 'possible', 'as', 'originally', 'proposed', 'by', 'gough', 'and', 'mcintyre', '1998', 'but', 'contrary', 'to', 'a', 'recent', 'claim', 'by', 'brun', 'and', 'zahn', 'aa', '2006', 'mean', 'downwell... | [-0.13784824982993224, 0.18076298298322677, -0.04206316220463307, 0.06420634235440044, -0.07263573300963194, -0.09159948534049127, 0.05644851824984627, 0.32737827207816206, -0.2500713509181822, -0.3213162700879482, 0.11018941303948966, -0.2032563765582309, -0.0631801439100458, 0.18905430255121333, -0.06628754531804652,... |
709.1378 | Chaos in the thermal regime for pinned manifolds via functional RG | The statistical correlations of two copies of a d-dimensional elastic
manifold embedded in slightly different frozen disorder are studied using the
Functional Renormalization Group to one-loop accuracy, order O(eps = 4-d).
Determining the initial (short scale) growth of mutual correlations, i.e. chaos
exponents, requ... | cond-mat.dis-nn | the statistical correlations of two copies of a ddimensional elastic manifold embedded in slightly different frozen disorder are studied using the functional renormalization group to oneloop accuracy order oeps 4d determining the initial short scale growth of mutual correlations ie chaos exponents requires control of a... | [['the', 'statistical', 'correlations', 'of', 'two', 'copies', 'of', 'a', 'ddimensional', 'elastic', 'manifold', 'embedded', 'in', 'slightly', 'different', 'frozen', 'disorder', 'are', 'studied', 'using', 'the', 'functional', 'renormalization', 'group', 'to', 'oneloop', 'accuracy', 'order', 'oeps', '4d', 'determining',... | [-0.19395086826949284, 0.18084380717241558, -0.09578845064187871, 0.0832804574711441, 0.005195476419436906, -0.1744813607507867, 0.026964702710292526, 0.3075228501890047, -0.2489090311308873, -0.2529395507134754, 0.08342512408672864, -0.3126830066963709, -0.13207528887252357, 0.13674032843896541, 0.00897387549489865, 0... |
709.1379 | Enhancement of the Benjamin-Feir instability with dissipation | It is shown that there is an overlooked mechanism whereby some kinds of
dissipation can enhance the Benjamin-Feir instability of water waves. This
observation is new, and although it is counterintuitive, it is due to the fact
that the Benjamin-Feir instability involves the collision of modes with
opposite energy sign... | physics.class-ph math.AP physics.ao-ph | it is shown that there is an overlooked mechanism whereby some kinds of dissipation can enhance the benjaminfeir instability of water waves this observation is new and although it is counterintuitive it is due to the fact that the benjaminfeir instability involves the collision of modes with opposite energy sign relati... | [['it', 'is', 'shown', 'that', 'there', 'is', 'an', 'overlooked', 'mechanism', 'whereby', 'some', 'kinds', 'of', 'dissipation', 'can', 'enhance', 'the', 'benjaminfeir', 'instability', 'of', 'water', 'waves', 'this', 'observation', 'is', 'new', 'and', 'although', 'it', 'is', 'counterintuitive', 'it', 'is', 'due', 'to', ... | [-0.19994571862133362, 0.21100331934083863, -0.10092290413494294, 0.07955922200881804, -0.10752875908063009, -0.10732313125179364, -0.033464113680215984, 0.31923574799528487, -0.3036661349810087, -0.2632080665001502, 0.09758301847256147, -0.27640949874543225, -0.20274937069759918, 0.18204348611717042, -0.03664923496544... |
709.138 | Observation of GRBs by the MAGIC Telescope, Status and Outlook | Observation of Gamma Ray Bursts (GRBs) in the Very High Energy (VHE) domain
will provide important information on the physical conditions in GRB outflows.
The MAGIC telescope is the best suited Imaging Atmospheric Cherenkov Telescope
(IACT) for these observations. Thanks to its fast repositioning time and low
energy ... | astro-ph | observation of gamma ray bursts grbs in the very high energy vhe domain will provide important information on the physical conditions in grb outflows the magic telescope is the best suited imaging atmospheric cherenkov telescope iact for these observations thanks to its fast repositioning time and low energy threshold ... | [['observation', 'of', 'gamma', 'ray', 'bursts', 'grbs', 'in', 'the', 'very', 'high', 'energy', 'vhe', 'domain', 'will', 'provide', 'important', 'information', 'on', 'the', 'physical', 'conditions', 'in', 'grb', 'outflows', 'the', 'magic', 'telescope', 'is', 'the', 'best', 'suited', 'imaging', 'atmospheric', 'cherenkov... | [-0.04680801460265436, 0.1994365364151952, -0.03889323912814937, 0.1526605800600285, -0.14601692219377693, -0.11182261115843148, 0.09417365675802682, 0.49523708991932147, -0.16695683462559385, -0.37117776387568674, 0.09795757024160896, -0.2966860987909251, -0.02104457614901052, 0.25024652682160115, -0.00816551641081318... |
709.1381 | Towards a dephasing diode: asymmetric and geometric dephasing | We study the effect of a noisy environment on spin and charge transport in
ballistic quantum wires with spin-orbit coupling (Rashba coupling). We find
that the wire then acts as a ``dephasing diode'', inducing very different
dephasing of the spins of right and left movers. We also show how Berry phase
(geometric phas... | cond-mat.mes-hall cond-mat.dis-nn quant-ph | we study the effect of a noisy environment on spin and charge transport in ballistic quantum wires with spinorbit coupling rashba coupling we find that the wire then acts as a dephasing diode inducing very different dephasing of the spins of right and left movers we also show how berry phase geometric phase in a curved... | [['we', 'study', 'the', 'effect', 'of', 'a', 'noisy', 'environment', 'on', 'spin', 'and', 'charge', 'transport', 'in', 'ballistic', 'quantum', 'wires', 'with', 'spinorbit', 'coupling', 'rashba', 'coupling', 'we', 'find', 'that', 'the', 'wire', 'then', 'acts', 'as', 'a', 'dephasing', 'diode', 'inducing', 'very', 'differ... | [-0.2154534433530756, 0.25624258796044863, -0.08581379524162824, 0.024234467066813214, -0.0395828843991979, -0.21089594552562718, 0.022113543584471547, 0.4663721413676997, -0.30995806611805077, -0.24257589556860276, -0.018908770153220428, -0.28129581519099606, -0.158946196627186, 0.17873999597336424, -0.041925455078886... |
709.1382 | Hysteretic response of electron-nuclear spin system in single InAlAs
quantum dots:Excitation power and polarization dependences | We report the hysteresis of optically-pumped nuclear spin polarization and
the degree of circular polarization of photoluminescence on the excitation
power and electron spin polarization in single InAlAs quantum dots. By
increasing (or decreasing) the excitation power at a particular excitation
polarization, an abrup... | cond-mat.mtrl-sci cond-mat.other | we report the hysteresis of opticallypumped nuclear spin polarization and the degree of circular polarization of photoluminescence on the excitation power and electron spin polarization in single inalas quantum dots by increasing or decreasing the excitation power at a particular excitation polarization an abrupt rise ... | [['we', 'report', 'the', 'hysteresis', 'of', 'opticallypumped', 'nuclear', 'spin', 'polarization', 'and', 'the', 'degree', 'of', 'circular', 'polarization', 'of', 'photoluminescence', 'on', 'the', 'excitation', 'power', 'and', 'electron', 'spin', 'polarization', 'in', 'single', 'inalas', 'quantum', 'dots', 'by', 'incre... | [-0.15444038814632222, 0.2403481691995694, -0.03437047024955973, 0.026752424216247163, 0.030133325960487126, -0.13863351709442212, 0.032427919136825946, 0.42131938971579075, -0.25654769863103866, -0.3017987553495914, -0.027808109893230723, -0.28244027790613474, -0.07909867793903685, 0.1783367153769359, 0.06301097419694... |
709.1383 | Decoherence induced by an interacting spin environment in the transition
from integrability to chaos | We investigate the decoherence properties of a central system composed of two
spins 1/2 in contact with a spin bath. The dynamical regime of the bath ranges
from a fully integrable integrable limit to complete chaoticity. We show that
the dynamical regime of the bath determines the efficiency of the decoherence
proce... | cond-mat.mes-hall astro-ph cond-mat.dis-nn quant-ph | we investigate the decoherence properties of a central system composed of two spins 12 in contact with a spin bath the dynamical regime of the bath ranges from a fully integrable integrable limit to complete chaoticity we show that the dynamical regime of the bath determines the efficiency of the decoherence process fo... | [['we', 'investigate', 'the', 'decoherence', 'properties', 'of', 'a', 'central', 'system', 'composed', 'of', 'two', 'spins', '12', 'in', 'contact', 'with', 'a', 'spin', 'bath', 'the', 'dynamical', 'regime', 'of', 'the', 'bath', 'ranges', 'from', 'a', 'fully', 'integrable', 'integrable', 'limit', 'to', 'complete', 'chao... | [-0.16070280866397574, 0.18398001489130725, -0.09054126636350923, 0.09235136721256575, 0.008575253992934118, -0.1338367711031231, 0.04395243878984316, 0.29805521432761894, -0.24961269071861875, -0.20500842476207198, 0.07738097377340168, -0.28830320293182565, -0.09442795404042541, 0.2285911789230974, -0.0134773816186652... |
709.1384 | Flavor states of mixed neutrinos | By resorting to previous results on flavor mixing in Quantum Field Theory, we
show how to consistently define flavor states of mixed neutrinos as eigenstates
of the flavor charge operators.
| hep-ph | by resorting to previous results on flavor mixing in quantum field theory we show how to consistently define flavor states of mixed neutrinos as eigenstates of the flavor charge operators | [['by', 'resorting', 'to', 'previous', 'results', 'on', 'flavor', 'mixing', 'in', 'quantum', 'field', 'theory', 'we', 'show', 'how', 'to', 'consistently', 'define', 'flavor', 'states', 'of', 'mixed', 'neutrinos', 'as', 'eigenstates', 'of', 'the', 'flavor', 'charge', 'operators']] | [-0.05697279297746718, 0.3361723560063789, -0.05326009690761566, 0.1365638759297629, -0.0008402223465964198, -0.11063591521233321, 0.11454121560867254, 0.32460513344655434, -0.20432732912401358, -0.28607478297005096, -0.012130202093006422, -0.24521713554859162, -0.07527070119976997, 0.08075618703539172, -0.026389941697... |
709.1385 | A nonlinear Poisson formula for the Schrodinger operator | We prove a nonlinear Poisson type formula for the Schrodinger group. Such a
formula had been derived in a previous paper by the authors, as a consequence
of the study of the asymptotic behavior of nonlinear wave operators for small
data. In this note, we propose a direct proof, and extend the range allowed for
the po... | math.AP math.FA | we prove a nonlinear poisson type formula for the schrodinger group such a formula had been derived in a previous paper by the authors as a consequence of the study of the asymptotic behavior of nonlinear wave operators for small data in this note we propose a direct proof and extend the range allowed for the power of ... | [['we', 'prove', 'a', 'nonlinear', 'poisson', 'type', 'formula', 'for', 'the', 'schrodinger', 'group', 'such', 'a', 'formula', 'had', 'been', 'derived', 'in', 'a', 'previous', 'paper', 'by', 'the', 'authors', 'as', 'a', 'consequence', 'of', 'the', 'study', 'of', 'the', 'asymptotic', 'behavior', 'of', 'nonlinear', 'wave... | [-0.14805994795201577, 0.03902177474372191, -0.060419054013000774, 0.052074594230212476, -0.12616725462131612, -0.07475568168503169, 0.03386941262080704, 0.30282630465210303, -0.2479477685506213, -0.2481790869560552, 0.11907090439639781, -0.2646035276710579, -0.17196274664865374, 0.24454178357471343, -0.040833958517122... |
709.1386 | MAGIC upper limits on the high energy emission from GRBs | During its cycle-1 observation period, between April 2005 and March 2006, the
MAGIC telescope was able to observe nine Gamma Ray Burst (GRB) events since
their early beginning. Other observations were performed during the following
months in the cycle-2 observation period. The observations, with an energy
threshold s... | astro-ph | during its cycle1 observation period between april 2005 and march 2006 the magic telescope was able to observe nine gamma ray burst grb events since their early beginning other observations were performed during the following months in the cycle2 observation period the observations with an energy threshold spanning fro... | [['during', 'its', 'cycle1', 'observation', 'period', 'between', 'april', '2005', 'and', 'march', '2006', 'the', 'magic', 'telescope', 'was', 'able', 'to', 'observe', 'nine', 'gamma', 'ray', 'burst', 'grb', 'events', 'since', 'their', 'early', 'beginning', 'other', 'observations', 'were', 'performed', 'during', 'the', ... | [-0.061008429599718916, 0.2049588358302976, -0.08937748289253149, 0.09536014435191949, -0.10664796959091392, -0.08609443158946103, 0.07535750880940921, 0.4402449919221302, -0.17656701918717266, -0.421594039702581, 0.10270213112235069, -0.30781915727485387, -0.01681532754252354, 0.231092675578677, -0.013633953474668992,... |
709.1387 | Kurt Goedel and His Universe | A portrait of Kurt Goedel with emphasis on his work on relativity theory and
idealistic philosophy.
| physics.hist-ph gr-qc | a portrait of kurt goedel with emphasis on his work on relativity theory and idealistic philosophy | [['a', 'portrait', 'of', 'kurt', 'goedel', 'with', 'emphasis', 'on', 'his', 'work', 'on', 'relativity', 'theory', 'and', 'idealistic', 'philosophy']] | [-0.0961782522208523, -0.015566106711048633, -0.21578295645304024, 0.10701448214967968, -0.156377526873257, -0.20361179622705095, 0.03674371950182831, 0.21189614737522788, -0.07014942020759918, -0.3069795824121684, 0.1269494843436405, -0.2717239201301709, -0.2383053656667471, 0.2190911920624785, -0.268860969285015, -0.... |
709.1388 | Exact shering box solutions of MHD flows with resistivity, viscosity and
cooling | Axisymmetric incompressible modes of the magneto-rotational instability (MRI)
with a vertical wavenumber are exact solutions of the non-linear local
equations of motion for a disk (shearing box). They are referred to as "channel
solutions". Here, we generalize a class of these solutions to include energy
losses, visc... | astro-ph | axisymmetric incompressible modes of the magnetorotational instability mri with a vertical wavenumber are exact solutions of the nonlinear local equations of motion for a disk shearing box they are referred to as channel solutions here we generalize a class of these solutions to include energy losses viscous and resist... | [['axisymmetric', 'incompressible', 'modes', 'of', 'the', 'magnetorotational', 'instability', 'mri', 'with', 'a', 'vertical', 'wavenumber', 'are', 'exact', 'solutions', 'of', 'the', 'nonlinear', 'local', 'equations', 'of', 'motion', 'for', 'a', 'disk', 'shearing', 'box', 'they', 'are', 'referred', 'to', 'as', 'channel'... | [-0.14652104603326577, 0.11186429129093481, -0.06992583242548711, 0.08796983803799578, -0.09189918351552004, -0.08681653168700311, -0.03802247615227395, 0.31383574989867274, -0.28441000553657825, -0.289478598324501, 0.11262859833305297, -0.24930350390478334, -0.10248947079146645, 0.2290516584094882, 0.00148898160019282... |
709.1389 | One page proof of the Riemann hypothesis | We give a short Wiener measure proof of the Riemann hypothesis based on a
surprising, unexpected and deep relation between the Riemann zeta $\zeta(s)$
and the trivial zeta $\zeta_{t}(s):=Im(s)(2Re(s)-1)$.
| math.GM | we give a short wiener measure proof of the riemann hypothesis based on a surprising unexpected and deep relation between the riemann zeta zetas and the trivial zeta zeta_tsims2res1 | [['we', 'give', 'a', 'short', 'wiener', 'measure', 'proof', 'of', 'the', 'riemann', 'hypothesis', 'based', 'on', 'a', 'surprising', 'unexpected', 'and', 'deep', 'relation', 'between', 'the', 'riemann', 'zeta', 'zetas', 'and', 'the', 'trivial', 'zeta', 'zeta_tsims2res1']] | [-0.267664855113253, 0.030674562423623035, -0.2815148998051882, 0.20272848602118237, -0.152353531414909, -0.15281580092518457, 0.12154311127960682, 0.28397777011351927, -0.2523074277809688, -0.2039078892474728, 0.048424142778718045, -0.21010166393326862, -0.25548721264515606, 0.24445965769700706, -0.0350819355142968, 0... |
709.139 | Non-universality of transverse momentum dependent parton distribution
functions | In the field theoretical description of hadronic scattering processes, single
transverse-spin asymmetries arise due to gluon initial and final state
interactions. These interactions lead to process dependent Wilson lines in the
operator definitions of transverse momentum dependent parton distribution
functions. In pa... | hep-ph | in the field theoretical description of hadronic scattering processes single transversespin asymmetries arise due to gluon initial and final state interactions these interactions lead to process dependent wilson lines in the operator definitions of transverse momentum dependent parton distribution functions in particul... | [['in', 'the', 'field', 'theoretical', 'description', 'of', 'hadronic', 'scattering', 'processes', 'single', 'transversespin', 'asymmetries', 'arise', 'due', 'to', 'gluon', 'initial', 'and', 'final', 'state', 'interactions', 'these', 'interactions', 'lead', 'to', 'process', 'dependent', 'wilson', 'lines', 'in', 'the', ... | [-0.07743809438036854, 0.23841379785242417, -0.18179821859039225, 0.17349762673174995, -0.04241123600002691, -0.039266607837879476, -0.04312358469122893, 0.4006099482244663, -0.22821004876781625, -0.18596294524062795, -0.040130058028877404, -0.281229845937768, -0.07457281247435407, 0.11132319088143702, 0.06977547581526... |
709.1391 | Observational signatures of f(R) dark energy models that satisfy
cosmological and local gravity constraints | We discuss observational consequences of f(R) dark energy scenarios that
satisfy local gravity constraints (LGC) as well as conditions of the
cosmological viability. The model we study is given by m(r)=C(-r-1)^p (C>0,
p>1) with m=Rf_{,RR}/f_{,R} and r=-Rf_{,R}/f, which cover viable f(R) models
proposed so far in a hi... | astro-ph gr-qc hep-ph hep-th | we discuss observational consequences of fr dark energy scenarios that satisfy local gravity constraints lgc as well as conditions of the cosmological viability the model we study is given by mrcr1p c0 p1 with mrf_rrf_r and rrf_rf which cover viable fr models proposed so far in a highcurvature region designed to be com... | [['we', 'discuss', 'observational', 'consequences', 'of', 'fr', 'dark', 'energy', 'scenarios', 'that', 'satisfy', 'local', 'gravity', 'constraints', 'lgc', 'as', 'well', 'as', 'conditions', 'of', 'the', 'cosmological', 'viability', 'the', 'model', 'we', 'study', 'is', 'given', 'by', 'mrcr1p', 'c0', 'p1', 'with', 'mrf_r... | [-0.12628975151141578, 0.1050768495294705, -0.11172421808655866, 0.1120237645464028, -0.11115795735364412, -0.1267094236265066, -0.02276335844401529, 0.3070991151375674, -0.24092430989432304, -0.3419736123887852, 0.1090985973948304, -0.2570126240843917, -0.07203509238795103, 0.1784631575723577, -0.0156398619275184, 0.0... |
709.1392 | On the measurement of the proton-air cross section using cosmic ray data | Cosmic ray data may allow the determination of the proton-air cross section
at ultra-high energy. For example, the distribution of the first interaction
point in air showers reflects the particle production cross section. As it is
not possible to observe the point of the first interaction $X_{\rm 1}$ of a
cosmic ray ... | astro-ph | cosmic ray data may allow the determination of the protonair cross section at ultrahigh energy for example the distribution of the first interaction point in air showers reflects the particle production cross section as it is not possible to observe the point of the first interaction x_rm 1 of a cosmic ray primary part... | [['cosmic', 'ray', 'data', 'may', 'allow', 'the', 'determination', 'of', 'the', 'protonair', 'cross', 'section', 'at', 'ultrahigh', 'energy', 'for', 'example', 'the', 'distribution', 'of', 'the', 'first', 'interaction', 'point', 'in', 'air', 'showers', 'reflects', 'the', 'particle', 'production', 'cross', 'section', 'a... | [-0.058712409651311845, 0.19690501868595753, -0.10590232511901337, 0.14321862699706916, -0.010404837188189445, -0.004602530643181956, -0.046226246863522606, 0.35930923824401007, -0.2782854404543405, -0.356722626802714, -0.007605917477453856, -0.35271522732775495, -0.008496987236582714, 0.17581468357947533, 0.0765495843... |
709.1393 | In-medium modification and decay asymmetry of omega mesons in cold
nuclear matter | We discuss an asymmetry of the decay $\omega->e^+e^-$ in nuclear matter with
respect to the electron and positron energies. This asymmetry is sensitive to
the properties of the $\omega$ meson self-energy and, in particular, it has a
non-trivial dependence on the $\omega$ energy and momentum. Therefore, this
asymmetry... | nucl-th | we discuss an asymmetry of the decay omegaee in nuclear matter with respect to the electron and positron energies this asymmetry is sensitive to the properties of the omega meson selfenergy and in particular it has a nontrivial dependence on the omega energy and momentum therefore this asymmetry may serve as a powerful... | [['we', 'discuss', 'an', 'asymmetry', 'of', 'the', 'decay', 'omegaee', 'in', 'nuclear', 'matter', 'with', 'respect', 'to', 'the', 'electron', 'and', 'positron', 'energies', 'this', 'asymmetry', 'is', 'sensitive', 'to', 'the', 'properties', 'of', 'the', 'omega', 'meson', 'selfenergy', 'and', 'in', 'particular', 'it', 'h... | [-0.0989641078389608, 0.17431473873327308, -0.1545525483142298, 0.13942546347836748, -0.06096089834777208, -0.04614301445679023, 0.011618581510936985, 0.3398003421150721, -0.2613062922412959, -0.2569285478989164, -0.00338771423110022, -0.30496624088487945, -0.003585302457213402, 0.1493895272885521, 0.05810340869312103,... |
709.1394 | Recent Star Formation in Nearby Early-type Galaxies | Motivated by recent progress in the study of early-type galaxies owing to
technological advances, the launch of new space telescopes and large
ground-based surveys, we attempt a short review of our current understanding of
the recent star-formation activity in such intriguing galactic systems.
| astro-ph | motivated by recent progress in the study of earlytype galaxies owing to technological advances the launch of new space telescopes and large groundbased surveys we attempt a short review of our current understanding of the recent starformation activity in such intriguing galactic systems | [['motivated', 'by', 'recent', 'progress', 'in', 'the', 'study', 'of', 'earlytype', 'galaxies', 'owing', 'to', 'technological', 'advances', 'the', 'launch', 'of', 'new', 'space', 'telescopes', 'and', 'large', 'groundbased', 'surveys', 'we', 'attempt', 'a', 'short', 'review', 'of', 'our', 'current', 'understanding', 'of... | [-0.11705572363855533, 0.0938960881037421, 0.010240887226753457, 0.04998921931093169, -0.14328244241864183, 0.016410277950642413, 0.014429033603952375, 0.39841456867234654, -0.15105298933638042, -0.3611611312385215, 0.10550950013296029, -0.28090671442319143, -0.18851019203836142, 0.2534471740404707, -0.1009573366514645... |
709.1395 | Statistical stability of equilibrium states for interval maps | We consider families of multimodal interval maps with polynomial growth of
the derivative along the critical orbits. For these maps Bruin and Todd have
shown the existence and uniqueness of equilibrium states for the potential
$\phi_t:x\mapsto-t\log|Df(x)|$, for $t$ close to 1. We show that these
equilibrium states v... | math.DS | we consider families of multimodal interval maps with polynomial growth of the derivative along the critical orbits for these maps bruin and todd have shown the existence and uniqueness of equilibrium states for the potential phi_txmapstotlogdfx for t close to 1 we show that these equilibrium states vary continuously i... | [['we', 'consider', 'families', 'of', 'multimodal', 'interval', 'maps', 'with', 'polynomial', 'growth', 'of', 'the', 'derivative', 'along', 'the', 'critical', 'orbits', 'for', 'these', 'maps', 'bruin', 'and', 'todd', 'have', 'shown', 'the', 'existence', 'and', 'uniqueness', 'of', 'equilibrium', 'states', 'for', 'the', ... | [-0.12236127260652727, 0.17357425763628181, -0.07475673084084036, 0.07375310274001992, 0.05596793511951411, -0.10639737239452424, 0.02298321818679939, 0.39842479217820514, -0.32249390920279203, -0.2263318916795672, 0.10600075106147999, -0.3027963889877737, -0.089410434189586, 0.17428151281251583, -0.03169805618623892, ... |
709.1396 | A Brownian quasi-helix in IR4, built from an automatic sequence | We describe a brownian quasi-helix in R^4 by means of an automatic sequence
| math.CO | we describe a brownian quasihelix in r4 by means of an automatic sequence | [['we', 'describe', 'a', 'brownian', 'quasihelix', 'in', 'r4', 'by', 'means', 'of', 'an', 'automatic', 'sequence']] | [-0.12005824804509757, 0.11321770761787775, -0.08733536240955193, 0.03434369899332523, -0.007786053232848644, -0.010155752572851876, -0.004139361117267981, 0.466553704192241, -0.2720738844946027, -0.22281572548672557, 0.07275848229376909, -0.23601393510277072, -0.25203414137164754, 0.2129826700935761, -0.21390553509506... |
709.1397 | THEA: ontology-driven analysis of microarray data | MOTIVATION: Microarray technology makes it possible to measure thousands of
variables and to compare their values under hundreds of conditions. Once
microarray data are quantified, normalized and classified, the analysis phase
is essentially a manual and subjective task based on visual inspection of
classes in the li... | q-bio.QM | motivation microarray technology makes it possible to measure thousands of variables and to compare their values under hundreds of conditions once microarray data are quantified normalized and classified the analysis phase is essentially a manual and subjective task based on visual inspection of classes in the light of... | [['motivation', 'microarray', 'technology', 'makes', 'it', 'possible', 'to', 'measure', 'thousands', 'of', 'variables', 'and', 'to', 'compare', 'their', 'values', 'under', 'hundreds', 'of', 'conditions', 'once', 'microarray', 'data', 'are', 'quantified', 'normalized', 'and', 'classified', 'the', 'analysis', 'phase', 'i... | [-0.03750842679718059, -0.0017170840514796402, -0.07897524060864075, 0.09129064854879687, -0.17876666276472214, -0.1451311757775888, 0.10395265801572333, 0.39470977993876816, -0.27671133305609613, -0.3948084259393558, 0.14248283529042394, -0.35014153605646964, -0.09795499373428232, 0.2565029212091045, -0.08977036251461... |
709.1398 | A topological characterisation of holomorphic parabolic germs in the
plane | Gambaudo and P\'ecou introduced the ``linking property'' to study the
dynamics of germs of planar homeomorphims and provide a new proof of Naishul
theorem in their paper "A topological invariant for volume preserving
diffeomorphisms" (Ergodic Theory Dynam. Systems 15 (1995), no. 3, 535--541). In
this paper we prove t... | math.DS | gambaudo and pecou introduced the linking property to study the dynamics of germs of planar homeomorphims and provide a new proof of naishul theorem in their paper a topological invariant for volume preserving diffeomorphisms ergodic theory dynam systems 15 1995 no 3 535541 in this paper we prove that the negation of g... | [['gambaudo', 'and', 'pecou', 'introduced', 'the', 'linking', 'property', 'to', 'study', 'the', 'dynamics', 'of', 'germs', 'of', 'planar', 'homeomorphims', 'and', 'provide', 'a', 'new', 'proof', 'of', 'naishul', 'theorem', 'in', 'their', 'paper', 'a', 'topological', 'invariant', 'for', 'volume', 'preserving', 'diffeomo... | [-0.22104261333511754, 0.08739964607437807, -0.11005116860730225, 0.07346304409221265, -0.05746836999461955, -0.12866772391454695, 0.041794474969699895, 0.2834178598413428, -0.31145516700101095, -0.19317719927774027, 0.0905344656817001, -0.26642692849746197, -0.15673405132614648, 0.21517336551755012, -0.129336669856866... |
709.1399 | Weakly polydisperse systems: Perturbative phase diagrams that include
the critical region | The phase behaviour of a weakly polydisperse system, such as a colloid with a
small spread of particle sizes, can be related perturbatively to that of its
monodisperse counterpart. I show how this approach can be generalized to remain
well-behaved near critical points, avoiding the divergences of existing methods
and... | cond-mat.soft cond-mat.mtrl-sci cond-mat.stat-mech | the phase behaviour of a weakly polydisperse system such as a colloid with a small spread of particle sizes can be related perturbatively to that of its monodisperse counterpart i show how this approach can be generalized to remain wellbehaved near critical points avoiding the divergences of existing methods and giving... | [['the', 'phase', 'behaviour', 'of', 'a', 'weakly', 'polydisperse', 'system', 'such', 'as', 'a', 'colloid', 'with', 'a', 'small', 'spread', 'of', 'particle', 'sizes', 'can', 'be', 'related', 'perturbatively', 'to', 'that', 'of', 'its', 'monodisperse', 'counterpart', 'i', 'show', 'how', 'this', 'approach', 'can', 'be', ... | [-0.12250563531611743, 0.14223920845876584, -0.1551202696884114, 0.07191813019303124, -0.012951169717596488, -0.1578920560187838, 0.0684456160380976, 0.3458637328964941, -0.2764898893172235, -0.27566299217052004, 0.1013547777828729, -0.3152349811110101, -0.16713651531281765, 0.1565529652779629, -0.08331214303276345, 0.... |
709.14 | Dark Energy as a Relic of the Vacuum-Energy Cancellation? | We analyze the dynamical implications of an exponential Lagrangian density
for the gravitational field, as referred to an isotropic FRW Universe. Then, we
discuss the features of the generalized deSitter phase, predicted by the new
Friedmann equation. The existence of a consistent deSitter solution arises only
if the... | gr-qc | we analyze the dynamical implications of an exponential lagrangian density for the gravitational field as referred to an isotropic frw universe then we discuss the features of the generalized desitter phase predicted by the new friedmann equation the existence of a consistent desitter solution arises only if the ratio ... | [['we', 'analyze', 'the', 'dynamical', 'implications', 'of', 'an', 'exponential', 'lagrangian', 'density', 'for', 'the', 'gravitational', 'field', 'as', 'referred', 'to', 'an', 'isotropic', 'frw', 'universe', 'then', 'we', 'discuss', 'the', 'features', 'of', 'the', 'generalized', 'desitter', 'phase', 'predicted', 'by',... | [-0.15909720457691168, 0.11849321161328892, -0.10073476556156363, 0.10043314377322704, -0.07248441844380328, -0.11407623832125129, -0.02641509543561066, 0.27968843389923376, -0.2395172274294531, -0.27043068829391687, 0.04752139252488546, -0.23461801391656212, -0.12313285005899767, 0.14294116124621636, -0.01318407600338... |
709.1401 | A proof of strong normalisation using domain theory | Ulrich Berger presented a powerful proof of strong normalisation using
domains, in particular it simplifies significantly Tait's proof of strong
normalisation of Spector's bar recursion. The main contribution of this paper
is to show that, using ideas from intersection types and Martin-Lof's domain
interpretation of ... | cs.LO cs.PL | ulrich berger presented a powerful proof of strong normalisation using domains in particular it simplifies significantly taits proof of strong normalisation of spectors bar recursion the main contribution of this paper is to show that using ideas from intersection types and martinlofs domain interpretation of type theo... | [['ulrich', 'berger', 'presented', 'a', 'powerful', 'proof', 'of', 'strong', 'normalisation', 'using', 'domains', 'in', 'particular', 'it', 'simplifies', 'significantly', 'taits', 'proof', 'of', 'strong', 'normalisation', 'of', 'spectors', 'bar', 'recursion', 'the', 'main', 'contribution', 'of', 'this', 'paper', 'is', ... | [-0.09031304085536539, 0.0009663739345712275, -0.12396017455421718, 0.09856170381571834, -0.17746814831975946, -0.18247185757927661, 0.061123029657524176, 0.29983674928100895, -0.3169092828721072, -0.2664596891994959, 0.07204333542994495, -0.19404143409234825, -0.13900774675915925, 0.18058644032798113, -0.1372300745276... |
709.1402 | Theoretical study of the recombination of Frenkel pairs in irradiated
silicon carbide | The recombination of Frenkel pairs resulting from low energy recoils in
3C-SiC has been investigated using first principles and Nudged Elastic Band
calculations. Several recombination mechanisms have been obtained, involving
direct interstitial migration, atoms exchange, or concerted displacements, with
activation en... | cond-mat.mtrl-sci | the recombination of frenkel pairs resulting from low energy recoils in 3csic has been investigated using first principles and nudged elastic band calculations several recombination mechanisms have been obtained involving direct interstitial migration atoms exchange or concerted displacements with activation energies r... | [['the', 'recombination', 'of', 'frenkel', 'pairs', 'resulting', 'from', 'low', 'energy', 'recoils', 'in', '3csic', 'has', 'been', 'investigated', 'using', 'first', 'principles', 'and', 'nudged', 'elastic', 'band', 'calculations', 'several', 'recombination', 'mechanisms', 'have', 'been', 'obtained', 'involving', 'direc... | [-0.04645015615840546, 0.19549022537345687, -0.021984412340033385, 0.03963208729336556, 0.02826863908622828, -0.12554845343240434, 0.08010853180247876, 0.45790671015468737, -0.2679814937110576, -0.35617811866104604, -0.064504684749732, -0.3621757693381773, -0.04366410532966256, 0.1649286749591637, 0.10148932810730507, ... |
709.1403 | Spherically symmetric ADM gravity with variable G and Lambda(c) | This paper investigates the Arnowitt--Deser--Misner (hereafter ADM) form of
spherically symmetric gravity with variable Newton parameter G and cosmological
term Lambda(c). The Newton parameter is here treated as a dynamical variable,
rather than being merely an external parameter as in previous work on closely
relate... | gr-qc | this paper investigates the arnowittdesermisner hereafter adm form of spherically symmetric gravity with variable newton parameter g and cosmological term lambdac the newton parameter is here treated as a dynamical variable rather than being merely an external parameter as in previous work on closely related topics the... | [['this', 'paper', 'investigates', 'the', 'arnowittdesermisner', 'hereafter', 'adm', 'form', 'of', 'spherically', 'symmetric', 'gravity', 'with', 'variable', 'newton', 'parameter', 'g', 'and', 'cosmological', 'term', 'lambdac', 'the', 'newton', 'parameter', 'is', 'here', 'treated', 'as', 'a', 'dynamical', 'variable', '... | [-0.1756703607496564, 0.07368914046857282, -0.08033269875654865, 0.04889990488343217, -0.12899984516617324, -0.16917497662016778, -0.012549327264746859, 0.27674794688268944, -0.253529612371629, -0.2685570072106741, 0.12243712290914523, -0.2620080136107626, -0.1281147414163031, 0.1957326647825539, -0.049565991593731776,... |
709.1404 | Occultation observation to probe the turbulence scale size in the plasma
tail of comet Schwassmann-Wachmann 3-B | We present the occultation observation of compact radio source B0019-000
through the plasma tail of comet Schwassmann-Wachmann 3-B. The observation was
made with the Ooty Radio Telescope at 326.5 MHz on 2006 May 26, when the plasma
tail of the comet was in front of this source. The scintillation was found to
be incre... | astro-ph | we present the occultation observation of compact radio source b0019000 through the plasma tail of comet schwassmannwachmann 3b the observation was made with the ooty radio telescope at 3265 mhz on 2006 may 26 when the plasma tail of the comet was in front of this source the scintillation was found to be increased sign... | [['we', 'present', 'the', 'occultation', 'observation', 'of', 'compact', 'radio', 'source', 'b0019000', 'through', 'the', 'plasma', 'tail', 'of', 'comet', 'schwassmannwachmann', '3b', 'the', 'observation', 'was', 'made', 'with', 'the', 'ooty', 'radio', 'telescope', 'at', '3265', 'mhz', 'on', '2006', 'may', '26', 'when'... | [-0.08477530563332603, 0.1707799548810694, -0.1338194993868536, 0.057426250768429804, -0.04735951131597095, -0.06962441513726933, -0.014499167225579113, 0.4014888249535476, -0.2323031113410896, -0.3440690924108556, 0.10521711721867982, -0.28502061313628096, -0.022259161152374165, 0.19164926613540909, -0.047393292699635... |
709.1405 | Degrees of freedom of tongue movements in speech may be constrained by
biomechanics | A number of studies carried out on different languages have found that tongue
movements in speech are made along two primary degrees of freedom (d.f.s): the
high-front to low-back axis and the high-back to low-front axis. We explore the
hypothesis that these two main d.f.s could find their origins in the physical
pro... | physics.med-ph | a number of studies carried out on different languages have found that tongue movements in speech are made along two primary degrees of freedom dfs the highfront to lowback axis and the highback to lowfront axis we explore the hypothesis that these two main dfs could find their origins in the physical properties of the... | [['a', 'number', 'of', 'studies', 'carried', 'out', 'on', 'different', 'languages', 'have', 'found', 'that', 'tongue', 'movements', 'in', 'speech', 'are', 'made', 'along', 'two', 'primary', 'degrees', 'of', 'freedom', 'dfs', 'the', 'highfront', 'to', 'lowback', 'axis', 'and', 'the', 'highback', 'to', 'lowfront', 'axis'... | [-0.12229205057024956, 0.09265315909869969, -0.1039205527678132, 0.05673884001653642, -0.07144700207747519, -0.07692750203236938, -0.008625272958539426, 0.43401553949713706, -0.2293928342759609, -0.30113514012936504, 0.06941401777230204, -0.24843613054975866, -0.1810914394631982, 0.21860783342830836, -0.054615889050066... |
709.1406 | The Discovery of Stellar Oscillations in the Planet Hosting Giant Star
Beta Geminorum | We present the results of a long time series of precise stellar radial
velocity measurements of the planet hosting K giant star Beta Geminorum. A
total of 20 hours of observations spanning three nights were obtained and the
radial velocity variations show the presence of solar-like stellar
oscillations. Our period an... | astro-ph | we present the results of a long time series of precise stellar radial velocity measurements of the planet hosting k giant star beta geminorum a total of 20 hours of observations spanning three nights were obtained and the radial velocity variations show the presence of solarlike stellar oscillations our period analysi... | [['we', 'present', 'the', 'results', 'of', 'a', 'long', 'time', 'series', 'of', 'precise', 'stellar', 'radial', 'velocity', 'measurements', 'of', 'the', 'planet', 'hosting', 'k', 'giant', 'star', 'beta', 'geminorum', 'a', 'total', 'of', '20', 'hours', 'of', 'observations', 'spanning', 'three', 'nights', 'were', 'obtain... | [-0.15988393497839268, 0.2127944601402246, -0.051691048068006513, 0.04358527571013554, -0.10201285726106545, -0.029898702088356405, 0.06743103743972281, 0.35557445956775074, -0.0764563564549793, -0.4185745648241469, 0.06417682563489932, -0.26507183501206627, -0.02244731432201897, 0.25379264153322423, -0.022511865290534... |
709.1407 | Wave-packet view of the Dirac electron | By viewing the electron as a wavepacket in the positive energy spectrum of
the Dirac equation, we are able to achieve a much clearer understanding of its
behavior under weak electromagnetic fields. The intrinsic spin magnetic moment
is found to be established from the self-rotation of the wavepacket. A
non-canonical ... | physics.gen-ph | by viewing the electron as a wavepacket in the positive energy spectrum of the dirac equation we are able to achieve a much clearer understanding of its behavior under weak electromagnetic fields the intrinsic spin magnetic moment is found to be established from the selfrotation of the wavepacket a noncanonical structu... | [['by', 'viewing', 'the', 'electron', 'as', 'a', 'wavepacket', 'in', 'the', 'positive', 'energy', 'spectrum', 'of', 'the', 'dirac', 'equation', 'we', 'are', 'able', 'to', 'achieve', 'a', 'much', 'clearer', 'understanding', 'of', 'its', 'behavior', 'under', 'weak', 'electromagnetic', 'fields', 'the', 'intrinsic', 'spin'... | [-0.16052965609425748, 0.18288546656940188, -0.10717973077273066, 0.10860021814759993, -0.07749484748476082, -0.10215064634448262, -0.019524746936103503, 0.33023370685124837, -0.26435670081560536, -0.30379637781772073, -0.012011337325761647, -0.2300200032165136, -0.12077266132864342, 0.185203147922746, -0.0027282844832... |
709.1408 | The Quest for Pionic and Kaonic Nuclear Bound Systems Following Yukawa
and Tomonaga | After sketching some historical events related to Yukawa and Tomonaga
concerning the birth of mesons, the author describes recent developments in the
spectroscopy of pion-nucleus bound states via "pion-transfer" reactions. The
role of pions as Nambu-Goldstone bosons in nuclear media is emphasized by
recently obtained... | nucl-ex | after sketching some historical events related to yukawa and tomonaga concerning the birth of mesons the author describes recent developments in the spectroscopy of pionnucleus bound states via piontransfer reactions the role of pions as nambugoldstone bosons in nuclear media is emphasized by recently obtained experime... | [['after', 'sketching', 'some', 'historical', 'events', 'related', 'to', 'yukawa', 'and', 'tomonaga', 'concerning', 'the', 'birth', 'of', 'mesons', 'the', 'author', 'describes', 'recent', 'developments', 'in', 'the', 'spectroscopy', 'of', 'pionnucleus', 'bound', 'states', 'via', 'piontransfer', 'reactions', 'the', 'rol... | [-0.10424905552891857, 0.2737465685568168, -0.09517752016910304, 0.09710149509512614, -0.0408554276514609, -0.1026549724056938, 0.06057869294121609, 0.31252535066954096, -0.21657001425441103, -0.23486414269970382, -0.01582361253173785, -0.3153183821399333, -0.12601892432292638, 0.10653693423117117, 0.0714770766622308, ... |
709.1409 | The effect of "pre-formed" hadron potentials on the dynamics of heavy
ion collisions and the HBT puzzle | The nuclear stopping, the elliptic flow, and the HBT interferometry are
calculated by the UrQMD transport model, in which potentials for "pre-formed"
particles (string fragments) from color fluxtube fragmentation as well as for
confined particles are considered. This description provides stronger pressure
at the earl... | nucl-th | the nuclear stopping the elliptic flow and the hbt interferometry are calculated by the urqmd transport model in which potentials for preformed particles string fragments from color fluxtube fragmentation as well as for confined particles are considered this description provides stronger pressure at the early stage and... | [['the', 'nuclear', 'stopping', 'the', 'elliptic', 'flow', 'and', 'the', 'hbt', 'interferometry', 'are', 'calculated', 'by', 'the', 'urqmd', 'transport', 'model', 'in', 'which', 'potentials', 'for', 'preformed', 'particles', 'string', 'fragments', 'from', 'color', 'fluxtube', 'fragmentation', 'as', 'well', 'as', 'for',... | [-0.03641013041848228, 0.2685451016362224, -0.18034123709879904, 0.15167237368877978, 0.011282085738189163, -0.14580636462640195, -0.08475803816247554, 0.33703008260400524, -0.2673393691091665, -0.2778801556854021, -0.013563784518988714, -0.32265373122035745, 0.05129998265987351, 0.12724741000981468, 0.0615227239295130... |
709.141 | Study of the performance and capability of the new ultra-fast 2
GSample/s FADC data acquisition system of the MAGIC telescope | In February 2007 the MAGIC Air Cherenkov Telescope for gamma-ray astronomy
was fully upgraded with an ultra fast 2 GSamples/s digitization system. Since
the Cherenkov light flashes are very short, a fast readout can minimize the
influence of the background from the light of the night sky. Also, the time
structure of ... | astro-ph | in february 2007 the magic air cherenkov telescope for gammaray astronomy was fully upgraded with an ultra fast 2 gsampless digitization system since the cherenkov light flashes are very short a fast readout can minimize the influence of the background from the light of the night sky also the time structure of the even... | [['in', 'february', '2007', 'the', 'magic', 'air', 'cherenkov', 'telescope', 'for', 'gammaray', 'astronomy', 'was', 'fully', 'upgraded', 'with', 'an', 'ultra', 'fast', '2', 'gsampless', 'digitization', 'system', 'since', 'the', 'cherenkov', 'light', 'flashes', 'are', 'very', 'short', 'a', 'fast', 'readout', 'can', 'min... | [-0.08790824318368157, 0.2037770510537071, -0.08830463452349332, 0.08630464598139621, -0.08869472118517892, -0.0494279803824611, -0.014203309060328385, 0.40535401222719386, -0.2042994695207612, -0.3844008287838237, 0.15649658110156783, -0.32084342723035, -0.06477416306734085, 0.25627045738722454, -0.06383314494847912, ... |
709.1411 | BV Yang-Mills as a Homotopy Chern-Simons via SFT | We show explicitly how BV Yang-Mills action emerges as a homotopy
generalization of Chern-Simons theory from the algebraic constructions arising
from String Field Theory.
| hep-th math-ph math.MP math.QA | we show explicitly how bv yangmills action emerges as a homotopy generalization of chernsimons theory from the algebraic constructions arising from string field theory | [['we', 'show', 'explicitly', 'how', 'bv', 'yangmills', 'action', 'emerges', 'as', 'a', 'homotopy', 'generalization', 'of', 'chernsimons', 'theory', 'from', 'the', 'algebraic', 'constructions', 'arising', 'from', 'string', 'field', 'theory']] | [-0.11771439640627553, 0.16241515167833617, -0.18429597653448582, 0.17364733999905488, -0.1064228107376645, -0.125722919338538, 0.008312610676512122, 0.24531061062589288, -0.3447520583868027, -0.25321149837691337, 0.017198431441405166, -0.23233066064616045, -0.3691643135001262, 0.09904791426379234, -0.20474649798901132... |
709.1412 | Heat Transport in Quantum Spin Chains: Stochastic Baths vs Quantum
Trajectories | We discuss the problem of heat conduction in quantum spin chain models. To
investigate this problem it is necessary to consider the finite open system
connected to heat baths. We describe two different procedures to couple the
system with the reservoirs: a model of stochastic heat baths and the quantum
trajectories s... | cond-mat.stat-mech quant-ph | we discuss the problem of heat conduction in quantum spin chain models to investigate this problem it is necessary to consider the finite open system connected to heat baths we describe two different procedures to couple the system with the reservoirs a model of stochastic heat baths and the quantum trajectories soluti... | [['we', 'discuss', 'the', 'problem', 'of', 'heat', 'conduction', 'in', 'quantum', 'spin', 'chain', 'models', 'to', 'investigate', 'this', 'problem', 'it', 'is', 'necessary', 'to', 'consider', 'the', 'finite', 'open', 'system', 'connected', 'to', 'heat', 'baths', 'we', 'describe', 'two', 'different', 'procedures', 'to',... | [-0.1476259006343725, 0.15678585311469004, -0.07190076561772642, 0.045919661116004276, -0.0016526342760629325, -0.16272290007261034, 0.06169484180526253, 0.35671880195727784, -0.30522274850149644, -0.23438700820667713, 0.08270115253625736, -0.3056665051387239, -0.10419042420907672, 0.2044089815014163, -0.00700228421714... |
709.1413 | Equivalence of Gutzwiller and slave-boson mean-field theories for
multi-band Hubbard models | We demonstrate that a recently introduced slave-boson mean-field theory is
equivalent to our Gutzwiller theory for multi-band Hubbard models with general
onsite interactions. We relate the different objects that appear in both
approaches at zero temperature and discuss the limitations of both methods.
| cond-mat.str-el | we demonstrate that a recently introduced slaveboson meanfield theory is equivalent to our gutzwiller theory for multiband hubbard models with general onsite interactions we relate the different objects that appear in both approaches at zero temperature and discuss the limitations of both methods | [['we', 'demonstrate', 'that', 'a', 'recently', 'introduced', 'slaveboson', 'meanfield', 'theory', 'is', 'equivalent', 'to', 'our', 'gutzwiller', 'theory', 'for', 'multiband', 'hubbard', 'models', 'with', 'general', 'onsite', 'interactions', 'we', 'relate', 'the', 'different', 'objects', 'that', 'appear', 'in', 'both',... | [-0.06525193156977725, 0.1164340824321952, -0.10932860250157023, 0.165232939702502, -0.022001884271239124, -0.17718227750210222, 0.05366662419184522, 0.3918402039034422, -0.2250038778712583, -0.2307902324273316, -0.003920093213944415, -0.30124873804404984, -0.20034607271389726, 0.13424208075847738, -0.02318337964717038... |
709.1414 | Magnetic fields and accretion flows on the classical T Tauri star V2129
Oph | From observations collected with the ESPaDOnS spectropolarimeter, we report
the discovery of magnetic fields at the surface of the mildly accreting
classical T Tauri star V2129 Oph. Zeeman signatures are detected, both in
photospheric lines and in the emission lines formed at the base of the
accretion funnels linking... | astro-ph | from observations collected with the espadons spectropolarimeter we report the discovery of magnetic fields at the surface of the mildly accreting classical t tauri star v2129 oph zeeman signatures are detected both in photospheric lines and in the emission lines formed at the base of the accretion funnels linking the ... | [['from', 'observations', 'collected', 'with', 'the', 'espadons', 'spectropolarimeter', 'we', 'report', 'the', 'discovery', 'of', 'magnetic', 'fields', 'at', 'the', 'surface', 'of', 'the', 'mildly', 'accreting', 'classical', 't', 'tauri', 'star', 'v2129', 'oph', 'zeeman', 'signatures', 'are', 'detected', 'both', 'in', ... | [-0.14202500389061412, 0.16240452339738923, -0.028871006988116253, 0.08785888373750436, -0.112643227578315, -0.1051676913286834, 0.020474991392639044, 0.43044951410709525, -0.21579167763034648, -0.32910607769359207, 0.06443521383607077, -0.22677660916564255, -0.03866445498956408, 0.20692819514455904, -0.011809513947705... |
709.1415 | Predicting the Ionization Threshold for Carriers in Excited
Semiconductors | A simple set of formulas is presented which allows prediction of the fraction
of ionized carriers in an electron-hole-exciton gas in a photoexcited
semiconductor. These results are related to recent experiments with excitons in
single and double quantum wells.
| cond-mat.other | a simple set of formulas is presented which allows prediction of the fraction of ionized carriers in an electronholeexciton gas in a photoexcited semiconductor these results are related to recent experiments with excitons in single and double quantum wells | [['a', 'simple', 'set', 'of', 'formulas', 'is', 'presented', 'which', 'allows', 'prediction', 'of', 'the', 'fraction', 'of', 'ionized', 'carriers', 'in', 'an', 'electronholeexciton', 'gas', 'in', 'a', 'photoexcited', 'semiconductor', 'these', 'results', 'are', 'related', 'to', 'recent', 'experiments', 'with', 'excitons... | [-0.07691246588671531, 0.1695917791868468, -0.010460727927765172, -0.005761062907128546, 0.021019839436600084, -0.1351543892861197, 0.06649642429731198, 0.3919510512955879, -0.2257108325138688, -0.2751059858618598, -0.03349494578402588, -0.34554291399552695, -0.10470256488770247, 0.281579428523975, -0.03442571531348604... |
709.1416 | A note on the component structure in random intersection graphs with
tunable clustering | We study the component structure in random intersection graphs with tunable
clustering, and show that the average degree works as a threshold for a phase
transition for the size of the largest component. That is, if the expected
degree is less than one, the size of the largest component is a.a.s. of
logarithmic order... | math.PR | we study the component structure in random intersection graphs with tunable clustering and show that the average degree works as a threshold for a phase transition for the size of the largest component that is if the expected degree is less than one the size of the largest component is aas of logarithmic order but if t... | [['we', 'study', 'the', 'component', 'structure', 'in', 'random', 'intersection', 'graphs', 'with', 'tunable', 'clustering', 'and', 'show', 'that', 'the', 'average', 'degree', 'works', 'as', 'a', 'threshold', 'for', 'a', 'phase', 'transition', 'for', 'the', 'size', 'of', 'the', 'largest', 'component', 'that', 'is', 'if... | [-0.15905521301888362, 0.14912461054912055, -0.05384495066543824, 0.010596762943287315, -0.048932545255263186, -0.07986095322967442, -0.01508517055650415, 0.3238382166966276, -0.24765749844901133, -0.2834969584851764, 0.12525925037943822, -0.35785623787100923, -0.1234951127580432, 0.1419418572318242, 0.0317310730082004... |
709.1417 | Jacobi fields along harmonic 2-spheres in $S^3$ and $S^4$ are not all
integrable | In a previous paper, we showed that any Jacobi field along a harmonic map
from the 2-sphere to the complex projective plane is integrable (i.e., is
tangent to a smooth variation through harmonic maps). In this paper, in
contrast, we show that there are (non-full) harmonic maps from the 2-sphere to
the 3-sphere and 4-... | math.DG | in a previous paper we showed that any jacobi field along a harmonic map from the 2sphere to the complex projective plane is integrable ie is tangent to a smooth variation through harmonic maps in this paper in contrast we show that there are nonfull harmonic maps from the 2sphere to the 3sphere and 4sphere which have ... | [['in', 'a', 'previous', 'paper', 'we', 'showed', 'that', 'any', 'jacobi', 'field', 'along', 'a', 'harmonic', 'map', 'from', 'the', '2sphere', 'to', 'the', 'complex', 'projective', 'plane', 'is', 'integrable', 'ie', 'is', 'tangent', 'to', 'a', 'smooth', 'variation', 'through', 'harmonic', 'maps', 'in', 'this', 'paper',... | [-0.19308392158911927, 0.06348215786578215, -0.08506105939412247, 0.023018432525492717, -0.08504749712554495, -0.11486721530293478, -0.06626441885221182, 0.392090800339761, -0.28517228390252136, -0.15223328388579513, 0.0821696792554576, -0.2763223873056552, -0.24219980503877866, 0.21003833933449959, -0.1435353293718831... |
709.1418 | Shock minimized supersonic flight by heating | Bow shocks radiate a lot of energy away around supersonic objects in air. To
minimize such waves is urgent for fast aircraft. Heat experiments exist where
air drag is minimized. Here is a theoretical description of how shocks can be
prevented by special distribution of heating.
| physics.flu-dyn | bow shocks radiate a lot of energy away around supersonic objects in air to minimize such waves is urgent for fast aircraft heat experiments exist where air drag is minimized here is a theoretical description of how shocks can be prevented by special distribution of heating | [['bow', 'shocks', 'radiate', 'a', 'lot', 'of', 'energy', 'away', 'around', 'supersonic', 'objects', 'in', 'air', 'to', 'minimize', 'such', 'waves', 'is', 'urgent', 'for', 'fast', 'aircraft', 'heat', 'experiments', 'exist', 'where', 'air', 'drag', 'is', 'minimized', 'here', 'is', 'a', 'theoretical', 'description', 'of'... | [-0.13680636807871255, 0.23571439694775187, -0.04275653519384239, 0.0860235786809505, -0.1400605362293351, -0.0725743644060972, 0.03281183891079348, 0.4132342566938504, -0.2902446591229502, -0.30887278047916683, 0.09577149704210056, -0.3368442433572415, -0.04583682190707844, 0.2472986831613209, -0.06748252737578815, 0.... |
709.1419 | Theory of subgap interchain tunneling in quasi one-dimensional
conductors | We suggest a theory of internal coherent tunneling in the pseudogap region,
when the applied voltage U is below the free electron gap 2Delta_0. We address
quasi 1D systems, where the gap is originated by spontaneous lattice
distortions of the Incommensurate Charge Density Wave (ICDW) type. Results can
be adjusted als... | cond-mat.str-el | we suggest a theory of internal coherent tunneling in the pseudogap region when the applied voltage u is below the free electron gap 2delta_0 we address quasi 1d systems where the gap is originated by spontaneous lattice distortions of the incommensurate charge density wave icdw type results can be adjusted also to qua... | [['we', 'suggest', 'a', 'theory', 'of', 'internal', 'coherent', 'tunneling', 'in', 'the', 'pseudogap', 'region', 'when', 'the', 'applied', 'voltage', 'u', 'is', 'below', 'the', 'free', 'electron', 'gap', '2delta_0', 'we', 'address', 'quasi', '1d', 'systems', 'where', 'the', 'gap', 'is', 'originated', 'by', 'spontaneous... | [-0.1987632009926317, 0.26188234674018745, -0.03508059555491389, 0.07973877339720148, -0.011295764015305267, -0.18072233190760018, 0.11115631580861762, 0.3260626518189214, -0.2703995349345902, -0.22999453986886628, 0.010524274830078317, -0.3234048335759516, -0.08134758258996488, 0.14203270614840263, 0.04378008348799614... |
709.142 | Compact differences of composition operators from Bloch space to bounded
holomorphic function space in the Polydisc | Let $\phi$ and $\psi$ be holomorphic self-maps of the unit polydisc $U^n$ in
the $n$-dimensional complex space, and denote by $C_{\phi}$ and $C_{\psi}$ the
induced composition operators. This paper gives some simple estimates of the
essential norm for the difference of composition operators $C_{\phi}-C_{\psi}$
from B... | math.FA math.CV | let phi and psi be holomorphic selfmaps of the unit polydisc un in the ndimensional complex space and denote by c_phi and c_psi the induced composition operators this paper gives some simple estimates of the essential norm for the difference of composition operators c_phic_psi from bloch space to bounded holomorphic fu... | [['let', 'phi', 'and', 'psi', 'be', 'holomorphic', 'selfmaps', 'of', 'the', 'unit', 'polydisc', 'un', 'in', 'the', 'ndimensional', 'complex', 'space', 'and', 'denote', 'by', 'c_phi', 'and', 'c_psi', 'the', 'induced', 'composition', 'operators', 'this', 'paper', 'gives', 'some', 'simple', 'estimates', 'of', 'the', 'esse... | [-0.14583363273413852, 0.12842720531625673, -0.04132024478576568, 0.04937853468436515, -0.07151947401143843, -0.009093064785702154, -0.012551659225209733, 0.3167064737644978, -0.35053131348104216, -0.1741000630427152, 0.09171473697278998, -0.2911863830377115, -0.1484102257345512, 0.18782997378730215, -0.120867076533613... |
709.1421 | Coherence in Linear Predicate Logic | Coherence with respect to Kelly-Mac Lane graphs is proved for categories that
correspond to the multiplicative fragment without constant propositions of
classical linear first-order predicate logic without or with mix. To obtain
this result, coherence is first established for categories that correspond to
the multipl... | math.LO math.CT | coherence with respect to kellymac lane graphs is proved for categories that correspond to the multiplicative fragment without constant propositions of classical linear firstorder predicate logic without or with mix to obtain this result coherence is first established for categories that correspond to the multiplicativ... | [['coherence', 'with', 'respect', 'to', 'kellymac', 'lane', 'graphs', 'is', 'proved', 'for', 'categories', 'that', 'correspond', 'to', 'the', 'multiplicative', 'fragment', 'without', 'constant', 'propositions', 'of', 'classical', 'linear', 'firstorder', 'predicate', 'logic', 'without', 'or', 'with', 'mix', 'to', 'obtai... | [-0.06476353907422853, 0.06217136506641302, -0.05429032329691223, 0.11920637680614704, -0.11979426355055063, -0.15893851215536198, 0.02895551453353745, 0.36680200884100234, -0.3349933903281102, -0.28207498310551066, 0.06647197342256435, -0.22991327789270938, -0.036940748842506865, 0.1745595651480489, -0.153533178473832... |
709.1422 | Pierre Auger Observatory status and results | The Pierre Auger Observatory, a hybrid detector for the study of ultra-high
energy cosmic rays (UHECRs), is now approaching completion. After describing
Auger present status and performance, with an emphasis on the advantages
provided by the combination of two different detection techniques, this
contribution present... | astro-ph | the pierre auger observatory a hybrid detector for the study of ultrahigh energy cosmic rays uhecrs is now approaching completion after describing auger present status and performance with an emphasis on the advantages provided by the combination of two different detection techniques this contribution presents a brief ... | [['the', 'pierre', 'auger', 'observatory', 'a', 'hybrid', 'detector', 'for', 'the', 'study', 'of', 'ultrahigh', 'energy', 'cosmic', 'rays', 'uhecrs', 'is', 'now', 'approaching', 'completion', 'after', 'describing', 'auger', 'present', 'status', 'and', 'performance', 'with', 'an', 'emphasis', 'on', 'the', 'advantages', ... | [-0.07843163166865845, 0.1167559999324913, -0.0443324165126837, 0.07449766842573673, -0.06690490116545958, 0.023385662488194545, 0.00940823918833995, 0.39432366006076336, -0.20920129002892038, -0.36941550580312066, 0.05104470714481909, -0.3262630901507922, -0.10489491829926621, 0.24893386811087492, 0.015552021139092854... |
709.1423 | Exotic Ground State Phases of $S=1/2$ Heisenberg $\Delta$-Chain with
Ferromagnetic Main Chain | The ground state phase diagram of the spin-1/2 Heisenberg frustrated
$\Delta$-chain with a ferromagnetic main chain is investigated. In addition to
the ferromagnetic phase, various nonmagnetic ground states are found. If the
ferromagnetic coupling between apical spins and the main chain is strong, this
model is appro... | cond-mat.str-el cond-mat.stat-mech | the ground state phase diagram of the spin12 heisenberg frustrated deltachain with a ferromagnetic main chain is investigated in addition to the ferromagnetic phase various nonmagnetic ground states are found if the ferromagnetic coupling between apical spins and the main chain is strong this model is approximated by a... | [['the', 'ground', 'state', 'phase', 'diagram', 'of', 'the', 'spin12', 'heisenberg', 'frustrated', 'deltachain', 'with', 'a', 'ferromagnetic', 'main', 'chain', 'is', 'investigated', 'in', 'addition', 'to', 'the', 'ferromagnetic', 'phase', 'various', 'nonmagnetic', 'ground', 'states', 'are', 'found', 'if', 'the', 'ferro... | [-0.20719246546958842, 0.27855346570485984, 0.03001062478080897, 0.030727468399425684, -0.016568210396236915, -0.16433792013154067, 0.03793817710218225, 0.3941839692514327, -0.23201914935893678, -0.23835678813560723, 0.055184082797988934, -0.32564923838096654, -0.09261893518900467, 0.13169448734931963, 0.11303834484542... |
709.1424 | Gauss sum factorization with cold atoms | We report the first implementation of a Gauss sum factorization algorithm by
an internal state Ramsey interferometer using cold atoms. A sequence of
appropriately designed light pulses interacts with an ensemble of cold rubidium
atoms. The final population in the involved atomic levels determines a Gauss
sum. With th... | quant-ph | we report the first implementation of a gauss sum factorization algorithm by an internal state ramsey interferometer using cold atoms a sequence of appropriately designed light pulses interacts with an ensemble of cold rubidium atoms the final population in the involved atomic levels determines a gauss sum with this te... | [['we', 'report', 'the', 'first', 'implementation', 'of', 'a', 'gauss', 'sum', 'factorization', 'algorithm', 'by', 'an', 'internal', 'state', 'ramsey', 'interferometer', 'using', 'cold', 'atoms', 'a', 'sequence', 'of', 'appropriately', 'designed', 'light', 'pulses', 'interacts', 'with', 'an', 'ensemble', 'of', 'cold', ... | [-0.14851625918634925, 0.21876222958100563, -0.05718278955599224, -0.012610231295521199, 0.022961043252575176, -0.07802017855768402, 0.10206039653685703, 0.43359026057576694, -0.2621503860724193, -0.3218616031938129, -0.018280588497873396, -0.23362010986440712, -0.05070527642965317, 0.13355847741735893, 0.0058038196336... |
709.1425 | A higher order model for image restoration: the one dimensional case | The one-dimensional version of the higher order total variation-based model
for image restoration proposed by Chan, Marquina, and Mulet in [4] is analyzed.
A suitable functional framework in which the minimization problem is well posed
is being proposed and it is proved analytically that the higher order
regularizing... | math.OC | the onedimensional version of the higher order total variationbased model for image restoration proposed by chan marquina and mulet in 4 is analyzed a suitable functional framework in which the minimization problem is well posed is being proposed and it is proved analytically that the higher order regularizing term pre... | [['the', 'onedimensional', 'version', 'of', 'the', 'higher', 'order', 'total', 'variationbased', 'model', 'for', 'image', 'restoration', 'proposed', 'by', 'chan', 'marquina', 'and', 'mulet', 'in', '4', 'is', 'analyzed', 'a', 'suitable', 'functional', 'framework', 'in', 'which', 'the', 'minimization', 'problem', 'is', '... | [-0.10099488598967178, 0.03617191566499295, -0.046174914852060656, 0.10721537831273896, -0.046358859373463526, -0.10513833247090655, 0.001511882964728607, 0.30945455462292387, -0.25848502429909315, -0.34131215824918065, 0.1513422842491073, -0.26025893429458075, -0.20985981891000713, 0.1231226582011139, -0.0850347266187... |
709.1426 | Non-supersymmetric Tachyon-free Type-II and Type-I Closed Strings from
RCFT | We consider non-supersymmetric four-dimensional closed string theories
constructed out of tensor products of N=2 minimal models. Generically such
theories have closed string tachyons, but these may be removed either by
choosing a non-trivial partition function or a suitable Klein bottle
projection. We find large numb... | hep-th | we consider nonsupersymmetric fourdimensional closed string theories constructed out of tensor products of n2 minimal models generically such theories have closed string tachyons but these may be removed either by choosing a nontrivial partition function or a suitable klein bottle projection we find large numbers of ex... | [['we', 'consider', 'nonsupersymmetric', 'fourdimensional', 'closed', 'string', 'theories', 'constructed', 'out', 'of', 'tensor', 'products', 'of', 'n2', 'minimal', 'models', 'generically', 'such', 'theories', 'have', 'closed', 'string', 'tachyons', 'but', 'these', 'may', 'be', 'removed', 'either', 'by', 'choosing', 'a... | [-0.1833601347869262, 0.22044786341954023, -0.024400267470628022, 0.15662715520709752, -0.06593105871230363, -0.23768385661765934, 0.00687175746075809, 0.30461403434164824, -0.2080370233207941, -0.26045331384986636, 0.0868918921239674, -0.25609585985541344, -0.17884835367556662, 0.13973205675836653, -0.0642081879358738... |
709.1427 | Computing Knot Floer Homology in Cyclic Branched Covers | We use grid diagrams to give a combinatorial algorithm for computing the knot
Floer homology of the pullback of a knot K in its m-fold cyclic branched cover
Sigma^m(K), and we give computations when m=2 for over fifty three-bridge knots
with up to eleven crossings.
| math.GT math.SG | we use grid diagrams to give a combinatorial algorithm for computing the knot floer homology of the pullback of a knot k in its mfold cyclic branched cover sigmamk and we give computations when m2 for over fifty threebridge knots with up to eleven crossings | [['we', 'use', 'grid', 'diagrams', 'to', 'give', 'a', 'combinatorial', 'algorithm', 'for', 'computing', 'the', 'knot', 'floer', 'homology', 'of', 'the', 'pullback', 'of', 'a', 'knot', 'k', 'in', 'its', 'mfold', 'cyclic', 'branched', 'cover', 'sigmamk', 'and', 'we', 'give', 'computations', 'when', 'm2', 'for', 'over', '... | [-0.2559659562962638, 0.03221851377747953, -0.1137350157157264, 0.0653236696750603, -0.08847751349888065, -0.18773045916829936, 0.09623671511706727, 0.3792199449275028, -0.29940993508154695, -0.3561805657703768, 0.10141372201013094, -0.209921809760007, -0.15713871462503448, 0.18666075282883618, -0.13319422482428225, -0... |
709.1428 | Fluctuations in Statistical Models | The multiplicity fluctuations of hadrons are studied within the statistical
hadron-resonance gas model in the large volume limit. The role of quantum
statistics and resonance decay effects are discussed. The microscopic
correlator method is used to enforce conservation of three charges -- baryon
number, electric char... | nucl-th | the multiplicity fluctuations of hadrons are studied within the statistical hadronresonance gas model in the large volume limit the role of quantum statistics and resonance decay effects are discussed the microscopic correlator method is used to enforce conservation of three charges baryon number electric charge and st... | [['the', 'multiplicity', 'fluctuations', 'of', 'hadrons', 'are', 'studied', 'within', 'the', 'statistical', 'hadronresonance', 'gas', 'model', 'in', 'the', 'large', 'volume', 'limit', 'the', 'role', 'of', 'quantum', 'statistics', 'and', 'resonance', 'decay', 'effects', 'are', 'discussed', 'the', 'microscopic', 'correla... | [-0.06685326605849236, 0.20611676871022222, -0.12865179591416115, 0.1593718154686396, 0.0670804061348839, -0.0833570597018918, -0.04079931371794457, 0.3009822507731445, -0.17036674450949135, -0.2905919271034199, -0.044687000291298906, -0.36357403683593903, 0.06353787334646559, 0.1377280645257119, 0.031614361579754745, ... |
709.1429 | The 191 orientable octahedral manifolds | We enumerate all spaces obtained by gluing in pairs the faces of the
octahedron in an orientation-reversing fashion. Whenever such a gluing gives
rise to non-manifold points, we remove small open neighbourhoods of these
points, so we actually deal with three-dimensional manifolds with (possibly
empty) boundary.
The... | math.GT | we enumerate all spaces obtained by gluing in pairs the faces of the octahedron in an orientationreversing fashion whenever such a gluing gives rise to nonmanifold points we remove small open neighbourhoods of these points so we actually deal with threedimensional manifolds with possibly empty boundary there are 298 co... | [['we', 'enumerate', 'all', 'spaces', 'obtained', 'by', 'gluing', 'in', 'pairs', 'the', 'faces', 'of', 'the', 'octahedron', 'in', 'an', 'orientationreversing', 'fashion', 'whenever', 'such', 'a', 'gluing', 'gives', 'rise', 'to', 'nonmanifold', 'points', 'we', 'remove', 'small', 'open', 'neighbourhoods', 'of', 'these', ... | [-0.13497351521456089, 0.11217488927889606, -0.07367681631034143, 0.08762885852545303, -0.09896106863284092, -0.1636774253718996, 0.03453823817912244, 0.39497434148123783, -0.252381878788583, -0.3127970246193734, 0.1339434094491145, -0.3225512060361277, -0.17033765072885312, 0.2247742977993575, -0.14587598126749263, 0.... |
709.143 | Difference of composition operators in the Polydiscs | This paper gives some simple estimates of the essential norm for the
difference of composition operators induced by $\phi$ and $\psi$ acting on
bounded function space in the unit polydiscs $U^n$, where $\phi(z)$ and
$\psi(z)$be holomorphic self-maps of $U^n$. As its applications, a
characterization of compact differe... | math.FA | this paper gives some simple estimates of the essential norm for the difference of composition operators induced by phi and psi acting on bounded function space in the unit polydiscs un where phiz and psizbe holomorphic selfmaps of un as its applications a characterization of compact difference is given for composition... | [['this', 'paper', 'gives', 'some', 'simple', 'estimates', 'of', 'the', 'essential', 'norm', 'for', 'the', 'difference', 'of', 'composition', 'operators', 'induced', 'by', 'phi', 'and', 'psi', 'acting', 'on', 'bounded', 'function', 'space', 'in', 'the', 'unit', 'polydiscs', 'un', 'where', 'phiz', 'and', 'psizbe', 'holo... | [-0.14296100713443338, 0.14387681109732703, -0.04999597562250289, 0.041943930702185946, -0.07106526619182867, -0.007177045650518777, -0.019571388481397247, 0.3234769985602613, -0.28973248264376533, -0.2028925910984215, 0.12177930926503777, -0.2896086675392693, -0.16871205756538793, 0.22992018639649214, -0.1053125349674... |
709.1431 | Essential Norms of Weighted Composition Operators between Hardy Spaces
in the unit Ball | Let $\phi(z)=(\phi_1(z),...,\phi_n(z))$ be a holomorphic self-map of $B_n$
and $\psi(z)$ a holomorphic function on $B_n$, and $H(B_n)$ the class of all
holomorphic functions on $B_n$, where $B_n$ is the unit ball of $C^n$, the
weight composition operator $W_{\psi,\phi}$ is defined by $W_{\psi,\phi}=\psi
f(\phi)$ for ... | math.FA math.CV | let phizphi_1zphi_nz be a holomorphic selfmap of b_n and psiz a holomorphic function on b_n and hb_n the class of all holomorphic functions on b_n where b_n is the unit ball of cn the weight composition operator w_psiphi is defined by w_psiphipsi fphi for fin hb_n in this paper we estimate the essential norm for the we... | [['let', 'phizphi_1zphi_nz', 'be', 'a', 'holomorphic', 'selfmap', 'of', 'b_n', 'and', 'psiz', 'a', 'holomorphic', 'function', 'on', 'b_n', 'and', 'hb_n', 'the', 'class', 'of', 'all', 'holomorphic', 'functions', 'on', 'b_n', 'where', 'b_n', 'is', 'the', 'unit', 'ball', 'of', 'cn', 'the', 'weight', 'composition', 'operat... | [-0.09329040566441214, 0.11813778702061718, -0.053132323512595, 0.08035724161269632, -0.08398739445403001, -0.09616717349882554, -0.0045955928768148845, 0.3717206195358512, -0.32216671581190187, -0.12213598978389235, 0.10788305466700779, -0.2663220182440958, -0.12563359954799028, 0.20055398243723563, -0.089123896386438... |
709.1432 | On the integrality of the Taylor coefficients of mirror maps | We show that the Taylor coefficients of the series ${\bf q}(z)=z\exp({\bf
G}(z)/{\bf F}(z))$ are integers, where ${\bf F}(z)$ and ${\bf G}(z)+\log(z)
{\bf F}(z)$ are specific solutions of certain hypergeometric differential
equations with maximal unipotent monodromy at $z=0$. We also address the
question of finding t... | math.NT hep-th math.AG | we show that the taylor coefficients of the series bf qzzexpbf gzbf fz are integers where bf fz and bf gzlogz bf fz are specific solutions of certain hypergeometric differential equations with maximal unipotent monodromy at z0 we also address the question of finding the largest integer u such that the taylor coefficien... | [['we', 'show', 'that', 'the', 'taylor', 'coefficients', 'of', 'the', 'series', 'bf', 'qzzexpbf', 'gzbf', 'fz', 'are', 'integers', 'where', 'bf', 'fz', 'and', 'bf', 'gzlogz', 'bf', 'fz', 'are', 'specific', 'solutions', 'of', 'certain', 'hypergeometric', 'differential', 'equations', 'with', 'maximal', 'unipotent', 'mono... | [-0.1996541555363978, 0.07436727554526891, -0.03709908038262655, 0.024264000916446093, -0.08501406626388681, -0.14686110477601544, -0.013138776993002282, 0.2896783460622256, -0.2949875768880998, -0.23185070394276736, 0.0917184880210003, -0.3025467613256756, -0.1619901626431017, 0.19514730110570913, -0.0808387859829105,... |
709.1433 | The Rank-Width of Edge-Colored Graphs | Clique-width is a complexity measure of directed as well as undirected
graphs. Rank-width is an equivalent complexity measure for undirected graphs
and has good algorithmic and structural properties. It is in particular related
to the vertex-minor relation. We discuss an extension of the notion of
rank-width to edge-... | cs.DM math.CO | cliquewidth is a complexity measure of directed as well as undirected graphs rankwidth is an equivalent complexity measure for undirected graphs and has good algorithmic and structural properties it is in particular related to the vertexminor relation we discuss an extension of the notion of rankwidth to edgecolored gr... | [['cliquewidth', 'is', 'a', 'complexity', 'measure', 'of', 'directed', 'as', 'well', 'as', 'undirected', 'graphs', 'rankwidth', 'is', 'an', 'equivalent', 'complexity', 'measure', 'for', 'undirected', 'graphs', 'and', 'has', 'good', 'algorithmic', 'and', 'structural', 'properties', 'it', 'is', 'in', 'particular', 'relat... | [-0.14854202038969436, 0.1051426767250445, -0.0571959524094595, 0.07710824788906767, -0.15434390299677242, -0.17944060793396033, 0.03822142475632211, 0.4515255837652244, -0.2888038346001379, -0.3118259143797262, 0.11665020332533563, -0.31010138029321743, -0.13890740786942, 0.11493302996239166, -0.15275022265073535, 0.0... |
709.1434 | Bose-Einstein Condensation of Pions | Particle number fluctuations are studied in the ideal pion gas approaching
Bose-Einstein condensation. Two different cases are considered: Bose
condensation of pions at large charge densities $\rho_Q$ and Bose condensation
at large total densities of pions $\rho_{\pi}$. Calculations are done in grand
canonical, canon... | hep-ph | particle number fluctuations are studied in the ideal pion gas approaching boseeinstein condensation two different cases are considered bose condensation of pions at large charge densities rho_q and bose condensation at large total densities of pions rho_pi calculations are done in grand canonical canonical and microca... | [['particle', 'number', 'fluctuations', 'are', 'studied', 'in', 'the', 'ideal', 'pion', 'gas', 'approaching', 'boseeinstein', 'condensation', 'two', 'different', 'cases', 'are', 'considered', 'bose', 'condensation', 'of', 'pions', 'at', 'large', 'charge', 'densities', 'rho_q', 'and', 'bose', 'condensation', 'at', 'larg... | [-0.11462193451238697, 0.3267125468506669, -0.032086709646128975, 0.13336608400650785, 0.12311697301075719, -0.1249720346330937, -0.02501112593758225, 0.3083234326728512, -0.13047973632470466, -0.3195425534901102, -0.05486393504800786, -0.3911415623095035, 0.07074101624466413, 0.10190242923697275, 0.07812120714348501, ... |
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