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 |
|---|---|---|---|---|---|---|
707.253 | New homogeneous iron abundances of double-mode Cepheids from
high-resolution echelle spectroscopy | Aims: We define the relationship between the double-mode pulsation of
Cepheids and metallicity in a more accurate way, determine the empirical
metallicities of double-mode Cepheids from homogeneous, high-resolution
spectroscopic data, and study of the period-ratio -- metallicity dependence.
Methods: The high S/N eche... | astro-ph | aims we define the relationship between the doublemode pulsation of cepheids and metallicity in a more accurate way determine the empirical metallicities of doublemode cepheids from homogeneous highresolution spectroscopic data and study of the periodratio metallicity dependence methods the high sn echelle spectra obta... | [['aims', 'we', 'define', 'the', 'relationship', 'between', 'the', 'doublemode', 'pulsation', 'of', 'cepheids', 'and', 'metallicity', 'in', 'a', 'more', 'accurate', 'way', 'determine', 'the', 'empirical', 'metallicities', 'of', 'doublemode', 'cepheids', 'from', 'homogeneous', 'highresolution', 'spectroscopic', 'data', ... | [-0.04567713110489822, 0.09482485657972241, -0.1068197191701433, 0.09206703613691647, -0.09175757738684706, -0.13861701342730073, 0.09984731446703844, 0.4738396324832505, -0.12277400973808328, -0.3894269021159602, -0.015992327120129463, -0.3067647199223348, -0.000569612635812218, 0.24760963447998627, -0.059948096564466... |
707.2531 | Renormalization Group Analysis of a Gursey Model Inspired Field Theory
II | Recently a model, which is equivalent to the scalar form of Gursey model, is
shown to be a nontrivial field theoretical model when it is gauged with a SU(N)
field. In this paper we study another model that is equivalent to the vector
form of the Gursey model. We get a trivial theory when it is coupled with a
scalar f... | hep-th | recently a model which is equivalent to the scalar form of gursey model is shown to be a nontrivial field theoretical model when it is gauged with a sun field in this paper we study another model that is equivalent to the vector form of the gursey model we get a trivial theory when it is coupled with a scalar field thi... | [['recently', 'a', 'model', 'which', 'is', 'equivalent', 'to', 'the', 'scalar', 'form', 'of', 'gursey', 'model', 'is', 'shown', 'to', 'be', 'a', 'nontrivial', 'field', 'theoretical', 'model', 'when', 'it', 'is', 'gauged', 'with', 'a', 'sun', 'field', 'in', 'this', 'paper', 'we', 'study', 'another', 'model', 'that', 'is... | [-0.1126389813517952, 0.13820449243610797, -0.10807427242737806, 0.04725828656505439, -0.08818567073848542, -0.18570194913384816, -0.026014235993248543, 0.3481826056460185, -0.24617995791846797, -0.2935988379620193, 0.07696279689220578, -0.23273528478152694, -0.2267302883833292, 0.13681826645707978, -0.0510669375681096... |
707.2532 | KLOE measurement of the charged kaon absolute semileptonic BR's | This paper is devoted to the measurement of the fully inclusive absolute
branching ratios of the charged kaon semileptonic decays,
$K^{\pm}\to\pi^0e^\pm\nu(\gamma)$ and $K^\pm \to \pi^0\mu^\pm\nu(\gamma)$. The
measurements have been done using a tag technique, employing the two-body
decays, $K^\pm \to \mu^\pm\nu$ and... | hep-ex | this paper is devoted to the measurement of the fully inclusive absolute branching ratios of the charged kaon semileptonic decays kpmtopi0epmnugamma and kpm to pi0mupmnugamma the measurements have been done using a tag technique employing the twobody decays kpm to mupmnu and kpm to pipmpi0 and using a sample of about 4... | [['this', 'paper', 'is', 'devoted', 'to', 'the', 'measurement', 'of', 'the', 'fully', 'inclusive', 'absolute', 'branching', 'ratios', 'of', 'the', 'charged', 'kaon', 'semileptonic', 'decays', 'kpmtopi0epmnugamma', 'and', 'kpm', 'to', 'pi0mupmnugamma', 'the', 'measurements', 'have', 'been', 'done', 'using', 'a', 'tag', ... | [0.0013377505623597048, 0.1599558265816823, -0.1389851296962415, 0.03479246495643983, -0.028049423573286953, -0.1037306639969953, 0.06772837793372723, 0.2706386832318999, -0.16448068291867604, -0.3085363150009495, 0.010811652887511897, -0.42533479506351257, 0.09204687146671317, 0.1718507672383173, 0.08078993542270886, ... |
707.2533 | Mixings of 4-quark components in light non-singlet scalar mesons in QCD
sum rules | Mixings of 4-quark components in the non-singlet scalar mesons are studied in
the QCD sum rules. We propose a formulation to evaluate the cross correlators
of q\bar q and qq\bar q \bar q operators and to define the mixings of different
Fock states in the sum rule. It is applied to the non-singlet scalar mesons,
a_0 a... | hep-ph | mixings of 4quark components in the nonsinglet scalar mesons are studied in the qcd sum rules we propose a formulation to evaluate the cross correlators of qbar q and qqbar q bar q operators and to define the mixings of different fock states in the sum rule it is applied to the nonsinglet scalar mesons a_0 and k_0ast i... | [['mixings', 'of', '4quark', 'components', 'in', 'the', 'nonsinglet', 'scalar', 'mesons', 'are', 'studied', 'in', 'the', 'qcd', 'sum', 'rules', 'we', 'propose', 'a', 'formulation', 'to', 'evaluate', 'the', 'cross', 'correlators', 'of', 'qbar', 'q', 'and', 'qqbar', 'q', 'bar', 'q', 'operators', 'and', 'to', 'define', 't... | [-0.12071224738475542, 0.2927224486741389, -0.05889965507180192, 0.16782714919522837, -0.024359754533073756, -0.12287710993117544, 0.06630904991233852, 0.30629923372247886, -0.1540778133433399, -0.17816793193044358, -0.06798494752729312, -0.32859624268183873, -0.023668414949666882, 0.031124598790653223, 0.0883559272407... |
707.2534 | Renyi Entropy of the XY Spin Chain | We consider the one-dimensional XY quantum spin chain in a transverse
magnetic field. We are interested in the Renyi entropy of a block of L
neighboring spins at zero temperature on an infinite lattice. The Renyi entropy
is essentially the trace of some power $\alpha$ of the density matrix of the
block. We calculate ... | quant-ph cond-mat.stat-mech hep-th | we consider the onedimensional xy quantum spin chain in a transverse magnetic field we are interested in the renyi entropy of a block of l neighboring spins at zero temperature on an infinite lattice the renyi entropy is essentially the trace of some power alpha of the density matrix of the block we calculate the asymp... | [['we', 'consider', 'the', 'onedimensional', 'xy', 'quantum', 'spin', 'chain', 'in', 'a', 'transverse', 'magnetic', 'field', 'we', 'are', 'interested', 'in', 'the', 'renyi', 'entropy', 'of', 'a', 'block', 'of', 'l', 'neighboring', 'spins', 'at', 'zero', 'temperature', 'on', 'an', 'infinite', 'lattice', 'the', 'renyi', ... | [-0.16139238032898526, 0.1713624041228663, -0.06633697353621446, 0.055130154922286546, 0.0008793193210915822, -0.11048206302859798, 0.037995863413983366, 0.32554160896234396, -0.3046947442574381, -0.2240010719510681, 0.08154599561197001, -0.3279391708460114, -0.0939150592598996, 0.1681942195393054, -0.02017199341434894... |
707.2535 | Simple theory of the measured current through quantum dots | A simple theory of the detected current I(t) flowing through charge qubits --
quantum dots -- is proposed in terms of standard continuous measurement theory.
Applied to a double dot, our formalism easily confirms previous results on
quantum Zeno effect, driven by growing ammeter performance gamma. Due to the
transpar... | cond-mat.mes-hall | a simple theory of the detected current it flowing through charge qubits quantum dots is proposed in terms of standard continuous measurement theory applied to a double dot our formalism easily confirms previous results on quantum zeno effect driven by growing ammeter performance gamma due to the transparent formalism ... | [['a', 'simple', 'theory', 'of', 'the', 'detected', 'current', 'it', 'flowing', 'through', 'charge', 'qubits', 'quantum', 'dots', 'is', 'proposed', 'in', 'terms', 'of', 'standard', 'continuous', 'measurement', 'theory', 'applied', 'to', 'a', 'double', 'dot', 'our', 'formalism', 'easily', 'confirms', 'previous', 'result... | [-0.14001328270328608, 0.1472218370598401, -0.0442035141891825, 0.0402125869201169, -0.006023709187158258, -0.16800889773671893, 0.07210414227714913, 0.34894521417673613, -0.2280467636253987, -0.2552789577308136, -0.006032434444736085, -0.2772941651275834, -0.12005198027032453, 0.26981111077239384, -0.03940176104220587... |
707.2536 | On Lee Smolin's The Trouble with Physics | Lee Smolin's casual accounting of special and general relativity in The
Trouble with Physics raises an interesting question: is it possible to develop
a legitimate argument concerning string theories starting from a shaky basis?
This is apparently what Lee Smolin succeeded in doing when he wrote The Trouble
with Phys... | physics.gen-ph | lee smolins casual accounting of special and general relativity in the trouble with physics raises an interesting question is it possible to develop a legitimate argument concerning string theories starting from a shaky basis this is apparently what lee smolin succeeded in doing when he wrote the trouble with physics t... | [['lee', 'smolins', 'casual', 'accounting', 'of', 'special', 'and', 'general', 'relativity', 'in', 'the', 'trouble', 'with', 'physics', 'raises', 'an', 'interesting', 'question', 'is', 'it', 'possible', 'to', 'develop', 'a', 'legitimate', 'argument', 'concerning', 'string', 'theories', 'starting', 'from', 'a', 'shaky',... | [-0.07326862046362034, 0.12318925620456866, -0.11067250331065484, 0.18874687201917237, -0.17923847838704074, -0.2780829002980941, 0.057280787865498235, 0.2721065450875488, -0.20497301536618448, -0.3685930428826915, 0.055753317898571755, -0.2748085185261776, -0.17217750284388394, 0.1497494814060961, -0.16832185055994028... |
707.2537 | A Combined Spitzer and Chandra Survey of Young Stellar Objects in the
Serpens Cloud Core | We present Spitzer and Chandra observations of the nearby (~260 pc) embedded
stellar cluster in the Serpens Cloud Core. We observed, using Spitzer's IRAC
and MIPS instruments, in six wavelength bands from 3 to 70 ${\mu}m$, to detect
thermal emission from circumstellar disks and protostellar envelopes, and to
classify... | astro-ph | we present spitzer and chandra observations of the nearby 260 pc embedded stellar cluster in the serpens cloud core we observed using spitzers irac and mips instruments in six wavelength bands from 3 to 70 mum to detect thermal emission from circumstellar disks and protostellar envelopes and to classify stars using col... | [['we', 'present', 'spitzer', 'and', 'chandra', 'observations', 'of', 'the', 'nearby', '260', 'pc', 'embedded', 'stellar', 'cluster', 'in', 'the', 'serpens', 'cloud', 'core', 'we', 'observed', 'using', 'spitzers', 'irac', 'and', 'mips', 'instruments', 'in', 'six', 'wavelength', 'bands', 'from', '3', 'to', '70', 'mum', ... | [-0.005070505430320594, 0.13319447355716266, -0.01752576454823273, 0.0884442643901287, -0.07627255672373431, -0.056517605377315, 0.05159123662054877, 0.48876100486675506, -0.14190037010337633, -0.3901597855988821, 0.07451849985311639, -0.31399114063964034, 0.015241315695149285, 0.13621709421267425, -0.02833340544549917... |
707.2538 | Non-parametric inversion of gravitational lensing systems with few
images using a multi-objective genetic algorithm | Galaxies acting as gravitational lenses are surrounded by, at most, a handful
of images. This apparent paucity of information forces one to make the best
possible use of what information is available to invert the lens system. In
this paper, we explore the use of a genetic algorithm to invert in a
non-parametric way ... | astro-ph | galaxies acting as gravitational lenses are surrounded by at most a handful of images this apparent paucity of information forces one to make the best possible use of what information is available to invert the lens system in this paper we explore the use of a genetic algorithm to invert in a nonparametric way strong l... | [['galaxies', 'acting', 'as', 'gravitational', 'lenses', 'are', 'surrounded', 'by', 'at', 'most', 'a', 'handful', 'of', 'images', 'this', 'apparent', 'paucity', 'of', 'information', 'forces', 'one', 'to', 'make', 'the', 'best', 'possible', 'use', 'of', 'what', 'information', 'is', 'available', 'to', 'invert', 'the', 'l... | [-0.10602377778452234, 0.03289438727752943, -0.0743855099107972, 0.1114283755899554, -0.13129134002435755, -0.09641755454634365, 0.019874842488206923, 0.364728845008894, -0.24518599176999967, -0.385284071557812, 0.10818784055606413, -0.27641033083200456, -0.12281209607486074, 0.19246876887658512, -0.06889501224029931, ... |
707.2539 | Three-dimensional Monte Carlo simulations of the quantum linear
Boltzmann equation | Recently the general form of a translation-covariant quantum Boltzmann
equation has been derived which describes the dynamics of a tracer particle in
a quantum gas. We develop a stochastic wave function algorithm that enables
full three-dimensional Monte Carlo simulations of this equation. The simulation
method is us... | quant-ph cond-mat.stat-mech | recently the general form of a translationcovariant quantum boltzmann equation has been derived which describes the dynamics of a tracer particle in a quantum gas we develop a stochastic wave function algorithm that enables full threedimensional monte carlo simulations of this equation the simulation method is used to ... | [['recently', 'the', 'general', 'form', 'of', 'a', 'translationcovariant', 'quantum', 'boltzmann', 'equation', 'has', 'been', 'derived', 'which', 'describes', 'the', 'dynamics', 'of', 'a', 'tracer', 'particle', 'in', 'a', 'quantum', 'gas', 'we', 'develop', 'a', 'stochastic', 'wave', 'function', 'algorithm', 'that', 'en... | [-0.08123632961999468, 0.12165643993743899, -0.17290508876789676, 0.10376535797770196, -0.003900711733638962, -0.07214243996944975, 0.0013459783339019968, 0.30728609677160457, -0.2815280887777003, -0.2746947719889615, 0.015900839198485155, -0.2815015544401151, -0.11609560940588746, 0.1876362176355253, 0.057363309688587... |
707.254 | On how good DFT exchange-correlation functionals are for H bonds in
small water clusters: Benchmarks approaching the complete basis set limit | The ability of several density-functional theory (DFT) exchange-correlation
functionals to describe hydrogen bonds in small water clusters (dimer to
pentamer) in their global minimum energy structures is evaluated with reference
to second order Moeller Plesset perturbation theory (MP2). Errors from basis
set incomple... | cond-mat.mtrl-sci | the ability of several densityfunctional theory dft exchangecorrelation functionals to describe hydrogen bonds in small water clusters dimer to pentamer in their global minimum energy structures is evaluated with reference to second order moeller plesset perturbation theory mp2 errors from basis set incompleteness have... | [['the', 'ability', 'of', 'several', 'densityfunctional', 'theory', 'dft', 'exchangecorrelation', 'functionals', 'to', 'describe', 'hydrogen', 'bonds', 'in', 'small', 'water', 'clusters', 'dimer', 'to', 'pentamer', 'in', 'their', 'global', 'minimum', 'energy', 'structures', 'is', 'evaluated', 'with', 'reference', 'to',... | [-0.04468211380299181, -0.01901417608106775, -0.10282904071001601, 0.15572547681871843, 0.03630928863796206, -0.09738622062390537, 0.09610119807309404, 0.4004434158705408, -0.21271225060055649, -0.33155704081790255, -0.03559765486092407, -0.35460244345345665, -0.10216883273928293, 0.11931674933085949, 0.004721407124634... |
707.2541 | Measurement of e^+e^- to pi^+pi^-J/psi Cross Section via Initial State
Radiation at Belle | The cross section for e^+e^- to pi^+pi^-J/psi between 3.8 and 5.5 GeV/c^2 is
measured using a 548 fb^{-1} data sample collected on or near the Upsilon(4S)
resonance with the Belle detector at KEKB. A peak near 4.25 GeV/c^2,
corresponding to the so called Y(4260), is observed. In addition, there is
another cluster of ... | hep-ex hep-ph | the cross section for ee to pipijpsi between 38 and 55 gevc2 is measured using a 548 fb1 data sample collected on or near the upsilon4s resonance with the belle detector at kekb a peak near 425 gevc2 corresponding to the so called y4260 is observed in addition there is another cluster of events at around 405 gevc2 a fi... | [['the', 'cross', 'section', 'for', 'ee', 'to', 'pipijpsi', 'between', '38', 'and', '55', 'gevc2', 'is', 'measured', 'using', 'a', '548', 'fb1', 'data', 'sample', 'collected', 'on', 'or', 'near', 'the', 'upsilon4s', 'resonance', 'with', 'the', 'belle', 'detector', 'at', 'kekb', 'a', 'peak', 'near', '425', 'gevc2', 'cor... | [-0.06445524479187596, 0.12271371378159236, -0.0799850394799449, 0.1354025383252415, -0.06335328575812452, -0.1300231937864988, 0.06860763978898182, 0.3547586080157894, -0.09882614025096784, -0.3568554944519339, -0.044396578448011016, -0.46254151224576195, 0.057391746512924634, 0.18889125516295605, 0.050311570655254795... |
707.2542 | Representation of finite connective spaces | After recalling the definition of connectivity spaces and some of their main
properties, a way is proposed to represent finite connectivity spaces by
directed simple graphs. Then a connectivity structure is associated to each
tame link. It is showed that all spaces of a certain class (the iterated
Brunnian ones) admi... | math.GN math.AT | after recalling the definition of connectivity spaces and some of their main properties a way is proposed to represent finite connectivity spaces by directed simple graphs then a connectivity structure is associated to each tame link it is showed that all spaces of a certain class the iterated brunnian ones admit repre... | [['after', 'recalling', 'the', 'definition', 'of', 'connectivity', 'spaces', 'and', 'some', 'of', 'their', 'main', 'properties', 'a', 'way', 'is', 'proposed', 'to', 'represent', 'finite', 'connectivity', 'spaces', 'by', 'directed', 'simple', 'graphs', 'then', 'a', 'connectivity', 'structure', 'is', 'associated', 'to', ... | [-0.24367842238682966, 0.036589036980428945, -0.17697193363251595, 0.10809757791531201, -0.14765228225419727, -0.14867359508151332, -0.21645697922660753, 0.16509945082048383, -0.2033801055011841, -0.21217920498635906, 0.06917637970405989, -0.3312676043697418, -0.27575778150214597, 0.14781368649072157, -0.34399367940003... |
707.2543 | Development of Tracking Detectors with industrially produced GEM Foils | The planned tracking upgrade of the STAR experiment at RHIC includes a
large-area GEM tracker used to determine the charge sign of electrons and
positrons produced from W+(-) decays. For such a large-scale project commercial
availability of GEM foils is necessary. We report first results obtained with a
triple GEM de... | physics.ins-det | the planned tracking upgrade of the star experiment at rhic includes a largearea gem tracker used to determine the charge sign of electrons and positrons produced from w decays for such a largescale project commercial availability of gem foils is necessary we report first results obtained with a triple gem detector usi... | [['the', 'planned', 'tracking', 'upgrade', 'of', 'the', 'star', 'experiment', 'at', 'rhic', 'includes', 'a', 'largearea', 'gem', 'tracker', 'used', 'to', 'determine', 'the', 'charge', 'sign', 'of', 'electrons', 'and', 'positrons', 'produced', 'from', 'w', 'decays', 'for', 'such', 'a', 'largescale', 'project', 'commerci... | [-0.043419561732673286, 0.09344029341300483, -0.08329645118704349, -0.00850545383185487, 0.02801513559551853, -0.15581148990119498, -0.027176689698755967, 0.398842680928382, -0.18446158371639973, -0.3560791507701982, 0.07991331955135772, -0.34108793119808206, 0.014001650261255263, 0.28569813519575155, -0.02965949454034... |
707.2544 | A polarizable ion model for the structure of molten AgI | The results are reported of the molecular dynamics simulations of the
coherent static structure factor of molten AgI at 923 K using a polarizable ion
model. This model is based on a rigid ion potential, to which the many body
interactions due to the anions induced polarization are added. The calculated
structure fact... | cond-mat.soft physics.chem-ph | the results are reported of the molecular dynamics simulations of the coherent static structure factor of molten agi at 923 k using a polarizable ion model this model is based on a rigid ion potential to which the many body interactions due to the anions induced polarization are added the calculated structure factor is... | [['the', 'results', 'are', 'reported', 'of', 'the', 'molecular', 'dynamics', 'simulations', 'of', 'the', 'coherent', 'static', 'structure', 'factor', 'of', 'molten', 'agi', 'at', '923', 'k', 'using', 'a', 'polarizable', 'ion', 'model', 'this', 'model', 'is', 'based', 'on', 'a', 'rigid', 'ion', 'potential', 'to', 'which... | [-0.08042233627404749, 0.12156880468600574, -0.06415269294208799, 0.024098093291389344, 0.010023561543929055, -0.09776822985005901, 0.008997344373504525, 0.4186502511507457, -0.2534651852491283, -0.31577861366659093, -0.005831641829140561, -0.3116876676525037, -0.09851513579295776, 0.149780763577209, 0.0571122014866277... |
707.2545 | Particle multiplicities in Lead-Lead collisions at the LHC from
non-linear evolution with running coupling | We present predictions for the pseudo-rapidity density of charged particles
produced in central Pb-Pb collisions at the LHC. Particle production in such
collisions is calculated in the framework of k_t-factorization. The nuclear
unintegrated gluon distributions at LHC energies are determined from numerical
solutions ... | hep-ph | we present predictions for the pseudorapidity density of charged particles produced in central pbpb collisions at the lhc particle production in such collisions is calculated in the framework of k_tfactorization the nuclear unintegrated gluon distributions at lhc energies are determined from numerical solutions of the ... | [['we', 'present', 'predictions', 'for', 'the', 'pseudorapidity', 'density', 'of', 'charged', 'particles', 'produced', 'in', 'central', 'pbpb', 'collisions', 'at', 'the', 'lhc', 'particle', 'production', 'in', 'such', 'collisions', 'is', 'calculated', 'in', 'the', 'framework', 'of', 'k_tfactorization', 'the', 'nuclear'... | [-0.026782510378278602, 0.24796629952601132, -0.16441771775507966, 0.1752159385061345, 0.06711002704329215, -0.08552113885227113, -0.12138616853954796, 0.35409824249262994, -0.1591059181313866, -0.32519795227413756, -0.07493079508481643, -0.3864572954435761, 0.19452991081664386, 0.1266954129588647, 0.15257893092572117,... |
707.2546 | High-order harmonic generation from diatomic molecules with large
internuclear distance: The effect of two-center interference | In the present paper, we investigate the high-order harmonic generation (HHG)
from diatomic molecules with large internuclear distance using a strong field
approximation (SFA) model. We find that the hump and dip structure emerges in
the plateau region of the harmonic spectrum, and the location of this striking
struc... | physics.atom-ph | in the present paper we investigate the highorder harmonic generation hhg from diatomic molecules with large internuclear distance using a strong field approximation sfa model we find that the hump and dip structure emerges in the plateau region of the harmonic spectrum and the location of this striking structure is se... | [['in', 'the', 'present', 'paper', 'we', 'investigate', 'the', 'highorder', 'harmonic', 'generation', 'hhg', 'from', 'diatomic', 'molecules', 'with', 'large', 'internuclear', 'distance', 'using', 'a', 'strong', 'field', 'approximation', 'sfa', 'model', 'we', 'find', 'that', 'the', 'hump', 'and', 'dip', 'structure', 'em... | [-0.12669852055609226, 0.1481586904078722, -0.05072145656216889, 0.09285630469210446, 0.015635939771309493, -0.13075886166654527, 0.02106543947593309, 0.40958483962807807, -0.2804340958222747, -0.30528481053348516, -0.01885101713007316, -0.2696008772403002, -0.17322130555985496, 0.1693453479395248, 0.04093358691985486,... |
707.2547 | An empirical model for the beams of radio pulsars | Motivated by recent results on the location of the radio emission in pulsar
magnetospheres, we have developed a model which can account for the large
diversity found in the average profile shapes of pulsars. At the centre of our
model lies the idea that radio emission at a particular frequency arises from a
wide rang... | astro-ph | motivated by recent results on the location of the radio emission in pulsar magnetospheres we have developed a model which can account for the large diversity found in the average profile shapes of pulsars at the centre of our model lies the idea that radio emission at a particular frequency arises from a wide range of... | [['motivated', 'by', 'recent', 'results', 'on', 'the', 'location', 'of', 'the', 'radio', 'emission', 'in', 'pulsar', 'magnetospheres', 'we', 'have', 'developed', 'a', 'model', 'which', 'can', 'account', 'for', 'the', 'large', 'diversity', 'found', 'in', 'the', 'average', 'profile', 'shapes', 'of', 'pulsars', 'at', 'the... | [-0.07807289955917723, 0.12450745489575932, -0.05153889639696442, 0.09139071806530635, -0.06455118192926697, -0.0654384794092581, 0.03215515815438876, 0.44401740804545997, -0.2256603052482437, -0.35326644027408977, 0.042729316489707375, -0.24405689533186717, -0.08219393203902689, 0.2567835475234257, -0.0111181773145911... |
707.2548 | The behavior of non-linear anisotropies in bouncing Bianchi I models of
loop quantum cosmology | In homogeneous and isotropic loop quantum cosmology, gravity can behave
repulsively at Planckian energy densities leading to the replacement of the big
bang singularity with a big bounce. Yet in any bouncing scenario it is
important to include non-linear effects from anisotropies which typically grow
during the colla... | gr-qc astro-ph | in homogeneous and isotropic loop quantum cosmology gravity can behave repulsively at planckian energy densities leading to the replacement of the big bang singularity with a big bounce yet in any bouncing scenario it is important to include nonlinear effects from anisotropies which typically grow during the collapsing... | [['in', 'homogeneous', 'and', 'isotropic', 'loop', 'quantum', 'cosmology', 'gravity', 'can', 'behave', 'repulsively', 'at', 'planckian', 'energy', 'densities', 'leading', 'to', 'the', 'replacement', 'of', 'the', 'big', 'bang', 'singularity', 'with', 'a', 'big', 'bounce', 'yet', 'in', 'any', 'bouncing', 'scenario', 'it'... | [-0.13191299261358966, 0.22151063276853944, -0.13538885288871824, 0.08401397794950753, -0.05024722710118762, -0.125028708138104, -0.05584213330210852, 0.30499988198945566, -0.29373108358787636, -0.24619153051504067, 0.08162703145062551, -0.282913144997188, -0.0874310773398195, 0.12547758178552612, 0.017520529242964194,... |
707.2549 | Cavity polaritons in the presence of symmetry-breaking disorder:
closed-path time formalism | According to the mean-field theory of Zittartz, when subject to a
symmetry-breaking disorder, the order parameter and the energy gap of an
excitonic insulator are gradually suppressed up to a critical disorder
strength. Recently, Marchetti, Simons, and Littlewood have used a replica trick
to investigate the effects o... | cond-mat.str-el cond-mat.dis-nn | according to the meanfield theory of zittartz when subject to a symmetrybreaking disorder the order parameter and the energy gap of an excitonic insulator are gradually suppressed up to a critical disorder strength recently marchetti simons and littlewood have used a replica trick to investigate the effects of disorder... | [['according', 'to', 'the', 'meanfield', 'theory', 'of', 'zittartz', 'when', 'subject', 'to', 'a', 'symmetrybreaking', 'disorder', 'the', 'order', 'parameter', 'and', 'the', 'energy', 'gap', 'of', 'an', 'excitonic', 'insulator', 'are', 'gradually', 'suppressed', 'up', 'to', 'a', 'critical', 'disorder', 'strength', 'rec... | [-0.10315655271528966, 0.1399455676097376, -0.10857647204679759, 0.08418966892578393, -0.04832215156589564, -0.13905626502631424, 0.061492488289360506, 0.329368045528507, -0.2401516496072285, -0.2896934301684289, 0.041613248373682486, -0.27286786690036946, -0.14891991189225773, 0.12252956723080188, 0.006903874603279703... |
707.255 | How Large is the Intrinsic Flux Noise of a Magnetic Flux Quantum, of
Half a Flux Quantum and of a Vortex-Free Superconductor? | This article addresses the question whether the magnetic flux of stationary
vortices or of half flux quanta generated by frustrated superconducting rings
is noisy. It is found that the flux noise generated intrinsically by a
superconductor is, in good approximation, not enhanced by stationary vortices.
Half flux quan... | cond-mat.supr-con cond-mat.stat-mech | this article addresses the question whether the magnetic flux of stationary vortices or of half flux quanta generated by frustrated superconducting rings is noisy it is found that the flux noise generated intrinsically by a superconductor is in good approximation not enhanced by stationary vortices half flux quanta gen... | [['this', 'article', 'addresses', 'the', 'question', 'whether', 'the', 'magnetic', 'flux', 'of', 'stationary', 'vortices', 'or', 'of', 'half', 'flux', 'quanta', 'generated', 'by', 'frustrated', 'superconducting', 'rings', 'is', 'noisy', 'it', 'is', 'found', 'that', 'the', 'flux', 'noise', 'generated', 'intrinsically', ... | [-0.20690502558967896, 0.3015908133238554, 0.04844306789787619, 0.11865780208609067, -0.018185612479490892, -0.13811253382924146, 0.05026189302277219, 0.3500480746318187, -0.21647470376254724, -0.3178283432165959, 0.058470101833726015, -0.2722309206479362, -0.07687745157246743, 0.21504098637212468, -0.06942733483239343... |
707.2551 | Coupling biochemistry and mechanics in cell adhesion: a model for
inhomogeneous stress fiber contraction | Biochemistry and mechanics are closely coupled in cell adhesion. At sites of
cell-matrix adhesion, mechanical force triggers signaling through the
Rho-pathway, which leads to structural reinforcement and increased
contractility in the actin cytoskeleton. The resulting force acts back to the
sites of adhesion, resulti... | q-bio.SC q-bio.CB | biochemistry and mechanics are closely coupled in cell adhesion at sites of cellmatrix adhesion mechanical force triggers signaling through the rhopathway which leads to structural reinforcement and increased contractility in the actin cytoskeleton the resulting force acts back to the sites of adhesion resulting in a p... | [['biochemistry', 'and', 'mechanics', 'are', 'closely', 'coupled', 'in', 'cell', 'adhesion', 'at', 'sites', 'of', 'cellmatrix', 'adhesion', 'mechanical', 'force', 'triggers', 'signaling', 'through', 'the', 'rhopathway', 'which', 'leads', 'to', 'structural', 'reinforcement', 'and', 'increased', 'contractility', 'in', 't... | [-0.15008942215198665, 0.1993026475049733, 0.006063976946383722, -0.031372384092670985, -0.03714042683380819, -0.17497662850122414, 0.004064537546568984, 0.4077783418350092, -0.30101596123275864, -0.19290752598006305, -0.006604939630745647, -0.23524014094581416, -0.27925709204193744, 0.14746939019612854, -0.03860031268... |
707.2552 | Observations of interior whispering gallery modes in asymmetric optical
resonators with rational caustics | We propose asymmetric resonant cavities with rational caustics and
experimentally demonstrate interior whispering gallery modes in monolithic
silicon mesoscopic microcavities. These microcavities demonstrate unique
robustness of cavity quality factor (Q) against roughness Rayleigh scattering.
Angle-resolved tapered f... | physics.optics | we propose asymmetric resonant cavities with rational caustics and experimentally demonstrate interior whispering gallery modes in monolithic silicon mesoscopic microcavities these microcavities demonstrate unique robustness of cavity quality factor q against roughness rayleigh scattering angleresolved tapered fiber me... | [['we', 'propose', 'asymmetric', 'resonant', 'cavities', 'with', 'rational', 'caustics', 'and', 'experimentally', 'demonstrate', 'interior', 'whispering', 'gallery', 'modes', 'in', 'monolithic', 'silicon', 'mesoscopic', 'microcavities', 'these', 'microcavities', 'demonstrate', 'unique', 'robustness', 'of', 'cavity', 'q... | [-0.14054512377414438, 0.17859510239213705, -0.0504353434616138, -0.10649502623294081, -0.073688589716478, -0.2580364386048464, -0.03257500561552921, 0.5309082287999373, -0.21834514973064265, -0.2405631917987078, -0.04740356530768738, -0.30405364286095377, -0.149208777805879, 0.2434888956920495, -0.0448209061213429, 0.... |
707.2553 | Electroweak corrections to W-boson hadroproduction at finite transverse
momentum | We calculate the full one-loop electroweak radiative corrections to the cross
section of single W-boson inclusive hadroproduction at finite transverse
momentum (p_T). This includes the O(alpha) corrections to W+j production, the
O(alpha_s) corrections to W+gamma production, and the tree-level contribution
from W+j ph... | hep-ph hep-ex | we calculate the full oneloop electroweak radiative corrections to the cross section of single wboson inclusive hadroproduction at finite transverse momentum p_t this includes the oalpha corrections to wj production the oalpha_s corrections to wgamma production and the treelevel contribution from wj photoproduction wit... | [['we', 'calculate', 'the', 'full', 'oneloop', 'electroweak', 'radiative', 'corrections', 'to', 'the', 'cross', 'section', 'of', 'single', 'wboson', 'inclusive', 'hadroproduction', 'at', 'finite', 'transverse', 'momentum', 'p_t', 'this', 'includes', 'the', 'oalpha', 'corrections', 'to', 'wj', 'production', 'the', 'oalp... | [-0.01026237911587073, 0.18750860292295163, -0.11717810212973166, 0.17448973750288133, -0.03868257156731984, -0.06309678059452298, 0.01084072718301534, 0.3118006620048122, -0.1942111031782009, -0.2369303601497615, -0.05921148266034751, -0.4160074058454484, 0.13509666108968138, 0.12901870423692427, 0.11306836671957915, ... |
707.2554 | On C1-robust transitivity of volume-preserving flows | We prove that a divergence-free and C1-robustly transitive vector field has
no singularities. Moreover, if the vector field is C4 then the linear Poincare
flow associated to it admits a dominated splitting over M.
| math.DS | we prove that a divergencefree and c1robustly transitive vector field has no singularities moreover if the vector field is c4 then the linear poincare flow associated to it admits a dominated splitting over m | [['we', 'prove', 'that', 'a', 'divergencefree', 'and', 'c1robustly', 'transitive', 'vector', 'field', 'has', 'no', 'singularities', 'moreover', 'if', 'the', 'vector', 'field', 'is', 'c4', 'then', 'the', 'linear', 'poincare', 'flow', 'associated', 'to', 'it', 'admits', 'a', 'dominated', 'splitting', 'over', 'm']] | [-0.24541795398930416, 0.15491478594348712, -0.10069651501801084, 0.06063918899813229, -0.15327763072598508, -0.15971828857436776, -0.06328611147096928, 0.3856605008682784, -0.3153545499286231, -0.10705943923333988, 0.11388644267914488, -0.2516900912365493, -0.15374023724785624, 0.16072536823476719, -0.0461494292077772... |
707.2555 | Generalization of escape rate from a metastable state driven by external
cross-correlated noise processes | We propose generalization of escape rate from a metastable state for
externally driven correlated noise processes in one dimension. In addition to
the internal non-Markovian thermal fluctuations, the external correlated noise
processes we consider are Gaussian, stationary in nature and are of
Ornstein-Uhlenbeck type.... | cond-mat.stat-mech cond-mat.soft | we propose generalization of escape rate from a metastable state for externally driven correlated noise processes in one dimension in addition to the internal nonmarkovian thermal fluctuations the external correlated noise processes we consider are gaussian stationary in nature and are of ornsteinuhlenbeck type based o... | [['we', 'propose', 'generalization', 'of', 'escape', 'rate', 'from', 'a', 'metastable', 'state', 'for', 'externally', 'driven', 'correlated', 'noise', 'processes', 'in', 'one', 'dimension', 'in', 'addition', 'to', 'the', 'internal', 'nonmarkovian', 'thermal', 'fluctuations', 'the', 'external', 'correlated', 'noise', 'p... | [-0.13294834605502812, 0.16387377080530668, -0.05399801490120282, 0.0902719632683953, 0.006024419857296816, -0.1181160504121549, 0.08475063308257579, 0.3360362386654231, -0.26864733154623777, -0.2719898812380458, 0.05415403712704424, -0.27618654045345614, -0.11561876554657852, 0.18135129343064055, -0.032065945904517223... |
707.2556 | Study of Initial and Final State Effects in Ultrarelativistic Heavy Ion
Collisions Using Hadronic Probes | It has been theorized that if heavy nuclei (e.g. Au, Pb) are collided at
sufficiently high energies, we might be to recreate the conditions that existed
in the universe a few microseconds after the Big Bang. The kinetic energy of
the colliding nuclei gets converted into heat, leading to a phase transition
into a new ... | nucl-ex | it has been theorized that if heavy nuclei eg au pb are collided at sufficiently high energies we might be to recreate the conditions that existed in the universe a few microseconds after the big bang the kinetic energy of the colliding nuclei gets converted into heat leading to a phase transition into a new state of m... | [['it', 'has', 'been', 'theorized', 'that', 'if', 'heavy', 'nuclei', 'eg', 'au', 'pb', 'are', 'collided', 'at', 'sufficiently', 'high', 'energies', 'we', 'might', 'be', 'to', 'recreate', 'the', 'conditions', 'that', 'existed', 'in', 'the', 'universe', 'a', 'few', 'microseconds', 'after', 'the', 'big', 'bang', 'the', 'k... | [-0.031122308531184754, 0.2840686527114095, -0.1985950571843349, 0.10774687745022617, -0.03733070111197848, -0.10181632421408145, 0.011977606619309102, 0.3440181237870886, -0.25361757420764736, -0.3070230384704672, 0.005022061134075066, -0.3330416558365825, 0.06271042672562457, 0.128641342385284, 0.031667224759797725, ... |
707.2557 | Uniform estimates for cubic oscillatory integrals | This paper establishes the optimal decay rate for scalar oscillatory
integrals in $n$ variables which satisfy a nondegeneracy condition on the third
derivatives. The estimates proved are stable under small linear perturbations,
as encountered when computing the Fourier transform of surface-carried
measures. The main ... | math.CA | this paper establishes the optimal decay rate for scalar oscillatory integrals in n variables which satisfy a nondegeneracy condition on the third derivatives the estimates proved are stable under small linear perturbations as encountered when computing the fourier transform of surfacecarried measures the main idea of ... | [['this', 'paper', 'establishes', 'the', 'optimal', 'decay', 'rate', 'for', 'scalar', 'oscillatory', 'integrals', 'in', 'n', 'variables', 'which', 'satisfy', 'a', 'nondegeneracy', 'condition', 'on', 'the', 'third', 'derivatives', 'the', 'estimates', 'proved', 'are', 'stable', 'under', 'small', 'linear', 'perturbations'... | [-0.19972878138562947, 0.14866443822216807, -0.09821123028682037, 0.10197133096781644, -0.06193300754988961, -0.1272649243121233, -0.016116530787919393, 0.27029959284559346, -0.3150465395583799, -0.21492121188026486, 0.1468957643673727, -0.22226333696479825, -0.14616220635291416, 0.1906107685698027, -0.0797761066880246... |
707.2558 | Faxen relations in solids - a generalized approach to particle motion in
elasticity and viscoelasticity | A movable inclusion in an elastic material oscillates as a rigid body with
six degrees of freedom. Displacement/rotation and force/moment tensors which
express the motion of the inclusion in terms of the displacement and force at
arbitrary exterior points are introduced. Using reciprocity arguments two
general identi... | cond-mat.mtrl-sci | a movable inclusion in an elastic material oscillates as a rigid body with six degrees of freedom displacementrotation and forcemoment tensors which express the motion of the inclusion in terms of the displacement and force at arbitrary exterior points are introduced using reciprocity arguments two general identities a... | [['a', 'movable', 'inclusion', 'in', 'an', 'elastic', 'material', 'oscillates', 'as', 'a', 'rigid', 'body', 'with', 'six', 'degrees', 'of', 'freedom', 'displacementrotation', 'and', 'forcemoment', 'tensors', 'which', 'express', 'the', 'motion', 'of', 'the', 'inclusion', 'in', 'terms', 'of', 'the', 'displacement', 'and'... | [-0.16521994884197527, 0.13793232029424055, -0.04949099178282687, 0.002672372899280909, -0.10012181414864384, -0.08216072712093592, -0.04767835619023595, 0.2910986076324032, -0.2658727945377811, -0.29790086818236605, 0.0819757180616785, -0.29212440961064434, -0.16873593525125238, 0.17705433620647407, -0.006133108573685... |
707.2559 | Recoil velocities from equal-mass binary black-hole mergers: a
systematic investigation of spin-orbit aligned configurations | Binary black-hole systems with spins aligned with the orbital angular
momentum are of special interest, as studies indicate that this configuration
is preferred in nature. If the spins of the two bodies differ, there can be a
prominent beaming of the gravitational radiation during the late plunge,
causing a recoil of... | gr-qc astro-ph | binary blackhole systems with spins aligned with the orbital angular momentum are of special interest as studies indicate that this configuration is preferred in nature if the spins of the two bodies differ there can be a prominent beaming of the gravitational radiation during the late plunge causing a recoil of the fi... | [['binary', 'blackhole', 'systems', 'with', 'spins', 'aligned', 'with', 'the', 'orbital', 'angular', 'momentum', 'are', 'of', 'special', 'interest', 'as', 'studies', 'indicate', 'that', 'this', 'configuration', 'is', 'preferred', 'in', 'nature', 'if', 'the', 'spins', 'of', 'the', 'two', 'bodies', 'differ', 'there', 'ca... | [-0.11503362337569312, 0.12796089237859726, -0.07627600487163765, 0.06383191064963023, -0.059221115242689845, -0.07649933624917925, 0.005258571594495769, 0.36452075090748653, -0.19881427379056685, -0.33362818895997004, 0.0703408393002573, -0.2731569939790199, -0.04873511838742484, 0.2401993773727662, -0.006500841775747... |
707.256 | Red Density Perturbations and Inflationary Gravitational Waves | We study the implications of recent indications for a red spectrum of
primordial density perturbations for the detection of inflationary
gravitational waves (IGWs) with forthcoming cosmic microwave background
experiments. We find that if inflation occurs with a single field with an
inflaton potential minimized at V=0... | astro-ph | we study the implications of recent indications for a red spectrum of primordial density perturbations for the detection of inflationary gravitational waves igws with forthcoming cosmic microwave background experiments we find that if inflation occurs with a single field with an inflaton potential minimized at v0 then ... | [['we', 'study', 'the', 'implications', 'of', 'recent', 'indications', 'for', 'a', 'red', 'spectrum', 'of', 'primordial', 'density', 'perturbations', 'for', 'the', 'detection', 'of', 'inflationary', 'gravitational', 'waves', 'igws', 'with', 'forthcoming', 'cosmic', 'microwave', 'background', 'experiments', 'we', 'find'... | [-0.12631200222345068, 0.1642416689118836, -0.07995652833208441, 0.1260162231689319, -0.08447644148766995, -0.12616620241850615, -0.003805746916681528, 0.3382021497786045, -0.1942145263887942, -0.3252650715261698, 0.08352069606911391, -0.29812877063453197, -0.09844843247532845, 0.2177191288676113, -0.001161950517445802... |
707.2561 | Atomic-scale structure of the SrTiO3(001)-c(6x2) reconstruction:
Experiments and first-principles calculations | The c(6x2) is a reconstruction of the SrTiO3(001) surface that is formed
between 1050-1100oC in oxidizing annealing conditions. This work proposes a
model for the atomic structure for the c(6x2) obtained through a combination of
results from transmission electron diffraction, surface x-ray diffraction,
direct methods... | cond-mat.mtrl-sci | the c6x2 is a reconstruction of the srtio3001 surface that is formed between 10501100oc in oxidizing annealing conditions this work proposes a model for the atomic structure for the c6x2 obtained through a combination of results from transmission electron diffraction surface xray diffraction direct methods analysis com... | [['the', 'c6x2', 'is', 'a', 'reconstruction', 'of', 'the', 'srtio3001', 'surface', 'that', 'is', 'formed', 'between', '10501100oc', 'in', 'oxidizing', 'annealing', 'conditions', 'this', 'work', 'proposes', 'a', 'model', 'for', 'the', 'atomic', 'structure', 'for', 'the', 'c6x2', 'obtained', 'through', 'a', 'combination'... | [-0.11327968819455665, 0.14284304643207985, -0.1062228274048429, 0.03486214122923864, -0.002823007870729099, -0.11350668067077421, 0.04526339269315666, 0.4386284795747894, -0.26590102277081107, -0.3233855676327674, 0.061567467544008186, -0.3130250550138782, -0.18223670925417879, 0.20384874093381442, 0.01222528395998590... |
707.2562 | A Characterisation of First-Order Constraint Satisfaction Problems | We describe simple algebraic and combinatorial characterisations of finite
relational core structures admitting finitely many obstructions. As a
consequence, we show that it is decidable to determine whether a constraint
satisfaction problem is first-order definable: we show the general problem to
be NP-complete, and... | cs.LO cs.CC | we describe simple algebraic and combinatorial characterisations of finite relational core structures admitting finitely many obstructions as a consequence we show that it is decidable to determine whether a constraint satisfaction problem is firstorder definable we show the general problem to be npcomplete and give a ... | [['we', 'describe', 'simple', 'algebraic', 'and', 'combinatorial', 'characterisations', 'of', 'finite', 'relational', 'core', 'structures', 'admitting', 'finitely', 'many', 'obstructions', 'as', 'a', 'consequence', 'we', 'show', 'that', 'it', 'is', 'decidable', 'to', 'determine', 'whether', 'a', 'constraint', 'satisfac... | [-0.15124521886018363, 0.0031464878691699694, -0.09092163052806194, 0.1501039074971638, -0.18793946601688227, -0.15233841235749424, 0.07268241039437658, 0.37138840254951033, -0.36305263518613384, -0.2994928376035804, 0.08764861039495334, -0.20152209348917166, -0.1555805392563343, 0.1971082332187352, -0.1093571075793117... |
707.2563 | Stability for large forbidden subgraphs | We extend the classical stability theorem of Erdos and Simonovits for
forbidden graphs of logarithmic order.
| math.CO | we extend the classical stability theorem of erdos and simonovits for forbidden graphs of logarithmic order | [['we', 'extend', 'the', 'classical', 'stability', 'theorem', 'of', 'erdos', 'and', 'simonovits', 'for', 'forbidden', 'graphs', 'of', 'logarithmic', 'order']] | [-0.1219376320950687, 0.06359456508653238, -0.054608694510534406, 0.15462429367471486, -0.04824292048579082, -0.11484300758456811, 0.14112468728308158, 0.22396660852245986, -0.2811298614833504, -0.3202728405594826, 0.09980859334609704, -0.32261237781494856, -0.11180023825727403, 0.10902491817250848, -0.1869235378690064... |
707.2564 | Renormalizable 1/N_f Expansion for Field Theories in Extra Dimensions | We demonstrate how one can construct renormalizable perturbative expansion in
formally nonrenormalizable higher dimensional field theories. It is based on
$1/N_f$-expansion and results in a logarithmically divergent perturbation
theory in arbitrary high space-time dimension. First, we consider a simple
example of $N$... | hep-th hep-ph | we demonstrate how one can construct renormalizable perturbative expansion in formally nonrenormalizable higher dimensional field theories it is based on 1n_fexpansion and results in a logarithmically divergent perturbation theory in arbitrary high spacetime dimension first we consider a simple example of ncomponent sc... | [['we', 'demonstrate', 'how', 'one', 'can', 'construct', 'renormalizable', 'perturbative', 'expansion', 'in', 'formally', 'nonrenormalizable', 'higher', 'dimensional', 'field', 'theories', 'it', 'is', 'based', 'on', '1n_fexpansion', 'and', 'results', 'in', 'a', 'logarithmically', 'divergent', 'perturbation', 'theory', ... | [-0.13677794537974886, 0.20718609560091655, -0.09280593581631352, 0.08251131721493749, -0.0808433587529193, -0.15270100052927457, -0.0059462317090668675, 0.32514899152299864, -0.19335268022554913, -0.27833938437768, 0.058262836755672245, -0.25795167195276497, -0.17988294259974796, 0.13277670160341457, -0.03222190416039... |
707.2565 | Anomalous Hall effect for the phonon heat conductivity in paramagnetic
dielectric | The theory of anomalous Hall effect for the heat transfer in a paramagnetic
dielectric, discovered experimentally in [1], is developed. The appearance of
the phonon heat flux normal to both the temperature gradient and the magnetic
field is connected with the interaction of magnetic ions with the crystal field
oscill... | cond-mat.other | the theory of anomalous hall effect for the heat transfer in a paramagnetic dielectric discovered experimentally in 1 is developed the appearance of the phonon heat flux normal to both the temperature gradient and the magnetic field is connected with the interaction of magnetic ions with the crystal field oscillations ... | [['the', 'theory', 'of', 'anomalous', 'hall', 'effect', 'for', 'the', 'heat', 'transfer', 'in', 'a', 'paramagnetic', 'dielectric', 'discovered', 'experimentally', 'in', '1', 'is', 'developed', 'the', 'appearance', 'of', 'the', 'phonon', 'heat', 'flux', 'normal', 'to', 'both', 'the', 'temperature', 'gradient', 'and', 't... | [-0.1771671183161409, 0.24275866247106542, -0.046335478601674494, 0.0009501289733096349, -0.06107993180179322, -0.07854399850534997, 0.01458215575109293, 0.36860731194670104, -0.2856407399593415, -0.24363176081785742, -0.008997514624177118, -0.31282633678644317, -0.11909808263619792, 0.17174803779213405, 0.084264505588... |
707.2566 | The environments and clustering properties of 2dFGRS-selected starburst
galaxies | We investigate the environments and clustering properties of starburst
galaxies selected from the 2dF Galaxy Redshift Survey (2dFGRS) in order to
determine which, if any, environmental factors play a role in triggering a
starburst. We quantify the local environments, clustering properties and
luminosity functions of ... | astro-ph | we investigate the environments and clustering properties of starburst galaxies selected from the 2df galaxy redshift survey 2dfgrs in order to determine which if any environmental factors play a role in triggering a starburst we quantify the local environments clustering properties and luminosity functions of our star... | [['we', 'investigate', 'the', 'environments', 'and', 'clustering', 'properties', 'of', 'starburst', 'galaxies', 'selected', 'from', 'the', '2df', 'galaxy', 'redshift', 'survey', '2dfgrs', 'in', 'order', 'to', 'determine', 'which', 'if', 'any', 'environmental', 'factors', 'play', 'a', 'role', 'in', 'triggering', 'a', 's... | [-0.0705757694379192, 0.08506477552030793, -0.07929675030294243, 0.1438941020877, -0.08510906295704307, -0.01671097027774391, 0.038131055884229076, 0.4531318115928083, -0.14456904123370995, -0.35007052964416985, 0.03051331138651627, -0.2922507172681579, -0.07492714506831931, 0.18547684704573328, -0.020142300423777414, ... |
707.2567 | Searches for Direct Pair Production of Supersymmetric Top and
Supersymmetric Bottom Quarks in p-pbar Collisions at sqrt(s)=1.96 TeV | We search for direct pair production of supersymmetric top quarks and
supersymmetric bottom quarks in proton-antiproton collisions at sqrt(s)=1.96
TeV, using 295 pb^-1 of data recorded by the Collider Detector at Fermilab (CDF
II) experiment. The supersymmetric top (supersymmetric bottom) quarks are
selected by recon... | hep-ex | we search for direct pair production of supersymmetric top quarks and supersymmetric bottom quarks in protonantiproton collisions at sqrts196 tev using 295 pb1 of data recorded by the collider detector at fermilab cdf ii experiment the supersymmetric top supersymmetric bottom quarks are selected by reconstructing their... | [['we', 'search', 'for', 'direct', 'pair', 'production', 'of', 'supersymmetric', 'top', 'quarks', 'and', 'supersymmetric', 'bottom', 'quarks', 'in', 'protonantiproton', 'collisions', 'at', 'sqrts196', 'tev', 'using', '295', 'pb1', 'of', 'data', 'recorded', 'by', 'the', 'collider', 'detector', 'at', 'fermilab', 'cdf', '... | [0.012685991883266806, 0.29614347403791424, -0.041085038398921914, 0.19802239988596393, -0.03245503637368702, -0.15093551665458585, 0.0848399612295907, 0.3012082592925123, -0.1269583951327063, -0.3468818237361986, -0.030251575191089484, -0.38927691821230664, 0.14881260526211312, 0.11140955083482411, 0.08116279354795725... |
707.2568 | Logarithmic geometry, minimal free resolutions and toric algebraic
stacks | In this paper we will introduce a certain type of morphisms of log schemes
(in the sense of Fontaine, Illusie, and Kato) and investigate their moduli.
Then by applying this we define a notion of toric algebraic stacks over
arbitrary schemes, which may be regarded as torus embeddings within the
framework of algebraic ... | math.AG | in this paper we will introduce a certain type of morphisms of log schemes in the sense of fontaine illusie and kato and investigate their moduli then by applying this we define a notion of toric algebraic stacks over arbitrary schemes which may be regarded as torus embeddings within the framework of algebraic stacks a... | [['in', 'this', 'paper', 'we', 'will', 'introduce', 'a', 'certain', 'type', 'of', 'morphisms', 'of', 'log', 'schemes', 'in', 'the', 'sense', 'of', 'fontaine', 'illusie', 'and', 'kato', 'and', 'investigate', 'their', 'moduli', 'then', 'by', 'applying', 'this', 'we', 'define', 'a', 'notion', 'of', 'toric', 'algebraic', '... | [-0.17509410690571017, 0.033027529209742654, -0.11579477118656915, 0.11620709911906435, -0.07187443314229741, -0.08841125334284324, 0.03422289589755511, 0.3350048873518758, -0.34927404443185556, -0.23350239456083408, 0.11082473002470043, -0.1592844014042331, -0.19980357871527837, 0.2041935358360848, -0.2033569409737966... |
707.2569 | A Particle-Particle, Particle-Density (P3D) algorithm for the
calculation of electrostatic interactions of particles with slab-like
geometry | We present a fast and accurate method to calculate the electrostatic energy
and forces of interacting particles with the boundary conditions appropriate to
surfaces, i.e periodic in the two directions parallel to the surface and free
in the perpendicular direction. In the spirit of the Ewald method the problem
is div... | physics.comp-ph physics.chem-ph | we present a fast and accurate method to calculate the electrostatic energy and forces of interacting particles with the boundary conditions appropriate to surfaces ie periodic in the two directions parallel to the surface and free in the perpendicular direction in the spirit of the ewald method the problem is divided ... | [['we', 'present', 'a', 'fast', 'and', 'accurate', 'method', 'to', 'calculate', 'the', 'electrostatic', 'energy', 'and', 'forces', 'of', 'interacting', 'particles', 'with', 'the', 'boundary', 'conditions', 'appropriate', 'to', 'surfaces', 'ie', 'periodic', 'in', 'the', 'two', 'directions', 'parallel', 'to', 'the', 'sur... | [-0.17025039694493727, 0.16819182597100735, -0.0415743329251806, 0.02196185166526231, -0.02725612010496358, -0.07649633118527986, 0.00940261826229592, 0.37269888490970643, -0.2890918542852714, -0.30315138326203894, 0.0686371089746466, -0.2310610118100331, -0.07734809707229336, 0.2186779485156183, -0.011074792630859606,... |
707.257 | Evaluation of effective resistances in pseudo-distance-regular resistor
networks | In Refs.[1] and [2], calculation of effective resistances on distance-regular
networks was investigated, where in the first paper, the calculation was based
on the stratification of the network and Stieltjes function associated with the
network, whereas in the latter one a recursive formula for effective
resistances ... | cond-mat.stat-mech cond-mat.other | in refs1 and 2 calculation of effective resistances on distanceregular networks was investigated where in the first paper the calculation was based on the stratification of the network and stieltjes function associated with the network whereas in the latter one a recursive formula for effective resistances was given ba... | [['in', 'refs1', 'and', '2', 'calculation', 'of', 'effective', 'resistances', 'on', 'distanceregular', 'networks', 'was', 'investigated', 'where', 'in', 'the', 'first', 'paper', 'the', 'calculation', 'was', 'based', 'on', 'the', 'stratification', 'of', 'the', 'network', 'and', 'stieltjes', 'function', 'associated', 'wi... | [-0.13488794376177196, 0.06866143448418058, -0.02506376674095177, 0.018029073118909143, -0.03646036064547655, -0.15624766936730838, 0.030498408461153703, 0.3552628368680829, -0.24941483420619356, -0.2601556895843847, 0.06764667705091185, -0.28570296144367313, -0.20250904109659257, 0.1748964148829999, -0.040374390590148... |
707.2571 | Dynamical and energetic instabilities in multi-component Bose-Einstein
condensates in optical lattices | We study dynamical and energetic instabilities in the transport properties of
Bloch waves for atomic multi-component Bose-Einstein condensates in optical
lattices in the tight-binding limit. We obtain stability criteria analytically,
as a function of superfluid velocities and interaction parameters, in several
cases ... | cond-mat.other physics.optics quant-ph | we study dynamical and energetic instabilities in the transport properties of bloch waves for atomic multicomponent boseeinstein condensates in optical lattices in the tightbinding limit we obtain stability criteria analytically as a function of superfluid velocities and interaction parameters in several cases for twoc... | [['we', 'study', 'dynamical', 'and', 'energetic', 'instabilities', 'in', 'the', 'transport', 'properties', 'of', 'bloch', 'waves', 'for', 'atomic', 'multicomponent', 'boseeinstein', 'condensates', 'in', 'optical', 'lattices', 'in', 'the', 'tightbinding', 'limit', 'we', 'obtain', 'stability', 'criteria', 'analytically',... | [-0.2052944483950388, 0.22808545959439167, -0.07222379934197913, 0.0743156378717126, -0.01444611125267469, -0.11130908831210735, 0.002639603401080538, 0.34869301023009497, -0.24886941209059352, -0.23022468112862837, 0.04960968245107394, -0.2426954233468188, -0.11570730059741972, 0.17457071016841114, 0.06747821882331315... |
707.2572 | Noise effects in extended chaotic system: study on the Lorenz'96 model | We investigate the effects of a time-correlated noise on an extended chaotic
system. The chosen model is the Lorenz'96, a kind of toy model used for climate
studies. The system is subjected to both temporal and spatiotemporal
perturbations. Through the analysis of the system's time evolution and its time
correlations... | nlin.CD cond-mat.stat-mech nlin.PS physics.ao-ph | we investigate the effects of a timecorrelated noise on an extended chaotic system the chosen model is the lorenz96 a kind of toy model used for climate studies the system is subjected to both temporal and spatiotemporal perturbations through the analysis of the systems time evolution and its time correlations we have ... | [['we', 'investigate', 'the', 'effects', 'of', 'a', 'timecorrelated', 'noise', 'on', 'an', 'extended', 'chaotic', 'system', 'the', 'chosen', 'model', 'is', 'the', 'lorenz96', 'a', 'kind', 'of', 'toy', 'model', 'used', 'for', 'climate', 'studies', 'the', 'system', 'is', 'subjected', 'to', 'both', 'temporal', 'and', 'spa... | [-0.163613910918806, 0.09203643517467416, -0.0979684395660595, 0.128905941107985, -0.00033002929014014446, -0.09633441438795778, 0.021729948468447672, 0.3449165987686848, -0.2756517750951718, -0.27792212611988304, 0.13824556547209738, -0.2755194015390291, -0.20979846164210164, 0.20436814083446433, -0.03321983909058407,... |
707.2573 | Model for curvature-driven pearling instability in membranes | A phase-field model for dealing with dynamic instabilities in membranes is
presented. We use it to study curvature-driven pearling instability in vesicles
induced by the anchorage of amphiphilic polymers on the membrane. Within this
model, we obtain the morphological changes reported in recent experiments. The
format... | q-bio.QM cond-mat.soft q-bio.CB | a phasefield model for dealing with dynamic instabilities in membranes is presented we use it to study curvaturedriven pearling instability in vesicles induced by the anchorage of amphiphilic polymers on the membrane within this model we obtain the morphological changes reported in recent experiments the formation of a... | [['a', 'phasefield', 'model', 'for', 'dealing', 'with', 'dynamic', 'instabilities', 'in', 'membranes', 'is', 'presented', 'we', 'use', 'it', 'to', 'study', 'curvaturedriven', 'pearling', 'instability', 'in', 'vesicles', 'induced', 'by', 'the', 'anchorage', 'of', 'amphiphilic', 'polymers', 'on', 'the', 'membrane', 'with... | [-0.13330494027738413, 0.14751133088369917, -0.047019737921463155, 0.020306303177854604, -0.026276187433563556, -0.10215496366421126, -0.02598803023538869, 0.4106691490436338, -0.2292596131716807, -0.248189241476549, 0.07657379082994555, -0.23178004424481355, -0.15953496522894225, 0.16285840628342224, -0.04429364243051... |
707.2574 | Is a gas of strongly interacting atomic fermions a nearly perfect fluid? | We use all-optical methods to produce a highly-degenerate Fermi gas of
spin-1/2 $^6$Li atoms. A magnetic field tunes the gas near a collisional
(Feshbach) resonance, producing strong interactions between spin-up and
spin-down atoms. This atomic gas is a paradigm for strong interactions in
nature, and provides tests o... | cond-mat.other | we use alloptical methods to produce a highlydegenerate fermi gas of spin12 6li atoms a magnetic field tunes the gas near a collisional feshbach resonance producing strong interactions between spinup and spindown atoms this atomic gas is a paradigm for strong interactions in nature and provides tests of current quantum... | [['we', 'use', 'alloptical', 'methods', 'to', 'produce', 'a', 'highlydegenerate', 'fermi', 'gas', 'of', 'spin12', '6li', 'atoms', 'a', 'magnetic', 'field', 'tunes', 'the', 'gas', 'near', 'a', 'collisional', 'feshbach', 'resonance', 'producing', 'strong', 'interactions', 'between', 'spinup', 'and', 'spindown', 'atoms', ... | [-0.1172982518014928, 0.19192619667431782, -0.0822471325745424, 0.05550501379602326, -0.002598285622512683, -0.10614923554209944, 0.06846921665486522, 0.3158931484350409, -0.23118189984502702, -0.30230946348239784, 0.03214622443088163, -0.28399843477572384, -0.012427809448220218, 0.2388269710760468, 0.04443626960691733... |
707.2575 | Electric-field-induced displacement of a charged spherical colloid
embedded in an elastic Brinkman medium | When an electric field is applied to an electrolyte-saturated polymer gel
embedded with charged colloidal particles, the force that must be exerted by
the hydrogel on each particle reflects a delicate balance of electrical,
hydrodynamic and elastic stresses. This paper examines the displacement of a
single charged sp... | cond-mat.soft cond-mat.mtrl-sci | when an electric field is applied to an electrolytesaturated polymer gel embedded with charged colloidal particles the force that must be exerted by the hydrogel on each particle reflects a delicate balance of electrical hydrodynamic and elastic stresses this paper examines the displacement of a single charged spherica... | [['when', 'an', 'electric', 'field', 'is', 'applied', 'to', 'an', 'electrolytesaturated', 'polymer', 'gel', 'embedded', 'with', 'charged', 'colloidal', 'particles', 'the', 'force', 'that', 'must', 'be', 'exerted', 'by', 'the', 'hydrogel', 'on', 'each', 'particle', 'reflects', 'a', 'delicate', 'balance', 'of', 'electric... | [-0.10510390892286424, 0.2155564550240874, -0.09640447596912502, -0.02536533569441243, -0.02247159965997918, -0.1434914908738288, -0.04678298006612869, 0.36525974995736543, -0.2911111765765061, -0.2594988918608777, 0.017405258888592484, -0.2881684548786429, -0.15171498417106197, 0.1363703805700077, -0.03697340617298601... |
707.2576 | A note on the incidence coloring of outerplanar graphs | A proof that every outerplanar graph is \Delta+2 colorable. This is slightly
stronger then an unpublished result of Wang Shudong, Ma Fangfang, Xu Jin, and
Yan Lijun proving the same for 2-connected outerplanar graphs.
| math.CO | a proof that every outerplanar graph is delta2 colorable this is slightly stronger then an unpublished result of wang shudong ma fangfang xu jin and yan lijun proving the same for 2connected outerplanar graphs | [['a', 'proof', 'that', 'every', 'outerplanar', 'graph', 'is', 'delta2', 'colorable', 'this', 'is', 'slightly', 'stronger', 'then', 'an', 'unpublished', 'result', 'of', 'wang', 'shudong', 'ma', 'fangfang', 'xu', 'jin', 'and', 'yan', 'lijun', 'proving', 'the', 'same', 'for', '2connected', 'outerplanar', 'graphs']] | [-0.1913158805259774, 0.1142272091092309, -0.03482994515328638, 0.05702815960807305, -0.19031661051896312, -0.25233725048301203, 0.07054250981778867, 0.3554391992548781, -0.19524496853832277, -0.30958622600883245, 0.0317839534292298, -0.3299246153253461, -0.1505130099943809, 0.1335684013883433, -0.23669175422119518, -0... |
707.2577 | Age-Rotation-Activity Relations for M Dwarf Stars Based on ASAS
Photometric Data | Based on analysis of photometric observations of nearby M type stars obtained
with ASAS, 31 periodic variables were detected. The determined periods are
assumed to be related to rotation periods of the investigated stars. Among them
10 new variables with periods longer than 10 days were found, which brings the
total ... | astro-ph | based on analysis of photometric observations of nearby m type stars obtained with asas 31 periodic variables were detected the determined periods are assumed to be related to rotation periods of the investigated stars among them 10 new variables with periods longer than 10 days were found which brings the total number... | [['based', 'on', 'analysis', 'of', 'photometric', 'observations', 'of', 'nearby', 'm', 'type', 'stars', 'obtained', 'with', 'asas', '31', 'periodic', 'variables', 'were', 'detected', 'the', 'determined', 'periods', 'are', 'assumed', 'to', 'be', 'related', 'to', 'rotation', 'periods', 'of', 'the', 'investigated', 'stars... | [-0.12232112457821091, 0.21368538955678817, -0.05596887315521493, 0.08551505652985393, -0.1071326832990604, -0.0995734162003237, 0.1005935637122292, 0.38432651117824723, -0.15018440742405934, -0.388864172637432, 0.06326330921028055, -0.30316863582557896, -0.015926179200764338, 0.23387986112022296, -0.09145042011437829,... |
707.2578 | Weak convergence of CD kernels and applications | We prove a general result on equality of the weak limits of the zero counting
measure, $d\nu_n$, of orthogonal polynomials (defined by a measure $d\mu$) and
$\frac{1}{n} K_n(x,x) d\mu(x)$. By combining this with Mate--Nevai and Totik
upper bounds on $n\lambda_n(x)$, we prove some general results on $\int_I
\frac{1}{n... | math.SP math-ph math.MP | we prove a general result on equality of the weak limits of the zero counting measure dnu_n of orthogonal polynomials defined by a measure dmu and frac1n k_nxx dmux by combining this with matenevai and totik upper bounds on nlambda_nx we prove some general results on int_i frac1n k_nxx dmu_sto 0 for the singular part o... | [['we', 'prove', 'a', 'general', 'result', 'on', 'equality', 'of', 'the', 'weak', 'limits', 'of', 'the', 'zero', 'counting', 'measure', 'dnu_n', 'of', 'orthogonal', 'polynomials', 'defined', 'by', 'a', 'measure', 'dmu', 'and', 'frac1n', 'k_nxx', 'dmux', 'by', 'combining', 'this', 'with', 'matenevai', 'and', 'totik', 'u... | [-0.1686306311748922, 0.11092862192567231, -0.08365004296582709, 0.045749184190450855, 0.028454041606487915, -0.12236613209825009, 0.08128550384814541, 0.2761842298787087, -0.2587101335844232, -0.14773291671493402, 0.13357293252677968, -0.33571709050900406, -0.0694917267990402, 0.14874414736146313, -0.05921953924310704... |
707.2579 | Dynamical invariants and nonadiabatic geometric phases in open quantum
systems | We introduce an operational framework to analyze non-adiabatic Abelian and
non-Abelian, cyclic and non-cyclic, geometric phases in open quantum systems.
In order to remove the adiabaticity condition, we generalize the theory of
dynamical invariants to the context of open systems evolving under arbitrary
convolutionle... | quant-ph cond-mat.stat-mech hep-th | we introduce an operational framework to analyze nonadiabatic abelian and nonabelian cyclic and noncyclic geometric phases in open quantum systems in order to remove the adiabaticity condition we generalize the theory of dynamical invariants to the context of open systems evolving under arbitrary convolutionless master... | [['we', 'introduce', 'an', 'operational', 'framework', 'to', 'analyze', 'nonadiabatic', 'abelian', 'and', 'nonabelian', 'cyclic', 'and', 'noncyclic', 'geometric', 'phases', 'in', 'open', 'quantum', 'systems', 'in', 'order', 'to', 'remove', 'the', 'adiabaticity', 'condition', 'we', 'generalize', 'the', 'theory', 'of', '... | [-0.1763163916311486, 0.1551812681750459, -0.123137556359564, 0.0586545016618142, -0.019237286316693053, -0.15029513522373386, 0.037949901414664, 0.33161386123445247, -0.2941438963258625, -0.2550691020205841, 0.08971207439759396, -0.2008208460769707, -0.2085141886018665, 0.18406388960442596, -0.08881578580091211, 0.056... |
707.258 | Optimization of Apodized Pupil Lyot Coronagraph for ELTs | We study the optimization of the Apodized Pupil Lyot Coronagraph (APLC) in
the context of exoplanet imaging with ground-based telescopes. The APLC
combines an apodization in the pupil plane with a small Lyot mask in the focal
plane of the instrument. It has been intensively studied in the literature from
a theoretica... | astro-ph | we study the optimization of the apodized pupil lyot coronagraph aplc in the context of exoplanet imaging with groundbased telescopes the aplc combines an apodization in the pupil plane with a small lyot mask in the focal plane of the instrument it has been intensively studied in the literature from a theoretical point... | [['we', 'study', 'the', 'optimization', 'of', 'the', 'apodized', 'pupil', 'lyot', 'coronagraph', 'aplc', 'in', 'the', 'context', 'of', 'exoplanet', 'imaging', 'with', 'groundbased', 'telescopes', 'the', 'aplc', 'combines', 'an', 'apodization', 'in', 'the', 'pupil', 'plane', 'with', 'a', 'small', 'lyot', 'mask', 'in', '... | [-0.12390825360651231, 0.058105147660741076, -0.09005213160458199, 0.06263211515151208, -0.10689675311365099, -0.16453179382869618, -0.019848674088904655, 0.4747627864431853, -0.17654880457040337, -0.3307223231875634, 0.1784634555630019, -0.2625959890487726, -0.17077379079413307, 0.24661855074116076, -0.135350753604951... |
707.2581 | Electric-field-enhanced transport in polyacrylamide hydrogel
nano-composites | Electroosmotic pumping through uncharged hydrogels can be achieved by
embedding the polymer network with charged colloidal inclusions. Matos and
co-workers (2006) recently used the concept to enhance the diffusion-limited
flux of uncharged molecules across polyacrylamide hydrogel membraness for the
purpose of improvi... | cond-mat.soft cond-mat.mtrl-sci | electroosmotic pumping through uncharged hydrogels can be achieved by embedding the polymer network with charged colloidal inclusions matos and coworkers 2006 recently used the concept to enhance the diffusionlimited flux of uncharged molecules across polyacrylamide hydrogel membraness for the purpose of improving the ... | [['electroosmotic', 'pumping', 'through', 'uncharged', 'hydrogels', 'can', 'be', 'achieved', 'by', 'embedding', 'the', 'polymer', 'network', 'with', 'charged', 'colloidal', 'inclusions', 'matos', 'and', 'coworkers', '2006', 'recently', 'used', 'the', 'concept', 'to', 'enhance', 'the', 'diffusionlimited', 'flux', 'of', ... | [-0.0733028707652674, 0.16295554514722208, -0.022868298872589544, -0.01371201739532621, -0.03377762390097286, -0.14746438188063526, 0.027744727978364903, 0.3953211955587872, -0.23223932581601917, -0.33993291799548414, 0.05049031010298181, -0.2775011223834415, -0.08302856214531579, 0.18403061068267054, -0.02972566252716... |
707.2582 | Monte Carlo simulation of uncoupled continuous-time random walks
yielding a stochastic solution of the space-time fractional diffusion
equation | We present a numerical method for the Monte Carlo simulation of uncoupled
continuous-time random walks with a Levy alpha-stable distribution of jumps in
space and a Mittag-Leffler distribution of waiting times, and apply it to the
stochastic solution of the Cauchy problem for a partial differential equation
with frac... | cond-mat.stat-mech | we present a numerical method for the monte carlo simulation of uncoupled continuoustime random walks with a levy alphastable distribution of jumps in space and a mittagleffler distribution of waiting times and apply it to the stochastic solution of the cauchy problem for a partial differential equation with fractional... | [['we', 'present', 'a', 'numerical', 'method', 'for', 'the', 'monte', 'carlo', 'simulation', 'of', 'uncoupled', 'continuoustime', 'random', 'walks', 'with', 'a', 'levy', 'alphastable', 'distribution', 'of', 'jumps', 'in', 'space', 'and', 'a', 'mittagleffler', 'distribution', 'of', 'waiting', 'times', 'and', 'apply', 'i... | [-0.030744712112067786, 0.09686985697573453, -0.11128631827131204, 0.11548064481512366, -0.0773748443885283, -0.13984581600124765, 0.025301538164388727, 0.41488642832748107, -0.29618374892062954, -0.2437058817202153, 0.13559196277086127, -0.2698777805644922, -0.14231559485892536, 0.18150300263463484, -0.060804662450410... |
707.2583 | The Eternal Sunshine of the Spotless Mind | We extend the worldline measure for pocket formation in eternal inflation to
allow for time-ordered bubble formation. Such a time-ordering is equivalent to
imposing a preferred time-slicing on the "parent" de Sitter space. Using this
measure, we describe a covariant version of the youngness paradox and show that
the ... | hep-th | we extend the worldline measure for pocket formation in eternal inflation to allow for timeordered bubble formation such a timeordering is equivalent to imposing a preferred timeslicing on the parent de sitter space using this measure we describe a covariant version of the youngness paradox and show that the youngness ... | [['we', 'extend', 'the', 'worldline', 'measure', 'for', 'pocket', 'formation', 'in', 'eternal', 'inflation', 'to', 'allow', 'for', 'timeordered', 'bubble', 'formation', 'such', 'a', 'timeordering', 'is', 'equivalent', 'to', 'imposing', 'a', 'preferred', 'timeslicing', 'on', 'the', 'parent', 'de', 'sitter', 'space', 'us... | [-0.12953983028098806, 0.16887861769222742, -0.16922510011251307, 0.1454551093699558, -0.1453039388590834, -0.09711728492586673, 0.005469138887298258, 0.3335362182859379, -0.23307665547096654, -0.232984391238564, 0.0969378963253561, -0.20757160149809398, -0.10009726270137331, 0.10921845285117308, -0.09556424849124366, ... |
707.2584 | Six Conjectures which Generalize or Are Related to Andrica's Conjecture | Six conjectures on pairs of consecutive primes are listed in this paper,
together with examples for each case.
| math.GM | six conjectures on pairs of consecutive primes are listed in this paper together with examples for each case | [['six', 'conjectures', 'on', 'pairs', 'of', 'consecutive', 'primes', 'are', 'listed', 'in', 'this', 'paper', 'together', 'with', 'examples', 'for', 'each', 'case']] | [-0.1795723834592435, 0.08103936175919241, 0.023095163620180555, 0.04150837599687899, 0.016439509474568896, -0.1395389853666226, -0.005260119725587881, 0.38711558654904366, -0.1869993307110336, -0.35374416990412605, 0.0753771214836484, -0.41216675668127006, -0.11126624513417482, 0.2680674402250184, -0.11649483721703291... |
707.2585 | Derived completions in stable homotopy theory | We construct a notion of derived completion which applies to homomorphisms of
commutative S-algebras. We study the relationship of the construction with
other constructions of completions, and prove various invariance properties.
The construction is expected to have applications within algebraic K-theory.
| math.AT math.AC | we construct a notion of derived completion which applies to homomorphisms of commutative salgebras we study the relationship of the construction with other constructions of completions and prove various invariance properties the construction is expected to have applications within algebraic ktheory | [['we', 'construct', 'a', 'notion', 'of', 'derived', 'completion', 'which', 'applies', 'to', 'homomorphisms', 'of', 'commutative', 'salgebras', 'we', 'study', 'the', 'relationship', 'of', 'the', 'construction', 'with', 'other', 'constructions', 'of', 'completions', 'and', 'prove', 'various', 'invariance', 'properties',... | [-0.1464197971835369, 0.03956049196308524, -0.12890186131273101, 0.11671627684575846, -0.10929394717805269, -0.11947945095371545, -0.0419950504934915, 0.3353729534258203, -0.36903068804886285, -0.27121252964091735, 0.1250504537871698, -0.22401853948519224, -0.1839277354046339, 0.17224127417657434, -0.17459733807481825,... |
707.2586 | Effect of suppressed excitation on the amplitude distribution of 5-min
oscillations in sunspots | Five-minute oscillations on the Sun (acoustic and surface gravity waves) are
excited by subsurface turbulent convection. However, in sunspots the excitation
is suppressed because strong magnetic field inhibits convection. We use 3D
simulations to investigate how the suppression of excitation sources affects
the distr... | astro-ph | fiveminute oscillations on the sun acoustic and surface gravity waves are excited by subsurface turbulent convection however in sunspots the excitation is suppressed because strong magnetic field inhibits convection we use 3d simulations to investigate how the suppression of excitation sources affects the distribution ... | [['fiveminute', 'oscillations', 'on', 'the', 'sun', 'acoustic', 'and', 'surface', 'gravity', 'waves', 'are', 'excited', 'by', 'subsurface', 'turbulent', 'convection', 'however', 'in', 'sunspots', 'the', 'excitation', 'is', 'suppressed', 'because', 'strong', 'magnetic', 'field', 'inhibits', 'convection', 'we', 'use', '3... | [-0.13462295598695956, 0.23829723231329192, 0.0003036439935151007, 0.1289675369716039, -0.04274246735017626, 0.0004201806510888761, 0.05576537161945335, 0.34278354549840573, -0.20741396106539234, -0.35294135808944704, 0.07826887356913498, -0.283224986409468, -0.10128194349066864, 0.20969419128321592, -0.033865130138057... |
707.2587 | The Shared Reward Dilemma | One of the most direct human mechanisms of promoting cooperation is rewarding
it. We study the effect of sharing a reward among cooperators in the most
stringent form of social dilemma, namely the Prisoner's Dilemma. Specifically,
for a group of players that collect payoffs by playing a pairwise Prisoner's
Dilemma ga... | q-bio.PE | one of the most direct human mechanisms of promoting cooperation is rewarding it we study the effect of sharing a reward among cooperators in the most stringent form of social dilemma namely the prisoners dilemma specifically for a group of players that collect payoffs by playing a pairwise prisoners dilemma game with ... | [['one', 'of', 'the', 'most', 'direct', 'human', 'mechanisms', 'of', 'promoting', 'cooperation', 'is', 'rewarding', 'it', 'we', 'study', 'the', 'effect', 'of', 'sharing', 'a', 'reward', 'among', 'cooperators', 'in', 'the', 'most', 'stringent', 'form', 'of', 'social', 'dilemma', 'namely', 'the', 'prisoners', 'dilemma', ... | [-0.13855477733124558, 0.101011582192292, -0.11992964549877104, 0.1320569490510804, -0.12141928886800694, -0.23050000360845366, 0.1277351369804126, 0.41037634482684854, -0.25683653449855876, -0.2868953594893572, 0.08455769605002604, -0.2799834696176861, -0.1885039091707551, 0.08124866561168649, -0.1278530009218403, -0.... |
707.2588 | Formation of superheavy nuclei in cold fusion reactions | Within the concept of the dinuclear system (DNS), a dynamical model is
proposed for describing the formation of superheavy nuclei in complete fusion
reactions by incorporating the coupling of the relative motion to the nucleon
transfer process. The capture of two heavy colliding nuclei, the formation of
the compound ... | nucl-th | within the concept of the dinuclear system dns a dynamical model is proposed for describing the formation of superheavy nuclei in complete fusion reactions by incorporating the coupling of the relative motion to the nucleon transfer process the capture of two heavy colliding nuclei the formation of the compound nucleus... | [['within', 'the', 'concept', 'of', 'the', 'dinuclear', 'system', 'dns', 'a', 'dynamical', 'model', 'is', 'proposed', 'for', 'describing', 'the', 'formation', 'of', 'superheavy', 'nuclei', 'in', 'complete', 'fusion', 'reactions', 'by', 'incorporating', 'the', 'coupling', 'of', 'the', 'relative', 'motion', 'to', 'the', ... | [-0.03123007214248732, 0.19581655914802534, -0.053709870976982294, 0.1025227476412881, 0.0781956726167765, -0.09097153691971606, 0.0349720865962337, 0.3507350685695807, -0.22504798793751332, -0.2860748586624309, -0.04293812124265565, -0.33837390126039585, 0.019727489607477628, 0.1313874592590663, 0.0738427171052468, 0.... |
707.2589 | Determination of the strong coupling constant from the CLEO measurement
of the total hadronic cross section in $e^+e^-$ annihilation below 10.56 GeV | Using recent CLEO III results for the cross section for $e^+e^- \to {\rm
hadrons}$ at seven centre-of-mass energies between 6.964 and 10.538 GeV, we
derive a value for the strong coupling constant
$\alpha_s(M_Z^2)=0.110_{-0.012}^{-0.010}{}_{-0.011}^{+0.010}$ where the
uncertainties are uncorrelated and correlated, re... | hep-ph | using recent cleo iii results for the cross section for ee to rm hadrons at seven centreofmass energies between 6964 and 10538 gev we derive a value for the strong coupling constant alpha_sm_z20110_00120010_00110010 where the uncertainties are uncorrelated and correlated respectively our result differs significantly fr... | [['using', 'recent', 'cleo', 'iii', 'results', 'for', 'the', 'cross', 'section', 'for', 'ee', 'to', 'rm', 'hadrons', 'at', 'seven', 'centreofmass', 'energies', 'between', '6964', 'and', '10538', 'gev', 'we', 'derive', 'a', 'value', 'for', 'the', 'strong', 'coupling', 'constant', 'alpha_sm_z20110_00120010_00110010', 'wh... | [-0.046004058461851224, 0.14346950761025185, -0.03453392590969228, 0.0697190655840901, 0.003164496948906722, -0.08596628856657144, 0.06335005662717427, 0.340578340459615, -0.15285847311203654, -0.371797065053565, 0.013851612187304104, -0.34315289940255195, 0.008976261561306624, 0.2215609248893228, 0.056550349473512215,... |
707.259 | General Covariant Gauge Fixing for Massless Spin-Two Fields | The most general covariant gauge fixing Lagrangian is considered for a
spin-two gauge theory in the context of the Faddeev-Popov procedure. In
general, five parameters characterize this gauge fixing. Certain limiting
values for these parameters give rise to a spin-two propagator that is either
traceless or transverse... | hep-th | the most general covariant gauge fixing lagrangian is considered for a spintwo gauge theory in the context of the faddeevpopov procedure in general five parameters characterize this gauge fixing certain limiting values for these parameters give rise to a spintwo propagator that is either traceless or transverse but for... | [['the', 'most', 'general', 'covariant', 'gauge', 'fixing', 'lagrangian', 'is', 'considered', 'for', 'a', 'spintwo', 'gauge', 'theory', 'in', 'the', 'context', 'of', 'the', 'faddeevpopov', 'procedure', 'in', 'general', 'five', 'parameters', 'characterize', 'this', 'gauge', 'fixing', 'certain', 'limiting', 'values', 'fo... | [-0.17822321191219506, 0.23858540286873556, -0.11001421302070569, 0.09706237512658451, -0.15792557600571233, -0.14686490057902352, -0.06462740697260282, 0.33235997668686945, -0.18648030186312237, -0.25082412884113897, 0.03696589817583656, -0.20217125260443158, -0.1517941575263075, 0.07940959119368463, -0.02594204016539... |
707.2591 | An Elementary Proof of the Fundamental Theorem of Tropical Algebra | In this paper we give an elementary proof of the Fundamental Theorem of
Algebra for polynomials over the rational tropical semi-ring. We prove that,
tropically, the rational numbers are algebraically closed. We provide a simple
algorithm for factoring tropical polynomials of a single variable. A central
idea is the c... | math.CO | in this paper we give an elementary proof of the fundamental theorem of algebra for polynomials over the rational tropical semiring we prove that tropically the rational numbers are algebraically closed we provide a simple algorithm for factoring tropical polynomials of a single variable a central idea is the concept o... | [['in', 'this', 'paper', 'we', 'give', 'an', 'elementary', 'proof', 'of', 'the', 'fundamental', 'theorem', 'of', 'algebra', 'for', 'polynomials', 'over', 'the', 'rational', 'tropical', 'semiring', 'we', 'prove', 'that', 'tropically', 'the', 'rational', 'numbers', 'are', 'algebraically', 'closed', 'we', 'provide', 'a', ... | [-0.1935555171345671, 0.06762554451376976, -0.14146855399012565, 0.08372174026289333, -0.0999789600695173, -0.12400233922526241, 0.032120385891757905, 0.2661914337178071, -0.3873456947008769, -0.1906571930212279, 0.09480545215153446, -0.18339242158457636, -0.19882395692247276, 0.26542944110929967, -0.14630212303251028,... |
707.2592 | The Fermat-Torricelli problem in normed planes and spaces | We investigate the Fermat-Torricelli problem in d-dimensional real normed
spaces or Minkowski spaces, mainly for d=2. Our approach is to study the
Fermat-Torricelli locus in a geometric way. We present many new results, as
well as give an exposition of known results that are scattered in various
sources, with proofs ... | math.OC math.MG | we investigate the fermattorricelli problem in ddimensional real normed spaces or minkowski spaces mainly for d2 our approach is to study the fermattorricelli locus in a geometric way we present many new results as well as give an exposition of known results that are scattered in various sources with proofs for some of... | [['we', 'investigate', 'the', 'fermattorricelli', 'problem', 'in', 'ddimensional', 'real', 'normed', 'spaces', 'or', 'minkowski', 'spaces', 'mainly', 'for', 'd2', 'our', 'approach', 'is', 'to', 'study', 'the', 'fermattorricelli', 'locus', 'in', 'a', 'geometric', 'way', 'we', 'present', 'many', 'new', 'results', 'as', '... | [-0.09336701460229728, 0.0637223464190685, -0.09082088511972193, 0.12672126306929288, -0.07151458995723899, -0.07973670165371546, -0.0056263113647025634, 0.3874148770899294, -0.27649792275847274, -0.25865246103878353, 0.15150677233295357, -0.27740090100609877, -0.1823809450774632, 0.2597797666354343, -0.150154109598395... |
707.2593 | Many lives in many worlds | I argue that accepting quantum mechanics to be universally true means that
you should also believe in parallel universes. I give my assessment of
Everett's theory as it celebrates its 50th anniversary.
| quant-ph hep-th | i argue that accepting quantum mechanics to be universally true means that you should also believe in parallel universes i give my assessment of everetts theory as it celebrates its 50th anniversary | [['i', 'argue', 'that', 'accepting', 'quantum', 'mechanics', 'to', 'be', 'universally', 'true', 'means', 'that', 'you', 'should', 'also', 'believe', 'in', 'parallel', 'universes', 'i', 'give', 'my', 'assessment', 'of', 'everetts', 'theory', 'as', 'it', 'celebrates', 'its', '50th', 'anniversary']] | [-0.033220204245481, 0.1749578533854219, -0.2035864822100848, 0.15864370483905077, -0.13904809078667313, -0.23808678930799942, 0.04474153064438724, 0.2776409030047944, -0.2377134090056643, -0.23252932840841822, 0.05446794408999267, -0.26215756055898964, -0.16182819055393338, 0.15326502920652274, -0.1986339919967577, -0... |
707.2594 | A New Constraint on the Escape Fraction in Distant Galaxies Using
Gamma-ray Burst Afterglow Spectroscopy | We describe a new method to measure the escape fraction fesc of ionizing
radiation from distant star-forming galaxies using the afterglow spectra of
long-duration gamma-ray bursts (GRBs). Optical spectra of GRB afterglows allow
us to evaluate the optical depth of the host ISM, according to the neutral
hydrogen column... | astro-ph | we describe a new method to measure the escape fraction fesc of ionizing radiation from distant starforming galaxies using the afterglow spectra of longduration gammaray bursts grbs optical spectra of grb afterglows allow us to evaluate the optical depth of the host ism according to the neutral hydrogen column density ... | [['we', 'describe', 'a', 'new', 'method', 'to', 'measure', 'the', 'escape', 'fraction', 'fesc', 'of', 'ionizing', 'radiation', 'from', 'distant', 'starforming', 'galaxies', 'using', 'the', 'afterglow', 'spectra', 'of', 'longduration', 'gammaray', 'bursts', 'grbs', 'optical', 'spectra', 'of', 'grb', 'afterglows', 'allow... | [-0.01849758433208728, 0.10865477865002283, -0.036572541380416095, 0.125004775055642, -0.09978109010813352, -0.07839813614417435, 0.12058773299165591, 0.5030657241902785, -0.12303944205943833, -0.3286635967914337, -0.0439943245021864, -0.33582905771923655, 0.04421220249913196, 0.20292435932440736, 0.011461605471164829,... |
707.2595 | Mechanisms of Diffusional Nucleation of Nanocrystals and Their
Self-Assembly into Uniform Colloids | We survey our research on modeling the mechanisms of control of uniformity in
growth of nanosize and colloid particles. The former are produced as
nanocrystals, by burst-nucleation from solution. The latter, colloid-size
particles, are formed by self-assembly (aggregation) of the nanocrystals. In
the colloid particle... | cond-mat.soft cond-mat.dis-nn cond-mat.mtrl-sci cond-mat.stat-mech | we survey our research on modeling the mechanisms of control of uniformity in growth of nanosize and colloid particles the former are produced as nanocrystals by burstnucleation from solution the latter colloidsize particles are formed by selfassembly aggregation of the nanocrystals in the colloid particle synthesis th... | [['we', 'survey', 'our', 'research', 'on', 'modeling', 'the', 'mechanisms', 'of', 'control', 'of', 'uniformity', 'in', 'growth', 'of', 'nanosize', 'and', 'colloid', 'particles', 'the', 'former', 'are', 'produced', 'as', 'nanocrystals', 'by', 'burstnucleation', 'from', 'solution', 'the', 'latter', 'colloidsize', 'partic... | [-0.0714573915180718, 0.18915243001718973, -0.06636597148688703, 0.03267703444887894, 0.007134692062591684, -0.10125140521819864, 0.003963270801087391, 0.39153323148473584, -0.27857970357711975, -0.31101208262563007, 0.06433246004363072, -0.29352677991977044, -0.13700377149186257, 0.15191972884510097, 0.017854436350472... |
707.2596 | Effect of triple interaction on energy delocalization in the strongly
disordered system of interacting two-level defects | We accurately treat the effect of the double and triple interactions of
two-level systems (TLS) in glasses onto the energy delocalization due to the
long-range interaction of TLS. Although this work qualitatively reproduces the
estimates of our previous work we believe that it is important because in this
paper the e... | cond-mat.dis-nn cond-mat.soft | we accurately treat the effect of the double and triple interactions of twolevel systems tls in glasses onto the energy delocalization due to the longrange interaction of tls although this work qualitatively reproduces the estimates of our previous work we believe that it is important because in this paper the estimate... | [['we', 'accurately', 'treat', 'the', 'effect', 'of', 'the', 'double', 'and', 'triple', 'interactions', 'of', 'twolevel', 'systems', 'tls', 'in', 'glasses', 'onto', 'the', 'energy', 'delocalization', 'due', 'to', 'the', 'longrange', 'interaction', 'of', 'tls', 'although', 'this', 'work', 'qualitatively', 'reproduces', ... | [-0.1090676537266484, 0.09408800048393594, -0.058750089094542934, 0.06635323503503093, -0.00017960902855352118, -0.09965776175398518, 0.02745640702907824, 0.3382844982272083, -0.2286773214151186, -0.33563268731037776, 0.032312765391543506, -0.3172126143894814, -0.17570907804011196, 0.17820646015030367, -0.0628745925573... |
707.2597 | Rapidly varying accretion and AGN feedback | Accretion rates onto AGN are likely to be extremely variable on short
timescales; much shorter than the typical cooling time of X-ray emitting gas in
elliptical galaxies and galaxy clusters. Using the Langevin approach it is
shown that, for a simple feedback system, this can induce variability in the
AGN power output... | astro-ph | accretion rates onto agn are likely to be extremely variable on short timescales much shorter than the typical cooling time of xray emitting gas in elliptical galaxies and galaxy clusters using the langevin approach it is shown that for a simple feedback system this can induce variability in the agn power output that i... | [['accretion', 'rates', 'onto', 'agn', 'are', 'likely', 'to', 'be', 'extremely', 'variable', 'on', 'short', 'timescales', 'much', 'shorter', 'than', 'the', 'typical', 'cooling', 'time', 'of', 'xray', 'emitting', 'gas', 'in', 'elliptical', 'galaxies', 'and', 'galaxy', 'clusters', 'using', 'the', 'langevin', 'approach', ... | [-0.08084274147018451, 0.1567175708826437, -0.06995503527873828, 0.1336804317311739, -0.0925008713020763, -0.08197197309844402, 0.04579981753746696, 0.42385904968443494, -0.21015674680875338, -0.33378077535092504, 0.05537215313483133, -0.250982020141699, -0.05396041729055263, 0.25870313150911123, -0.06823651241241487, ... |
707.2598 | How much 56Ni can be produced in Core-Collapse Supernovae? : Evolution
and Explosions of 30 - 100 Msun Stars | Motivated by the discovery of extremely bright supernovae SNe1999as and
2006gy, we have investigated how much 56Ni mass can be synthesized in
core-collapse massive supernovae (SNe). We calculate the evolution of several
very massive stars with initial masses M <~ 100 Msun from the main-sequence to
the beginning of th... | astro-ph | motivated by the discovery of extremely bright supernovae sne1999as and 2006gy we have investigated how much 56ni mass can be synthesized in corecollapse massive supernovae sne we calculate the evolution of several very massive stars with initial masses m 100 msun from the mainsequence to the beginning of the fecore co... | [['motivated', 'by', 'the', 'discovery', 'of', 'extremely', 'bright', 'supernovae', 'sne1999as', 'and', '2006gy', 'we', 'have', 'investigated', 'how', 'much', '56ni', 'mass', 'can', 'be', 'synthesized', 'in', 'corecollapse', 'massive', 'supernovae', 'sne', 'we', 'calculate', 'the', 'evolution', 'of', 'several', 'very',... | [-0.01936185048982399, 0.18596487401104342, 0.03641824353407626, 0.18019896345882844, -0.06459257030140898, -0.09236549967942445, 0.08422695250424757, 0.41061425637708954, -0.1087115216058292, -0.42033235054276036, 0.07533679499904057, -0.2887382989995964, 0.06611533640335275, 0.19128168850380195, -0.019273023829185703... |
707.2599 | Extreme photo-polarimetric behaviour of the blazar AO 0235+164 | We present optical photo-polarimetric observations with high temporal
resolution of the blazar AO 0235+164. Our data, the first to test the
photo-polarimetric behaviour of this object at very short time-scales, show
significant micro-variability in total flux, colour index, linear polarization
degree, and position an... | astro-ph | we present optical photopolarimetric observations with high temporal resolution of the blazar ao 0235164 our data the first to test the photopolarimetric behaviour of this object at very short timescales show significant microvariability in total flux colour index linear polarization degree and position angle strong in... | [['we', 'present', 'optical', 'photopolarimetric', 'observations', 'with', 'high', 'temporal', 'resolution', 'of', 'the', 'blazar', 'ao', '0235164', 'our', 'data', 'the', 'first', 'to', 'test', 'the', 'photopolarimetric', 'behaviour', 'of', 'this', 'object', 'at', 'very', 'short', 'timescales', 'show', 'significant', '... | [-0.09361008854020757, 0.107062689448195, -0.09813186358912168, 0.12690995559662682, -0.0855086857604014, -0.11918571595152891, 0.003519710021194171, 0.5314977870465399, -0.1667803917308275, -0.40421539138969, 0.05521286024422561, -0.2824307173964576, -0.09334163143727425, 0.17710860514895874, -0.10243110870522959, -0.... |
707.26 | Subnanosecond switching of local spin-exchange coupled to ferromagnets | The dynamics of a single spin embedded in a the tunnel junction between
ferromagnetic contacts is strongly affected by the exchange coupling to the
tunneling electrons. Using time-dependent equation of motion for the spin under
influence of the spin-polarized tunneling current, it is shown that the
magnetic field ind... | cond-mat.mes-hall | the dynamics of a single spin embedded in a the tunnel junction between ferromagnetic contacts is strongly affected by the exchange coupling to the tunneling electrons using timedependent equation of motion for the spin under influence of the spinpolarized tunneling current it is shown that the magnetic field induced b... | [['the', 'dynamics', 'of', 'a', 'single', 'spin', 'embedded', 'in', 'a', 'the', 'tunnel', 'junction', 'between', 'ferromagnetic', 'contacts', 'is', 'strongly', 'affected', 'by', 'the', 'exchange', 'coupling', 'to', 'the', 'tunneling', 'electrons', 'using', 'timedependent', 'equation', 'of', 'motion', 'for', 'the', 'spi... | [-0.19446610789700394, 0.21063528529168038, -0.06150134506763196, 0.05797207573264399, -0.01807999829122541, -0.12955558315540353, 0.025921702375818118, 0.39417720965895, -0.2903305610970539, -0.2921228537920351, -0.008364292040841617, -0.2593846844679587, -0.11024659808140759, 0.24244607995063358, 0.05354304158347933,... |
707.2601 | Camouflaged galactic CMB foregrounds: total and polarized contributions
of the kinetic Sunyaev Zeldovich effect | We consider the role of the galactic kinetic Sunyaev Zeldovich (SZ) effect as
a CMB foreground. While the galactic thermal Sunyaev Zeldovich effect has
previously been studied and discarded as a potential CMB foreground, we find
that the kinetic SZ effect is dominant in the galactic case. We analyse the
detectability... | astro-ph | we consider the role of the galactic kinetic sunyaev zeldovich sz effect as a cmb foreground while the galactic thermal sunyaev zeldovich effect has previously been studied and discarded as a potential cmb foreground we find that the kinetic sz effect is dominant in the galactic case we analyse the detectability of the... | [['we', 'consider', 'the', 'role', 'of', 'the', 'galactic', 'kinetic', 'sunyaev', 'zeldovich', 'sz', 'effect', 'as', 'a', 'cmb', 'foreground', 'while', 'the', 'galactic', 'thermal', 'sunyaev', 'zeldovich', 'effect', 'has', 'previously', 'been', 'studied', 'and', 'discarded', 'as', 'a', 'potential', 'cmb', 'foreground',... | [-0.06896364729906494, 0.08834028711175011, -0.08738137395274671, 0.1407398434501694, -0.1272632285011011, -0.025027754467753387, 0.021985462472702447, 0.36031929016174685, -0.23697743733454454, -0.2937138061381999, 0.03125370497902303, -0.3313040171166534, -0.0822146670089441, 0.21190906253612632, 0.04553926549084321,... |
707.2602 | Hochschild cohomology, the characteristic morphism and derived
deformations | A notion of Hochschild cohomology of an abelian category was defined by Lowen
and Van den Bergh (2005) and they showed the existence of a characteristic
morphism from the Hochschild cohomology into the graded centre of the (bounded)
derived category. An element in the second Hochschild cohomology group
corresponds to... | math.KT | a notion of hochschild cohomology of an abelian category was defined by lowen and van den bergh 2005 and they showed the existence of a characteristic morphism from the hochschild cohomology into the graded centre of the bounded derived category an element in the second hochschild cohomology group corresponds to a firs... | [['a', 'notion', 'of', 'hochschild', 'cohomology', 'of', 'an', 'abelian', 'category', 'was', 'defined', 'by', 'lowen', 'and', 'van', 'den', 'bergh', '2005', 'and', 'they', 'showed', 'the', 'existence', 'of', 'a', 'characteristic', 'morphism', 'from', 'the', 'hochschild', 'cohomology', 'into', 'the', 'graded', 'centre',... | [-0.18969160159641918, 0.01025714924287928, -0.1179784666135037, 0.06540306379345592, -0.08887864419524252, -0.10378535334224792, -0.03013259753581463, 0.30952794728188837, -0.4125309330419753, -0.24302894545270362, 0.049011331285268446, -0.1815394809381207, -0.1850706607810337, 0.14988371437877743, -0.2348031698110901... |
707.2603 | The Mather measure and a Large Deviation Principle for the Entropy
Penalized Method | We present a large deviation principle for the entropy penalized Mather
problem when the Lagrangian L is generic (in this case the Mather measure $\mu$
is unique and the support of $\mu$ is the Aubry set). Consider, for each value
of $\epsilon $ and h, the entropy penalized Mather problem $\min
\{\int_{\tn\times\rn}
... | math.DS math.AP | we present a large deviation principle for the entropy penalized mather problem when the lagrangian l is generic in this case the mather measure mu is unique and the support of mu is the aubry set consider for each value of epsilon and h the entropy penalized mather problem min int_tntimesrn lxvdmuxvepsilon smu where t... | [['we', 'present', 'a', 'large', 'deviation', 'principle', 'for', 'the', 'entropy', 'penalized', 'mather', 'problem', 'when', 'the', 'lagrangian', 'l', 'is', 'generic', 'in', 'this', 'case', 'the', 'mather', 'measure', 'mu', 'is', 'unique', 'and', 'the', 'support', 'of', 'mu', 'is', 'the', 'aubry', 'set', 'consider', '... | [-0.14390903674842168, 0.09367929631456112, -0.07085781518835574, 0.05997235818261591, -0.014204679084165643, -0.17379610372784857, 0.07049081880250015, 0.27694022776558996, -0.3161682866513729, -0.2198964959708974, 0.07886914820216286, -0.3443588932588076, -0.07966592469407867, 0.12315898060721035, -0.0945105952268932... |
707.2604 | Photometry of Polar-Ring Galaxies | We have obtained photometry in B and R for seven confirmed or probable
polar-ring galaxies from the Polar-Ring Catalog of Whitmore et al. (1990). The
rings show a range of colors from B-R \approx 0.6 to B-R \approx 1.7. The
bluest rings have bright HII regions, which are direct evidence for recent star
formation. The... | astro-ph | we have obtained photometry in b and r for seven confirmed or probable polarring galaxies from the polarring catalog of whitmore et al 1990 the rings show a range of colors from br approx 06 to br approx 17 the bluest rings have bright hii regions which are direct evidence for recent star formation the minimum age of t... | [['we', 'have', 'obtained', 'photometry', 'in', 'b', 'and', 'r', 'for', 'seven', 'confirmed', 'or', 'probable', 'polarring', 'galaxies', 'from', 'the', 'polarring', 'catalog', 'of', 'whitmore', 'et', 'al', '1990', 'the', 'rings', 'show', 'a', 'range', 'of', 'colors', 'from', 'br', 'approx', '06', 'to', 'br', 'approx', ... | [-0.07648588117204361, 0.07799595403246878, -0.08240228263692052, 0.057174804098981104, -0.09050002408575666, -0.1085453928825407, 0.04256800974696136, 0.4298088717185854, -0.19517704037841688, -0.3577136064741052, 0.09258848379081315, -0.28673019922316295, -0.053211929417053654, 0.18797774774345669, -0.093142868947114... |
707.2605 | A sheaf of Hochschild complexes on quasi-compact opens | For a scheme X, we construct a sheaf C of complexes on X such that for every
quasi-compact open subset U of X, C(U) is quasi-isomorphic to the Hochschild
complex of the scheme U. Since C is moreover acyclic for taking sections on
quasi-compact opens, we obtain a local to global spectral sequence for
Hochschild cohomo... | math.AG | for a scheme x we construct a sheaf c of complexes on x such that for every quasicompact open subset u of x cu is quasiisomorphic to the hochschild complex of the scheme u since c is moreover acyclic for taking sections on quasicompact opens we obtain a local to global spectral sequence for hochschild cohomology if x i... | [['for', 'a', 'scheme', 'x', 'we', 'construct', 'a', 'sheaf', 'c', 'of', 'complexes', 'on', 'x', 'such', 'that', 'for', 'every', 'quasicompact', 'open', 'subset', 'u', 'of', 'x', 'cu', 'is', 'quasiisomorphic', 'to', 'the', 'hochschild', 'complex', 'of', 'the', 'scheme', 'u', 'since', 'c', 'is', 'moreover', 'acyclic', '... | [-0.2556266799219884, -0.0034732769864300886, -0.06148667614907026, 0.040843795144852875, -0.04393538326645891, -0.19258875981128465, 0.054470647485383474, 0.4684962386886279, -0.4108810319254796, -0.11586571813871463, 0.05566520414625605, -0.1994274555395047, -0.05916527380274298, 0.20016128644347192, -0.1358039466741... |
707.2606 | Measuring H-beta BLR Flows in NGC 5548 | Using archival International AGN Watch observations we find a correlation
between the asymmetry of the H-beta line and the system luminosity: the line
becomes bluer as the system gets brighter. We also find a differential lag
between the red and blue wings of the line: the blue wing lags the red by ~4
days, suggestin... | astro-ph | using archival international agn watch observations we find a correlation between the asymmetry of the hbeta line and the system luminosity the line becomes bluer as the system gets brighter we also find a differential lag between the red and blue wings of the line the blue wing lags the red by 4 days suggesting an inf... | [['using', 'archival', 'international', 'agn', 'watch', 'observations', 'we', 'find', 'a', 'correlation', 'between', 'the', 'asymmetry', 'of', 'the', 'hbeta', 'line', 'and', 'the', 'system', 'luminosity', 'the', 'line', 'becomes', 'bluer', 'as', 'the', 'system', 'gets', 'brighter', 'we', 'also', 'find', 'a', 'different... | [-0.062439746574544513, 0.07103433037681513, -0.06490298336158033, 0.08599674591764075, -0.12161011645784144, -0.12992905639111996, 0.05385390180544775, 0.5247893757873872, -0.11130896746562641, -0.29212557111454546, 0.07225909708525802, -0.3812416775274228, -0.05537702130978225, 0.16883396339358486, -0.016399710179596... |
707.2607 | DTFE analysis of the PSCz local Universe: Density Field and Cosmic Flow | We apply the Delaunay Tessellation Field Estimator (DTFE) to reconstruct and
analyze the matter distribution and cosmic velocity flows in the Local Universe
on the basis of the PSCz galaxy survey. The prime objective of this study is
the production of optimal resolution three-dimensional maps fully
volume-covering of... | astro-ph | we apply the delaunay tessellation field estimator dtfe to reconstruct and analyze the matter distribution and cosmic velocity flows in the local universe on the basis of the pscz galaxy survey the prime objective of this study is the production of optimal resolution threedimensional maps fully volumecovering of the vo... | [['we', 'apply', 'the', 'delaunay', 'tessellation', 'field', 'estimator', 'dtfe', 'to', 'reconstruct', 'and', 'analyze', 'the', 'matter', 'distribution', 'and', 'cosmic', 'velocity', 'flows', 'in', 'the', 'local', 'universe', 'on', 'the', 'basis', 'of', 'the', 'pscz', 'galaxy', 'survey', 'the', 'prime', 'objective', 'o... | [-0.0637000225696658, 0.04859590120245497, -0.11698946612715885, 0.07792012019918355, -0.05383431246274781, 0.02293776711645906, -8.660584674490725e-05, 0.35866732090738984, -0.2467601122561438, -0.3065577130422325, 0.05567491121238324, -0.26292218622641966, -0.06451307172183614, 0.12918996601472507, -0.002498481800029... |
707.2608 | Multi-Wavelength Imaging of Young Stellar Object Disks: Toward an
Understanding of Disk Structure and Dust Evolution | We review recent progress in high-resolution imaging of scattered light from
disks around young stellar objects. Many new disks have been discovered or
imaged in scattered light, and improved instrumentation and observing
techniques have led to better disk images at optical, near-infrared, and
thermal-infrared wavele... | astro-ph | we review recent progress in highresolution imaging of scattered light from disks around young stellar objects many new disks have been discovered or imaged in scattered light and improved instrumentation and observing techniques have led to better disk images at optical nearinfrared and thermalinfrared wavelengths mul... | [['we', 'review', 'recent', 'progress', 'in', 'highresolution', 'imaging', 'of', 'scattered', 'light', 'from', 'disks', 'around', 'young', 'stellar', 'objects', 'many', 'new', 'disks', 'have', 'been', 'discovered', 'or', 'imaged', 'in', 'scattered', 'light', 'and', 'improved', 'instrumentation', 'and', 'observing', 'te... | [-0.035871861066541395, 0.08329108016857621, -0.12247154222850025, 0.07113260964579954, -0.11552185435426342, -0.07369082278626807, -0.03988342456142205, 0.48703432160740096, -0.19254536623305646, -0.3460484821489385, 0.12051003291408587, -0.2630009389257217, -0.07990273011671806, 0.2414458417105397, -0.090886196170270... |
707.2609 | Impact of the new solar abundances on the calibration of the PMS binary
system RS Cha | Context: In a recent work, we tried to obtain a calibration of the two
components of the pre-main sequence binary system RS Cha by means of
theoretical stellar models. We found that the only way to reproduce the
observational parameters of RS Cha with standard stellar models is to decrease
the initial abundances of c... | astro-ph | context in a recent work we tried to obtain a calibration of the two components of the premain sequence binary system rs cha by means of theoretical stellar models we found that the only way to reproduce the observational parameters of rs cha with standard stellar models is to decrease the initial abundances of carbon ... | [['context', 'in', 'a', 'recent', 'work', 'we', 'tried', 'to', 'obtain', 'a', 'calibration', 'of', 'the', 'two', 'components', 'of', 'the', 'premain', 'sequence', 'binary', 'system', 'rs', 'cha', 'by', 'means', 'of', 'theoretical', 'stellar', 'models', 'we', 'found', 'that', 'the', 'only', 'way', 'to', 'reproduce', 'th... | [0.0012889433126866945, 0.13840234431885548, -0.058011247163556295, 0.06644863733113286, -0.03761046146745702, -0.12027258217088221, 0.06717344641505156, 0.3959145044140956, -0.20040758725200944, -0.35614802138611684, 0.03679859306601643, -0.2697070391264324, -0.051449611570419884, 0.1529410140572901, -0.07712108023948... |
707.261 | Chemical Abundances of Luminous Cool Stars in the Galactic Center from
High-Resolution Infrared Spectroscopy | We present chemical abundances in a sample of luminous cool stars located
within 30 pc of the Galactic Center. Abundances of carbon, nitrogen, oxygen,
calcium, and iron were derived from high-resolution infrared spectra in the H-
and K-bands. The abundance results indicate that both [O/Fe] and [Ca/Fe] are
enhanced re... | astro-ph | we present chemical abundances in a sample of luminous cool stars located within 30 pc of the galactic center abundances of carbon nitrogen oxygen calcium and iron were derived from highresolution infrared spectra in the h and kbands the abundance results indicate that both ofe and cafe are enhanced respectively by ave... | [['we', 'present', 'chemical', 'abundances', 'in', 'a', 'sample', 'of', 'luminous', 'cool', 'stars', 'located', 'within', '30', 'pc', 'of', 'the', 'galactic', 'center', 'abundances', 'of', 'carbon', 'nitrogen', 'oxygen', 'calcium', 'and', 'iron', 'were', 'derived', 'from', 'highresolution', 'infrared', 'spectra', 'in',... | [0.03181728005317822, 0.16156186186646018, 0.020789005191110366, 0.060411970424637244, -0.008705821448931344, -0.014490081470151163, 0.10318057967401309, 0.45482761248306264, -0.1524235746891815, -0.4262386819339169, -0.037008257698484814, -0.3604432342265464, 0.10034813513076561, 0.1721270595656619, -0.071393005392782... |
707.2611 | Do all states undergo sudden death of entanglement at finite
temperature? | In this paper we consider the decay of quantum entanglement, quantified by
the concurrence, of a pair of two-level systems each of which is interacting
with a reservoir at finite temperature T. For a broad class of initially
entangled states, we demonstrate that the system always becomes disentangled in
a finite time... | quant-ph | in this paper we consider the decay of quantum entanglement quantified by the concurrence of a pair of twolevel systems each of which is interacting with a reservoir at finite temperature t for a broad class of initially entangled states we demonstrate that the system always becomes disentangled in a finite time ieenta... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'decay', 'of', 'quantum', 'entanglement', 'quantified', 'by', 'the', 'concurrence', 'of', 'a', 'pair', 'of', 'twolevel', 'systems', 'each', 'of', 'which', 'is', 'interacting', 'with', 'a', 'reservoir', 'at', 'finite', 'temperature', 't', 'for', 'a', 'broad', 'class', 'o... | [-0.14969913686466654, 0.2639532625725246, -0.06381434779727786, 0.027247108337355823, 0.07828028227213951, -0.20708802749016664, 0.024467644632351015, 0.3397812044656858, -0.22713517326089303, -0.23567285092274953, 0.052706019440381904, -0.27413488465656594, -0.07789782722616886, 0.18572512475728262, -0.02414642749127... |
707.2612 | Exceptional covers of surfaces | Consider a finite morphism f:X -> Y of smooth projective varieties over a
finite field k. Suppose X is the vanishing locus in projective N-space of at
most r forms of degree at most d. We show there is a constant C, depending only
on N, r, d and deg(f) such that if #k > C, then f(k):X(k) -> Y(k) is injective
if and o... | math.AG | consider a finite morphism fx y of smooth projective varieties over a finite field k suppose x is the vanishing locus in projective nspace of at most r forms of degree at most d we show there is a constant c depending only on n r d and degf such that if k c then fkxk yk is injective if and only if its surjective | [['consider', 'a', 'finite', 'morphism', 'fx', 'y', 'of', 'smooth', 'projective', 'varieties', 'over', 'a', 'finite', 'field', 'k', 'suppose', 'x', 'is', 'the', 'vanishing', 'locus', 'in', 'projective', 'nspace', 'of', 'at', 'most', 'r', 'forms', 'of', 'degree', 'at', 'most', 'd', 'we', 'show', 'there', 'is', 'a', 'con... | [-0.2472153326489206, 0.0962008624774171, -0.05502745871490333, -0.04246113800218154, -0.030389004648895934, -0.29252866984461434, 0.0022609777515754104, 0.3707923798938282, -0.38298171617861954, -0.10006493855325971, 0.057636792573248385, -0.29001594933561137, -0.09171343584239366, 0.17014647397445515, -0.086409305797... |
707.2613 | Do static atoms outside a Schwarzschild black hole spontaneously excite? | The spontaneous excitation of a two-level atom held static outside a four
dimensional Schwarzschild black hole and in interaction with a massless scalar
field in the Boulware, Unruh and Hartle-Hawking vacuum is investigated and the
contributions of the vacuum fluctuations and radiation reaction to the rate of
change ... | gr-qc hep-th | the spontaneous excitation of a twolevel atom held static outside a four dimensional schwarzschild black hole and in interaction with a massless scalar field in the boulware unruh and hartlehawking vacuum is investigated and the contributions of the vacuum fluctuations and radiation reaction to the rate of change of th... | [['the', 'spontaneous', 'excitation', 'of', 'a', 'twolevel', 'atom', 'held', 'static', 'outside', 'a', 'four', 'dimensional', 'schwarzschild', 'black', 'hole', 'and', 'in', 'interaction', 'with', 'a', 'massless', 'scalar', 'field', 'in', 'the', 'boulware', 'unruh', 'and', 'hartlehawking', 'vacuum', 'is', 'investigated'... | [-0.09963980289283154, 0.26327716055583417, -0.07603384443473783, 0.08263307090195689, -0.0051055595963850784, -0.1135533965251612, -0.008943490087236652, 0.3507945703492425, -0.16309673547070344, -0.25559350336505765, 0.05522145222318519, -0.29714558954382764, -0.00268937231191359, 0.14213101319358523, -0.004455629502... |
707.2614 | X-MAS2: Study Systematics on the ICM Metallicity Measurements | (Abridged)The X-ray measurements of the ICM metallicity are becoming more
frequent due to the availability of powerful X-ray telescope with excellent
spatial and spectral resolutions. The information which can be extracted from
the measurements of the alpha-elements, like Oxygen, Magnesium and Silicon with
respect to... | astro-ph | abridgedthe xray measurements of the icm metallicity are becoming more frequent due to the availability of powerful xray telescope with excellent spatial and spectral resolutions the information which can be extracted from the measurements of the alphaelements like oxygen magnesium and silicon with respect to the iron ... | [['abridgedthe', 'xray', 'measurements', 'of', 'the', 'icm', 'metallicity', 'are', 'becoming', 'more', 'frequent', 'due', 'to', 'the', 'availability', 'of', 'powerful', 'xray', 'telescope', 'with', 'excellent', 'spatial', 'and', 'spectral', 'resolutions', 'the', 'information', 'which', 'can', 'be', 'extracted', 'from',... | [-0.03666520364182261, 0.1070637548763356, -0.0525854871335618, 0.08520916316894278, -0.06069815553180963, -0.11560184791148322, 0.05734122827870784, 0.4297670289134122, -0.22069635575681873, -0.3740231328357206, 0.06700230923868805, -0.33302367553965084, -0.02589499918992746, 0.20120798029987882, -0.043867136795099265... |
707.2615 | NMR Evidence for Antiferromagnetic Transition in the Single-Component
Molecular Conductor, [Au(tmdt)_{2}] at 110 K | We present the results of a ^{1}H NMR study of the single-component molecular
conductor, [Au(tmdt)_{2}].
A steep increase in the NMR line width and a peak formation of the nuclear
spin-lattice relaxation rate, 1/T_{1}, were observed at around 110 K.
This behavior provides clear and microscopic evidences for a mag... | cond-mat.str-el | we present the results of a 1h nmr study of the singlecomponent molecular conductor autmdt_2 a steep increase in the nmr line width and a peak formation of the nuclear spinlattice relaxation rate 1t_1 were observed at around 110 k this behavior provides clear and microscopic evidences for a magnetic phase transition at... | [['we', 'present', 'the', 'results', 'of', 'a', '1h', 'nmr', 'study', 'of', 'the', 'singlecomponent', 'molecular', 'conductor', 'autmdt_2', 'a', 'steep', 'increase', 'in', 'the', 'nmr', 'line', 'width', 'and', 'a', 'peak', 'formation', 'of', 'the', 'nuclear', 'spinlattice', 'relaxation', 'rate', '1t_1', 'were', 'observ... | [-0.15929916031707667, 0.18844026290906568, -0.06438252283260226, 0.011451099924191735, 0.012350609921237552, -0.14642545759163209, 0.079884843061384, 0.3947892411562957, -0.20798543675482506, -0.3016551119791601, -0.002522778093790341, -0.32381226014541953, -0.0604976503864715, 0.19662829550399788, 0.09853262999891549... |
707.2616 | Preserving Monotonicity in Anisotropic Diffusion | We show that standard algorithms for anisotropic diffusion based on centered
differencing (including the recent symmetric algorithm) do not preserve
monotonicity. In the context of anisotropic thermal conduction, this can lead
to the violation of the entropy constraints of the second law of
thermodynamics, causing he... | astro-ph physics.comp-ph physics.plasm-ph | we show that standard algorithms for anisotropic diffusion based on centered differencing including the recent symmetric algorithm do not preserve monotonicity in the context of anisotropic thermal conduction this can lead to the violation of the entropy constraints of the second law of thermodynamics causing heat to f... | [['we', 'show', 'that', 'standard', 'algorithms', 'for', 'anisotropic', 'diffusion', 'based', 'on', 'centered', 'differencing', 'including', 'the', 'recent', 'symmetric', 'algorithm', 'do', 'not', 'preserve', 'monotonicity', 'in', 'the', 'context', 'of', 'anisotropic', 'thermal', 'conduction', 'this', 'can', 'lead', 't... | [-0.0858083823668387, 0.1215266172445434, -0.06628700295353637, 0.07512080254759092, -0.09489552288535325, -0.14261346433640404, -0.006782160869196934, 0.38325123724472876, -0.2625655591761803, -0.29724349162253716, 0.12001527026775019, -0.2644872424630996, -0.07157574717147167, 0.23182154522510245, -0.0810432661105604... |
707.2617 | A New Sample of Low-mass Black Holes in Active Galaxies | We present an expanded sample of low-mass black holes (BHs) found in galactic
nuclei. Using standard virial mass techniques to estimate BH masses, we select
from the Fourth Data Release of the Sloan Digital Sky Survey all broad-line
active galaxies with masses < 2 x 10^6 M_sun. BHs in this mass regime provide
unique ... | astro-ph | we present an expanded sample of lowmass black holes bhs found in galactic nuclei using standard virial mass techniques to estimate bh masses we select from the fourth data release of the sloan digital sky survey all broadline active galaxies with masses 2 x 106 m_sun bhs in this mass regime provide unique tests of the... | [['we', 'present', 'an', 'expanded', 'sample', 'of', 'lowmass', 'black', 'holes', 'bhs', 'found', 'in', 'galactic', 'nuclei', 'using', 'standard', 'virial', 'mass', 'techniques', 'to', 'estimate', 'bh', 'masses', 'we', 'select', 'from', 'the', 'fourth', 'data', 'release', 'of', 'the', 'sloan', 'digital', 'sky', 'survey... | [-0.056214758582667994, 0.10686096104519785, -0.0028332250561776025, 0.13045443102260523, -0.0864668533188414, -0.055760965077206494, 0.06488414289131057, 0.4323730184292456, -0.09602030487994681, -0.41379223145579674, 0.0811380298454578, -0.37293101459530725, 0.03382578681306562, 0.2195198121089664, -0.032556544588703... |
707.2618 | Domino Waves | Motivated by a proposal of Daykin (Problem 71-19*, SIAM Review 13 (1971)
569), we study the wave that propagates along an infinite chain of dominoes and
find the limiting speed of the wave in an extreme case.
| math.DS math.HO | motivated by a proposal of daykin problem 7119 siam review 13 1971 569 we study the wave that propagates along an infinite chain of dominoes and find the limiting speed of the wave in an extreme case | [['motivated', 'by', 'a', 'proposal', 'of', 'daykin', 'problem', '7119', 'siam', 'review', '13', '1971', '569', 'we', 'study', 'the', 'wave', 'that', 'propagates', 'along', 'an', 'infinite', 'chain', 'of', 'dominoes', 'and', 'find', 'the', 'limiting', 'speed', 'of', 'the', 'wave', 'in', 'an', 'extreme', 'case']] | [-0.15354433112467328, 0.13184758214386724, 0.0010038835720883475, -0.0061474805180397295, -0.031803590142064624, -0.05858359738097837, 0.05318371679944297, 0.32857750578679973, -0.23354348090166846, -0.28861476336088443, 0.1381078702365307, -0.2832503417610294, -0.14923662822305536, 0.1913739750161767, -0.045768935310... |
707.2619 | Photoinduced melting of charge order in a quarter-filled electron system
coupled with different types of phonons | Photoinduced melting of charge order is calculated by using the exact
many-electron wave function coupled with classically treated phonons in the
one-dimensional quarter-filled Hubbard model with Peierls and Holstein types of
electron-phonon couplings. The model parameters are taken from recent
experiments on (EDO-TT... | cond-mat.str-el | photoinduced melting of charge order is calculated by using the exact manyelectron wave function coupled with classically treated phonons in the onedimensional quarterfilled hubbard model with peierls and holstein types of electronphonon couplings the model parameters are taken from recent experiments on edottf_2pf_6 e... | [['photoinduced', 'melting', 'of', 'charge', 'order', 'is', 'calculated', 'by', 'using', 'the', 'exact', 'manyelectron', 'wave', 'function', 'coupled', 'with', 'classically', 'treated', 'phonons', 'in', 'the', 'onedimensional', 'quarterfilled', 'hubbard', 'model', 'with', 'peierls', 'and', 'holstein', 'types', 'of', 'e... | [-0.09361957857618108, 0.2533117601226582, -0.01825211206975747, 0.05702524266654993, 0.0291873451492841, -0.11776852091236538, 0.042222412696606676, 0.42020913481738575, -0.24407663576068803, -0.2618530848601335, -0.01983032979540081, -0.3233044941640708, -0.0866075725160198, 0.1787001052445037, 0.09037611806030635, 0... |
707.262 | Non-Gaussianity of the Cosmic Baryon Fluid: Log-Poisson Hierarchy Model | In the nonlinear regime of cosmic clustering, the mass density field of the
cosmic baryon fluid is highly non-Gaussian. It shows different dynamical
behavior from collisionless dark matter. Nevertheless, the evolved field of
baryon fluid is scale-covariant in the range from the Jeans length to a few ten
h^{-1} Mpc, i... | astro-ph | in the nonlinear regime of cosmic clustering the mass density field of the cosmic baryon fluid is highly nongaussian it shows different dynamical behavior from collisionless dark matter nevertheless the evolved field of baryon fluid is scalecovariant in the range from the jeans length to a few ten h1 mpc in which the d... | [['in', 'the', 'nonlinear', 'regime', 'of', 'cosmic', 'clustering', 'the', 'mass', 'density', 'field', 'of', 'the', 'cosmic', 'baryon', 'fluid', 'is', 'highly', 'nongaussian', 'it', 'shows', 'different', 'dynamical', 'behavior', 'from', 'collisionless', 'dark', 'matter', 'nevertheless', 'the', 'evolved', 'field', 'of',... | [-0.1411486485936061, 0.20877960395710732, -0.09582354943939628, 0.11773154399638595, -0.039964858124921405, -0.07364680286487922, -0.056530566296714824, 0.27722611922609547, -0.25830505685399446, -0.30095935181284755, 0.02675624286684279, -0.26858715108559966, -0.07497235478233331, 0.1768157946073468, 0.04663026819113... |
707.2621 | Higher Energies in Kahler Geometry I | Let $X\hookrightarrow \cpn $ be a smooth complex projective variety of
dimension $n$. Let $\lambda$ be an algebraic one parameter subgroup of
$G:=\gc$. Let $ 0\leq l\leq n+1$. We associate to the coefficients
$F_{l}(\lambda)$ of the normalized weight of $\lambda$ on the $mth$ Hilbert
point of $X$ new energies $F_{\om... | math.DG math.AG | let xhookrightarrow cpn be a smooth complex projective variety of dimension n let lambda be an algebraic one parameter subgroup of ggc let 0leq lleq n1 we associate to the coefficients f_llambda of the normalized weight of lambda on the mth hilbert point of x new energies f_omlvp the logarithmic asymptotics of f_omlvp ... | [['let', 'xhookrightarrow', 'cpn', 'be', 'a', 'smooth', 'complex', 'projective', 'variety', 'of', 'dimension', 'n', 'let', 'lambda', 'be', 'an', 'algebraic', 'one', 'parameter', 'subgroup', 'of', 'ggc', 'let', '0leq', 'lleq', 'n1', 'we', 'associate', 'to', 'the', 'coefficients', 'f_llambda', 'of', 'the', 'normalized', ... | [-0.1699569552352554, 0.09365593524493497, -0.04709856958177529, 0.026021821812824593, -0.07095432650591982, -0.19707478315716512, -0.01940695657272284, 0.26919976976749144, -0.32196080660643545, -0.20687651103484983, 0.03447294301892582, -0.31403200439128437, -0.06071781961149291, 0.1594480917543957, -0.08354866368401... |
707.2622 | ATCA 1.2 cm Observations of the Massive Star Forming Region G305.2+0.2 | We report on Australia Telescope observations of the massive star forming
region G305.2+0.2 at 1.2 cm. We detected emission in five molecules towards
G305A, confirming its hot core nature. We determined a rotational temperature
of 26 K for methanol. A non-LTE excitation calculation suggests a kinematic
temperature of... | astro-ph | we report on australia telescope observations of the massive star forming region g305202 at 12 cm we detected emission in five molecules towards g305a confirming its hot core nature we determined a rotational temperature of 26 k for methanol a nonlte excitation calculation suggests a kinematic temperature of order 200 ... | [['we', 'report', 'on', 'australia', 'telescope', 'observations', 'of', 'the', 'massive', 'star', 'forming', 'region', 'g305202', 'at', '12', 'cm', 'we', 'detected', 'emission', 'in', 'five', 'molecules', 'towards', 'g305a', 'confirming', 'its', 'hot', 'core', 'nature', 'we', 'determined', 'a', 'rotational', 'temperatu... | [-0.08212403252192806, 0.08573056511808577, -0.0028081803881962386, 0.0035250454640758802, -0.05560584813134656, -0.10877827897812017, 0.08407883685902648, 0.47396529419347644, -0.136337754638156, -0.28874029682040037, 0.06680562135062203, -0.2677771513339221, -0.0016963418096392637, 0.15035746460835936, 0.054677414513... |
707.2623 | Spectroscopy of Mesons with Heavy Quarks | I will give a concise overview of mesons with heavy quarks including p-wave
charmed mesons and charmonium (or charmonium-like) states such as X(3872),
Y(4260), X(3940), Y(3940), Z(3930) etc. The effect from the nearby S-wave open
channels on the quark model spectrum is emphasized.
| hep-ph hep-ex nucl-th | i will give a concise overview of mesons with heavy quarks including pwave charmed mesons and charmonium or charmoniumlike states such as x3872 y4260 x3940 y3940 z3930 etc the effect from the nearby swave open channels on the quark model spectrum is emphasized | [['i', 'will', 'give', 'a', 'concise', 'overview', 'of', 'mesons', 'with', 'heavy', 'quarks', 'including', 'pwave', 'charmed', 'mesons', 'and', 'charmonium', 'or', 'charmoniumlike', 'states', 'such', 'as', 'x3872', 'y4260', 'x3940', 'y3940', 'z3930', 'etc', 'the', 'effect', 'from', 'the', 'nearby', 'swave', 'open', 'ch... | [-0.08808705390452645, 0.3330271611813196, -0.11205617399063221, 0.24847283835122144, -0.1023545936183181, -0.2438864182832456, 0.11533104390079199, 0.29792942643858666, -0.09290609593221615, -0.1249223810425678, -0.15513751725124758, -0.41625913570440093, 0.04808371212485051, -0.0007846673928894275, 0.1204660277445475... |
707.2624 | Analytic Approach for Controlling Realistic Quantum Chaotic Systems | An analytic approach for controlling quantum states, which was originally
applied to fully random matrix systems [T. Takami and H. Fujisaki, Phys. Rev. E
75, 036219 (2007)], is extended to deal with more realistic quantum systems
with a banded random matrix (BRM). The validity of the new analytic field is
confirmed b... | nlin.CD physics.chem-ph quant-ph | an analytic approach for controlling quantum states which was originally applied to fully random matrix systems t takami and h fujisaki phys rev e 75 036219 2007 is extended to deal with more realistic quantum systems with a banded random matrix brm the validity of the new analytic field is confirmed by directly solvin... | [['an', 'analytic', 'approach', 'for', 'controlling', 'quantum', 'states', 'which', 'was', 'originally', 'applied', 'to', 'fully', 'random', 'matrix', 'systems', 't', 'takami', 'and', 'h', 'fujisaki', 'phys', 'rev', 'e', '75', '036219', '2007', 'is', 'extended', 'to', 'deal', 'with', 'more', 'realistic', 'quantum', 'sy... | [-0.10287274690965811, 0.12809740512340795, -0.054629397975901765, 0.004875083475684126, -0.07283802047371864, -0.16955735792095464, 0.031173940527563292, 0.3153412237887581, -0.2121665646880865, -0.28666368070989845, 0.05012236402370036, -0.22882409729684391, -0.13690120761593183, 0.20920567815502486, -0.0247916493533... |
707.2625 | Radio Frequency Spectroscopy of Trapped Fermi Gases with Population
Imbalance | Motivated by recent experiments, we address, in a fully self consistent
fashion, the behavior and evolution of radio frequency (RF) spectra as
temperature and polarization are varied in population imbalanced Fermi gases.
We discuss a series of scenarios for the experimentally observed zero
temperature pseudogap phase... | cond-mat.str-el cond-mat.quant-gas cond-mat.supr-con | motivated by recent experiments we address in a fully self consistent fashion the behavior and evolution of radio frequency rf spectra as temperature and polarization are varied in population imbalanced fermi gases we discuss a series of scenarios for the experimentally observed zero temperature pseudogap phase and sho... | [['motivated', 'by', 'recent', 'experiments', 'we', 'address', 'in', 'a', 'fully', 'self', 'consistent', 'fashion', 'the', 'behavior', 'and', 'evolution', 'of', 'radio', 'frequency', 'rf', 'spectra', 'as', 'temperature', 'and', 'polarization', 'are', 'varied', 'in', 'population', 'imbalanced', 'fermi', 'gases', 'we', '... | [-0.15133139667703271, 0.21913553117374618, -0.06297599260855202, 0.06168163634573269, -0.03461858347020667, -0.11770067577052748, 0.11626616625275199, 0.4135934075321814, -0.2430121214552359, -0.29489300769255167, 0.06426146419159127, -0.2987103388842308, -0.0986569124377436, 0.1728848137873968, 0.02479217111161261, 0... |
707.2626 | Higgs-free confinement hierarchy in five colour QCD | I consider the monopole condensate of five color QCD. The naive lowest energy
state is unobtainable at one-loop for five or more colors due to simple
geometric considerations. The consequent adjustment of the vacuum condensate
generates a hierarchy of confinement scales in a natural Higgs-free manner. The
accompanyin... | hep-th | i consider the monopole condensate of five color qcd the naive lowest energy state is unobtainable at oneloop for five or more colors due to simple geometric considerations the consequent adjustment of the vacuum condensate generates a hierarchy of confinement scales in a natural higgsfree manner the accompanying symme... | [['i', 'consider', 'the', 'monopole', 'condensate', 'of', 'five', 'color', 'qcd', 'the', 'naive', 'lowest', 'energy', 'state', 'is', 'unobtainable', 'at', 'oneloop', 'for', 'five', 'or', 'more', 'colors', 'due', 'to', 'simple', 'geometric', 'considerations', 'the', 'consequent', 'adjustment', 'of', 'the', 'vacuum', 'co... | [-0.13759718032711785, 0.21551274144336016, -0.10182300038702254, 0.14670757444816576, -0.09322114255545395, -0.1466604940776181, 0.030146701793585504, 0.32577284013054203, -0.18836924111071443, -0.3075350173083799, 0.027595828867301213, -0.27147264193211285, -0.05304223936400376, 0.043987416088514565, -0.0066674459085... |
707.2627 | On the linear fractional self-attracting diffusion | In this paper, we introduce the linear fractional self-attracting diffusion
driven by a fractional Brownian motion with Hurst index 1/2<H<1, which is
analogous to the linear self-attracting diffusion. For 1-dimensional process we
study its convergence and the corresponding weighted local time. For
2-dimensional proce... | math.PR | in this paper we introduce the linear fractional selfattracting diffusion driven by a fractional brownian motion with hurst index 12h1 which is analogous to the linear selfattracting diffusion for 1dimensional process we study its convergence and the corresponding weighted local time for 2dimensional process as a relat... | [['in', 'this', 'paper', 'we', 'introduce', 'the', 'linear', 'fractional', 'selfattracting', 'diffusion', 'driven', 'by', 'a', 'fractional', 'brownian', 'motion', 'with', 'hurst', 'index', '12h1', 'which', 'is', 'analogous', 'to', 'the', 'linear', 'selfattracting', 'diffusion', 'for', '1dimensional', 'process', 'we', '... | [-0.0967325218487531, 0.14569267670740374, -0.06596434488892555, 0.045386909043797156, -0.055990230897441505, -0.11015287233361354, 0.010918679074772323, 0.37364413316051165, -0.3795601846029361, -0.18078659274615347, 0.12743293983318532, -0.2560086471339067, -0.20456937067210673, 0.15763985499118766, -0.09495337552701... |
707.2628 | A fitting formula for the merger timescale of galaxies in hierarchical
clustering | We study galaxy mergers using a high-resolution cosmological hydro/N-body
simulation with star formation, and compare the measured merger timescales with
theoretical predictions based on the Chandrasekhar formula. In contrast to
Navarro et al., our numerical results indicate, that the commonly used equation
for the m... | astro-ph | we study galaxy mergers using a highresolution cosmological hydronbody simulation with star formation and compare the measured merger timescales with theoretical predictions based on the chandrasekhar formula in contrast to navarro et al our numerical results indicate that the commonly used equation for the merger time... | [['we', 'study', 'galaxy', 'mergers', 'using', 'a', 'highresolution', 'cosmological', 'hydronbody', 'simulation', 'with', 'star', 'formation', 'and', 'compare', 'the', 'measured', 'merger', 'timescales', 'with', 'theoretical', 'predictions', 'based', 'on', 'the', 'chandrasekhar', 'formula', 'in', 'contrast', 'to', 'nav... | [-0.0693886050183366, 0.0678137249698373, -0.11943857682748668, 0.1442052927218698, -0.09179252348915343, -0.06276418463957886, 0.015228450937967708, 0.35790633829811247, -0.14759290275434334, -0.3421483827875026, 0.03674009068173066, -0.2628158560843878, -0.08338823665298963, 0.23713208664889618, -0.013256052624113777... |
707.2629 | Temporal evolution of the Evershed flow in sunspots. I. Observational
characterization of Evershed clouds | [Abridged] The magnetic and kinematic properties of the photospheric Evershed
flow are relatively well known, but we are still far from a complete
understanding of its nature. The evolution of the flow with time, which is
mainly due to appearance of velocity packets called Evershed clouds (ECs), may
provide informati... | astro-ph | abridged the magnetic and kinematic properties of the photospheric evershed flow are relatively well known but we are still far from a complete understanding of its nature the evolution of the flow with time which is mainly due to appearance of velocity packets called evershed clouds ecs may provide information to furt... | [['abridged', 'the', 'magnetic', 'and', 'kinematic', 'properties', 'of', 'the', 'photospheric', 'evershed', 'flow', 'are', 'relatively', 'well', 'known', 'but', 'we', 'are', 'still', 'far', 'from', 'a', 'complete', 'understanding', 'of', 'its', 'nature', 'the', 'evolution', 'of', 'the', 'flow', 'with', 'time', 'which',... | [-0.12549112347635225, 0.1614876304153952, -0.043305369143818544, 0.05658156352143709, -0.10014639166346588, -0.06037437407685756, 0.013179021431589043, 0.4279775999981415, -0.2588568056564798, -0.32160069702060445, 0.11265148826340747, -0.23505141386938105, -0.07274322786410763, 0.1866273515112047, -0.0458175462094246... |
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