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 |
|---|---|---|---|---|---|---|
710.4353 | Reduction to the Simplest - The Complexity of Minimalistic Heteropolymer
Models | Simple coarse-grained hydrophobic-polar models for heteropolymers as the
lattice HP and the off-lattice AB model allow a general classification of
characteristic behaviors for hydrophobic-core based tertiary folding. The
strongly reduced computational efforts enable one to reveal systematically the
thermodynamic prop... | cond-mat.soft physics.bio-ph | simple coarsegrained hydrophobicpolar models for heteropolymers as the lattice hp and the offlattice ab model allow a general classification of characteristic behaviors for hydrophobiccore based tertiary folding the strongly reduced computational efforts enable one to reveal systematically the thermodynamic properties ... | [['simple', 'coarsegrained', 'hydrophobicpolar', 'models', 'for', 'heteropolymers', 'as', 'the', 'lattice', 'hp', 'and', 'the', 'offlattice', 'ab', 'model', 'allow', 'a', 'general', 'classification', 'of', 'characteristic', 'behaviors', 'for', 'hydrophobiccore', 'based', 'tertiary', 'folding', 'the', 'strongly', 'reduc... | [-0.09716311780534484, 0.16173207323142402, -0.12173040855575253, 0.10673591276832126, -0.04329865816131083, -0.17889161217907393, 0.06666907692655318, 0.4238936921732651, -0.30012599869656403, -0.2792698635493179, 0.002921135232444047, -0.18292238254955895, -0.18360086342294676, 0.1824583994331644, 0.02715395816375275... |
710.4354 | Studying the galactic outflow in NGC 1569 | We present deep WIYN H-alpha imaging of the dwarf irregular starburst galaxy
NGC 1569, together with WIYN SparsePak spatially-resolved optical spectroscopy
of the galactic outflow. This leads on from our previous detailed analyses of
the state of the ISM in the central regions of this galaxy. Our deep imaging
reveals... | astro-ph | we present deep wiyn halpha imaging of the dwarf irregular starburst galaxy ngc 1569 together with wiyn sparsepak spatiallyresolved optical spectroscopy of the galactic outflow this leads on from our previous detailed analyses of the state of the ism in the central regions of this galaxy our deep imaging reveals previo... | [['we', 'present', 'deep', 'wiyn', 'halpha', 'imaging', 'of', 'the', 'dwarf', 'irregular', 'starburst', 'galaxy', 'ngc', '1569', 'together', 'with', 'wiyn', 'sparsepak', 'spatiallyresolved', 'optical', 'spectroscopy', 'of', 'the', 'galactic', 'outflow', 'this', 'leads', 'on', 'from', 'our', 'previous', 'detailed', 'ana... | [-0.058176910200460945, 0.08191357755552732, -0.08834240387529689, 0.02768868765383474, -0.09747719787646321, -0.023328783524181124, 0.020163690643194634, 0.4575907450487844, -0.19268871733631426, -0.3136375949161515, 0.0386411453303829, -0.26275176330916167, -0.015701240143257446, 0.16626250079346536, -0.0067910301262... |
710.4355 | Adsorption Phenomena at Organic-Inorganic Interfaces | The qualitative solvent- and temperature-dependent conformational behavior of
a peptide in the proximity of solid substrates with different adsorption
properties is investigated by means of a simple lattice model. The resulting
pseudophase diagrams exhibit a complex structure, which can be understood by
analysing the... | cond-mat.soft physics.bio-ph | the qualitative solvent and temperaturedependent conformational behavior of a peptide in the proximity of solid substrates with different adsorption properties is investigated by means of a simple lattice model the resulting pseudophase diagrams exhibit a complex structure which can be understood by analysing the minim... | [['the', 'qualitative', 'solvent', 'and', 'temperaturedependent', 'conformational', 'behavior', 'of', 'a', 'peptide', 'in', 'the', 'proximity', 'of', 'solid', 'substrates', 'with', 'different', 'adsorption', 'properties', 'is', 'investigated', 'by', 'means', 'of', 'a', 'simple', 'lattice', 'model', 'the', 'resulting', ... | [-0.13173458354219542, 0.17533041956749829, -0.15230148410932584, 0.06606249927162108, -0.007453110102902759, -0.11957365840842778, 0.09576971753585067, 0.41081577546217224, -0.2807542131875049, -0.3008960032327609, 0.0037313651547513224, -0.2332988205281171, -0.20658230591904034, 0.13550715792225673, 0.023027756827121... |
710.4356 | Schemes for robust quantum computation with polar molecules: analysis of
experimental feasibility | We analyse recently proposed physical implementations of a quantum computer
based on polar molecules. A set of general requirements for a molecular system
is presented, which would provide an optimal combination of quantum gate times,
coherence times, number of operations, high gate accuracy and experimental
feasibil... | quant-ph | we analyse recently proposed physical implementations of a quantum computer based on polar molecules a set of general requirements for a molecular system is presented which would provide an optimal combination of quantum gate times coherence times number of operations high gate accuracy and experimental feasibility we ... | [['we', 'analyse', 'recently', 'proposed', 'physical', 'implementations', 'of', 'a', 'quantum', 'computer', 'based', 'on', 'polar', 'molecules', 'a', 'set', 'of', 'general', 'requirements', 'for', 'a', 'molecular', 'system', 'is', 'presented', 'which', 'would', 'provide', 'an', 'optimal', 'combination', 'of', 'quantum'... | [-0.20383284590626136, 0.13645213251025415, -0.00934429148817435, 0.03839799405820668, 0.006232477188110351, -0.21018506358936428, 0.12850031320378183, 0.444874427318573, -0.2080331279486418, -0.27768233931437136, 0.027086938709020614, -0.2154159882813692, -0.14468902663886546, 0.2326634619832039, 0.005948918079957366,... |
710.4357 | Charm Quarks and the QCD Equation of State | We present a study of the effect of charm quarks on the QCD equation of state
using partially-quenched p4 charm quarks on a dynamically generated 2+1 flavor
background, at zero chemical potential. We show preliminary results for the
charm quark contribution to the energy density and pressure in the high
temperature r... | hep-lat | we present a study of the effect of charm quarks on the qcd equation of state using partiallyquenched p4 charm quarks on a dynamically generated 21 flavor background at zero chemical potential we show preliminary results for the charm quark contribution to the energy density and pressure in the high temperature region ... | [['we', 'present', 'a', 'study', 'of', 'the', 'effect', 'of', 'charm', 'quarks', 'on', 'the', 'qcd', 'equation', 'of', 'state', 'using', 'partiallyquenched', 'p4', 'charm', 'quarks', 'on', 'a', 'dynamically', 'generated', '21', 'flavor', 'background', 'at', 'zero', 'chemical', 'potential', 'we', 'show', 'preliminary', ... | [-0.05776152008439641, 0.2941258614945754, -0.11143467733888207, 0.10194079677505116, -0.012027222864531182, -0.06328470374432367, 0.1582455583313178, 0.3197849341794043, -0.17494256898125232, -0.2404070650604931, -0.023583936412202043, -0.35016275982599, 0.06225061916267952, 0.09129130037665065, 0.09024610573927734, 0... |
710.4358 | Geometrization of 3-dimensional Coxeter orbifolds and Singer's
conjecture | Associated to any Coxeter system $(W,S)$, there is a labeled simplicial
complex $L$ and a contractible CW-complex $\Sigma_L$ (the Davis complex) on
which $W$ acts properly and cocompactly. $\Sigma_L$ admits a cellulation under
which the nerve of each vertex is $L$. It follows that if $L$ is a
triangulation of $\mathb... | math.GR math.AT math.GT | associated to any coxeter system ws there is a labeled simplicial complex l and a contractible cwcomplex sigma_l the davis complex on which w acts properly and cocompactly sigma_l admits a cellulation under which the nerve of each vertex is l it follows that if l is a triangulation of mathbbsn1 then sigma_l is a contra... | [['associated', 'to', 'any', 'coxeter', 'system', 'ws', 'there', 'is', 'a', 'labeled', 'simplicial', 'complex', 'l', 'and', 'a', 'contractible', 'cwcomplex', 'sigma_l', 'the', 'davis', 'complex', 'on', 'which', 'w', 'acts', 'properly', 'and', 'cocompactly', 'sigma_l', 'admits', 'a', 'cellulation', 'under', 'which', 'th... | [-0.18850977511278222, 0.14022813012623894, -0.11577909530273506, 0.0636506387198876, -0.126538703055121, -0.19902521677514803, -0.02735146171679454, 0.348855951069189, -0.2796957785729319, -0.12404633918111878, 0.08628123248599877, -0.28956059229926073, -0.15699465725338085, 0.17109058920260786, -0.18664541307412685, ... |
710.4359 | Effect of Interactions on Molecular Fluxes and Fluctuations in the
Transport Across Membrane Channels | Transport of molecules across membrane channels is investigated theoretically
using exactly solvable one-dimensional discrete-state stochastic models. An
interaction between molecules and membrane pores is modeled via a set of
binding sites with different energies. It is shown that the interaction
potential strongly ... | cond-mat.soft cond-mat.stat-mech | transport of molecules across membrane channels is investigated theoretically using exactly solvable onedimensional discretestate stochastic models an interaction between molecules and membrane pores is modeled via a set of binding sites with different energies it is shown that the interaction potential strongly influe... | [['transport', 'of', 'molecules', 'across', 'membrane', 'channels', 'is', 'investigated', 'theoretically', 'using', 'exactly', 'solvable', 'onedimensional', 'discretestate', 'stochastic', 'models', 'an', 'interaction', 'between', 'molecules', 'and', 'membrane', 'pores', 'is', 'modeled', 'via', 'a', 'set', 'of', 'bindin... | [-0.14782735325525678, 0.21726282534842709, -0.02893100483204987, 0.09339238171220862, 0.017370398764824976, -0.14537058201631695, -0.012306477026005765, 0.37415384234543697, -0.2920122852137303, -0.2801447199494338, 0.03682722341864533, -0.29763372716273073, -0.12353284310995956, 0.15230392031167567, 0.051551955752074... |
710.436 | The Extended Emission of Ultracompact HII Regions: An Overview and New
Observations | Here we present a brief overview of UC HII regions with EE (UC HII+EE)
including our most recent effort aimed at searching for UC HII regions
associated with extended emission.
| astro-ph | here we present a brief overview of uc hii regions with ee uc hiiee including our most recent effort aimed at searching for uc hii regions associated with extended emission | [['here', 'we', 'present', 'a', 'brief', 'overview', 'of', 'uc', 'hii', 'regions', 'with', 'ee', 'uc', 'hiiee', 'including', 'our', 'most', 'recent', 'effort', 'aimed', 'at', 'searching', 'for', 'uc', 'hii', 'regions', 'associated', 'with', 'extended', 'emission']] | [-0.038467297780102695, -0.0004083933951012019, 0.06315888848219967, -0.0020791540115044035, -0.06397772740958066, -0.10454240035072997, 0.10702323318651781, 0.3998742630416206, -0.036800125730223954, -0.2992466834598574, 0.12367702132604759, -0.2899342032855955, -0.05670791215680797, 0.20750069316348124, 0.03561146009... |
710.4361 | QWalk: A Quantum Monte Carlo Program for Electronic Structure | We describe QWalk, a new computational package capable of performing Quantum
Monte Carlo electronic structure calculations for molecules and solids with
many electrons. We describe the structure of the program and its implementation
of Quantum Monte Carlo methods. It is open-source, licensed under the GPL, and
availa... | physics.comp-ph physics.atm-clus physics.chem-ph | we describe qwalk a new computational package capable of performing quantum monte carlo electronic structure calculations for molecules and solids with many electrons we describe the structure of the program and its implementation of quantum monte carlo methods it is opensource licensed under the gpl and available at t... | [['we', 'describe', 'qwalk', 'a', 'new', 'computational', 'package', 'capable', 'of', 'performing', 'quantum', 'monte', 'carlo', 'electronic', 'structure', 'calculations', 'for', 'molecules', 'and', 'solids', 'with', 'many', 'electrons', 'we', 'describe', 'the', 'structure', 'of', 'the', 'program', 'and', 'its', 'imple... | [-0.08851047868237776, 0.07458409662449769, -0.0792500744573772, 0.10222449517973206, -0.007687773920741736, -0.16829357842239095, 0.03357252726609837, 0.4605624092852368, -0.30002281186627405, -0.3247712076294656, 0.052204214894742355, -0.2979553980278034, -0.09125818427213851, 0.23657847339670887, 0.08647006795759879... |
710.4362 | Using generalized PowerFlux methods to estimate the parameters of
periodic gravitational waves | We investigate methods to estimate the parameters of the gravitational-wave
signal from a spinning neutron star using Fourier transformed segments of the
strain response from an interferometric detector. Estimating the parameters
from the power, we find generalizations of the PowerFlux method. Using
simulated ellipti... | gr-qc | we investigate methods to estimate the parameters of the gravitationalwave signal from a spinning neutron star using fourier transformed segments of the strain response from an interferometric detector estimating the parameters from the power we find generalizations of the powerflux method using simulated elliptically ... | [['we', 'investigate', 'methods', 'to', 'estimate', 'the', 'parameters', 'of', 'the', 'gravitationalwave', 'signal', 'from', 'a', 'spinning', 'neutron', 'star', 'using', 'fourier', 'transformed', 'segments', 'of', 'the', 'strain', 'response', 'from', 'an', 'interferometric', 'detector', 'estimating', 'the', 'parameters... | [-0.0504683272461133, 0.07969141897954293, -0.08829841836191275, 0.07706508584430112, -0.0253449992988916, -0.06836259708575466, 0.007752871606498957, 0.3589918200803154, -0.2544680023798719, -0.28359886454418304, 0.06702119854744523, -0.2978991953984779, -0.11778653160641518, 0.2518055328469285, -0.006592436721000601,... |
710.4363 | Search for Standard Model Higgs Bosons Produced in Association with W
Bosons | We report on the results of a search for standard model Higgs bosons produced
in association with W bosons from p-pbar collisions at root s = 1.96 TeV. The
search uses a data sample corresponding to approximately 1 fb-1 of integrated
luminosity. Events consistent with the W to l-nu and H to b-bbar signature are
selec... | hep-ex | we report on the results of a search for standard model higgs bosons produced in association with w bosons from ppbar collisions at root s 196 tev the search uses a data sample corresponding to approximately 1 fb1 of integrated luminosity events consistent with the w to lnu and h to bbbar signature are selected by trig... | [['we', 'report', 'on', 'the', 'results', 'of', 'a', 'search', 'for', 'standard', 'model', 'higgs', 'bosons', 'produced', 'in', 'association', 'with', 'w', 'bosons', 'from', 'ppbar', 'collisions', 'at', 'root', 's', '196', 'tev', 'the', 'search', 'uses', 'a', 'data', 'sample', 'corresponding', 'to', 'approximately', '1... | [-0.027618531862950612, 0.2102548426923903, -0.014268426464650756, 0.1258600773521184, -0.04327458433911019, -0.1454094559220331, 0.13079463764706986, 0.33983996746481704, -0.1681207525898176, -0.3607726093057705, -0.009140801846674464, -0.4066465673389735, 0.152157612257747, 0.15995513228193411, 0.07591892617482761, 0... |
710.4364 | Stellar Objects of Extragalactic Origin in the Galactic Halo | We identified globular clusters and field stars of extragalactic origin and
investigated their chemical, physical, and kinematical properties. This objects
as supposed was captured by the Galaxy at different times from debris of the
dwarf satellite galaxies disrupted by its tidal forces. The results are
follows. (1) ... | astro-ph | we identified globular clusters and field stars of extragalactic origin and investigated their chemical physical and kinematical properties this objects as supposed was captured by the galaxy at different times from debris of the dwarf satellite galaxies disrupted by its tidal forces the results are follows 1 the major... | [['we', 'identified', 'globular', 'clusters', 'and', 'field', 'stars', 'of', 'extragalactic', 'origin', 'and', 'investigated', 'their', 'chemical', 'physical', 'and', 'kinematical', 'properties', 'this', 'objects', 'as', 'supposed', 'was', 'captured', 'by', 'the', 'galaxy', 'at', 'different', 'times', 'from', 'debris',... | [-0.05795490069373621, 0.15687968249742223, -0.060725971565369775, 0.07551470475149166, -0.06644008678066, 0.02513346640337812, 0.05868105521286713, 0.37054093121458764, -0.1649927559613001, -0.3762220309005294, -0.0155189503439573, -0.31506471358018345, -0.003104194595321718, 0.17567563754630894, -0.06263306467116138,... |
710.4365 | The Three-body Force and the Tetraquark Interpretation of Light Scalar
Mesons | We study the possible tetraquark interpretation of light scalar meson states
$a_0(980)$, $f_0(980)$, $\kappa$, $\sigma$ within the framework of the
non-relativistic potential model. The wave functions of tetraquark states are
obtained in a space spanned by multiple Gaussian functions. We find that the
mass spectra of... | hep-ph | we study the possible tetraquark interpretation of light scalar meson states a_0980 f_0980 kappa sigma within the framework of the nonrelativistic potential model the wave functions of tetraquark states are obtained in a space spanned by multiple gaussian functions we find that the mass spectra of the light scalar meso... | [['we', 'study', 'the', 'possible', 'tetraquark', 'interpretation', 'of', 'light', 'scalar', 'meson', 'states', 'a_0980', 'f_0980', 'kappa', 'sigma', 'within', 'the', 'framework', 'of', 'the', 'nonrelativistic', 'potential', 'model', 'the', 'wave', 'functions', 'of', 'tetraquark', 'states', 'are', 'obtained', 'in', 'a'... | [-0.11796343781765592, 0.26401487359609666, -0.10804761473215028, 0.18008309328572802, -0.04314134332738566, -0.14076987441545458, 0.08085852520268284, 0.3471625660326374, -0.2010100053183818, -0.18323438540310338, -0.08341995131857484, -0.25812959266052155, -0.09317620106962289, 0.08876732041473302, 0.1275989333889708... |
710.4366 | Conformally parametrized surfaces associated with CP^(N-1) sigma models | Two-dimensional conformally parametrized surfaces immersed in the su(N)
algebra are investigated. The focus is on surfaces parametrized by solutions of
the equations for the CP^(N-1) sigma model. The Lie-point symmetries of the
CP^(N-1) model are computed for arbitrary N. The Weierstrass formula for
immersion is dete... | math.DG | twodimensional conformally parametrized surfaces immersed in the sun algebra are investigated the focus is on surfaces parametrized by solutions of the equations for the cpn1 sigma model the liepoint symmetries of the cpn1 model are computed for arbitrary n the weierstrass formula for immersion is determined and an exp... | [['twodimensional', 'conformally', 'parametrized', 'surfaces', 'immersed', 'in', 'the', 'sun', 'algebra', 'are', 'investigated', 'the', 'focus', 'is', 'on', 'surfaces', 'parametrized', 'by', 'solutions', 'of', 'the', 'equations', 'for', 'the', 'cpn1', 'sigma', 'model', 'the', 'liepoint', 'symmetries', 'of', 'the', 'cpn... | [-0.15404670168848142, 0.09468014557838299, -0.06248918927714998, 0.08538742937937217, -0.05019851097756106, -0.13126246460268032, -0.05673436327640008, 0.3366138713839261, -0.23059318951614524, -0.2667344982897782, 0.08032266714043268, -0.28475447871087056, -0.17602727490720219, 0.20221523673516575, -0.081280075560283... |
710.4367 | A nuclear magnetic resonance spectrometer for operation around 1 MHz
with a sub 10 mK noise temperature based on a two stage dc SQUID | We have developed a nuclear magnetic resonance spectrometer with a series
tuned input circuit for measurements on samples at millikelvin temperatures
based on an integrated two-stage superconducting quantum interference device
current sensor, with an energy sensitivty e = 26 +/-1 h when operated at 1.4K.
To maximise ... | cond-mat.supr-con | we have developed a nuclear magnetic resonance spectrometer with a series tuned input circuit for measurements on samples at millikelvin temperatures based on an integrated twostage superconducting quantum interference device current sensor with an energy sensitivty e 26 1 h when operated at 14k to maximise the sensiti... | [['we', 'have', 'developed', 'a', 'nuclear', 'magnetic', 'resonance', 'spectrometer', 'with', 'a', 'series', 'tuned', 'input', 'circuit', 'for', 'measurements', 'on', 'samples', 'at', 'millikelvin', 'temperatures', 'based', 'on', 'an', 'integrated', 'twostage', 'superconducting', 'quantum', 'interference', 'device', 'c... | [-0.10635698918090428, 0.19179621783059173, 0.013370623735222712, -0.04868655024295293, -0.012459083975663462, -0.22933726548895383, 0.08146283436268206, 0.39717785185835897, -0.21662567330646393, -0.37466492827583864, 0.05251137821740715, -0.3147378360301039, 0.00403880186885306, 0.25192232834609246, -0.02463482500243... |
710.4368 | Topological Hochschild homology of l and ko | We calculate the integral homotopy groups of THH(l) at any prime and of
THH(ko) at p=2, where l is the Adams summand of the connective complex p-local
K-theory spectrum and ko is the connective real K-theory spectrum.
| math.AT math.KT | we calculate the integral homotopy groups of thhl at any prime and of thhko at p2 where l is the adams summand of the connective complex plocal ktheory spectrum and ko is the connective real ktheory spectrum | [['we', 'calculate', 'the', 'integral', 'homotopy', 'groups', 'of', 'thhl', 'at', 'any', 'prime', 'and', 'of', 'thhko', 'at', 'p2', 'where', 'l', 'is', 'the', 'adams', 'summand', 'of', 'the', 'connective', 'complex', 'plocal', 'ktheory', 'spectrum', 'and', 'ko', 'is', 'the', 'connective', 'real', 'ktheory', 'spectrum']... | [-0.24689016794519766, 0.019733692572585174, -0.11800277799900089, 0.11696768156252801, -0.07491529571956822, -0.18215404748916625, -0.05710381261472191, 0.3141172544764621, -0.40897170534091337, -0.2339743064184274, 0.08056370657203453, -0.23521905046821173, -0.12068721452461821, 0.17980884058134897, -0.13150623791984... |
710.4369 | Sensitivity and parameter-estimation precision for alternate LISA
configurations | We describe a simple framework to assess the LISA scientific performance
(more specifically, its sensitivity and expected parameter-estimation precision
for prescribed gravitational-wave signals) under the assumption of failure of
one or two inter-spacecraft laser measurements (links) and of one to four
intra-spacecr... | gr-qc | we describe a simple framework to assess the lisa scientific performance more specifically its sensitivity and expected parameterestimation precision for prescribed gravitationalwave signals under the assumption of failure of one or two interspacecraft laser measurements links and of one to four intraspacecraft laser m... | [['we', 'describe', 'a', 'simple', 'framework', 'to', 'assess', 'the', 'lisa', 'scientific', 'performance', 'more', 'specifically', 'its', 'sensitivity', 'and', 'expected', 'parameterestimation', 'precision', 'for', 'prescribed', 'gravitationalwave', 'signals', 'under', 'the', 'assumption', 'of', 'failure', 'of', 'one'... | [-0.12338328008456284, 0.11265745758151953, -0.02704004175458876, 0.07091848573686066, -0.031047729031753638, -0.12876913924207953, 0.0538021527462229, 0.3893630527665899, -0.20322380904408713, -0.3263609708356027, 0.11283828721119923, -0.28034199787569897, -0.1000108024717549, 0.2575650317707069, -0.017323292144316715... |
710.437 | Gamma-Ray Bursts May Be Biased Tracers of Star Formation | Based on a simulation of galaxy formation in the standard cosmological model,
we suggest that a consistent picture for Gamma-Ray Bursts and star formation
may be found that is in broad agreement with observations: GRBs preferentially
form in low metallicity environments and in galaxies substantially less
luminous tha... | astro-ph | based on a simulation of galaxy formation in the standard cosmological model we suggest that a consistent picture for gammaray bursts and star formation may be found that is in broad agreement with observations grbs preferentially form in low metallicity environments and in galaxies substantially less luminous that l w... | [['based', 'on', 'a', 'simulation', 'of', 'galaxy', 'formation', 'in', 'the', 'standard', 'cosmological', 'model', 'we', 'suggest', 'that', 'a', 'consistent', 'picture', 'for', 'gammaray', 'bursts', 'and', 'star', 'formation', 'may', 'be', 'found', 'that', 'is', 'in', 'broad', 'agreement', 'with', 'observations', 'grbs... | [-0.07382100100961102, 0.11416896163165326, -0.051522494744143034, 0.1484204977264124, -0.10131433799473538, -0.08003803181507793, 0.06189373692070119, 0.4432170334592706, -0.09987854425505292, -0.3332137859380636, 0.02813932614507856, -0.2520704154845052, -0.055086907495546046, 0.2663747229959926, -0.01966036100810790... |
710.4371 | Optical Absorption Study by Ab initio Downfolding Approach: Application
to GaAs | We examine whether essence and quantitative aspects of electronic excitation
spectra are correctly captured by an effective low-energy model constructed
from an {\em ab initio} downfolding scheme. A global electronic structure is
first calculated by {\em ab initio} density-functional calculations with the
generalized... | cond-mat.str-el cond-mat.mtrl-sci | we examine whether essence and quantitative aspects of electronic excitation spectra are correctly captured by an effective lowenergy model constructed from an em ab initio downfolding scheme a global electronic structure is first calculated by em ab initio densityfunctional calculations with the generalized gradient a... | [['we', 'examine', 'whether', 'essence', 'and', 'quantitative', 'aspects', 'of', 'electronic', 'excitation', 'spectra', 'are', 'correctly', 'captured', 'by', 'an', 'effective', 'lowenergy', 'model', 'constructed', 'from', 'an', 'em', 'ab', 'initio', 'downfolding', 'scheme', 'a', 'global', 'electronic', 'structure', 'is... | [-0.07203757858780377, 0.09337573439278297, -0.09920197090764037, 0.12046078854815706, 0.03347076436997775, -0.12401772773112445, 0.07066148872391376, 0.3748509652803049, -0.24470245683675304, -0.3151787763242336, -0.01244646271225065, -0.29337385269155836, -0.16309653115445946, 0.11900726283407387, 0.09047189449672313... |
710.4372 | Prediction Space Weather Using an Asymmetric Cone Model for Halo CMEs | Halo coronal mass ejections (HCMEs) are responsible of the most severe
geomagnetic storms. A prediction of their geoeffectiveness and travel time to
Earth's vicinity is crucial to forecast space weather.
Unfortunately coronagraphic observations are subjected to projection effects
and do not provide true characteris... | astro-ph | halo coronal mass ejections hcmes are responsible of the most severe geomagnetic storms a prediction of their geoeffectiveness and travel time to earths vicinity is crucial to forecast space weather unfortunately coronagraphic observations are subjected to projection effects and do not provide true characteristics of c... | [['halo', 'coronal', 'mass', 'ejections', 'hcmes', 'are', 'responsible', 'of', 'the', 'most', 'severe', 'geomagnetic', 'storms', 'a', 'prediction', 'of', 'their', 'geoeffectiveness', 'and', 'travel', 'time', 'to', 'earths', 'vicinity', 'is', 'crucial', 'to', 'forecast', 'space', 'weather', 'unfortunately', 'coronagraph... | [-0.09657491775515088, 0.21738718427391807, -0.01585548477974741, 0.1109472077516635, -0.07263817730271359, -0.026839301516947738, 0.030027773975646193, 0.4073028227885383, -0.18690297685148888, -0.39957975619302616, 0.12589646388868372, -0.2263183223430312, -0.12606580404863849, 0.23844691695574072, -0.104436322130657... |
710.4373 | Is Strangeness Still Strange at the LHC? | Strangeness production is calculated in a pQCD-based model (including nuclear
effects) in the high transverse momentum sector, where pQCD is expected to work
well. We investigate pion, kaon, proton and lambda production in pp and
heavy-ion collisions. Parton energy loss in AA collisions is taken into
account. We comp... | hep-ph | strangeness production is calculated in a pqcdbased model including nuclear effects in the high transverse momentum sector where pqcd is expected to work well we investigate pion kaon proton and lambda production in pp and heavyion collisions parton energy loss in aa collisions is taken into account we compare stranget... | [['strangeness', 'production', 'is', 'calculated', 'in', 'a', 'pqcdbased', 'model', 'including', 'nuclear', 'effects', 'in', 'the', 'high', 'transverse', 'momentum', 'sector', 'where', 'pqcd', 'is', 'expected', 'to', 'work', 'well', 'we', 'investigate', 'pion', 'kaon', 'proton', 'and', 'lambda', 'production', 'in', 'pp... | [-0.0002556018971113695, 0.26317583872005346, -0.14311807681806385, 0.19214735467685387, 0.012543665974711378, -0.11022485246972388, -0.029968804203801686, 0.34787777081494115, -0.17090300214994286, -0.23073439376635685, -0.0959904606298854, -0.37800932098438755, 0.11963005906695293, 0.11012821646355507, 0.101077866740... |
710.4374 | The IMF of Extremely Metal-Poor Stars and the Probe into the
Star-Formation Process of the Milky Way | We discuss the star formation history of the Galaxy, based on the
observations of extremely metal-poor stars (EMP) in the Galactic halo, to gain
an insight into the evolution and structure formation in the early universe.
The initialmass function (IMF) of EMP stars is derived from the observed
fraction of carbon-enha... | astro-ph | we discuss the star formation history of the galaxy based on the observations of extremely metalpoor stars emp in the galactic halo to gain an insight into the evolution and structure formation in the early universe the initialmass function imf of emp stars is derived from the observed fraction of carbonenhanced exp ce... | [['we', 'discuss', 'the', 'star', 'formation', 'history', 'of', 'the', 'galaxy', 'based', 'on', 'the', 'observations', 'of', 'extremely', 'metalpoor', 'stars', 'emp', 'in', 'the', 'galactic', 'halo', 'to', 'gain', 'an', 'insight', 'into', 'the', 'evolution', 'and', 'structure', 'formation', 'in', 'the', 'early', 'unive... | [-0.0483282524596852, 0.11330816765168072, -0.11505690625367257, 0.12254689875930452, -0.08635161389113188, 0.015535455715293304, 0.08095063839692813, 0.3518702113380035, -0.1870643970866998, -0.3699640058267575, -0.012733764799001316, -0.27876686099259995, -0.07492695068690526, 0.1764786415028935, -0.03160159145601285... |
710.4375 | Bergman kernels and equilibrium measures for line bundles over
projective manifolds | Let L be a holomorphic line bundle over a compact complex projective
Hermitian manifold X. Any fixed smooth hermitian metric h on L induces a
Hilbert space structure on the space of global holomorphic sections with values
in the k th tensor power of L. In this paper various convergence results are
obtained for the co... | math.CV math.DG | let l be a holomorphic line bundle over a compact complex projective hermitian manifold x any fixed smooth hermitian metric h on l induces a hilbert space structure on the space of global holomorphic sections with values in the k th tensor power of l in this paper various convergence results are obtained for the corres... | [['let', 'l', 'be', 'a', 'holomorphic', 'line', 'bundle', 'over', 'a', 'compact', 'complex', 'projective', 'hermitian', 'manifold', 'x', 'any', 'fixed', 'smooth', 'hermitian', 'metric', 'h', 'on', 'l', 'induces', 'a', 'hilbert', 'space', 'structure', 'on', 'the', 'space', 'of', 'global', 'holomorphic', 'sections', 'wit... | [-0.17223819532973064, 0.05370143225138827, -0.039948013027658665, 0.05666455767588712, -0.06320026897157666, -0.11384887570313301, -0.0043842569772008224, 0.3417652301288333, -0.2773355762754758, -0.19782106836988445, 0.11144185355087428, -0.2504680431672338, -0.12550837040530988, 0.2100681693809309, -0.07051975644931... |
710.4376 | Castelnuovo-Mumford regularity and reduction number of smooth monomial
curves | We compare, for smooth monomial projective curves, the Castel- nuovo-Mumford
regularity and the reduction number; we present an example where these two
numbers differ. However, we show they coin- cide for a certain class of
monomial curves. Furthermore, for smooth monomial curves we prove an inequality
which is stron... | math.AC | we compare for smooth monomial projective curves the castel nuovomumford regularity and the reduction number we present an example where these two numbers differ however we show they coin cide for a certain class of monomial curves furthermore for smooth monomial curves we prove an inequality which is stronger than the... | [['we', 'compare', 'for', 'smooth', 'monomial', 'projective', 'curves', 'the', 'castel', 'nuovomumford', 'regularity', 'and', 'the', 'reduction', 'number', 'we', 'present', 'an', 'example', 'where', 'these', 'two', 'numbers', 'differ', 'however', 'we', 'show', 'they', 'coin', 'cide', 'for', 'a', 'certain', 'class', 'of... | [-0.1740438721522137, 0.0696822084466004, -0.0769091736421817, 0.10865717758295229, -0.0622708436222402, -0.19780806194197526, -0.046823206034282014, 0.35243267600459083, -0.3202985139494693, -0.21326417089612396, 0.09713996434153092, -0.2623534823155583, -0.1501797371785398, 0.30888422105582086, -0.1505109061556006, 0... |
710.4377 | Deformation of Dijkgraaf-Vafa Relation via Spontaneously Broken N=2
Supersymmetry II | We consider the matter induced part of the effective superpotential of N=2,
U(N) gauge model in which N=2 supersymmetry is spontaneously broken to N=1, by
using the properties of the chiral ring and the generalized Konishi anomaly
equations derived in our previous paper arXiv:0704.1060. It is shown that the
effective... | hep-th | we consider the matter induced part of the effective superpotential of n2 un gauge model in which n2 supersymmetry is spontaneously broken to n1 by using the properties of the chiral ring and the generalized konishi anomaly equations derived in our previous paper arxiv07041060 it is shown that the effective superpotent... | [['we', 'consider', 'the', 'matter', 'induced', 'part', 'of', 'the', 'effective', 'superpotential', 'of', 'n2', 'un', 'gauge', 'model', 'in', 'which', 'n2', 'supersymmetry', 'is', 'spontaneously', 'broken', 'to', 'n1', 'by', 'using', 'the', 'properties', 'of', 'the', 'chiral', 'ring', 'and', 'the', 'generalized', 'koni... | [-0.13574945283416695, 0.16428887563810315, -0.043847840015209756, 0.0490044802943473, -0.050214478948135986, -0.10864412657178517, -0.05107250307875527, 0.2779252901849038, -0.2380689399598061, -0.3017152287768868, 0.08751608245623878, -0.28164403472658034, -0.20359636959180516, 0.06452883866325654, -0.012094379437841... |
710.4378 | On The Pomeron at Large 't Hooft Coupling | We begin the process of unitarizing the Pomeron at large 't Hooft coupling.
We do so first in the conformal regime, which applies to good accuracy to a
number of real and toy problems in QCD. We rewrite the conformal Pomeron in the
$J$-plane and transverse position space, and then work out the eikonal
approximation t... | hep-th | we begin the process of unitarizing the pomeron at large t hooft coupling we do so first in the conformal regime which applies to good accuracy to a number of real and toy problems in qcd we rewrite the conformal pomeron in the jplane and transverse position space and then work out the eikonal approximation to multiple... | [['we', 'begin', 'the', 'process', 'of', 'unitarizing', 'the', 'pomeron', 'at', 'large', 't', 'hooft', 'coupling', 'we', 'do', 'so', 'first', 'in', 'the', 'conformal', 'regime', 'which', 'applies', 'to', 'good', 'accuracy', 'to', 'a', 'number', 'of', 'real', 'and', 'toy', 'problems', 'in', 'qcd', 'we', 'rewrite', 'the'... | [-0.11982171574734736, 0.1334543620766855, -0.10093141856960693, 0.12769697722138137, -0.11802297928451755, -0.12796374289102333, 0.04347899058958256, 0.3424525861411767, -0.21742273373448096, -0.22993414527411724, 0.035405109712290904, -0.2808219599414029, -0.14997744388596781, 0.13414911200701216, 0.00291612776007156... |
710.4379 | Chemical freeze-out temperature in hydrodynamical description of Au+Au
collisions at sqrt(s_NN) = 200 GeV | We study the effect of separate chemical and kinetic freeze-outs to the ideal
hydrodynamical flow in Au+Au collisions at RHIC (sqrt(s_NN) = 200 GeV energy).
Unlike in earlier studies we explore how these effects can be counteracted by
changes in the initial state of the hydrodynamical evolution. We conclude that
the ... | nucl-th hep-ph nucl-ex | we study the effect of separate chemical and kinetic freezeouts to the ideal hydrodynamical flow in auau collisions at rhic sqrts_nn 200 gev energy unlike in earlier studies we explore how these effects can be counteracted by changes in the initial state of the hydrodynamical evolution we conclude that the reproduction... | [['we', 'study', 'the', 'effect', 'of', 'separate', 'chemical', 'and', 'kinetic', 'freezeouts', 'to', 'the', 'ideal', 'hydrodynamical', 'flow', 'in', 'auau', 'collisions', 'at', 'rhic', 'sqrts_nn', '200', 'gev', 'energy', 'unlike', 'in', 'earlier', 'studies', 'we', 'explore', 'how', 'these', 'effects', 'can', 'be', 'co... | [-0.08619839585510881, 0.2476086368505645, -0.14527205227118895, 0.10963094193583692, -0.027037831777285082, -0.1154093803286985, -0.0028167886303840425, 0.3467231654804053, -0.24451831456889786, -0.3318158012088828, -0.02053778843979872, -0.31630156709863916, 0.07855999679688509, 0.14802003307561354, 0.020922377241287... |
710.438 | Studies of penguin dominated B decays | We present measurements on penguin dominated B decays which are sensitive to
new physics, such as CP-violation parameters and branching fractions in $b \to
s q\bar{q}$ and $b \to d q\bar{q}$ gluonic and radiative decays using a large
sample of $B\bar{B}$ pairs recorded at the $\Upsilon(4S)$ resonance with the
Belle d... | hep-ex | we present measurements on penguin dominated b decays which are sensitive to new physics such as cpviolation parameters and branching fractions in b to s qbarq and b to d qbarq gluonic and radiative decays using a large sample of bbarb pairs recorded at the upsilon4s resonance with the belle detector at the kekb asymme... | [['we', 'present', 'measurements', 'on', 'penguin', 'dominated', 'b', 'decays', 'which', 'are', 'sensitive', 'to', 'new', 'physics', 'such', 'as', 'cpviolation', 'parameters', 'and', 'branching', 'fractions', 'in', 'b', 'to', 's', 'qbarq', 'and', 'b', 'to', 'd', 'qbarq', 'gluonic', 'and', 'radiative', 'decays', 'using'... | [-0.04154086576730559, 0.2705778833639262, -0.02707271307610489, 0.10486424896577053, -0.09118250476453325, -0.1857263949651528, 0.0808167396843883, 0.26590389372973605, -0.1542925468870792, -0.2469885879164112, -0.09046258369725647, -0.4493113458798877, 0.10708454607761111, 0.12404782501258084, 0.1511123971130442, 0.1... |
710.4381 | Solution and Asymptotic Behavior for a Nonlocal Coupled System of
Reaction-Diffusion | This paper concerns with existence, uniqueness and asymptotic behavior of the
solutions for a nonlocal coupled system of reaction-diffusion. We prove the
existence and uniqueness of weak solutions by the Faedo-Galerkin method and
exponential decay of solutions by the classic energy method. We improve the
results obta... | math.AP | this paper concerns with existence uniqueness and asymptotic behavior of the solutions for a nonlocal coupled system of reactiondiffusion we prove the existence and uniqueness of weak solutions by the faedogalerkin method and exponential decay of solutions by the classic energy method we improve the results obtained by... | [['this', 'paper', 'concerns', 'with', 'existence', 'uniqueness', 'and', 'asymptotic', 'behavior', 'of', 'the', 'solutions', 'for', 'a', 'nonlocal', 'coupled', 'system', 'of', 'reactiondiffusion', 'we', 'prove', 'the', 'existence', 'and', 'uniqueness', 'of', 'weak', 'solutions', 'by', 'the', 'faedogalerkin', 'method', ... | [-0.14857700801101223, -0.0067650485093352095, -0.08369111561152184, 0.043977106696572794, -0.009136273204509554, -0.14609994418148337, 0.03561232359638309, 0.2444224508222321, -0.24950402538324223, -0.2567866630370504, 0.15765989172384784, -0.28173335583816317, -0.16384978749957899, 0.19614971711717802, -0.01980912075... |
710.4382 | Isotopies of Legendrian 1-knots and Legendrian 2-tori | We construct a Legendrian 2-torus in the 1-jet space of $S^1\times\R$ (or of
$\R^2$) from a loop of Legendrian knots in the 1-jet space of $\R$. The
differential graded algebra (DGA) for the Legendrian contact homology of the
torus is explicitly computed in terms of the DGA of the knot and the monodromy
operator of t... | math.SG | we construct a legendrian 2torus in the 1jet space of s1timesr or of r2 from a loop of legendrian knots in the 1jet space of r the differential graded algebra dga for the legendrian contact homology of the torus is explicitly computed in terms of the dga of the knot and the monodromy operator of the loop the contact ho... | [['we', 'construct', 'a', 'legendrian', '2torus', 'in', 'the', '1jet', 'space', 'of', 's1timesr', 'or', 'of', 'r2', 'from', 'a', 'loop', 'of', 'legendrian', 'knots', 'in', 'the', '1jet', 'space', 'of', 'r', 'the', 'differential', 'graded', 'algebra', 'dga', 'for', 'the', 'legendrian', 'contact', 'homology', 'of', 'the'... | [-0.27187559091817093, 0.027539942471776158, -0.0849637314749998, 0.07138011372489927, -0.15045444773568306, -0.20156488215798163, -0.052681604817735206, 0.330128555156989, -0.32562090492865536, -0.24197818175889552, 0.08328863771021133, -0.22126861295521394, -0.17919463559701398, 0.17077819092628488, -0.17339771284605... |
710.4383 | Some matrices associated with the split decomposition for a Q-polynomial
distance-regular graph | We consider a $Q$-polynomial distance-regular graph $\Gamma$ with vertex set
$X$ and diameter $D \geq 3$. For $\mu, \nu \in \lbrace \downarrow, \uparrow
\rbrace$ we define a direct sum decomposition of the standard module $V=\C X$,
called the $(\mu,\nu)$--split decomposition. For this decomposition we compute
the com... | math.CO | we consider a qpolynomial distanceregular graph gamma with vertex set x and diameter d geq 3 for mu nu in lbrace downarrow uparrow rbrace we define a direct sum decomposition of the standard module vc x called the munusplit decomposition for this decomposition we compute the complex conjugate and transpose of the assoc... | [['we', 'consider', 'a', 'qpolynomial', 'distanceregular', 'graph', 'gamma', 'with', 'vertex', 'set', 'x', 'and', 'diameter', 'd', 'geq', '3', 'for', 'mu', 'nu', 'in', 'lbrace', 'downarrow', 'uparrow', 'rbrace', 'we', 'define', 'a', 'direct', 'sum', 'decomposition', 'of', 'the', 'standard', 'module', 'vc', 'x', 'called... | [-0.15724988098013892, 0.10748981895997295, 0.014836054620626446, -0.00791174358024887, -0.06473517747837508, -0.19866394460614298, 0.009155026585986353, 0.3627232542669732, -0.3510053299673616, -0.14949847911229383, 0.07813282762032181, -0.31589960622001595, -0.11223268697567744, 0.09980958445342131, -0.06956201351298... |
710.4384 | Dark Matter, Dark Energy and Rotation Curves | Models for DM are invoked with various density distributions, to account for
flat rotation curves of galaxies. The effect of DE on these profiles for large
galaxies and clusters are also studied. The rotation curves are shown to dip at
a particular distance, when the effect of DE became significant.
| astro-ph | models for dm are invoked with various density distributions to account for flat rotation curves of galaxies the effect of de on these profiles for large galaxies and clusters are also studied the rotation curves are shown to dip at a particular distance when the effect of de became significant | [['models', 'for', 'dm', 'are', 'invoked', 'with', 'various', 'density', 'distributions', 'to', 'account', 'for', 'flat', 'rotation', 'curves', 'of', 'galaxies', 'the', 'effect', 'of', 'de', 'on', 'these', 'profiles', 'for', 'large', 'galaxies', 'and', 'clusters', 'are', 'also', 'studied', 'the', 'rotation', 'curves', ... | [-0.10043628187617287, 0.12438103828579188, -0.1316949110571295, 0.1705967536009848, -0.073704595095478, -0.08055169415660203, -0.060454818047583105, 0.4097576539218426, -0.16376947773620487, -0.3663795737619512, 0.054301444198936226, -0.2866127687692642, -0.05895897816866636, 0.2603087853116449, -0.04021841755136848, ... |
710.4385 | Non-measurable automorphisms of Lie groups relative to the real- and
non-archimedean-valued measures | In this work the problem about an existence of non-measurable automorphisms
of Lie groups finite and as well infinite dimensional over the field of real
numbers and also over the non-archimedean local fields is investigated.
Non-measurability of automorphisms is considered relative to real-valued
measures and also me... | math.FA math.AT | in this work the problem about an existence of nonmeasurable automorphisms of lie groups finite and as well infinite dimensional over the field of real numbers and also over the nonarchimedean local fields is investigated nonmeasurability of automorphisms is considered relative to realvalued measures and also measures ... | [['in', 'this', 'work', 'the', 'problem', 'about', 'an', 'existence', 'of', 'nonmeasurable', 'automorphisms', 'of', 'lie', 'groups', 'finite', 'and', 'as', 'well', 'infinite', 'dimensional', 'over', 'the', 'field', 'of', 'real', 'numbers', 'and', 'also', 'over', 'the', 'nonarchimedean', 'local', 'fields', 'is', 'invest... | [-0.17135193943977356, 0.10066925870521484, -0.10739304434943509, 0.06215486716019449, -0.06439595280045812, -0.044547154241568084, 0.0009100104791003388, 0.3676271258139765, -0.2942800157969551, -0.23501040716353175, 0.12236530168961685, -0.22266634081962047, -0.1271313121935425, 0.23848498679165328, -0.10911226415305... |
710.4386 | Quantum stabilization of Z-strings, a status report on D=3+1 dimensions | We investigate an extension to the phase shift formalism for calculating
one-loop determinants. This extension is motivated by requirements of the
computation of Z-string quantum energies in D=3+1 dimensions. A subtlety that
seems to imply that the vacuum polarization diagram in this formalism is
(erroneously) finite... | hep-th | we investigate an extension to the phase shift formalism for calculating oneloop determinants this extension is motivated by requirements of the computation of zstring quantum energies in d31 dimensions a subtlety that seems to imply that the vacuum polarization diagram in this formalism is erroneously finite is thorou... | [['we', 'investigate', 'an', 'extension', 'to', 'the', 'phase', 'shift', 'formalism', 'for', 'calculating', 'oneloop', 'determinants', 'this', 'extension', 'is', 'motivated', 'by', 'requirements', 'of', 'the', 'computation', 'of', 'zstring', 'quantum', 'energies', 'in', 'd31', 'dimensions', 'a', 'subtlety', 'that', 'se... | [-0.14612227556656818, 0.18080952399848646, -0.09822503275865195, 0.12402040961825726, -0.038153599947690964, -0.07661569674442313, 0.0377094637678594, 0.34026969011340824, -0.19677827053950453, -0.24947303183832947, 0.046896060667361836, -0.22507268859415638, -0.17299061702868465, 0.1183734821079641, -0.05702398916913... |
710.4387 | Oxygen abundance methods in the SDSS: view from modern statistics | Our purpose is to find which is the most reliable one among various oxygen
abundance determination methods. We will test the validity of several different
oxygen abundance determination methods using methods of modern statistics.
These methods include Bayesian analysis and information scoring. We will
analyze a sampl... | astro-ph | our purpose is to find which is the most reliable one among various oxygen abundance determination methods we will test the validity of several different oxygen abundance determination methods using methods of modern statistics these methods include bayesian analysis and information scoring we will analyze a sample of ... | [['our', 'purpose', 'is', 'to', 'find', 'which', 'is', 'the', 'most', 'reliable', 'one', 'among', 'various', 'oxygen', 'abundance', 'determination', 'methods', 'we', 'will', 'test', 'the', 'validity', 'of', 'several', 'different', 'oxygen', 'abundance', 'determination', 'methods', 'using', 'methods', 'of', 'modern', 's... | [0.009061067986856719, 0.010972360241805963, -0.08610484959664429, 0.09538983699723272, -0.0693269130339324, -0.12467039011976426, 0.04014885249090897, 0.43360151502950367, -0.16476510673728742, -0.3464276832132637, 0.08700556648304911, -0.32194897297556235, -0.07771864764772024, 0.2608522554654865, -0.0408365171533196... |
710.4388 | Resolving the wave-vector and the refractive index from the coefficient
of reflectance | We resolve the existing controversy concerning the selection of the sign of
the normal-to-the-interface component of the wave-vector $k_z$ of an
electromagnetic wave in an active (gain) medium. Our method exploits the fact
that no ambiguity exists in the case of a {\em film} of the active medium since
its coefficient... | physics.optics | we resolve the existing controversy concerning the selection of the sign of the normaltotheinterface component of the wavevector k_z of an electromagnetic wave in an active gain medium our method exploits the fact that no ambiguity exists in the case of a em film of the active medium since its coefficient of reflectanc... | [['we', 'resolve', 'the', 'existing', 'controversy', 'concerning', 'the', 'selection', 'of', 'the', 'sign', 'of', 'the', 'normaltotheinterface', 'component', 'of', 'the', 'wavevector', 'k_z', 'of', 'an', 'electromagnetic', 'wave', 'in', 'an', 'active', 'gain', 'medium', 'our', 'method', 'exploits', 'the', 'fact', 'that... | [-0.2002035462508727, 0.11950832644757123, -0.0870111751917404, 0.013280787948067732, -0.08775273205462805, -0.0538934703853903, 0.051845360070841444, 0.399262881136893, -0.2725772837215324, -0.26597250735905675, 0.07335533895565811, -0.26337316903986574, -0.14832819200399303, 0.16030420983191004, -0.004468644311478765... |
710.4389 | Dynamic importance sampling for queueing networks | Importance sampling is a technique that is commonly used to speed up Monte
Carlo simulation of rare events. However, little is known regarding the design
of efficient importance sampling algorithms in the context of queueing
networks. The standard approach, which simulates the system using an a priori
fixed change of... | math.PR | importance sampling is a technique that is commonly used to speed up monte carlo simulation of rare events however little is known regarding the design of efficient importance sampling algorithms in the context of queueing networks the standard approach which simulates the system using an a priori fixed change of measu... | [['importance', 'sampling', 'is', 'a', 'technique', 'that', 'is', 'commonly', 'used', 'to', 'speed', 'up', 'monte', 'carlo', 'simulation', 'of', 'rare', 'events', 'however', 'little', 'is', 'known', 'regarding', 'the', 'design', 'of', 'efficient', 'importance', 'sampling', 'algorithms', 'in', 'the', 'context', 'of', 'q... | [-0.11163830779858269, 0.03909412632745241, -0.04869261517241183, 0.15003792847063677, -0.05061489027219876, -0.1683924232234454, 0.10199178662151098, 0.38684265637615073, -0.287355255555465, -0.3325414527660339, 0.11664360105755299, -0.25037571016906035, -0.19090801471611485, 0.21123963620953468, -0.10789419259203391,... |
710.439 | Chirality-Biased Point Defects Dynamics on a Disclination Line in a
Nematic Liquid Crystal | Chiral additives in the nematic liquid crystal can alter the dynamics of
point defects moving on a disclination line. They exert a constant force on
defects, leading to the bimodal distribution of distances between them at long
times. The evolution of the system of defects in the presence of chiral
additives provides... | cond-mat.soft | chiral additives in the nematic liquid crystal can alter the dynamics of point defects moving on a disclination line they exert a constant force on defects leading to the bimodal distribution of distances between them at long times the evolution of the system of defects in the presence of chiral additives provides a ve... | [['chiral', 'additives', 'in', 'the', 'nematic', 'liquid', 'crystal', 'can', 'alter', 'the', 'dynamics', 'of', 'point', 'defects', 'moving', 'on', 'a', 'disclination', 'line', 'they', 'exert', 'a', 'constant', 'force', 'on', 'defects', 'leading', 'to', 'the', 'bimodal', 'distribution', 'of', 'distances', 'between', 'th... | [-0.17385053315088836, 0.1665778924164217, -0.0856453047791889, -0.035734870949988506, 0.020471227701343256, -0.0984664117199702, 0.061813896937122775, 0.36494030717999565, -0.24541620303526385, -0.264558113953355, 0.019987026910904215, -0.33150376946827687, -0.12104746476328428, 0.09467987843079988, 0.0278085585375991... |
710.4391 | Scattering of sine-Gordon Breathers on Potential Wells | We analyse the scattering of sine-Gordon breathers on a square potential
well. We show that the scattering process depends not only on the vibration
frequency of the breather and its incoming speed but also on its phase as well
as the depth and width of the well. We show that the breather can pass through
the well an... | cond-mat.other | we analyse the scattering of sinegordon breathers on a square potential well we show that the scattering process depends not only on the vibration frequency of the breather and its incoming speed but also on its phase as well as the depth and width of the well we show that the breather can pass through the well and exi... | [['we', 'analyse', 'the', 'scattering', 'of', 'sinegordon', 'breathers', 'on', 'a', 'square', 'potential', 'well', 'we', 'show', 'that', 'the', 'scattering', 'process', 'depends', 'not', 'only', 'on', 'the', 'vibration', 'frequency', 'of', 'the', 'breather', 'and', 'its', 'incoming', 'speed', 'but', 'also', 'on', 'its'... | [-0.06876821951009333, 0.1530717951904871, -0.08829864324272975, 0.0878931740365458, -0.06643113284776717, -0.12057329848327715, 0.06611216181646222, 0.3960811012465021, -0.3262769938811012, -0.25273449940849907, 0.1678623945027104, -0.28193131973562036, -0.15110089850369032, 0.2223480652835544, 0.024827059098195447, 0... |
710.4392 | Kernel estimation of Greek weights by parameter randomization | A Greek weight associated to a parameterized random variable $Z(\lambda)$ is
a random variable $\pi$ such that
$\nabla_{\lambda}E[\phi(Z(\lambda))]=E[\phi(Z(\lambda))\pi]$ for any function
$\phi$. The importance of the set of Greek weights for the purpose of Monte
Carlo simulations has been highlighted in the recent ... | math.PR | a greek weight associated to a parameterized random variable zlambda is a random variable pi such that nabla_lambdaephizlambdaephizlambdapi for any function phi the importance of the set of greek weights for the purpose of monte carlo simulations has been highlighted in the recent literature our main concern in this pa... | [['a', 'greek', 'weight', 'associated', 'to', 'a', 'parameterized', 'random', 'variable', 'zlambda', 'is', 'a', 'random', 'variable', 'pi', 'such', 'that', 'nabla_lambdaephizlambdaephizlambdapi', 'for', 'any', 'function', 'phi', 'the', 'importance', 'of', 'the', 'set', 'of', 'greek', 'weights', 'for', 'the', 'purpose',... | [-0.048503729207672985, 0.03462859682503843, -0.13783795496798384, 0.09620505858136855, -0.08901151111012333, -0.09089876385194953, 0.060181697762604985, 0.37627568352562946, -0.26952177999600163, -0.26927528968628717, 0.12389890832259695, -0.2574691897009529, -0.17600241872693762, 0.1873476674650665, -0.10654984718416... |
710.4393 | Quantum reference frames and deformed symmetries | In the context of constrained quantum mechanics, reference systems are used
to construct relational observables that are invariant under the action of the
symmetry group. Upon measurement of a relational observable, the reference
system undergoes an unavoidable measurement "back-action" that modifies its
properties. ... | gr-qc quant-ph | in the context of constrained quantum mechanics reference systems are used to construct relational observables that are invariant under the action of the symmetry group upon measurement of a relational observable the reference system undergoes an unavoidable measurement backaction that modifies its properties in a quan... | [['in', 'the', 'context', 'of', 'constrained', 'quantum', 'mechanics', 'reference', 'systems', 'are', 'used', 'to', 'construct', 'relational', 'observables', 'that', 'are', 'invariant', 'under', 'the', 'action', 'of', 'the', 'symmetry', 'group', 'upon', 'measurement', 'of', 'a', 'relational', 'observable', 'the', 'refe... | [-0.13674808618460976, 0.1466765682839756, -0.14803712141100867, 0.07789326148999264, -0.07524437373576238, -0.13642299911657044, -0.0068666324752216885, 0.3459489123224346, -0.278137872356546, -0.27852829367954773, 0.09439369026199705, -0.25299105864169813, -0.16220321240040741, 0.18326588680917152, -0.081866549634800... |
710.4394 | Markovian perturbation, response and fluctuation dissipation theorem | We consider the Fluctuation Dissipation Theorem (FDT) of statistical physics
from a mathematical perspective. We formalize the concept of "linear response
function" in the general framework of Markov processes. We show that for
processes out of equilibrium it depends not only on the given Markov process
X(s) but also... | math.PR math-ph math.MP | we consider the fluctuation dissipation theorem fdt of statistical physics from a mathematical perspective we formalize the concept of linear response function in the general framework of markov processes we show that for processes out of equilibrium it depends not only on the given markov process xs but also on the ch... | [['we', 'consider', 'the', 'fluctuation', 'dissipation', 'theorem', 'fdt', 'of', 'statistical', 'physics', 'from', 'a', 'mathematical', 'perspective', 'we', 'formalize', 'the', 'concept', 'of', 'linear', 'response', 'function', 'in', 'the', 'general', 'framework', 'of', 'markov', 'processes', 'we', 'show', 'that', 'for... | [-0.11072229077216497, 0.1396493027361007, -0.10544097358523327, 0.08421587141693995, -0.016568436354485364, -0.12748684510588645, 0.06541139790571707, 0.3330204552689264, -0.3337652123814752, -0.1828412207969746, 0.08809935010666417, -0.27409182144328953, -0.11638557318338127, 0.1735922977869767, -0.01556023633659839,... |
710.4395 | The base components of the dualizing sheaf of a curve on a surface | This note studies the structure of the divisorial fixed part of the dualizing
sheaf of a 1-connected curve D on a smooth surface S. It is shown that if the
divisorial fixed part F of the dualizing sheaf is non empty then it has
arithmetic genus<1 and each component of F is a smooth rational curve.
| math.AG | this note studies the structure of the divisorial fixed part of the dualizing sheaf of a 1connected curve d on a smooth surface s it is shown that if the divisorial fixed part f of the dualizing sheaf is non empty then it has arithmetic genus1 and each component of f is a smooth rational curve | [['this', 'note', 'studies', 'the', 'structure', 'of', 'the', 'divisorial', 'fixed', 'part', 'of', 'the', 'dualizing', 'sheaf', 'of', 'a', '1connected', 'curve', 'd', 'on', 'a', 'smooth', 'surface', 's', 'it', 'is', 'shown', 'that', 'if', 'the', 'divisorial', 'fixed', 'part', 'f', 'of', 'the', 'dualizing', 'sheaf', 'is... | [-0.25840262765788274, -0.012433679533257549, -0.17009144046876049, 0.019774432364751453, -0.09488456612286557, -0.1838533767815014, -0.0004651788455833282, 0.3308085763294782, -0.3732270784676075, -0.09667253133375198, 0.08116773243195244, -0.2515685495787433, -0.16696013596707157, 0.16352049860870466, -0.166373217811... |
710.4396 | A general dynamical statistical model with possible causal
interpretation | We develop a general dynamical model as a framework for possible causal
interpretation. We first state a criterion of local independence in terms of
measurability of processes involved in the Doob-Meyer decomposition of
stochastic processes, as in Aalen (1987); then we define direct and indirect
influence. We propose... | math.ST stat.TH | we develop a general dynamical model as a framework for possible causal interpretation we first state a criterion of local independence in terms of measurability of processes involved in the doobmeyer decomposition of stochastic processes as in aalen 1987 then we define direct and indirect influence we propose a defini... | [['we', 'develop', 'a', 'general', 'dynamical', 'model', 'as', 'a', 'framework', 'for', 'possible', 'causal', 'interpretation', 'we', 'first', 'state', 'a', 'criterion', 'of', 'local', 'independence', 'in', 'terms', 'of', 'measurability', 'of', 'processes', 'involved', 'in', 'the', 'doobmeyer', 'decomposition', 'of', '... | [-0.1050291562101224, 0.04500912093407624, -0.11725371475559432, 0.12817380083252683, -0.08986769687592774, -0.10702357237500797, 0.1156486461954224, 0.31360183041086875, -0.28085895578382647, -0.28735316737222816, 0.06970655247064346, -0.2460162895992138, -0.2197233555265344, 0.1614446381230715, -0.06706399417163192, ... |
710.4397 | A Direct Multigrid Poisson Solver for Oct-Tree Adaptive Meshes | We describe a finite-volume method for solving the Poisson equation on
oct-tree adaptive meshes using direct solvers for individual mesh blocks. The
method is a modified version of the method presented by Huang and Greengard
(2000), which works with finite-difference meshes and does not allow for shared
boundaries be... | astro-ph | we describe a finitevolume method for solving the poisson equation on octtree adaptive meshes using direct solvers for individual mesh blocks the method is a modified version of the method presented by huang and greengard 2000 which works with finitedifference meshes and does not allow for shared boundaries between ref... | [['we', 'describe', 'a', 'finitevolume', 'method', 'for', 'solving', 'the', 'poisson', 'equation', 'on', 'octtree', 'adaptive', 'meshes', 'using', 'direct', 'solvers', 'for', 'individual', 'mesh', 'blocks', 'the', 'method', 'is', 'a', 'modified', 'version', 'of', 'the', 'method', 'presented', 'by', 'huang', 'and', 'gre... | [-0.045950258671793906, -0.03376781521434341, -0.1298913106854473, 0.04467890982881987, -0.09370402409695089, -0.17684558331079425, 0.030412834800136762, 0.425863235069084, -0.23593170814482228, -0.34935836737886783, 0.10012336619686157, -0.18122835425726538, -0.14103469289174037, 0.24718703178777582, -0.05718308695802... |
710.4398 | Thermodynamics of DNA loops with long-range correlated structural
disorder | We study the influence of a structural disorder on the thermodynamical
properties of 2D-elastic chains submitted to mechanical/topological constraint
as loops. The disorder is introduced via a spontaneous curvature whose
distribution along the chain presents either no correlation or long-range
correlations (LRC). The... | q-bio.GN cond-mat.stat-mech | we study the influence of a structural disorder on the thermodynamical properties of 2delastic chains submitted to mechanicaltopological constraint as loops the disorder is introduced via a spontaneous curvature whose distribution along the chain presents either no correlation or longrange correlations lrc the equilibr... | [['we', 'study', 'the', 'influence', 'of', 'a', 'structural', 'disorder', 'on', 'the', 'thermodynamical', 'properties', 'of', '2delastic', 'chains', 'submitted', 'to', 'mechanicaltopological', 'constraint', 'as', 'loops', 'the', 'disorder', 'is', 'introduced', 'via', 'a', 'spontaneous', 'curvature', 'whose', 'distribut... | [-0.21014777962182468, 0.18271485915185387, -0.05256348330561721, 0.12600843108754708, 0.007208529381303612, -0.13223275249191654, -0.014399384736903695, 0.40981790645543587, -0.2616496410118331, -0.2257931289698826, 0.061450725948916526, -0.28943888890373287, -0.1626256655991385, 0.13549175009840603, 0.035550007528258... |
710.4399 | Magnetic tight-binding and the iron-chromium enthalpy anomaly | We describe a self consistent magnetic tight-binding theory based in an
expansion of the Hohenberg-Kohn density functional to second order, about a non
spin polarised reference density. We show how a first order expansion about a
density having a trial input magnetic moment leads to the Stoner--Slater rigid
band mode... | cond-mat.mtrl-sci | we describe a self consistent magnetic tightbinding theory based in an expansion of the hohenbergkohn density functional to second order about a non spin polarised reference density we show how a first order expansion about a density having a trial input magnetic moment leads to the stonerslater rigid band model we emp... | [['we', 'describe', 'a', 'self', 'consistent', 'magnetic', 'tightbinding', 'theory', 'based', 'in', 'an', 'expansion', 'of', 'the', 'hohenbergkohn', 'density', 'functional', 'to', 'second', 'order', 'about', 'a', 'non', 'spin', 'polarised', 'reference', 'density', 'we', 'show', 'how', 'a', 'first', 'order', 'expansion'... | [-0.10859389531111077, 0.11069156382148646, -0.07096164262409067, 0.09061948246390956, -0.054071984963712995, -0.07366054108157963, 0.07724660361011454, 0.427110667991732, -0.2573472339907414, -0.3014319166826032, -0.007355010892440389, -0.25876412299702634, -0.1707990955812954, 0.12970600669049182, 0.03834027071138258... |
710.44 | HNC, HCN and CN in Seyfert galaxies | Bright HNC 1--0 emission has been found towards several Seyfert galaxies.
This is unexpected since traditionally HNC is a tracer of cold (10 K) gas, and
the molecular gas of luminous galaxies like Seyferts is thought to have bulk
kinetic temperatures surpassing 50 K. In this work we aim to distinguish the
cause of th... | astro-ph | bright hnc 10 emission has been found towards several seyfert galaxies this is unexpected since traditionally hnc is a tracer of cold 10 k gas and the molecular gas of luminous galaxies like seyferts is thought to have bulk kinetic temperatures surpassing 50 k in this work we aim to distinguish the cause of the bright ... | [['bright', 'hnc', '10', 'emission', 'has', 'been', 'found', 'towards', 'several', 'seyfert', 'galaxies', 'this', 'is', 'unexpected', 'since', 'traditionally', 'hnc', 'is', 'a', 'tracer', 'of', 'cold', '10', 'k', 'gas', 'and', 'the', 'molecular', 'gas', 'of', 'luminous', 'galaxies', 'like', 'seyferts', 'is', 'thought',... | [-0.03204674364921326, 0.0029608698890990367, 0.026060253292404162, 0.0989697013425922, 0.024141470124284626, -0.11141214484265426, -0.006488559879626165, 0.5156467395582758, -0.007808755699592004, -0.34039186446125025, 0.012265241179913986, -0.28274823541301974, 0.04122116811754352, 0.1311044048113486, 0.0276355817169... |
710.4401 | Dynamics of axialized laser-cooled ions in a Penning trap | We report the experimental characterization of axialization - a method of
reducing the magnetron motion of a small number of ions stored in a Penning
trap. This is an important step in the investigation of the suitability of
Penning traps for quantum information processing. The magnetron motion was
coupled to the las... | quant-ph | we report the experimental characterization of axialization a method of reducing the magnetron motion of a small number of ions stored in a penning trap this is an important step in the investigation of the suitability of penning traps for quantum information processing the magnetron motion was coupled to the lasercool... | [['we', 'report', 'the', 'experimental', 'characterization', 'of', 'axialization', 'a', 'method', 'of', 'reducing', 'the', 'magnetron', 'motion', 'of', 'a', 'small', 'number', 'of', 'ions', 'stored', 'in', 'a', 'penning', 'trap', 'this', 'is', 'an', 'important', 'step', 'in', 'the', 'investigation', 'of', 'the', 'suita... | [-0.1506565765518209, 0.1709119844829505, -0.030056750224700765, -0.034021211473399475, -0.010206273267639504, -0.09948371717557851, 0.048227979749292674, 0.36672961705809703, -0.23005415125331585, -0.2907736530988072, 0.04704809824023328, -0.24731075641550665, -0.04377857938010678, 0.2604375051712428, -0.0315391761790... |
710.4402 | Control of Optical Dynamic Memory Capacity of an Atomic Bose-Einstein
Condensate | Light storage in an atomic Bose-Einstein condensate is one of the most
practical usage of these coherent atom-optical systems. In order to make them
even more practical, it is necessary to enhance our ability to inject multiple
pulses into the condensate. In this paper, we report that dispersion of pulses
injected in... | quant-ph cond-mat.other | light storage in an atomic boseeinstein condensate is one of the most practical usage of these coherent atomoptical systems in order to make them even more practical it is necessary to enhance our ability to inject multiple pulses into the condensate in this paper we report that dispersion of pulses injected into the c... | [['light', 'storage', 'in', 'an', 'atomic', 'boseeinstein', 'condensate', 'is', 'one', 'of', 'the', 'most', 'practical', 'usage', 'of', 'these', 'coherent', 'atomoptical', 'systems', 'in', 'order', 'to', 'make', 'them', 'even', 'more', 'practical', 'it', 'is', 'necessary', 'to', 'enhance', 'our', 'ability', 'to', 'inje... | [-0.15678449928577237, 0.17119116602407303, -0.08132076329809237, -0.0006848135046621269, -0.07511852596430703, -0.12758310510222107, 0.05453886691743429, 0.4316844247043767, -0.2563584374940082, -0.2787685943965582, 0.06312105118698302, -0.2657376554338856, -0.10168542251228652, 0.23874496559344946, -0.067324312656444... |
710.4403 | Deterministic distributed dense coding with stabilizer states | We consider the possibility of using stabilizer states to perform
deterministic dense coding among multiple senders and a single receiver. In the
model we studied, the utilized stabilizer state is partitioned into several
subsystems and then each subsystem is held by a distinct party. We present a
sufficient conditio... | quant-ph | we consider the possibility of using stabilizer states to perform deterministic dense coding among multiple senders and a single receiver in the model we studied the utilized stabilizer state is partitioned into several subsystems and then each subsystem is held by a distinct party we present a sufficient condition for... | [['we', 'consider', 'the', 'possibility', 'of', 'using', 'stabilizer', 'states', 'to', 'perform', 'deterministic', 'dense', 'coding', 'among', 'multiple', 'senders', 'and', 'a', 'single', 'receiver', 'in', 'the', 'model', 'we', 'studied', 'the', 'utilized', 'stabilizer', 'state', 'is', 'partitioned', 'into', 'several',... | [-0.12208794252060827, 0.09092369338314209, -0.09512849433743742, 0.011901326198652109, -0.01991403812834465, -0.2206366712317816, 0.0980778710322399, 0.379153646410568, -0.3031217181610305, -0.25427998828010134, 0.06688732307173187, -0.22068035111540177, -0.11155909470129591, 0.17951179620177388, -0.10660158794672131,... |
710.4404 | Attrition and Non-Response in Panel Data: The Case of the Canadian
Survey of Labor and Income Dynamics | This paper provides an analysis of the effects of attrition and non-response
on employment and wages using the Canadian Survey of Labour and Income
Dynamics. We consider a structural model composed of three freely correlated
equations for nonattrition/response, employment and wages. The model is
estimated using micro... | stat.AP | this paper provides an analysis of the effects of attrition and nonresponse on employment and wages using the canadian survey of labour and income dynamics we consider a structural model composed of three freely correlated equations for nonattritionresponse employment and wages the model is estimated using microdata fr... | [['this', 'paper', 'provides', 'an', 'analysis', 'of', 'the', 'effects', 'of', 'attrition', 'and', 'nonresponse', 'on', 'employment', 'and', 'wages', 'using', 'the', 'canadian', 'survey', 'of', 'labour', 'and', 'income', 'dynamics', 'we', 'consider', 'a', 'structural', 'model', 'composed', 'of', 'three', 'freely', 'cor... | [-0.043742908354033716, 0.13266595650668478, -0.06856330948357936, 0.092376316397349, -0.07893411015174934, -0.10747568971419241, 0.08784859531442635, 0.36834567427285947, -0.1972326125833206, -0.3246380281634629, 0.1304220653403263, -0.3651007245935034, -0.11615497793536633, 0.1919719698089466, -0.11230039722431684, -... |
710.4405 | Chiral Low-Energy Constants: Status and Prospects | Chiral low-energy constants (LECs) carry the information of short-distance
dynamics involving heavier degrees of freedom not present in the chiral
Lagrangian. Our knowledge of the LECs is all-important at phenomenological
level because their relevance in the prediction of hadronic observables at
low-energies and on t... | hep-ph | chiral lowenergy constants lecs carry the information of shortdistance dynamics involving heavier degrees of freedom not present in the chiral lagrangian our knowledge of the lecs is allimportant at phenomenological level because their relevance in the prediction of hadronic observables at lowenergies and on the other ... | [['chiral', 'lowenergy', 'constants', 'lecs', 'carry', 'the', 'information', 'of', 'shortdistance', 'dynamics', 'involving', 'heavier', 'degrees', 'of', 'freedom', 'not', 'present', 'in', 'the', 'chiral', 'lagrangian', 'our', 'knowledge', 'of', 'the', 'lecs', 'is', 'allimportant', 'at', 'phenomenological', 'level', 'be... | [-0.12440224879178895, 0.20517431785135645, -0.08901462382764543, 0.06369197737482976, -0.07760152299824642, -0.10466509029805048, 0.051003921807309845, 0.28844178684234417, -0.21421362436695457, -0.25001861144826837, 0.05745515665071315, -0.30351980438787646, -0.10607646463107165, 0.08621555724984979, 0.04875864625640... |
710.4406 | Rigidity and non local connectivity of Julia sets of some quadratic
polynomials | For an infinitely renormalizable quadratic map $f_c: z\mapsto z^2+c$ with the
sequence of renormalization periods ${k_m}$ and rotation numbers
${t_m=p_m/q_m}, we prove that if $\limsup k_m^{-1}\log |p_m|>0$, then the
Mandelbrot set is locally connected at $c$. We prove also that if $\limsup
|t_{m+1}|^{1/q_m}<1$ and $... | math.DS math.CV | for an infinitely renormalizable quadratic map f_c zmapsto z2c with the sequence of renormalization periods k_m and rotation numbers t_mp_mq_m we prove that if limsup k_m1log p_m0 then the mandelbrot set is locally connected at c we prove also that if limsup t_m11q_m1 and q_mto infty then the julia set of f_c is not lo... | [['for', 'an', 'infinitely', 'renormalizable', 'quadratic', 'map', 'f_c', 'zmapsto', 'z2c', 'with', 'the', 'sequence', 'of', 'renormalization', 'periods', 'k_m', 'and', 'rotation', 'numbers', 't_mp_mq_m', 'we', 'prove', 'that', 'if', 'limsup', 'k_m1log', 'p_m0', 'then', 'the', 'mandelbrot', 'set', 'is', 'locally', 'con... | [-0.1771764944833104, 0.14718629232746674, -0.051204591500803386, 0.05387808253186395, -0.059227186130673286, -0.14408385892407877, 0.06219382617290657, 0.2980532306476985, -0.3038121234662462, -0.1866495516888871, 0.08326196129258612, -0.3184885688066727, -0.1662196183097687, 0.20511877515680607, -0.08784723061189922,... |
710.4407 | Planetesimal accretion in binary star systems | Numerical simulations of planetesimal accretion in circumprimary and
circumbinary orbits are described. The secular perturbations by the com- panion
star and gas drag are included in our models. We derive limits on the
parameters of the binary system for which accretion and then planetary forma-
tion are possible. In... | astro-ph | numerical simulations of planetesimal accretion in circumprimary and circumbinary orbits are described the secular perturbations by the com panion star and gas drag are included in our models we derive limits on the parameters of the binary system for which accretion and then planetary forma tion are possible in the ci... | [['numerical', 'simulations', 'of', 'planetesimal', 'accretion', 'in', 'circumprimary', 'and', 'circumbinary', 'orbits', 'are', 'described', 'the', 'secular', 'perturbations', 'by', 'the', 'com', 'panion', 'star', 'and', 'gas', 'drag', 'are', 'included', 'in', 'our', 'models', 'we', 'derive', 'limits', 'on', 'the', 'pa... | [-0.1002912782516267, 0.06638094129845161, -0.07510860586030917, 0.05961873777083714, -0.03403889046008275, -0.027246099917895415, -0.0004922666544602675, 0.34080273882401263, -0.20984730712635527, -0.28096051229460334, 0.11051959721027577, -0.25626426257870416, -0.10432316045361487, 0.24218095653023655, -0.03509068426... |
710.4408 | Generation of two-mode field squeezing through selective dynamics in
cavity QED | We propose a scheme for the generation of a two-mode field squeezed state in
cavity QED. It is based on two-channel Raman excitations of a beam of
three-level atoms with random arrival times by two classical fields and two
high-Q resonator modes. It is shown that by suitably choosing the intensities
and detunings of ... | quant-ph | we propose a scheme for the generation of a twomode field squeezed state in cavity qed it is based on twochannel raman excitations of a beam of threelevel atoms with random arrival times by two classical fields and two highq resonator modes it is shown that by suitably choosing the intensities and detunings of fields t... | [['we', 'propose', 'a', 'scheme', 'for', 'the', 'generation', 'of', 'a', 'twomode', 'field', 'squeezed', 'state', 'in', 'cavity', 'qed', 'it', 'is', 'based', 'on', 'twochannel', 'raman', 'excitations', 'of', 'a', 'beam', 'of', 'threelevel', 'atoms', 'with', 'random', 'arrival', 'times', 'by', 'two', 'classical', 'field... | [-0.14866467376753265, 0.3112263085282187, -0.07027147252223041, -0.034740821835248896, 0.02510809864772042, -0.19563335592296818, 0.054089810808438846, 0.43860552974582945, -0.2087304255896315, -0.21526270302387013, 0.02663373247931529, -0.2334552881567134, -0.04589018914560528, 0.20990509979580482, 0.0153564111960898... |
710.4409 | The sharp lower bound for the volume of 3-folds of general type with
\chi(\Co{X})=1 | Let $V$ be a smooth projective 3-fold of general type. Denote by $K^{3}$, a
rational number, the self-intersection of the canonical sheaf of any minimal
model of $V$. One defines $K^{3}$ as a canonical volume of $V$. The paper is
devoted to proving the sharp lower bound $K^{3}\ge {1/420}$ which can be
reached by an e... | math.AG | let v be a smooth projective 3fold of general type denote by k3 a rational number the selfintersection of the canonical sheaf of any minimal model of v one defines k3 as a canonical volume of v the paper is devoted to proving the sharp lower bound k3ge 1420 which can be reached by an example x_46subseteq mathbbp456723 | [['let', 'v', 'be', 'a', 'smooth', 'projective', '3fold', 'of', 'general', 'type', 'denote', 'by', 'k3', 'a', 'rational', 'number', 'the', 'selfintersection', 'of', 'the', 'canonical', 'sheaf', 'of', 'any', 'minimal', 'model', 'of', 'v', 'one', 'defines', 'k3', 'as', 'a', 'canonical', 'volume', 'of', 'v', 'the', 'paper... | [-0.1917664287654175, 0.08639828672193371, -0.08411971022459594, 0.02217812217475677, -0.07643769430843267, -0.20856272965161637, 0.03230981268200346, 0.2317574276588857, -0.3024846835231239, -0.24824766811322083, 0.04287380488081412, -0.2331614894115112, -0.10675662054087628, 0.21719661205583676, -0.160480724376711, -... |
710.441 | A Multi-level Blocking Distinct Degree Factorization Algorithm | We give a new algorithm for performing the distinct-degree factorization of a
polynomial P(x) over GF(2), using a multi-level blocking strategy. The coarsest
level of blocking replaces GCD computations by multiplications, as suggested by
Pollard (1975), von zur Gathen and Shoup (1992), and others. The novelty of our
... | cs.DS | we give a new algorithm for performing the distinctdegree factorization of a polynomial px over gf2 using a multilevel blocking strategy the coarsest level of blocking replaces gcd computations by multiplications as suggested by pollard 1975 von zur gathen and shoup 1992 and others the novelty of our approach is that a... | [['we', 'give', 'a', 'new', 'algorithm', 'for', 'performing', 'the', 'distinctdegree', 'factorization', 'of', 'a', 'polynomial', 'px', 'over', 'gf2', 'using', 'a', 'multilevel', 'blocking', 'strategy', 'the', 'coarsest', 'level', 'of', 'blocking', 'replaces', 'gcd', 'computations', 'by', 'multiplications', 'as', 'sugge... | [-0.16515030769744155, 0.04318308561984179, -0.08258413065770509, 0.016406925291650824, -0.02971270132599389, -0.1791279581069683, 0.10251619304898384, 0.32964904825532376, -0.27430664072509364, -0.305125466566721, 0.06560957675265863, -0.2409927597118899, -0.12013862740878731, 0.24753953738025192, -0.04773060439346767... |
710.4411 | Cluster radioactivity of Th isotopes in the mean-field HFB theory | Cluster radioactivity is described as a very mass asymmetric fission process.
The reflection symmetry breaking octupole moment has been used in a mean field
HFB theory as leading coordinate instead of the quadrupole moment usually used
in standard fission calculations. The procedure has been applied to the study
of t... | nucl-th | cluster radioactivity is described as a very mass asymmetric fission process the reflection symmetry breaking octupole moment has been used in a mean field hfb theory as leading coordinate instead of the quadrupole moment usually used in standard fission calculations the procedure has been applied to the study of the v... | [['cluster', 'radioactivity', 'is', 'described', 'as', 'a', 'very', 'mass', 'asymmetric', 'fission', 'process', 'the', 'reflection', 'symmetry', 'breaking', 'octupole', 'moment', 'has', 'been', 'used', 'in', 'a', 'mean', 'field', 'hfb', 'theory', 'as', 'leading', 'coordinate', 'instead', 'of', 'the', 'quadrupole', 'mom... | [-0.03421422177584978, 0.15982021062447485, -0.07458415894382973, 0.15856442186267064, 0.005495264226139137, -0.07917935164963327, -0.009699915240450604, 0.39325658141112907, -0.1695623346320467, -0.30865584313869476, 0.03462926437226465, -0.2618566934564492, 0.0006982709065352272, 0.1682435521918417, 0.030647239443369... |
710.4412 | Large-Scale Magnetic Field Re-generation by Resonant MHD Wave
Interactions | We investigate numerically the long-time behavior of balanced Alfven wave
turbulence forced at intermediate scales. Whereas the usual constant-flux
solution is found at the smallest scales, two new scalings are obtained at the
forcing scales and at the largest scales of the system. In the latter case we
show, in part... | astro-ph | we investigate numerically the longtime behavior of balanced alfven wave turbulence forced at intermediate scales whereas the usual constantflux solution is found at the smallest scales two new scalings are obtained at the forcing scales and at the largest scales of the system in the latter case we show in particular t... | [['we', 'investigate', 'numerically', 'the', 'longtime', 'behavior', 'of', 'balanced', 'alfven', 'wave', 'turbulence', 'forced', 'at', 'intermediate', 'scales', 'whereas', 'the', 'usual', 'constantflux', 'solution', 'is', 'found', 'at', 'the', 'smallest', 'scales', 'two', 'new', 'scalings', 'are', 'obtained', 'at', 'th... | [-0.19447669756685404, 0.21572903268645668, -0.059806964825838804, 0.13980814163318597, -0.013053388009930765, -0.06679986998828691, -0.035735784445044605, 0.2748517741470836, -0.2969450640903656, -0.27388573676174466, 0.08159304609208173, -0.26882264439319803, -0.06993409669903908, 0.20511514210510393, 0.0995430398710... |
710.4413 | QCD Factorizations in Exclusive gamma* gamma* -> rho0_L rho0_L | The exclusive process e+ e- -> e+ e-rho0_L rho0_L allows to study various
dynamics and factorization properties of perturbative QCD. At moderate energy,
we demonstrate how collinear QCD factorization emerges, involving either
generalized distribution amplitudes (GDA) or transition distribution amplitudes
(TDA). At hi... | hep-ph | the exclusive process e e e erho0_l rho0_l allows to study various dynamics and factorization properties of perturbative qcd at moderate energy we demonstrate how collinear qcd factorization emerges involving either generalized distribution amplitudes gda or transition distribution amplitudes tda at higher energies in ... | [['the', 'exclusive', 'process', 'e', 'e', 'e', 'erho0_l', 'rho0_l', 'allows', 'to', 'study', 'various', 'dynamics', 'and', 'factorization', 'properties', 'of', 'perturbative', 'qcd', 'at', 'moderate', 'energy', 'we', 'demonstrate', 'how', 'collinear', 'qcd', 'factorization', 'emerges', 'involving', 'either', 'generali... | [-0.09926482078365305, 0.16445674694312568, -0.22540577015641963, 0.1628598794695239, -0.042639021169055595, -0.09046438218545959, 0.03870222848755392, 0.36347380184540246, -0.23522411650187816, -0.17952329323937496, -0.03756234974240546, -0.3020005185109877, -0.03596998783971437, 0.0792169199610891, 0.1203801134728233... |
710.4414 | A remark on odd dimensional normalized Ricci flow | Let $(M^n,g_0)$ ($n$ odd) be a compact Riemannian manifold with
$\lambda(g_0)>0$, where $\lambda(g_0)$ is the first eigenvalue of the operator
$-4\Delta_{g_0}+R(g_0)$, and $R(g_0)$ is the scalar curvature of $(M^n,g_0)$.
Assume the maximal solution $g(t)$ to the normalized Ricci flow with initial
data $(M^n,g_0)$ sat... | math.DG | let mng_0 n odd be a compact riemannian manifold with lambdag_00 where lambdag_0 is the first eigenvalue of the operator 4delta_g_0rg_0 and rg_0 is the scalar curvature of mng_0 assume the maximal solution gt to the normalized ricci flow with initial data mng_0 satisfies rgt leq c and int_m rmgtn2dmu_t leq c uniformly ... | [['let', 'mng_0', 'n', 'odd', 'be', 'a', 'compact', 'riemannian', 'manifold', 'with', 'lambdag_00', 'where', 'lambdag_0', 'is', 'the', 'first', 'eigenvalue', 'of', 'the', 'operator', '4delta_g_0rg_0', 'and', 'rg_0', 'is', 'the', 'scalar', 'curvature', 'of', 'mng_0', 'assume', 'the', 'maximal', 'solution', 'gt', 'to', '... | [-0.22019634536174063, 0.14827421877839386, -0.07263923126387678, -0.0008646395178639317, -0.11603814031137791, -0.27861284899002275, -0.08505078225894129, 0.340918222426322, -0.2675644484897182, -0.19243069925689943, 0.13625941721543874, -0.3386114646923052, -0.0454228740115331, 0.10318376401388278, -0.039591191527880... |
710.4415 | Proof of the combinatorial Kirillov-Reshetikhin conjecture | In this paper we give a direct proof of the equality of certain generating
function associated with tensor product multiplicities of Kirillov-Reshetikhin
modules for each simple Lie algebra g. Together with the theorems of Nakajima
and Hernandez, this gives the proof of the combinatorial version of the
Kirillov-Reshe... | math.QA math-ph math.CO math.MP math.RT | in this paper we give a direct proof of the equality of certain generating function associated with tensor product multiplicities of kirillovreshetikhin modules for each simple lie algebra g together with the theorems of nakajima and hernandez this gives the proof of the combinatorial version of the kirillovreshetikhin... | [['in', 'this', 'paper', 'we', 'give', 'a', 'direct', 'proof', 'of', 'the', 'equality', 'of', 'certain', 'generating', 'function', 'associated', 'with', 'tensor', 'product', 'multiplicities', 'of', 'kirillovreshetikhin', 'modules', 'for', 'each', 'simple', 'lie', 'algebra', 'g', 'together', 'with', 'the', 'theorems', '... | [-0.1766433018259704, 0.07683557850929598, -0.09800960487918928, -0.009925179947943737, -0.13869286691769958, -0.12376388607081026, -0.037488386157201604, 0.24792251052955785, -0.2969615291804075, -0.24374966320271294, 0.04525595234008506, -0.1813378951783913, -0.12504993529679875, 0.16286970051393534, -0.1219984013432... |
710.4416 | Direct calculation of the probability of pionium ionization in the
target | We performed the first direct calculation of the probability of pionium
(pi+pi- atom) ionization in the target. The dependence of the probability of
pionium ionization in the target as a function of the pionium lifetime is
established. These calculations are of interest of the DIRAC experiment at
CERN, which aims to ... | hep-ph | we performed the first direct calculation of the probability of pionium pipi atom ionization in the target the dependence of the probability of pionium ionization in the target as a function of the pionium lifetime is established these calculations are of interest of the dirac experiment at cern which aims to measure t... | [['we', 'performed', 'the', 'first', 'direct', 'calculation', 'of', 'the', 'probability', 'of', 'pionium', 'pipi', 'atom', 'ionization', 'in', 'the', 'target', 'the', 'dependence', 'of', 'the', 'probability', 'of', 'pionium', 'ionization', 'in', 'the', 'target', 'as', 'a', 'function', 'of', 'the', 'pionium', 'lifetime'... | [-0.08767536568359055, 0.16054314970649008, -0.07921574846841395, 0.04867154070987077, 0.07148876712368481, -0.047100888476867615, 0.09768630130666084, 0.3406666963650235, -0.19782530709073462, -0.31383851385707484, -0.02979139296000759, -0.31633417083528537, 0.028028865392994266, 0.13763005093366293, 0.057086805764842... |
710.4417 | A particle acceleration site in the Coma cluster? | We present the results of a deep (1.1 Ms) observation of the Coma cluster of
galaxies in the 18-30 keV band with the IBIS/ISGRI imager on board the INTEGRAL
satellite. We show that the source extension in the North-East to South-West
(SW) direction ($\sim 17'$) significantly exceeds the size of the point spread
funct... | astro-ph | we present the results of a deep 11 ms observation of the coma cluster of galaxies in the 1830 kev band with the ibisisgri imager on board the integral satellite we show that the source extension in the northeast to southwest sw direction sim 17 significantly exceeds the size of the point spread function of isgri and t... | [['we', 'present', 'the', 'results', 'of', 'a', 'deep', '11', 'ms', 'observation', 'of', 'the', 'coma', 'cluster', 'of', 'galaxies', 'in', 'the', '1830', 'kev', 'band', 'with', 'the', 'ibisisgri', 'imager', 'on', 'board', 'the', 'integral', 'satellite', 'we', 'show', 'that', 'the', 'source', 'extension', 'in', 'the', '... | [-0.06446019770871651, 0.04587324992497876, -0.09437194035052951, 0.07103805652977936, -0.07203120763530495, -0.07034579898242044, 0.04007361036054187, 0.46693318708976994, -0.24931852243131833, -0.328726080227417, 0.07456042623521594, -0.3306630378860513, -0.02645985107974485, 0.20281929118362696, -0.00397460251152967... |
710.4418 | Noncommutative Geometries and Gravity | We briefly review ideas about ``noncommutativity of space-time'' and
approaches toward a corresponding theory of gravity.
| gr-qc | we briefly review ideas about noncommutativity of spacetime and approaches toward a corresponding theory of gravity | [['we', 'briefly', 'review', 'ideas', 'about', 'noncommutativity', 'of', 'spacetime', 'and', 'approaches', 'toward', 'a', 'corresponding', 'theory', 'of', 'gravity']] | [-0.1185980808804743, 0.12855337061773753, -0.15615977148991078, 0.1117512984201312, -0.0958064234291669, -0.1502765149634797, 0.028600140030903276, 0.28437201294582337, -0.17972367722541094, -0.2639626699965447, 0.09859435728867538, -0.27342890202999115, -0.23593202768824995, 0.13309381681028754, -0.14187944208970293,... |
710.4419 | Spin dynamics of a trapped spin-1 Bose Gas above the Bose-Einstein
transition temperature | We study collective spin oscillations in a spin-1 Bose gas above the
Bose-Einstein transition temperature. Starting from the Heisenberg equation of
motion, we derive a kinetic equation describing the dynamics of a thermal gas
with the spin-1 degree of freedom. Applying the moment method to the kinetic
equation, we st... | cond-mat.other | we study collective spin oscillations in a spin1 bose gas above the boseeinstein transition temperature starting from the heisenberg equation of motion we derive a kinetic equation describing the dynamics of a thermal gas with the spin1 degree of freedom applying the moment method to the kinetic equation we study spinw... | [['we', 'study', 'collective', 'spin', 'oscillations', 'in', 'a', 'spin1', 'bose', 'gas', 'above', 'the', 'boseeinstein', 'transition', 'temperature', 'starting', 'from', 'the', 'heisenberg', 'equation', 'of', 'motion', 'we', 'derive', 'a', 'kinetic', 'equation', 'describing', 'the', 'dynamics', 'of', 'a', 'thermal', '... | [-0.18995572329908045, 0.23668728195862243, -0.059178214708361966, 0.021950284495357086, -0.03174527109873415, -0.09164963696961, -0.021756721365928763, 0.3052018392605312, -0.2452024374829812, -0.24114550209858202, 0.03837983664995379, -0.3060962682721591, -0.0519957238851783, 0.1497914796257674, 0.12638618566585008, ... |
710.442 | Fermion Systems in Discrete Space-Time Exemplifying the Spontaneous
Generation of a Causal Structure | As toy models for space-time on the Planck scale, we consider examples of
fermion systems in discrete space-time which are composed of one or two
particles defined on two up to nine space-time points. We study the
self-organization of the particles as described by a variational principle both
analytically and numeric... | math-ph gr-qc hep-th math.MP | as toy models for spacetime on the planck scale we consider examples of fermion systems in discrete spacetime which are composed of one or two particles defined on two up to nine spacetime points we study the selforganization of the particles as described by a variational principle both analytically and numerically we ... | [['as', 'toy', 'models', 'for', 'spacetime', 'on', 'the', 'planck', 'scale', 'we', 'consider', 'examples', 'of', 'fermion', 'systems', 'in', 'discrete', 'spacetime', 'which', 'are', 'composed', 'of', 'one', 'or', 'two', 'particles', 'defined', 'on', 'two', 'up', 'to', 'nine', 'spacetime', 'points', 'we', 'study', 'the'... | [-0.1464118711596382, 0.18505192035998966, -0.05975565293709329, 0.10234645457155463, -0.04506601614580638, -0.11052073445508553, 0.001845604056775894, 0.32725723546700203, -0.24290934861030267, -0.30502354343543236, 0.09413695819102282, -0.25593178528124816, -0.1649857131474098, 0.1509524907451123, 0.02609527294618496... |
710.4421 | A long-lived memory qubit on a low-decoherence quantum bus | We demonstrate long-lived coherence in internal hyperfine states of a single
\Ca{43} trapped-ion qubit $[T_2=1.2(2)\s]$, and in external motional states of
a single \Ca{40} trapped-ion qubit $[T_2'=0.18(4)\s]$, in the same apparatus.
The motional decoherence rate is consistent with the heating rate, which was
measure... | quant-ph | we demonstrate longlived coherence in internal hyperfine states of a single ca43 trappedion qubit t_2122s and in external motional states of a single ca40 trappedion qubit t_20184s in the same apparatus the motional decoherence rate is consistent with the heating rate which was measured to be 31 quantasec long coherenc... | [['we', 'demonstrate', 'longlived', 'coherence', 'in', 'internal', 'hyperfine', 'states', 'of', 'a', 'single', 'ca43', 'trappedion', 'qubit', 't_2122s', 'and', 'in', 'external', 'motional', 'states', 'of', 'a', 'single', 'ca40', 'trappedion', 'qubit', 't_20184s', 'in', 'the', 'same', 'apparatus', 'the', 'motional', 'de... | [-0.14287345964501735, 0.2681459751035272, -0.00650872322230626, 0.014881419519644598, 0.09632293016216914, -0.21348435288085274, 0.08304262079272262, 0.45038374146105536, -0.18537230442710956, -0.2933682742246597, 0.01773414821659123, -0.2189547506515199, 0.023413614586362957, 0.25999092079803976, -0.04382496073343594... |
710.4422 | Lattice QCD approach to nuclear force | We present our updated results of the nucleon-nucleon potential in quenched
lattice QCD simulations with the plaquette gauge action and the Wilson quark
action on the 32^4(\simeq (4.4 fm)^4) lattice. From the equal-time
Bethe-Salpeter (BS) wave function, the NN potential is constructed through the
Schroedinger-type e... | hep-lat | we present our updated results of the nucleonnucleon potential in quenched lattice qcd simulations with the plaquette gauge action and the wilson quark action on the 324simeq 44 fm4 lattice from the equaltime bethesalpeter bs wave function the nn potential is constructed through the schroedingertype equation resulting ... | [['we', 'present', 'our', 'updated', 'results', 'of', 'the', 'nucleonnucleon', 'potential', 'in', 'quenched', 'lattice', 'qcd', 'simulations', 'with', 'the', 'plaquette', 'gauge', 'action', 'and', 'the', 'wilson', 'quark', 'action', 'on', 'the', '324simeq', '44', 'fm4', 'lattice', 'from', 'the', 'equaltime', 'bethesalp... | [-0.10411486946671766, 0.16701202715889815, -0.1070204732096652, 0.10410522557981992, -0.0019438037995918634, -0.1154472925258379, 0.060895241836058725, 0.3905302168747043, -0.20878158800684624, -0.2591634903810103, -0.0006456704101572833, -0.36270515688688215, -0.05780333979549201, 0.08768829555135138, 0.1073593309803... |
710.4423 | Transverse momentum distributions of quarks from the lattice using
extended gauge links | We present preliminary numerical studies in Lattice QCD related to the
intrinsic transverse momentum distribution of partons in the nucleon. We employ
non-local operators, consisting of spatially separated quark creation and
annihilation operators connected by a straight Wilson line. A clear signal is
already obtaine... | hep-lat | we present preliminary numerical studies in lattice qcd related to the intrinsic transverse momentum distribution of partons in the nucleon we employ nonlocal operators consisting of spatially separated quark creation and annihilation operators connected by a straight wilson line a clear signal is already obtained from... | [['we', 'present', 'preliminary', 'numerical', 'studies', 'in', 'lattice', 'qcd', 'related', 'to', 'the', 'intrinsic', 'transverse', 'momentum', 'distribution', 'of', 'partons', 'in', 'the', 'nucleon', 'we', 'employ', 'nonlocal', 'operators', 'consisting', 'of', 'spatially', 'separated', 'quark', 'creation', 'and', 'an... | [-0.10332206636133236, 0.2206784966969147, -0.11792263673370652, 0.10797790184386348, -0.06834286972805602, -0.051474340430913715, 0.029908776704068166, 0.4099007163436041, -0.19085215731206726, -0.26942419915229354, -0.011471261558712486, -0.31844984200022636, -0.018522480434370697, 0.16097931620246225, 0.031117434177... |
710.4424 | Valuations for matroid polytope subdivisions | We prove that the ranks of the subsets and the activities of the bases of a
matroid define valuations for the subdivisions of a matroid polytope into
smaller matroid polytopes.
| math.CO | we prove that the ranks of the subsets and the activities of the bases of a matroid define valuations for the subdivisions of a matroid polytope into smaller matroid polytopes | [['we', 'prove', 'that', 'the', 'ranks', 'of', 'the', 'subsets', 'and', 'the', 'activities', 'of', 'the', 'bases', 'of', 'a', 'matroid', 'define', 'valuations', 'for', 'the', 'subdivisions', 'of', 'a', 'matroid', 'polytope', 'into', 'smaller', 'matroid', 'polytopes']] | [-0.2001206404219071, 0.044937346844623485, -0.07499833746502797, 0.07376019437797368, -0.05785053468619784, -0.03277671781058113, 0.10358429476618766, 0.31207499926288923, -0.3984222610791524, -0.1847224857037266, 0.09751236749871169, -0.25382942197223507, -0.14841857105493544, 0.08435419291102637, -0.1920289924368262... |
710.4425 | Gauge and constraint degrees of freedom: from analytical to numerical
approximations in General Relativity | The harmonic formulation of Einstein's field equations is considered, where
the gauge conditions are introduced as dynamical constraints. The difference
between the fully constrained approach (used in analytical approximations) and
the free evolution one (used in most numerical approximations) is pointed out.
As a ge... | gr-qc | the harmonic formulation of einsteins field equations is considered where the gauge conditions are introduced as dynamical constraints the difference between the fully constrained approach used in analytical approximations and the free evolution one used in most numerical approximations is pointed out as a generalizati... | [['the', 'harmonic', 'formulation', 'of', 'einsteins', 'field', 'equations', 'is', 'considered', 'where', 'the', 'gauge', 'conditions', 'are', 'introduced', 'as', 'dynamical', 'constraints', 'the', 'difference', 'between', 'the', 'fully', 'constrained', 'approach', 'used', 'in', 'analytical', 'approximations', 'and', '... | [-0.10152698435938792, 0.11480439206022325, -0.11195432213343569, 0.12357474238187797, -0.07280550488625277, -0.15832410128735033, -0.03143852646115111, 0.35003163899058726, -0.21622825413681707, -0.2870513111658728, 0.10107992921257392, -0.21755473277663617, -0.1611450208184212, 0.19939175830309544, -0.018515227821224... |
710.4426 | Cohomological characterization of relative hyperbolicity and combination
theorem | We give a cohomological characterization of Gromov relative hyperbolicity. As
an application we prove a converse to the combination theorem for graphs of
relatively hyperbolic groups given in a previous paper of the first author. We
build upon, and follow the ideas of, the work of S. Gersten in ``Cohom. lower
bounds ... | math.GR | we give a cohomological characterization of gromov relative hyperbolicity as an application we prove a converse to the combination theorem for graphs of relatively hyperbolic groups given in a previous paper of the first author we build upon and follow the ideas of the work of s gersten in cohom lower bounds for isoper... | [['we', 'give', 'a', 'cohomological', 'characterization', 'of', 'gromov', 'relative', 'hyperbolicity', 'as', 'an', 'application', 'we', 'prove', 'a', 'converse', 'to', 'the', 'combination', 'theorem', 'for', 'graphs', 'of', 'relatively', 'hyperbolic', 'groups', 'given', 'in', 'a', 'previous', 'paper', 'of', 'the', 'fir... | [-0.13771682474436922, 0.06603740559234318, -0.13150154611588838, 0.08778024526477299, -0.10899389869369128, -0.06385639454375076, 0.10450724020826302, 0.304144871297895, -0.2453181979328613, -0.3162086693131748, 0.10860930478049662, -0.25129153059028525, -0.15237645333742394, 0.23435495571260723, -0.21180377237717896,... |
710.4427 | On the disconnection of a discrete cylinder by a biased random walk | We consider a random walk on the discrete cylinder
$({\mathbb{Z}}/N{\mathbb{Z}})^d\times{\mathbb{Z}}$, $d\geq3$ with drift
$N^{-d\alpha}$ in the $\mathbb{Z}$-direction and investigate the large
$N$-behavior of the disconnection time $T^{\mathrm{disc}}_N$, defined as the
first time when the trajectory of the random wa... | math.PR | we consider a random walk on the discrete cylinder mathbbznmathbbzdtimesmathbbz dgeq3 with drift ndalpha in the mathbbzdirection and investigate the large nbehavior of the disconnection time tmathrmdisc_n defined as the first time when the trajectory of the random walk disconnects the cylinder into two infinite compone... | [['we', 'consider', 'a', 'random', 'walk', 'on', 'the', 'discrete', 'cylinder', 'mathbbznmathbbzdtimesmathbbz', 'dgeq3', 'with', 'drift', 'ndalpha', 'in', 'the', 'mathbbzdirection', 'and', 'investigate', 'the', 'large', 'nbehavior', 'of', 'the', 'disconnection', 'time', 'tmathrmdisc_n', 'defined', 'as', 'the', 'first',... | [-0.157031302578574, 0.20000273989903372, -0.057174086570739746, 0.04382347935664489, 0.01551244706443381, -0.15806837836930224, 0.030616687074693484, 0.3384111102150623, -0.23675833532023569, -0.20066268404209336, 0.16005349644530176, -0.2845695919118995, -0.11033632110013779, 0.1501943896914464, -0.032807715334604644... |
710.4428 | Nonlinear theory of mirror instability near threshold | An asymptotic model based on a reductive perturbative expansion of the drift
kinetic and the Maxwell equations is used to demonstrate that, near the
instability threshold, the nonlinear dynamics of mirror modes in a magnetized
plasma with anisotropic ion temperatures involves a subcritical
bifurcation,leading to the ... | physics.plasm-ph physics.space-ph | an asymptotic model based on a reductive perturbative expansion of the drift kinetic and the maxwell equations is used to demonstrate that near the instability threshold the nonlinear dynamics of mirror modes in a magnetized plasma with anisotropic ion temperatures involves a subcritical bifurcationleading to the forma... | [['an', 'asymptotic', 'model', 'based', 'on', 'a', 'reductive', 'perturbative', 'expansion', 'of', 'the', 'drift', 'kinetic', 'and', 'the', 'maxwell', 'equations', 'is', 'used', 'to', 'demonstrate', 'that', 'near', 'the', 'instability', 'threshold', 'the', 'nonlinear', 'dynamics', 'of', 'mirror', 'modes', 'in', 'a', 'm... | [-0.16945801615273873, 0.19713969864671144, -0.09816110836701435, 0.03146367648150772, -0.07909514449471444, -0.0604354467716787, -0.06804608270166475, 0.301610549160263, -0.22963853706524037, -0.25097836694565784, 0.06165084191148676, -0.21689054079092385, -0.08910554594343953, 0.19619553279246024, 0.05275255289713019... |
710.4429 | On photoionization of the subvalent subshells of noble gas endohedral
atoms | We demonstrate strong interference patterns in the photoionization
cross-section of the subvalent subshells of noble gas (NG) endohedral atoms
NG@F. This interference is a result of common action of three factors: the
effect of neighboring atomic subshells, reflection of photoelectron waves by
the fullerene F shell a... | physics.atm-clus physics.atom-ph | we demonstrate strong interference patterns in the photoionization crosssection of the subvalent subshells of noble gas ng endohedral atoms ngf this interference is a result of common action of three factors the effect of neighboring atomic subshells reflection of photoelectron waves by the fullerene f shell and resona... | [['we', 'demonstrate', 'strong', 'interference', 'patterns', 'in', 'the', 'photoionization', 'crosssection', 'of', 'the', 'subvalent', 'subshells', 'of', 'noble', 'gas', 'ng', 'endohedral', 'atoms', 'ngf', 'this', 'interference', 'is', 'a', 'result', 'of', 'common', 'action', 'of', 'three', 'factors', 'the', 'effect', ... | [-0.08628469053934368, 0.12750489781632948, -0.03560683624144938, 0.044918970511802894, 0.021045762881788128, -0.08545674737453746, 0.017744312194314157, 0.3974452069893693, -0.20819903468004647, -0.2753280981234386, -0.050961223101738, -0.30959391129608643, -0.06304158944676688, 0.12007739092334749, 0.0435624199061048... |
710.443 | Unparticles and CP-violation | We give a brief summary of the unparticle scenario proposed by Georgi. The
CP-even phase of the propagator is exploited to study the CP-asymmetry in B+
--> tau+ + nu, which is neither experimentally searched for nor predicted by
any other model. Furthermore we show that the novel CP-violation is consistent
with the C... | hep-ph | we give a brief summary of the unparticle scenario proposed by georgi the cpeven phase of the propagator is exploited to study the cpasymmetry in b tau nu which is neither experimentally searched for nor predicted by any other model furthermore we show that the novel cpviolation is consistent with the cpt theorem by id... | [['we', 'give', 'a', 'brief', 'summary', 'of', 'the', 'unparticle', 'scenario', 'proposed', 'by', 'georgi', 'the', 'cpeven', 'phase', 'of', 'the', 'propagator', 'is', 'exploited', 'to', 'study', 'the', 'cpasymmetry', 'in', 'b', 'tau', 'nu', 'which', 'is', 'neither', 'experimentally', 'searched', 'for', 'nor', 'predicte... | [-0.12631407064065092, 0.213351612483136, -0.08043893815980094, 0.12696598604374917, -0.0881105892848773, -0.19054032852262504, 0.07364165633306151, 0.2974759721365131, -0.19651713519983116, -0.2588678060297961, 0.03197245936092661, -0.22627042111803275, -0.15264810185085553, 0.139421347127922, 0.019585173886238795, 0.... |
710.4431 | Heterogeneous Condensation | Vapor condensation on nanoparticle with radius smaller than the Kelvin radius
is considered as fluctuation or as the heterogeneous nucleation. The expression
for steady-state heterogeneous nucleation rate is obtained. Nucleation on
negatively charged nanoparticles is discussed. The report was made at 17th
Internation... | cond-mat.stat-mech | vapor condensation on nanoparticle with radius smaller than the kelvin radius is considered as fluctuation or as the heterogeneous nucleation the expression for steadystate heterogeneous nucleation rate is obtained nucleation on negatively charged nanoparticles is discussed the report was made at 17th international nuc... | [['vapor', 'condensation', 'on', 'nanoparticle', 'with', 'radius', 'smaller', 'than', 'the', 'kelvin', 'radius', 'is', 'considered', 'as', 'fluctuation', 'or', 'as', 'the', 'heterogeneous', 'nucleation', 'the', 'expression', 'for', 'steadystate', 'heterogeneous', 'nucleation', 'rate', 'is', 'obtained', 'nucleation', 'o... | [-0.0846081257564947, 0.22752727995160968, -0.03325883219949901, 0.05838249258464202, -0.011789847926702351, -0.09164292328059673, 0.031693385438993575, 0.32522638492286204, -0.13166674539446832, -0.3291164437308908, 0.11961225643754006, -0.3348955379985273, -0.07490724107716233, 0.18646468251477927, -0.007060282193124... |
710.4432 | On the Role of the Normalization Factors $\kappa_n$ and of the
Pseudo-Metric ${\cal P} \neq {\cal P}^\dagger$ in Crypto-Hermitian Quantum
Models | Among ${\cal P}$-pseudo-Hermitian Hamiltonians $H ={\cal P}^{-1} H^\dagger
\cal P}$ with real spectra, the ''weakly pseudo-Hermitian" ones (i.e., those
employing non-self-adjoint ${\cal P} \neq {\cal P}^\dagger$) form a remarkable
subfamily. We list some reasons why it deserves a special attention. In
particular we s... | math-ph math.MP quant-ph | among cal ppseudohermitian hamiltonians h cal p1 hdagger cal p with real spectra the weakly pseudohermitian ones ie those employing nonselfadjoint cal p neq cal pdagger form a remarkable subfamily we list some reasons why it deserves a special attention in particular we show that whenever cal p neq cal pdagger the curr... | [['among', 'cal', 'ppseudohermitian', 'hamiltonians', 'h', 'cal', 'p1', 'hdagger', 'cal', 'p', 'with', 'real', 'spectra', 'the', 'weakly', 'pseudohermitian', 'ones', 'ie', 'those', 'employing', 'nonselfadjoint', 'cal', 'p', 'neq', 'cal', 'pdagger', 'form', 'a', 'remarkable', 'subfamily', 'we', 'list', 'some', 'reasons'... | [-0.15915405616520883, 0.17945443443518053, -0.0069826984916754225, 0.060977403034872195, -0.0684120555438022, -0.22658447892048417, -0.0351300976422437, 0.3510777361175798, -0.2470586182985534, -0.17931959887055007, 0.011084112642144666, -0.33482396348250754, -0.16396060665237142, 0.07946373064113048, -0.0918570012733... |
710.4433 | Hot electrons induced by (rather) cold ions | Thin film metal-insulator-metal junctions are used in a novel approach to
investigate the dissipation of potential energy of multiply charged ions
impinging on a polycrystalline metal surface. The ion-metal interaction leads
to excited electrons and holes within the top layer. A substantial fraction of
these charge c... | cond-mat.mtrl-sci | thin film metalinsulatormetal junctions are used in a novel approach to investigate the dissipation of potential energy of multiply charged ions impinging on a polycrystalline metal surface the ionmetal interaction leads to excited electrons and holes within the top layer a substantial fraction of these charge carriers... | [['thin', 'film', 'metalinsulatormetal', 'junctions', 'are', 'used', 'in', 'a', 'novel', 'approach', 'to', 'investigate', 'the', 'dissipation', 'of', 'potential', 'energy', 'of', 'multiply', 'charged', 'ions', 'impinging', 'on', 'a', 'polycrystalline', 'metal', 'surface', 'the', 'ionmetal', 'interaction', 'leads', 'to'... | [-0.10631407856934273, 0.2298388375229343, 0.007511745043682741, 0.020029895106650222, 0.03760403738384927, -0.12796378768667746, 0.04764320200340433, 0.3823855617153111, -0.24706075516348677, -0.3864803131384803, -0.06042417591010262, -0.35159961809056683, 0.04189098198244821, 0.1803935229250077, 0.02886557638638222, ... |
710.4434 | Lectures on the three--dimensional non--commutative spheres | These are expanded notes for a short course given at the Universidad Nacional
de La Plata. They aim at giving a self-contained account of the results of
Alain Connes and Michel Dubois--Violette.
| math.QA gr-qc | these are expanded notes for a short course given at the universidad nacional de la plata they aim at giving a selfcontained account of the results of alain connes and michel duboisviolette | [['these', 'are', 'expanded', 'notes', 'for', 'a', 'short', 'course', 'given', 'at', 'the', 'universidad', 'nacional', 'de', 'la', 'plata', 'they', 'aim', 'at', 'giving', 'a', 'selfcontained', 'account', 'of', 'the', 'results', 'of', 'alain', 'connes', 'and', 'michel', 'duboisviolette']] | [-0.11943763867020607, 0.09369135880842805, -0.19490222542663105, 0.16644066525623202, -0.11223500443156809, -0.1254451809618331, -0.07515880302526057, 0.2297460253466852, -0.14958721864968538, -0.2932571795536205, 0.13831911695888266, -0.32151344732847065, -0.08831731689861044, 0.22754431364592165, -0.2055692228605039... |
710.4435 | Manifestation of spin-orbit interaction in tunneling between 2D electron
layers | An influence of spin-orbit interaction on the tunneling between two 2D
electron layers is considered. Particular attention is addressed to the
relation between the contribution of Rashba and Dresselhaus types. It is shown
that without scattering of the electrons, the tunneling conductance can either
exhibit resonance... | cond-mat.other | an influence of spinorbit interaction on the tunneling between two 2d electron layers is considered particular attention is addressed to the relation between the contribution of rashba and dresselhaus types it is shown that without scattering of the electrons the tunneling conductance can either exhibit resonances at c... | [['an', 'influence', 'of', 'spinorbit', 'interaction', 'on', 'the', 'tunneling', 'between', 'two', '2d', 'electron', 'layers', 'is', 'considered', 'particular', 'attention', 'is', 'addressed', 'to', 'the', 'relation', 'between', 'the', 'contribution', 'of', 'rashba', 'and', 'dresselhaus', 'types', 'it', 'is', 'shown', ... | [-0.20048567636977577, 0.17639463500273084, 0.0011287595496387846, 0.06474130524847128, -0.04842192403026926, -0.16201917936594518, 0.03256242591435952, 0.37715970210508626, -0.2925868631660271, -0.3335251455236949, -0.05449610268836146, -0.2986385235736675, -0.10403864679392427, 0.2193867538954868, 0.0501847935201072,... |
710.4436 | Thermodynamic Casimir effects involving interacting field theories with
zero modes | Systems with an O(n) symmetrical Hamiltonian are considered in a
$d$-dimensional slab geometry of macroscopic lateral extension and finite
thickness $L$ that undergo a continuous bulk phase transition in the limit
$L\to\infty$. The effective forces induced by thermal fluctuations at and above
the bulk critical temper... | cond-mat.stat-mech hep-th | systems with an on symmetrical hamiltonian are considered in a ddimensional slab geometry of macroscopic lateral extension and finite thickness l that undergo a continuous bulk phase transition in the limit ltoinfty the effective forces induced by thermal fluctuations at and above the bulk critical temperature t_cinfty... | [['systems', 'with', 'an', 'on', 'symmetrical', 'hamiltonian', 'are', 'considered', 'in', 'a', 'ddimensional', 'slab', 'geometry', 'of', 'macroscopic', 'lateral', 'extension', 'and', 'finite', 'thickness', 'l', 'that', 'undergo', 'a', 'continuous', 'bulk', 'phase', 'transition', 'in', 'the', 'limit', 'ltoinfty', 'the',... | [-0.14760071002410768, 0.20931943715133153, -0.07891037238156666, 0.05516598088797764, -0.0017809553913442262, -0.11924581467610551, 0.03769065108341844, 0.325320495464742, -0.20545010261260663, -0.28212037245733274, 0.048411488099494214, -0.31374619472626364, -0.12721543531006319, 0.17431060750823235, 0.00543392843057... |
710.4437 | Homotopy dimension of orbits of Morse functions on surfaces | Let $f$ be a real- or circle-valued Morse function on a compact surface M
having exactly $n>0$ critical points. Denote by $O$ the orbit of $f$ with
respect to the right action of the group of diffeomorphisms of $M$. We show
that the connected components of $O$ have the homotopy type of a
finite-dimensional CW-complex... | math.AT math.GT | let f be a real or circlevalued morse function on a compact surface m having exactly n0 critical points denote by o the orbit of f with respect to the right action of the group of diffeomorphisms of m we show that the connected components of o have the homotopy type of a finitedimensional cwcomplex actually these conne... | [['let', 'f', 'be', 'a', 'real', 'or', 'circlevalued', 'morse', 'function', 'on', 'a', 'compact', 'surface', 'm', 'having', 'exactly', 'n0', 'critical', 'points', 'denote', 'by', 'o', 'the', 'orbit', 'of', 'f', 'with', 'respect', 'to', 'the', 'right', 'action', 'of', 'the', 'group', 'of', 'diffeomorphisms', 'of', 'm', ... | [-0.2255172501128091, 0.10438177838199297, -0.07257416876679172, -0.01855435877520477, -0.06338209728710353, -0.11555018933603958, 0.05081476712342808, 0.33857673083489037, -0.29128995068770436, -0.24170568178951912, 0.07669148201655064, -0.25321159373056523, -0.1124177767386736, 0.17215087779141885, -0.108467267826199... |
710.4438 | Modified Actions for Gravity: Theory and Phenomenology | This thesis is devoted to the study of gravitational theories which can be
seen as modifications or generalisations of General Relativity. The motivation
for considering such theories, stemming from Cosmology, High Energy Physics and
Astrophysics is thoroughly discussed (cosmological problems, dark energy and
dark ma... | gr-qc astro-ph hep-th | this thesis is devoted to the study of gravitational theories which can be seen as modifications or generalisations of general relativity the motivation for considering such theories stemming from cosmology high energy physics and astrophysics is thoroughly discussed cosmological problems dark energy and dark matter pr... | [['this', 'thesis', 'is', 'devoted', 'to', 'the', 'study', 'of', 'gravitational', 'theories', 'which', 'can', 'be', 'seen', 'as', 'modifications', 'or', 'generalisations', 'of', 'general', 'relativity', 'the', 'motivation', 'for', 'considering', 'such', 'theories', 'stemming', 'from', 'cosmology', 'high', 'energy', 'ph... | [-0.132985896284726, 0.1007419458704604, -0.09591597617076514, 0.1767937632083051, -0.13667860177247765, -0.18648146498006382, -0.04761522544439474, 0.29461736866957655, -0.23132258459721525, -0.3349244519876801, 0.07914640118217002, -0.21525639706380564, -0.15169152570037878, 0.18706756174302827, -0.06750249222865047,... |
710.4439 | Supersymmetric Interpretation of the EGRET Excess in Diffuse Galactic
Gamma Rays | Recently it was shown that the excess of diffuse Galactic gamma rays above 1
GeV could be interpreted as a Dark Matter annihilation signal. From the
spectral shape of the excess it is possible to determine a range for the
allowed WIMP mass which can be used to test the supersymmetric parameter space.
It is found that... | hep-ph | recently it was shown that the excess of diffuse galactic gamma rays above 1 gev could be interpreted as a dark matter annihilation signal from the spectral shape of the excess it is possible to determine a range for the allowed wimp mass which can be used to test the supersymmetric parameter space it is found that the... | [['recently', 'it', 'was', 'shown', 'that', 'the', 'excess', 'of', 'diffuse', 'galactic', 'gamma', 'rays', 'above', '1', 'gev', 'could', 'be', 'interpreted', 'as', 'a', 'dark', 'matter', 'annihilation', 'signal', 'from', 'the', 'spectral', 'shape', 'of', 'the', 'excess', 'it', 'is', 'possible', 'to', 'determine', 'a', ... | [-0.021511488336977642, 0.2211467737618547, -0.052691507511414014, 0.20085121267398431, -0.1440199273791942, -0.11924942324940975, 0.018095435190863988, 0.382772061999396, -0.2321966626927011, -0.40536247717810203, 0.04930231170242673, -0.2891049595692983, 0.036999960048738255, 0.21202691813808058, 0.021144991100939748... |
710.444 | Role of symmetry in the interplay of T=0 quantum-phase transitions with
unconventional T>0 transport properties in integrable quantum lattice systems | We show that a generalized charge SU(2) symmetry of the one-dimensional (1D)
Hubbard model in an infinitesimal flux $\phi$ generates half-filling states
from metallic states which lead to a finite charge stiffness $D(T)$ at finite
temperature $T$, whose $T$ dependence we study. Our results are of general
nature for m... | cond-mat.str-el cond-mat.other | we show that a generalized charge su2 symmetry of the onedimensional 1d hubbard model in an infinitesimal flux phi generates halffilling states from metallic states which lead to a finite charge stiffness dt at finite temperature t whose t dependence we study our results are of general nature for many integrable quantu... | [['we', 'show', 'that', 'a', 'generalized', 'charge', 'su2', 'symmetry', 'of', 'the', 'onedimensional', '1d', 'hubbard', 'model', 'in', 'an', 'infinitesimal', 'flux', 'phi', 'generates', 'halffilling', 'states', 'from', 'metallic', 'states', 'which', 'lead', 'to', 'a', 'finite', 'charge', 'stiffness', 'dt', 'at', 'fini... | [-0.1631953847613566, 0.2709157244619802, -0.06008482630820755, 0.033129795045800964, 0.010705553415725579, -0.20136755719134697, 0.05029476084152465, 0.36857779114982303, -0.2687722332110362, -0.17929767220452122, 0.002032431603970044, -0.34939672570314484, -0.130086500801108, 0.12774632815794296, 0.08563757703249932,... |
710.4441 | Calabi-Yau cones from contact reduction | We consider a generalization of Einstein-Sasaki manifolds, which we
characterize in terms both of spinors and differential forms, that in the real
analytic case corresponds to contact manifolds whose symplectic cone is
Calabi-Yau. We construct solvable examples in seven dimensions. Then, we
consider circle actions th... | math.DG | we consider a generalization of einsteinsasaki manifolds which we characterize in terms both of spinors and differential forms that in the real analytic case corresponds to contact manifolds whose symplectic cone is calabiyau we construct solvable examples in seven dimensions then we consider circle actions that preser... | [['we', 'consider', 'a', 'generalization', 'of', 'einsteinsasaki', 'manifolds', 'which', 'we', 'characterize', 'in', 'terms', 'both', 'of', 'spinors', 'and', 'differential', 'forms', 'that', 'in', 'the', 'real', 'analytic', 'case', 'corresponds', 'to', 'contact', 'manifolds', 'whose', 'symplectic', 'cone', 'is', 'calab... | [-0.1764406935831943, 0.029463778354428625, -0.05218154431000207, 0.10098667618177541, -0.10992538945616356, -0.13117178216237912, -0.020672637695603846, 0.3612280989718902, -0.2421606524859543, -0.2259865570027236, 0.12832796367568677, -0.25974833444002776, -0.2355262730754428, 0.1786273049747015, -0.1065356693678088,... |
710.4442 | Neutron star sequences and the starquake glitch model for the Crab and
the Vela pulsars | We construct for the first time, the sequences of stable neutron star (NS)
models capable of explaining simultaneously, the glitch healing parameters,
$Q$, of both the pulsars, the Crab ($Q \geq 0.7$) and the Vela ($Q \leq 0.2$),
on the basis of starquake mechanism of glitch generation, whereas the
conventional NS mo... | astro-ph | we construct for the first time the sequences of stable neutron star ns models capable of explaining simultaneously the glitch healing parameters q of both the pulsars the crab q geq 07 and the vela q leq 02 on the basis of starquake mechanism of glitch generation whereas the conventional ns models cannot give such con... | [['we', 'construct', 'for', 'the', 'first', 'time', 'the', 'sequences', 'of', 'stable', 'neutron', 'star', 'ns', 'models', 'capable', 'of', 'explaining', 'simultaneously', 'the', 'glitch', 'healing', 'parameters', 'q', 'of', 'both', 'the', 'pulsars', 'the', 'crab', 'q', 'geq', '07', 'and', 'the', 'vela', 'q', 'leq', '0... | [-0.08733484830306232, 0.15897359940870054, -0.03809782630002575, 0.10133875373761123, -0.0625756485578876, -0.06368620393298104, 0.07486251886529563, 0.325075136980273, -0.19953468961328485, -0.36264782814975205, 0.05591490598613002, -0.24714147417812887, 0.0057779583284617774, 0.29074971091229956, -0.0067597122516238... |
710.4443 | Are neutrino masses dynamically generated by quantum gravity
attractions? | It is argued that the quantum gravity attractions dynamically generate tiny
degenerate Majorana masses for the neutrinos. The unequal masses of the charged
leptons then induce a computable neutrino mass matrix with splittings and
mixings through the electroweak interactions. In this way the Standard Model
including q... | hep-th hep-ph | it is argued that the quantum gravity attractions dynamically generate tiny degenerate majorana masses for the neutrinos the unequal masses of the charged leptons then induce a computable neutrino mass matrix with splittings and mixings through the electroweak interactions in this way the standard model including quant... | [['it', 'is', 'argued', 'that', 'the', 'quantum', 'gravity', 'attractions', 'dynamically', 'generate', 'tiny', 'degenerate', 'majorana', 'masses', 'for', 'the', 'neutrinos', 'the', 'unequal', 'masses', 'of', 'the', 'charged', 'leptons', 'then', 'induce', 'a', 'computable', 'neutrino', 'mass', 'matrix', 'with', 'splitti... | [-0.11195586525249265, 0.39656165311293257, -0.01393330991437148, 0.26730661110712156, -0.048164771148754705, -0.2002131377361835, 0.013517968589439988, 0.2936608075134216, -0.2256266468715283, -0.31749917434588554, -0.023300159454060297, -0.2809003706600878, -0.06158677224753304, 0.13463899279539024, 0.046846332419062... |
710.4444 | Charge and Spin Transport in the One-dimensional Hubbard Model | In this paper we study the charge and spin currents transported by the
elementary excitations of the one-dimensional Hubbard model. The corresponding
current spectra are obtained by both analytic methods and numerical solution of
the Bethe-ansatz equations. For the case of half-filling, we find that the
spin-triplet ... | cond-mat.str-el | in this paper we study the charge and spin currents transported by the elementary excitations of the onedimensional hubbard model the corresponding current spectra are obtained by both analytic methods and numerical solution of the betheansatz equations for the case of halffilling we find that the spintriplet excitatio... | [['in', 'this', 'paper', 'we', 'study', 'the', 'charge', 'and', 'spin', 'currents', 'transported', 'by', 'the', 'elementary', 'excitations', 'of', 'the', 'onedimensional', 'hubbard', 'model', 'the', 'corresponding', 'current', 'spectra', 'are', 'obtained', 'by', 'both', 'analytic', 'methods', 'and', 'numerical', 'solut... | [-0.19560028479124109, 0.21923618101670098, -0.010960829630494117, 0.09440102242399007, -0.007754082127163808, -0.13961149954547486, 0.06412130405039837, 0.3521270220478376, -0.16756717878083388, -0.21325620516125735, 0.013011003700084985, -0.36201356709003446, -0.06140492394644146, 0.110998443858698, 0.134026371762156... |
710.4445 | On two pictures in the heuristic approach to gravity | We examine the heuristic approach to constant gravitational field by Dehnen,
H\"onl and Westpfahl, extending it everywhere beyond linear approximation. Then
it becomes flexible to accommodate possible modifications of General
Relativity. We have found that two pictures introduced in the related paper by
Thirring are ... | gr-qc | we examine the heuristic approach to constant gravitational field by dehnen honl and westpfahl extending it everywhere beyond linear approximation then it becomes flexible to accommodate possible modifications of general relativity we have found that two pictures introduced in the related paper by thirring are helpful ... | [['we', 'examine', 'the', 'heuristic', 'approach', 'to', 'constant', 'gravitational', 'field', 'by', 'dehnen', 'honl', 'and', 'westpfahl', 'extending', 'it', 'everywhere', 'beyond', 'linear', 'approximation', 'then', 'it', 'becomes', 'flexible', 'to', 'accommodate', 'possible', 'modifications', 'of', 'general', 'relati... | [-0.12297872367817612, 0.12591033690853418, -0.12465090502057195, 0.10175606139403369, -0.13784691392784082, -0.16540516158639793, -0.014044487410934553, 0.3350363303205028, -0.2229916082606429, -0.2852563271077261, 0.061317976773901293, -0.21255005052911916, -0.19980321021100123, 0.1716228088554335, -0.064909169021698... |
710.4446 | Comment on the history of the stretched exponential function | The original article of Rudolf Kohlrausch (1854) on stretched exponentials
and their application to describe relaxation phenomena has been often misquoted
in the literature after its rediscovery around 1984. We discuss here this fact
and attempt to set the record straight.
| physics.hist-ph | the original article of rudolf kohlrausch 1854 on stretched exponentials and their application to describe relaxation phenomena has been often misquoted in the literature after its rediscovery around 1984 we discuss here this fact and attempt to set the record straight | [['the', 'original', 'article', 'of', 'rudolf', 'kohlrausch', '1854', 'on', 'stretched', 'exponentials', 'and', 'their', 'application', 'to', 'describe', 'relaxation', 'phenomena', 'has', 'been', 'often', 'misquoted', 'in', 'the', 'literature', 'after', 'its', 'rediscovery', 'around', '1984', 'we', 'discuss', 'here', '... | [-0.04927197988145053, 0.04472068473696709, -0.129938605154166, 0.047380505022010765, -0.09085216242820024, -0.06355241348501295, 0.05315944822505116, 0.3724410191643983, -0.2688626187853515, -0.2969627087237313, 0.1796813217777526, -0.2811385650886223, -0.15269067231565714, 0.16924219061620532, -0.14251347937388345, 0... |
710.4447 | X-ray and optical followup of gamma-ray (up to TeV) sources | The imaging capabilities of the INTEGRAL and HESS observatories allow the
study of hard X-ray and TeV sources with unprecedented positional accuracy.
Here I review the multiwavelength followup studies which are currently being
performed on the unidentified sources detected by these facilities in order to
unveil their... | astro-ph | the imaging capabilities of the integral and hess observatories allow the study of hard xray and tev sources with unprecedented positional accuracy here i review the multiwavelength followup studies which are currently being performed on the unidentified sources detected by these facilities in order to unveil their act... | [['the', 'imaging', 'capabilities', 'of', 'the', 'integral', 'and', 'hess', 'observatories', 'allow', 'the', 'study', 'of', 'hard', 'xray', 'and', 'tev', 'sources', 'with', 'unprecedented', 'positional', 'accuracy', 'here', 'i', 'review', 'the', 'multiwavelength', 'followup', 'studies', 'which', 'are', 'currently', 'be... | [-0.08270338637640282, 0.08660515038087507, -0.032350433933339556, 0.11265154658075498, -0.1506137181909717, -0.06270471340691557, 0.06582592199651563, 0.48164420628121923, -0.17971958093611257, -0.4230077199789943, 0.15246513195820532, -0.3778540899558943, -0.03387153912715766, 0.20175370342117183, 0.05469703948129995... |
710.4448 | Spitzer-IRS high resolution spectroscopy of the 12\mu m Seyfert
galaxies: I. First results | The first high resolution Spitzer IRS 9-37um spectra of 29 Seyfert galaxies
(about one quarter) of the 12um Active Galaxy Sample are presented and
discussed. The high resolution spectroscopy was obtained with corresponding
off-source observations. This allows excellent background subtraction, so that
the continuum le... | astro-ph | the first high resolution spitzer irs 937um spectra of 29 seyfert galaxies about one quarter of the 12um active galaxy sample are presented and discussed the high resolution spectroscopy was obtained with corresponding offsource observations this allows excellent background subtraction so that the continuum levels and ... | [['the', 'first', 'high', 'resolution', 'spitzer', 'irs', '937um', 'spectra', 'of', '29', 'seyfert', 'galaxies', 'about', 'one', 'quarter', 'of', 'the', '12um', 'active', 'galaxy', 'sample', 'are', 'presented', 'and', 'discussed', 'the', 'high', 'resolution', 'spectroscopy', 'was', 'obtained', 'with', 'corresponding', ... | [-0.026322035776142595, 0.06691298236241998, -0.01681204584053566, 0.1009311229728303, -0.016590646912105555, -0.11620529364368538, 0.04034227590065796, 0.48706636626937594, -0.14379329013082293, -0.3333287988897673, 0.0436712599372087, -0.2996211373771188, 0.009340837958599116, 0.137919562219014, 0.01701531303115189, ... |
710.4449 | Characterization of researchers in condensed matter physics using simple
quantity based on h-index | Analysis of citation records of 52 active and productive condensed matter
physicists shows that the ratio of h-index to the mean age of h most highly
cited publications is a reliable quantity that allows meaningful comparison of
scientists of different age.
| physics.soc-ph | analysis of citation records of 52 active and productive condensed matter physicists shows that the ratio of hindex to the mean age of h most highly cited publications is a reliable quantity that allows meaningful comparison of scientists of different age | [['analysis', 'of', 'citation', 'records', 'of', '52', 'active', 'and', 'productive', 'condensed', 'matter', 'physicists', 'shows', 'that', 'the', 'ratio', 'of', 'hindex', 'to', 'the', 'mean', 'age', 'of', 'h', 'most', 'highly', 'cited', 'publications', 'is', 'a', 'reliable', 'quantity', 'that', 'allows', 'meaningful',... | [-0.0678056214386654, 0.15714999597247054, -0.1182505510542996, 0.13610143129566185, -0.14363627923970543, -0.12155870917230481, 0.10100449757968508, 0.35871061664528964, -0.1240492463935303, -0.43667676545134404, -0.02160075238746841, -0.3378603397928911, -0.06608143156939526, 0.20644353997961776, -0.10516166866461678... |
710.445 | HST/WFPC2 imaging of the circumnuclear structure of LLAGNs. I Data and
nuclear morphology | To advance our knowledge of the nature of the central source in LLAGNs and
its relation with stellar clusters, we are carrying out several imaging
projects with HST at near-UV, optical and near-IR wavelengths. In this paper,
we present the first results obtained with observations of the central regions
of 57 LLAGNs i... | astro-ph | to advance our knowledge of the nature of the central source in llagns and its relation with stellar clusters we are carrying out several imaging projects with hst at nearuv optical and nearir wavelengths in this paper we present the first results obtained with observations of the central regions of 57 llagns imaged wi... | [['to', 'advance', 'our', 'knowledge', 'of', 'the', 'nature', 'of', 'the', 'central', 'source', 'in', 'llagns', 'and', 'its', 'relation', 'with', 'stellar', 'clusters', 'we', 'are', 'carrying', 'out', 'several', 'imaging', 'projects', 'with', 'hst', 'at', 'nearuv', 'optical', 'and', 'nearir', 'wavelengths', 'in', 'this... | [-0.03035194240878091, 0.08123297319296142, -0.05514757949532124, 0.08800764427185385, -0.03479928061970624, -0.04959208368601506, -0.006750781303925211, 0.47642725349256865, -0.14891995456429166, -0.3273639576346205, 0.09270094612882913, -0.3120070241457015, -0.0462978994375781, 0.2042394492174744, -0.0484453712777937... |
710.4451 | Measurements of e+e- -> K+K-eta, K+K-pi0 and KsK+pi- Cross Sections
Using Initial State Radiation Events | This paper reports measurements of processes: e+e- -> gamma KsK+pi-, e+e- ->
gamma K+K-pi0, e+e- -> gamma phi eta, and e+e- -> gamma phi pi0. The initial
state radiated photon allows to cover the hadronic final state in the energy
range from thresholds up to ~4.6 GeV. The overall size of the data sample
analyzed is 2... | hep-ex | this paper reports measurements of processes ee gamma kskpi ee gamma kkpi0 ee gamma phi eta and ee gamma phi pi0 the initial state radiated photon allows to cover the hadronic final state in the energy range from thresholds up to 46 gev the overall size of the data sample analyzed is 232 fb1 collected by the babar dete... | [['this', 'paper', 'reports', 'measurements', 'of', 'processes', 'ee', 'gamma', 'kskpi', 'ee', 'gamma', 'kkpi0', 'ee', 'gamma', 'phi', 'eta', 'and', 'ee', 'gamma', 'phi', 'pi0', 'the', 'initial', 'state', 'radiated', 'photon', 'allows', 'to', 'cover', 'the', 'hadronic', 'final', 'state', 'in', 'the', 'energy', 'range',... | [-0.12251113430673456, 0.1908993468363613, -0.13439878472595806, 0.0654816765658349, -0.005785267081286683, -0.10015535155536244, 0.09524037850616462, 0.29055369842872525, -0.21468020046767372, -0.2502088262168253, -0.07923414138842674, -0.40489830412511674, 0.055777538634974186, 0.16457243032609706, 0.141445886387471,... |
710.4452 | f0(1370) | A summary is given of the main sets of data requiring the existence of
f0(1370). Crystal Barrel data on pbar-p -> eta eta pizero contain a visible
f0(1370) peak and require at least a 19 standard deviation contribution. This
alone is sufficient to demonstrate its existence. More extensive data on pbar-p
-> 3pizero at... | hep-ex | a summary is given of the main sets of data requiring the existence of f01370 crystal barrel data on pbarp eta eta pizero contain a visible f01370 peak and require at least a 19 standard deviation contribution this alone is sufficient to demonstrate its existence more extensive data on pbarp 3pizero at rest contain del... | [['a', 'summary', 'is', 'given', 'of', 'the', 'main', 'sets', 'of', 'data', 'requiring', 'the', 'existence', 'of', 'f01370', 'crystal', 'barrel', 'data', 'on', 'pbarp', 'eta', 'eta', 'pizero', 'contain', 'a', 'visible', 'f01370', 'peak', 'and', 'require', 'at', 'least', 'a', '19', 'standard', 'deviation', 'contribution... | [-0.11335909088585877, 0.2001909640728584, -0.052520158242316935, 0.09655901015915827, -0.042588002361700045, -0.1302300219657358, 0.07310685329505895, 0.3510199851965106, -0.1442170784383367, -0.32248235087269755, 0.022326652194358643, -0.36967579469700734, 0.049792003803189815, 0.16564538702368736, 0.0292656216898742... |
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