id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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707.083 | A New Look at Mode Conversion in a Stratified Isothermal Atmosphere | Recent numerical investigations of wave propagation near coronal magnetic
null points (McLaughlin and Hood: Astron. Astrophys. 459, 641,2006) have
indicated how a fast MHD wave partially converts into a slow MHD wave as the
disturbance passes from a low-beta plasma to a high-beta plasma. This is a
complex process and... | astro-ph | recent numerical investigations of wave propagation near coronal magnetic null points mclaughlin and hood astron astrophys 459 6412006 have indicated how a fast mhd wave partially converts into a slow mhd wave as the disturbance passes from a lowbeta plasma to a highbeta plasma this is a complex process and a clear und... | [['recent', 'numerical', 'investigations', 'of', 'wave', 'propagation', 'near', 'coronal', 'magnetic', 'null', 'points', 'mclaughlin', 'and', 'hood', 'astron', 'astrophys', '459', '6412006', 'have', 'indicated', 'how', 'a', 'fast', 'mhd', 'wave', 'partially', 'converts', 'into', 'a', 'slow', 'mhd', 'wave', 'as', 'the',... | [-0.1746976719963748, 0.15636100008947218, -0.050914553617236805, 0.022691610832132083, -0.09322907035376, -0.0537809717181303, 0.05052450158965418, 0.3415808999253547, -0.17472179357440942, -0.28761311897987446, 0.08159626737367087, -0.2353625038479496, -0.12075760264826171, 0.23843736691325082, 0.027187281839467364, ... |
707.0831 | Half-space theorem, embedded minimal annuli and minimal graphs in the
Heisenberg group | We construct a one-parameter family of properly embedded minimal annuli in
the Heisenberg group Nil_3 endowed with a left-invariant Riemannian metric.
These annuli are not rotationally invariant. This family gives a vertical
half-space theorem and proves that each complete minimal graph in Nil_3 is
entire. Also, the ... | math.DG | we construct a oneparameter family of properly embedded minimal annuli in the heisenberg group nil_3 endowed with a leftinvariant riemannian metric these annuli are not rotationally invariant this family gives a vertical halfspace theorem and proves that each complete minimal graph in nil_3 is entire also the sister su... | [['we', 'construct', 'a', 'oneparameter', 'family', 'of', 'properly', 'embedded', 'minimal', 'annuli', 'in', 'the', 'heisenberg', 'group', 'nil_3', 'endowed', 'with', 'a', 'leftinvariant', 'riemannian', 'metric', 'these', 'annuli', 'are', 'not', 'rotationally', 'invariant', 'this', 'family', 'gives', 'a', 'vertical', '... | [-0.20524262278340757, 0.10589076263859169, -0.03137163902167231, 0.05955275124870241, -0.0798892060876824, -0.12294114471413195, -0.028405399657785893, 0.4386811307771131, -0.261262834565714, -0.22011242476291953, 0.09333284779917449, -0.28177072580903767, -0.1016268432000652, 0.13574526231270284, -0.1466718081315048,... |
707.0832 | HESS J1616-508: likely powered by PSR J1617-5055 | HESS J1616-508 is one of the brightest emitters in the TeV sky. Recent
observations with the IBIS/ISGRI telescope on board the INTEGRAL spacecraft
have revealed that a young, nearby and energetic pulsar, PSR J1617-5055, is a
powerful emitter of soft gamma-rays in the 20-100 keV domain. In this paper we
present an ana... | astro-ph | hess j1616508 is one of the brightest emitters in the tev sky recent observations with the ibisisgri telescope on board the integral spacecraft have revealed that a young nearby and energetic pulsar psr j16175055 is a powerful emitter of soft gammarays in the 20100 kev domain in this paper we present an analysis of all... | [['hess', 'j1616508', 'is', 'one', 'of', 'the', 'brightest', 'emitters', 'in', 'the', 'tev', 'sky', 'recent', 'observations', 'with', 'the', 'ibisisgri', 'telescope', 'on', 'board', 'the', 'integral', 'spacecraft', 'have', 'revealed', 'that', 'a', 'young', 'nearby', 'and', 'energetic', 'pulsar', 'psr', 'j16175055', 'is... | [-0.052345896551091314, 0.11811706744808807, -0.05669647351367142, 0.14688382387221166, -0.13804012360674753, -0.08562723706012677, 0.03776765833696483, 0.46416725681229615, -0.21434676227944993, -0.35530067007661364, 0.058402087096666534, -0.35414279640406743, 0.008594958192501296, 0.27262065426356874, -0.001993054209... |
707.0833 | Kirzhnits gradient expansion for a D-dimensional Fermi gas | For an ideal D-dimensional Fermi gas under generic external confinement we
derive the correcting coefficient $(D-2)/3D$ of the von Weizsacker term in the
kinetic energy density. To obtain this coefficient we use the Kirzhnits
semiclassical expansion of the number operator up to the second order in the
Planck constant... | cond-mat.stat-mech cond-mat.other | for an ideal ddimensional fermi gas under generic external confinement we derive the correcting coefficient d23d of the von weizsacker term in the kinetic energy density to obtain this coefficient we use the kirzhnits semiclassical expansion of the number operator up to the second order in the planck constant hbar with... | [['for', 'an', 'ideal', 'ddimensional', 'fermi', 'gas', 'under', 'generic', 'external', 'confinement', 'we', 'derive', 'the', 'correcting', 'coefficient', 'd23d', 'of', 'the', 'von', 'weizsacker', 'term', 'in', 'the', 'kinetic', 'energy', 'density', 'to', 'obtain', 'this', 'coefficient', 'we', 'use', 'the', 'kirzhnits'... | [-0.13961758386223377, 0.1078120224621589, -0.06837773208213405, 0.056473261442590045, -0.02177641974510939, -0.06451327284651526, 0.023419605432015458, 0.27976241867382373, -0.2701663036877813, -0.25156402211175877, 0.014618634188736088, -0.30013343191632397, -0.07430912992194964, 0.1308727588823714, 0.006409726479729... |
707.0834 | Interaction, Change, and Wholeness of Material Things | Interaction is the mode of being of material things amid other material
things and the driving force of change and wholeness. Through mutual influence,
changes of interacting things become interdependent and their properties
interrelated, which leads to formation of ensembles - material wholes of
correlated things, w... | physics.gen-ph | interaction is the mode of being of material things amid other material things and the driving force of change and wholeness through mutual influence changes of interacting things become interdependent and their properties interrelated which leads to formation of ensembles material wholes of correlated things where the... | [['interaction', 'is', 'the', 'mode', 'of', 'being', 'of', 'material', 'things', 'amid', 'other', 'material', 'things', 'and', 'the', 'driving', 'force', 'of', 'change', 'and', 'wholeness', 'through', 'mutual', 'influence', 'changes', 'of', 'interacting', 'things', 'become', 'interdependent', 'and', 'their', 'propertie... | [-0.19623726985796733, 0.22353429501419197, -0.08386657625454029, -0.045074222440167365, -0.07783308038398429, -0.11320850755846887, 0.03670116574869974, 0.33688137400895357, -0.2864124139563905, -0.2675478053214546, 0.08755847787122345, -0.3475736016235142, -0.15830982219065642, 0.13703989795909297, 0.0111996559792681... |
707.0835 | The Euler characteristic of a category as the sum of a divergent series | The Euler characteristic of a cell complex is often thought of as the
alternating sum of the number of cells of each dimension. When the complex is
infinite, the sum diverges. Nevertheless, it can sometimes be evaluated; in
particular, this is possible when the complex is the nerve of a finite
category. This provides... | math.CT math.AT | the euler characteristic of a cell complex is often thought of as the alternating sum of the number of cells of each dimension when the complex is infinite the sum diverges nevertheless it can sometimes be evaluated in particular this is possible when the complex is the nerve of a finite category this provides an alter... | [['the', 'euler', 'characteristic', 'of', 'a', 'cell', 'complex', 'is', 'often', 'thought', 'of', 'as', 'the', 'alternating', 'sum', 'of', 'the', 'number', 'of', 'cells', 'of', 'each', 'dimension', 'when', 'the', 'complex', 'is', 'infinite', 'the', 'sum', 'diverges', 'nevertheless', 'it', 'can', 'sometimes', 'be', 'eva... | [-0.15098155475523625, 0.12025970723531114, -0.07243817249262655, 0.08513323308088237, -0.08179639099162651, -0.10540421370643417, -0.03671337923387418, 0.2988560191682867, -0.3306371933163924, -0.21205591889274483, 0.11366346596450722, -0.20468430225485684, -0.17677490576799657, 0.20121517678017956, -0.110121120837189... |
707.0836 | Repr\'esentations de Springer pour les groupes de r\'eflexions complexes
imprimitifs | To a spetsial complex reflection group, equipped with a root lattice in the
sense of Nebe, we attach a certain finite set playing a role which is analogous
to the role of the set of unipotent classes of an algebraic group. In the case
of imprimitive groups, we give a combinatoric parametrization of it in terms of
Mal... | math.RT | to a spetsial complex reflection group equipped with a root lattice in the sense of nebe we attach a certain finite set playing a role which is analogous to the role of the set of unipotent classes of an algebraic group in the case of imprimitive groups we give a combinatoric parametrization of it in terms of malleshoj... | [['to', 'a', 'spetsial', 'complex', 'reflection', 'group', 'equipped', 'with', 'a', 'root', 'lattice', 'in', 'the', 'sense', 'of', 'nebe', 'we', 'attach', 'a', 'certain', 'finite', 'set', 'playing', 'a', 'role', 'which', 'is', 'analogous', 'to', 'the', 'role', 'of', 'the', 'set', 'of', 'unipotent', 'classes', 'of', 'an... | [-0.25186506379395723, 0.018388981702800438, -0.19927161791160503, 0.055008617043495175, -0.13742190667906323, -0.09455399482536155, -0.17836530220166252, 0.09514767687541206, -0.1687927309842151, -0.27436016723010187, 0.01811885278942567, -0.32454431516596594, -0.2323939711912661, 0.16518808106413563, -0.3212298241318... |
707.0837 | Explicit Formula for Constructing Binomial Confidence Interval with
Guaranteed Coverage Probability | In this paper, we derive an explicit formula for constructing the confidence
interval of binomial parameter with guaranteed coverage probability. The
formula overcomes the limitation of normal approximation which is asymptotic in
nature and thus inevitably introduce unknown errors in applications. Moreover,
the formu... | math.ST math.PR stat.ME stat.TH | in this paper we derive an explicit formula for constructing the confidence interval of binomial parameter with guaranteed coverage probability the formula overcomes the limitation of normal approximation which is asymptotic in nature and thus inevitably introduce unknown errors in applications moreover the formula is ... | [['in', 'this', 'paper', 'we', 'derive', 'an', 'explicit', 'formula', 'for', 'constructing', 'the', 'confidence', 'interval', 'of', 'binomial', 'parameter', 'with', 'guaranteed', 'coverage', 'probability', 'the', 'formula', 'overcomes', 'the', 'limitation', 'of', 'normal', 'approximation', 'which', 'is', 'asymptotic', ... | [-0.0910788505885599, -0.0003998283958738997, -0.10866648409314253, 0.1045810880872572, -0.08369887756133401, -0.13685166942761154, 0.1694736100774183, 0.36104021230209116, -0.19297025284440433, -0.3321901515528962, 0.08662669989595038, -0.21686125960125513, -0.1548510288970696, 0.22036664512927165, -0.1201541797260712... |
707.0838 | Membrane instantons from mirror symmetry | We use mirror symmetry to determine and sum up a class of membrane instanton
corrections to the hypermultiplet moduli space metric arising in Calabi-Yau
threefold compactifications of type IIA strings. These corrections are mirror
to the D1 and D(-1)-brane instantons on the IIB side and are given explicitly
in terms ... | hep-th | we use mirror symmetry to determine and sum up a class of membrane instanton corrections to the hypermultiplet moduli space metric arising in calabiyau threefold compactifications of type iia strings these corrections are mirror to the d1 and d1brane instantons on the iib side and are given explicitly in terms of a sin... | [['we', 'use', 'mirror', 'symmetry', 'to', 'determine', 'and', 'sum', 'up', 'a', 'class', 'of', 'membrane', 'instanton', 'corrections', 'to', 'the', 'hypermultiplet', 'moduli', 'space', 'metric', 'arising', 'in', 'calabiyau', 'threefold', 'compactifications', 'of', 'type', 'iia', 'strings', 'these', 'corrections', 'are... | [-0.18419616579820838, 0.13299245083309663, -0.04628547575749174, 0.12639116767729056, -0.10434845045998786, -0.16410181111408562, -0.0005882348028259187, 0.2795569065816795, -0.21023104361058037, -0.25441259614934647, 0.09900014378171697, -0.2899635960141645, -0.1773573858309773, 0.09748036969641719, -0.17677508110675... |
707.0839 | A Gravitational Wave Background from Reheating after Hybrid Inflation | The reheating of the universe after hybrid inflation proceeds through the
nucleation and subsequent collision of large concentrations of energy density
in the form of bubble-like structures moving at relativistic speeds. This
generates a significant fraction of energy in the form of a stochastic
background of gravita... | hep-ph | the reheating of the universe after hybrid inflation proceeds through the nucleation and subsequent collision of large concentrations of energy density in the form of bubblelike structures moving at relativistic speeds this generates a significant fraction of energy in the form of a stochastic background of gravitation... | [['the', 'reheating', 'of', 'the', 'universe', 'after', 'hybrid', 'inflation', 'proceeds', 'through', 'the', 'nucleation', 'and', 'subsequent', 'collision', 'of', 'large', 'concentrations', 'of', 'energy', 'density', 'in', 'the', 'form', 'of', 'bubblelike', 'structures', 'moving', 'at', 'relativistic', 'speeds', 'this'... | [-0.1473980437857361, 0.22842836381012807, -0.10289069555611127, 0.13300847117296624, -0.09676240436285251, -0.07492657684195923, -0.001314069716047165, 0.30697765631109347, -0.24890534578745951, -0.3003948266492971, 0.09236998651761287, -0.2469052833046873, -0.08873616147068736, 0.2315367170926022, 0.05021839776606545... |
707.084 | Fredholm Modules on P.C.F. Self-Similar Fractals and their Conformal
Geometry | The aim of the present work is to show how, using the differential calculus
associated to Dirichlet forms, it is possible to construct Fredholm modules on
post critically finite fractals by regular harmonic structures. The modules are
d-summable, the summability exponent d coinciding with the spectral dimension
of th... | math.FA math.OA | the aim of the present work is to show how using the differential calculus associated to dirichlet forms it is possible to construct fredholm modules on post critically finite fractals by regular harmonic structures the modules are dsummable the summability exponent d coinciding with the spectral dimension of the gener... | [['the', 'aim', 'of', 'the', 'present', 'work', 'is', 'to', 'show', 'how', 'using', 'the', 'differential', 'calculus', 'associated', 'to', 'dirichlet', 'forms', 'it', 'is', 'possible', 'to', 'construct', 'fredholm', 'modules', 'on', 'post', 'critically', 'finite', 'fractals', 'by', 'regular', 'harmonic', 'structures', ... | [-0.107367049412278, 0.08768260690849275, -0.12720062802545726, 0.10919936781137948, -0.13678553955178357, -0.1324429631815292, -0.08024768777249847, 0.33771907272748647, -0.3446128336276161, -0.17092640868504533, 0.11691996891750023, -0.2560417678556405, -0.1949403770675417, 0.16299524795031176, -0.08276416247244925, ... |
707.0841 | Neutrino masses, mixing and leptogenesis in TeV scale B-L extension of
the standard model | We address the issue of the neutrino masses and mixing in TeV scale $B-L$
extension of the Standard Model. We show that if Dirac neutrino masses are of
order $10^{-4}$ Gev, then the measured neutrino masses are correctly obtained.
We propose a mass relation between quarks and leptons that may account for such
small D... | hep-ph | we address the issue of the neutrino masses and mixing in tev scale bl extension of the standard model we show that if dirac neutrino masses are of order 104 gev then the measured neutrino masses are correctly obtained we propose a mass relation between quarks and leptons that may account for such small dirac neutrino ... | [['we', 'address', 'the', 'issue', 'of', 'the', 'neutrino', 'masses', 'and', 'mixing', 'in', 'tev', 'scale', 'bl', 'extension', 'of', 'the', 'standard', 'model', 'we', 'show', 'that', 'if', 'dirac', 'neutrino', 'masses', 'are', 'of', 'order', '104', 'gev', 'then', 'the', 'measured', 'neutrino', 'masses', 'are', 'correc... | [-0.08897886047227763, 0.31281058700007247, 0.0041735492258032, 0.2403256667660564, -0.08849153592889233, -0.18228101754363069, 0.06591015723423929, 0.3457698484105388, -0.19432917606877528, -0.3202763419739506, 0.002561960655345222, -0.2634605656223973, -0.02349537543541803, 0.13747825072968275, 0.03566718687519695, 0... |
707.0842 | Classical approximation to quantum cosmological correlations | We investigate up to which order quantum effects can be neglected in
calculating cosmological correlation functions after horizon exit. As a toy
model, we study $\phi^3$ theory on a de Sitter background for a massless
minimally coupled scalar field $\phi$. We find that for tree level and one loop
contributions in the... | hep-th astro-ph gr-qc hep-ph | we investigate up to which order quantum effects can be neglected in calculating cosmological correlation functions after horizon exit as a toy model we study phi3 theory on a de sitter background for a massless minimally coupled scalar field phi we find that for tree level and one loop contributions in the quantum the... | [['we', 'investigate', 'up', 'to', 'which', 'order', 'quantum', 'effects', 'can', 'be', 'neglected', 'in', 'calculating', 'cosmological', 'correlation', 'functions', 'after', 'horizon', 'exit', 'as', 'a', 'toy', 'model', 'we', 'study', 'phi3', 'theory', 'on', 'a', 'de', 'sitter', 'background', 'for', 'a', 'massless', '... | [-0.09703365947081855, 0.19126471924881674, -0.1327701389733679, 0.15417149164229815, -0.07253260932180404, -0.14988535245543919, 0.007591832494870345, 0.31780909136554925, -0.23928082608479526, -0.29123822925151277, 0.0819718315119689, -0.2750746592911569, -0.12435462253426413, 0.19198886104767202, -0.0179737246327913... |
707.0843 | Two chiral nonet model with massless quarks | We present a detailed study of a linear sigma model containing one chiral
nonet transforming under U(1)$_A$ as a quark-antiquark composite and another
chiral nonet transforming as a diquark-anti diquark composite (or, equivalently
from a symmetry point of view, as a two meson molecule). The model provides an
intuitiv... | hep-ph | we present a detailed study of a linear sigma model containing one chiral nonet transforming under u1_a as a quarkantiquark composite and another chiral nonet transforming as a diquarkanti diquark composite or equivalently from a symmetry point of view as a two meson molecule the model provides an intuitive explanation... | [['we', 'present', 'a', 'detailed', 'study', 'of', 'a', 'linear', 'sigma', 'model', 'containing', 'one', 'chiral', 'nonet', 'transforming', 'under', 'u1_a', 'as', 'a', 'quarkantiquark', 'composite', 'and', 'another', 'chiral', 'nonet', 'transforming', 'as', 'a', 'diquarkanti', 'diquark', 'composite', 'or', 'equivalentl... | [-0.1066649898842814, 0.3002319979462559, -0.11027230805568937, 0.1225563120091298, -0.08778637145749396, -0.19464814575200062, 0.033878547952685883, 0.32985932357015385, -0.1447132196466344, -0.24960256838532174, 0.009141146949973804, -0.31806483451762924, -0.041276480661759124, 0.054459786954772285, 0.086038668421749... |
707.0844 | Spherical Needlets for CMB Data Analysis | We discuss Spherical Needlets and their properties. Needlets are a form of
spherical wavelets which do not rely on any kind of tangent plane approximation
and enjoy good localization properties in both pixel and harmonic space;
moreover needlets coefficients are asymptotically uncorrelated at any fixed
angular distan... | astro-ph | we discuss spherical needlets and their properties needlets are a form of spherical wavelets which do not rely on any kind of tangent plane approximation and enjoy good localization properties in both pixel and harmonic space moreover needlets coefficients are asymptotically uncorrelated at any fixed angular distance w... | [['we', 'discuss', 'spherical', 'needlets', 'and', 'their', 'properties', 'needlets', 'are', 'a', 'form', 'of', 'spherical', 'wavelets', 'which', 'do', 'not', 'rely', 'on', 'any', 'kind', 'of', 'tangent', 'plane', 'approximation', 'and', 'enjoy', 'good', 'localization', 'properties', 'in', 'both', 'pixel', 'and', 'harm... | [-0.06168422946643274, 0.046579007161939044, -0.13514567337440864, 0.10900026194132682, -0.1363420180179242, -0.1027987476663222, -0.017418257663247443, 0.43317098369411494, -0.2333329933206156, -0.25258262013479815, 0.15369564509492809, -0.2764998375678877, -0.13349916539707427, 0.25185098547302975, -0.037365096342015... |
707.0845 | Logarithmic limit sets of real semi-algebraic sets | This paper is about the logarithmic limit sets of real semi-algebraic sets,
and, more generally, about the logarithmic limit sets of sets definable in an
o-minimal, polynomially bounded structure. We prove that most of the properties
of the logarithmic limit sets of complex algebraic sets hold in the real case.
This ... | math.AG | this paper is about the logarithmic limit sets of real semialgebraic sets and more generally about the logarithmic limit sets of sets definable in an ominimal polynomially bounded structure we prove that most of the properties of the logarithmic limit sets of complex algebraic sets hold in the real case this include th... | [['this', 'paper', 'is', 'about', 'the', 'logarithmic', 'limit', 'sets', 'of', 'real', 'semialgebraic', 'sets', 'and', 'more', 'generally', 'about', 'the', 'logarithmic', 'limit', 'sets', 'of', 'sets', 'definable', 'in', 'an', 'ominimal', 'polynomially', 'bounded', 'structure', 'we', 'prove', 'that', 'most', 'of', 'the... | [-0.16119586699136088, 0.03640955646941607, -0.09114612419954568, 0.14488117478322238, -0.055127219499453255, -0.006503380484123161, 0.025825568001997402, 0.26493095441896847, -0.34734156433040736, -0.20977244258898756, 0.0930649079821086, -0.2823917908809971, -0.17602570381933363, 0.255754679441452, -0.113144255681908... |
707.0846 | Solitons in interacting Dicke models of coupled cavities with two-level
systems | We consider an array of coupled optical cavities, each containing a
multi-atom ensemble. We show that the nonlinearity inherent in the cooperative
dynamics of the atoms in each ensemble coupled to the respective cavity field
allows for the formation of solitary waves. Such a prediction can be tested in
state-of-the-a... | quant-ph | we consider an array of coupled optical cavities each containing a multiatom ensemble we show that the nonlinearity inherent in the cooperative dynamics of the atoms in each ensemble coupled to the respective cavity field allows for the formation of solitary waves such a prediction can be tested in stateoftheart semico... | [['we', 'consider', 'an', 'array', 'of', 'coupled', 'optical', 'cavities', 'each', 'containing', 'a', 'multiatom', 'ensemble', 'we', 'show', 'that', 'the', 'nonlinearity', 'inherent', 'in', 'the', 'cooperative', 'dynamics', 'of', 'the', 'atoms', 'in', 'each', 'ensemble', 'coupled', 'to', 'the', 'respective', 'cavity', ... | [-0.18293831787637568, 0.13729823549744782, 0.006263925922602149, -0.0404282758078937, 0.02585000916899714, -0.19001964346638747, -0.039718368537640866, 0.45704987781521467, -0.22729672927276365, -0.23665965330188296, 0.017699067474625605, -0.3072959992945731, -0.1399806951438742, 0.148699813730283, 0.01536548399599269... |
707.0847 | Stochastic Inflationary Scalar Electrodynamics | We stochastically formulate the theory of scalar quantum electrodynamics on a
de Sitter background. This reproduces the leading infrared logarithms at each
loop order. It also allows one to sum the series of leading infrared logarithms
to obtain explicit, nonperturbative results about the late time behavior of the
sy... | gr-qc astro-ph hep-ph | we stochastically formulate the theory of scalar quantum electrodynamics on a de sitter background this reproduces the leading infrared logarithms at each loop order it also allows one to sum the series of leading infrared logarithms to obtain explicit nonperturbative results about the late time behavior of the system ... | [['we', 'stochastically', 'formulate', 'the', 'theory', 'of', 'scalar', 'quantum', 'electrodynamics', 'on', 'a', 'de', 'sitter', 'background', 'this', 'reproduces', 'the', 'leading', 'infrared', 'logarithms', 'at', 'each', 'loop', 'order', 'it', 'also', 'allows', 'one', 'to', 'sum', 'the', 'series', 'of', 'leading', 'i... | [-0.15158643815113176, 0.17565900530426368, -0.11994441184630193, 0.09955878566033069, -0.06913657230094518, -0.11456554293134573, -0.0009061655197938037, 0.29201521986800405, -0.16153301243292223, -0.3085544505848153, 0.06027569632290282, -0.2792374252545991, -0.10885291350175544, 0.1529966184436021, -0.01845962255455... |
707.0848 | No-local-broadcasting theorem for quantum correlations | We prove that the correlations present in a multipartite quantum state have
an \emph{operational} quantum character as soon as the state does not simply
encode a multipartite classical probability distribution, i.e. does not
describe the joint state of many classical registers. Even unentangled states
may exhibit suc... | quant-ph | we prove that the correlations present in a multipartite quantum state have an emphoperational quantum character as soon as the state does not simply encode a multipartite classical probability distribution ie does not describe the joint state of many classical registers even unentangled states may exhibit such emphqua... | [['we', 'prove', 'that', 'the', 'correlations', 'present', 'in', 'a', 'multipartite', 'quantum', 'state', 'have', 'an', 'emphoperational', 'quantum', 'character', 'as', 'soon', 'as', 'the', 'state', 'does', 'not', 'simply', 'encode', 'a', 'multipartite', 'classical', 'probability', 'distribution', 'ie', 'does', 'not', ... | [-0.14371194326035355, 0.14377920218649323, -0.14968161332839425, 0.10228033327544783, 0.0013073141403172326, -0.20153498679291512, 0.08702548402547161, 0.31114584553068964, -0.2979515099786627, -0.23972787279500693, 0.0424315018108641, -0.2662915391037646, -0.12447607470001432, 0.18931526456034972, -0.0796582880716743... |
707.0849 | Deposition of Atoms on a Quasicrystalline Substrate: Molecular-Dynamics
Study in 3 Dimensions | We study the three-dimensional structure formation when atoms are deposited
onto a substrate with a decagonal quasicrystalline order.
Molecular-dynamicscalculations show that the adsorbate layer consists of
ordered nano-scale domains with orientations determined by the underlying
substrate symmetry. Depending on the ... | cond-mat.mtrl-sci cond-mat.soft | we study the threedimensional structure formation when atoms are deposited onto a substrate with a decagonal quasicrystalline order moleculardynamicscalculations show that the adsorbate layer consists of ordered nanoscale domains with orientations determined by the underlying substrate symmetry depending on the relativ... | [['we', 'study', 'the', 'threedimensional', 'structure', 'formation', 'when', 'atoms', 'are', 'deposited', 'onto', 'a', 'substrate', 'with', 'a', 'decagonal', 'quasicrystalline', 'order', 'moleculardynamicscalculations', 'show', 'that', 'the', 'adsorbate', 'layer', 'consists', 'of', 'ordered', 'nanoscale', 'domains', '... | [-0.11706216897863637, 0.2103976142865702, -0.007616492715395248, -0.0693789679268054, -0.006669634615938212, -0.09176008790683259, 0.0602305588123774, 0.4350119530128472, -0.31235265765933257, -0.33859132850895923, -0.025828462672130816, -0.2887526498786334, -0.12497847135467775, 0.11282862111091099, 0.074056455423927... |
707.085 | Regular and Completely Regular Differential Operators | We define the concept of completely regular ordinary differential operators
and give various criteria for operators to belong to this class. We give also
criteria for Birkhof regularity of ordinary differential operators in terms of
the growth of the Green function and basis property.
| math.SP math.OA | we define the concept of completely regular ordinary differential operators and give various criteria for operators to belong to this class we give also criteria for birkhof regularity of ordinary differential operators in terms of the growth of the green function and basis property | [['we', 'define', 'the', 'concept', 'of', 'completely', 'regular', 'ordinary', 'differential', 'operators', 'and', 'give', 'various', 'criteria', 'for', 'operators', 'to', 'belong', 'to', 'this', 'class', 'we', 'give', 'also', 'criteria', 'for', 'birkhof', 'regularity', 'of', 'ordinary', 'differential', 'operators', 'i... | [-0.10351364024330018, 0.03717617393839498, -0.1004881638123892, 0.11974813088200727, -0.0957153076847452, -0.07649038103950578, -0.005502573192812676, 0.2888689547842152, -0.29449453070586507, -0.2553385400408229, 0.13739454514769361, -0.2541635447983132, -0.1798256187764711, 0.18441038481284713, -0.07238723536910013,... |
707.0851 | Determinant of the SU(N) caloron with nontrivial holonomy | The 1-loop quantum weight of the SU(N) KvBLL caloron with nontrivial holonomy
is calculated. The latter is the most general self-dual solution with unit
topological charge in the 4d Yang-Mills theory with one compactified dimension
(finite temperature).
| hep-th | the 1loop quantum weight of the sun kvbll caloron with nontrivial holonomy is calculated the latter is the most general selfdual solution with unit topological charge in the 4d yangmills theory with one compactified dimension finite temperature | [['the', '1loop', 'quantum', 'weight', 'of', 'the', 'sun', 'kvbll', 'caloron', 'with', 'nontrivial', 'holonomy', 'is', 'calculated', 'the', 'latter', 'is', 'the', 'most', 'general', 'selfdual', 'solution', 'with', 'unit', 'topological', 'charge', 'in', 'the', '4d', 'yangmills', 'theory', 'with', 'one', 'compactified', ... | [-0.1469707924847466, 0.25983282329665647, -0.0247243122764819, 0.06080502216905557, -0.06000468896299198, -0.19407045659986702, -0.07580380521500735, 0.2731915100641247, -0.16576367228077976, -0.1782522691866836, 0.045651708776760544, -0.3257813565936443, -0.1630911779766147, 0.06351429674573042, -0.03966205331144502,... |
707.0852 | The CH2CN- molecule: Carrier of the lambda8037 diffuse interstellar
band? | The hypothesis that the cyanomethyl anion CH2CN- is responsible for the
relatively narrow diffuse interstellar band (DIB) at 8037.8 +- 0.15 Angstroms
is examined with reference to new observational data. The 0_0^0 absorption band
arising from the ^1B_1 - X ^1A' transition from the electronic ground state to
the first... | astro-ph | the hypothesis that the cyanomethyl anion ch2cn is responsible for the relatively narrow diffuse interstellar band dib at 80378 015 angstroms is examined with reference to new observational data the 0_00 absorption band arising from the 1b_1 x 1a transition from the electronic ground state to the first dipolebound stat... | [['the', 'hypothesis', 'that', 'the', 'cyanomethyl', 'anion', 'ch2cn', 'is', 'responsible', 'for', 'the', 'relatively', 'narrow', 'diffuse', 'interstellar', 'band', 'dib', 'at', '80378', '015', 'angstroms', 'is', 'examined', 'with', 'reference', 'to', 'new', 'observational', 'data', 'the', '0_00', 'absorption', 'band',... | [-0.07388921535854774, 0.1194958077119534, -0.01817655688398645, 0.01446332297304512, -0.03005418977108858, -0.14390781742247147, 0.09102683811492863, 0.44670494265174343, -0.22422741295812312, -0.2935389734270829, 0.0032847301146599448, -0.3011510997330622, -0.007783239828385708, 0.13612207184667655, 0.047681774602465... |
707.0853 | Spectral isolation of naturally reductive metrics on simple Lie groups | We show that within the class of left-invariant naturally reductive metrics
$\mathcal{M}_{\operatorname{Nat}}(G)$ on a compact simple Lie group $G$, every
metric is spectrally isolated. We also observe that any collection of
isospectral compact symmetric spaces is finite; this follows from a somewhat
stronger stateme... | math.DG math.SP | we show that within the class of leftinvariant naturally reductive metrics mathcalm_operatornamenatg on a compact simple lie group g every metric is spectrally isolated we also observe that any collection of isospectral compact symmetric spaces is finite this follows from a somewhat stronger statement involving only a ... | [['we', 'show', 'that', 'within', 'the', 'class', 'of', 'leftinvariant', 'naturally', 'reductive', 'metrics', 'mathcalm_operatornamenatg', 'on', 'a', 'compact', 'simple', 'lie', 'group', 'g', 'every', 'metric', 'is', 'spectrally', 'isolated', 'we', 'also', 'observe', 'that', 'any', 'collection', 'of', 'isospectral', 'c... | [-0.18695765251622481, 0.12230272661876299, -0.12776150207455253, 0.07176441400923639, -0.17989036970424885, -0.11576390753080155, -0.02332901218266902, 0.44210234896608575, -0.25329921065884475, -0.16512569832597293, 0.08959890596623368, -0.2466742581797435, -0.1593615332545311, 0.24300540328098863, -0.120926948506202... |
707.0854 | Adaptation and Coevolution on an Emergent Global Competitive Landscape | Notions of Darwinian selection have been implicit in economic theory for at
least sixty years. Richard Nelson and Sidney Winter have argued that while
evolutionary thinking was prevalent in prewar economics, the postwar
Neoclassical school became almost entirely preoccupied with equilibrium
conditions and their mathe... | q-fin.GN nlin.AO | notions of darwinian selection have been implicit in economic theory for at least sixty years richard nelson and sidney winter have argued that while evolutionary thinking was prevalent in prewar economics the postwar neoclassical school became almost entirely preoccupied with equilibrium conditions and their mathemati... | [['notions', 'of', 'darwinian', 'selection', 'have', 'been', 'implicit', 'in', 'economic', 'theory', 'for', 'at', 'least', 'sixty', 'years', 'richard', 'nelson', 'and', 'sidney', 'winter', 'have', 'argued', 'that', 'while', 'evolutionary', 'thinking', 'was', 'prevalent', 'in', 'prewar', 'economics', 'the', 'postwar', '... | [-0.04387219430917363, 0.09726294409981301, -0.13949843460737385, 0.10826511336538767, -0.11815046601557207, -0.15285140585993934, 0.05817962139712193, 0.314985753920103, -0.230441312584076, -0.3364095059826661, 0.11310730784723699, -0.2523154866172319, -0.20533246983149103, 0.14201899058996204, -0.1746781772060484, -0... |
707.0855 | On the Dynamical Behaviour of Cellular Automata | In this paper we study the dynamics of 1- and 2- dimensional cellular
automata, using a 2-adic representation of the states, we give a simple
graphical technique for finding periodic solutions. We also study the
continuity properties of the associated 2-adic system and show how to compute
the entropy.
| nlin.CG | in this paper we study the dynamics of 1 and 2 dimensional cellular automata using a 2adic representation of the states we give a simple graphical technique for finding periodic solutions we also study the continuity properties of the associated 2adic system and show how to compute the entropy | [['in', 'this', 'paper', 'we', 'study', 'the', 'dynamics', 'of', '1', 'and', '2', 'dimensional', 'cellular', 'automata', 'using', 'a', '2adic', 'representation', 'of', 'the', 'states', 'we', 'give', 'a', 'simple', 'graphical', 'technique', 'for', 'finding', 'periodic', 'solutions', 'we', 'also', 'study', 'the', 'contin... | [-0.1463005692907134, 0.04718821520479966, -0.11921989362762898, 0.09084122693308685, -0.011597400417133254, -0.0894784487365764, 0.061989246608632406, 0.32926004494027217, -0.3266897276043892, -0.23495383895173363, 0.10597123218728799, -0.24032182478326924, -0.23769263562043103, 0.16576482190237363, -0.069586493683104... |
707.0856 | Searching for tidal tails - investigating galaxy harassment | Galaxy harassment has been proposed as a physical process that
morphologically transforms low surface density disc galaxies into dwarf
elliptical galaxies in clusters. It has been used to link the observed very
different morphology of distant cluster galaxies (relatively more blue galaxies
with 'disturbed' morphologi... | astro-ph | galaxy harassment has been proposed as a physical process that morphologically transforms low surface density disc galaxies into dwarf elliptical galaxies in clusters it has been used to link the observed very different morphology of distant cluster galaxies relatively more blue galaxies with disturbed morphologies wit... | [['galaxy', 'harassment', 'has', 'been', 'proposed', 'as', 'a', 'physical', 'process', 'that', 'morphologically', 'transforms', 'low', 'surface', 'density', 'disc', 'galaxies', 'into', 'dwarf', 'elliptical', 'galaxies', 'in', 'clusters', 'it', 'has', 'been', 'used', 'to', 'link', 'the', 'observed', 'very', 'different',... | [-0.08889065162227967, 0.04859710295876049, -0.13909400981785253, 0.13877536708275492, -0.1502313933048684, -0.04255867993327765, 0.03721376110796626, 0.4545881203733958, -0.0835909501512129, -0.35295207804451006, 0.013187171303285047, -0.29393889539194507, -0.12092643343240549, 0.21883941257002357, -0.0328418610898109... |
707.0857 | Large-scale magnetic fields, curvature fluctuations and the thermal
history of the Universe | It is shown that gravitating magnetic fields affect the evolution of
curvature perturbations in a way that is reminiscent of a pristine
non-adiabatic pressure fluctuation. The gauge-invariant evolution of curvature
perturbations is used to constrain the magnetic power spectrum. Depending on
the essential features of ... | astro-ph | it is shown that gravitating magnetic fields affect the evolution of curvature perturbations in a way that is reminiscent of a pristine nonadiabatic pressure fluctuation the gaugeinvariant evolution of curvature perturbations is used to constrain the magnetic power spectrum depending on the essential features of the th... | [['it', 'is', 'shown', 'that', 'gravitating', 'magnetic', 'fields', 'affect', 'the', 'evolution', 'of', 'curvature', 'perturbations', 'in', 'a', 'way', 'that', 'is', 'reminiscent', 'of', 'a', 'pristine', 'nonadiabatic', 'pressure', 'fluctuation', 'the', 'gaugeinvariant', 'evolution', 'of', 'curvature', 'perturbations',... | [-0.14932300995425657, 0.14676524120258147, -0.13665414469547033, 0.09147960526662274, -0.07651621821461264, -0.03632512998622578, -0.030283664534415704, 0.27581846600724863, -0.24454455421373403, -0.3095895125789894, 0.07104466610813763, -0.2526808502296581, -0.08622072368725828, 0.21703021714137388, -0.00717840385959... |
707.0858 | Tracing Magnetic Fields with Aligned Grains | Magnetic fields play a crucial role in various astrophysical processes,
including star formation, accretion of matter, transport processes (e.g.,
transport of heat), and cosmic rays. One of the easiest ways to determine the
magnetic field direction is via polarization of radiation resulting from
extinction on or/and ... | astro-ph | magnetic fields play a crucial role in various astrophysical processes including star formation accretion of matter transport processes eg transport of heat and cosmic rays one of the easiest ways to determine the magnetic field direction is via polarization of radiation resulting from extinction on orand emission by a... | [['magnetic', 'fields', 'play', 'a', 'crucial', 'role', 'in', 'various', 'astrophysical', 'processes', 'including', 'star', 'formation', 'accretion', 'of', 'matter', 'transport', 'processes', 'eg', 'transport', 'of', 'heat', 'and', 'cosmic', 'rays', 'one', 'of', 'the', 'easiest', 'ways', 'to', 'determine', 'the', 'magn... | [-0.11204232187038363, 0.16143357487554777, -0.0556205259748102, 0.10357081616623576, -0.06428496621021214, -0.05940988327172351, -0.0002009923965794677, 0.40402884082121643, -0.2727358704663186, -0.3276853467472256, 0.0698270932843636, -0.23723757625084352, -0.11932075930819075, 0.19427071346896377, -0.019731191413061... |
707.0859 | Coherence and clock shifts in ultracold Fermi gases with resonant
interactions | Using arguments based on sum rules, we derive a general result for the
average shifts of rf lines in Fermi gases in terms of interatomic interaction
strengths and two-particle correlation functions. We show that near an
interaction resonance shifts vary inversely with the atomic scattering length,
rather than linearl... | cond-mat.str-el cond-mat.supr-con | using arguments based on sum rules we derive a general result for the average shifts of rf lines in fermi gases in terms of interatomic interaction strengths and twoparticle correlation functions we show that near an interaction resonance shifts vary inversely with the atomic scattering length rather than linearly as i... | [['using', 'arguments', 'based', 'on', 'sum', 'rules', 'we', 'derive', 'a', 'general', 'result', 'for', 'the', 'average', 'shifts', 'of', 'rf', 'lines', 'in', 'fermi', 'gases', 'in', 'terms', 'of', 'interatomic', 'interaction', 'strengths', 'and', 'twoparticle', 'correlation', 'functions', 'we', 'show', 'that', 'near',... | [-0.14134546493722208, 0.24787371349368947, -0.024703861207270354, 0.06899600376639126, 0.0190975708928682, -0.14809449391661964, 0.08922491369268565, 0.42037005566838964, -0.2212756521297869, -0.22822503192148713, -0.036997153922401146, -0.3094174217210332, -0.08528953995694642, 0.20130367643450067, 0.0951092551643056... |
707.086 | On the Minimum Number of Transmissions in Single-Hop Wireless Coding
Networks | The advent of network coding presents promising opportunities in many areas
of communication and networking. It has been recently shown that network coding
technique can significantly increase the overall throughput of wireless
networks by taking advantage of their broadcast nature. In wireless networks,
each transmi... | cs.IT cs.NI math.IT | the advent of network coding presents promising opportunities in many areas of communication and networking it has been recently shown that network coding technique can significantly increase the overall throughput of wireless networks by taking advantage of their broadcast nature in wireless networks each transmitted ... | [['the', 'advent', 'of', 'network', 'coding', 'presents', 'promising', 'opportunities', 'in', 'many', 'areas', 'of', 'communication', 'and', 'networking', 'it', 'has', 'been', 'recently', 'shown', 'that', 'network', 'coding', 'technique', 'can', 'significantly', 'increase', 'the', 'overall', 'throughput', 'of', 'wirele... | [-0.22632374203021755, 0.032382045487545176, -0.04944971620253372, -0.007941572140142935, -0.08156740480494178, -0.19581275755825284, 0.1357922320107305, 0.3935319143770771, -0.31200217229144817, -0.286469475032804, 0.0812941952873106, -0.2739807730249595, -0.22927417889480817, 0.14164542898652144, -0.13002380951895082... |
707.0861 | Data-driven efficient score tests for deconvolution problems | We consider testing statistical hypotheses about densities of signals in
deconvolution models. A new approach to this problem is proposed. We
constructed score tests for the deconvolution with the known noise density and
efficient score tests for the case of unknown density. The tests are
incorporated with model sele... | math.ST stat.AP stat.TH | we consider testing statistical hypotheses about densities of signals in deconvolution models a new approach to this problem is proposed we constructed score tests for the deconvolution with the known noise density and efficient score tests for the case of unknown density the tests are incorporated with model selection... | [['we', 'consider', 'testing', 'statistical', 'hypotheses', 'about', 'densities', 'of', 'signals', 'in', 'deconvolution', 'models', 'a', 'new', 'approach', 'to', 'this', 'problem', 'is', 'proposed', 'we', 'constructed', 'score', 'tests', 'for', 'the', 'deconvolution', 'with', 'the', 'known', 'noise', 'density', 'and', ... | [-0.03952287146105216, 0.0011440213626393906, -0.10255837934270788, 0.12423773178866562, -0.036428692220495294, -0.18413948920340492, 0.06846821809617373, 0.38453316619763006, -0.19395843039338406, -0.3540573203792939, 0.12543326982905945, -0.23591493729215401, -0.11483612751158384, 0.13462178852552406, -0.078623560171... |
707.0862 | Scheduling in Data Intensive and Network Aware (DIANA) Grid Environments | In Grids scheduling decisions are often made on the basis of jobs being
either data or computation intensive: in data intensive situations jobs may be
pushed to the data and in computation intensive situations data may be pulled
to the jobs. This kind of scheduling, in which there is no consideration of
network chara... | cs.DC | in grids scheduling decisions are often made on the basis of jobs being either data or computation intensive in data intensive situations jobs may be pushed to the data and in computation intensive situations data may be pulled to the jobs this kind of scheduling in which there is no consideration of network characteri... | [['in', 'grids', 'scheduling', 'decisions', 'are', 'often', 'made', 'on', 'the', 'basis', 'of', 'jobs', 'being', 'either', 'data', 'or', 'computation', 'intensive', 'in', 'data', 'intensive', 'situations', 'jobs', 'may', 'be', 'pushed', 'to', 'the', 'data', 'and', 'in', 'computation', 'intensive', 'situations', 'data',... | [-0.17642501628969467, 0.03230911470522265, -0.08252782724319381, 0.0239220623838342, -0.10112688180189652, -0.16739560254208077, 0.1377779186946967, 0.4265725303455781, -0.27890388987929443, -0.34231094256811684, 0.15333904489849473, -0.2340259133911273, -0.08723941690230502, 0.16414978059714458, -0.11383460093335364,... |
707.0863 | Kinetic description of hadron-hadron collisions | A transport model based on the mean free path approach to describe pp
collisions is proposed. We assume that hadrons can be treated as bags of
partons similarly to the MIT bag model. When the energy density in the
collision is higher than a critical value, the bags break and partons are
liberated. The partons expand ... | hep-ph | a transport model based on the mean free path approach to describe pp collisions is proposed we assume that hadrons can be treated as bags of partons similarly to the mit bag model when the energy density in the collision is higher than a critical value the bags break and partons are liberated the partons expand and ca... | [['a', 'transport', 'model', 'based', 'on', 'the', 'mean', 'free', 'path', 'approach', 'to', 'describe', 'pp', 'collisions', 'is', 'proposed', 'we', 'assume', 'that', 'hadrons', 'can', 'be', 'treated', 'as', 'bags', 'of', 'partons', 'similarly', 'to', 'the', 'mit', 'bag', 'model', 'when', 'the', 'energy', 'density', 'i... | [-0.02732918875328466, 0.2453038018132907, -0.17342138124912904, 0.14848362869701767, -0.04556428358031839, -0.08718441216293357, -0.03457889862029868, 0.3823703544022625, -0.1938630111844224, -0.284283179543255, 0.013784688822103335, -0.3388903688219394, 0.015701252200147685, 0.1250699359635987, 0.017367089833772064, ... |
707.0864 | Self-gravitating radiation in AdS(d) | We study spherically symmetric equilibrium configurations of self-gravitating
massless thermal radiation in asymptotically anti-de Sitter space. In d=4, it
was shown by Page and Phillips that there is a maximum red-shifted temperature,
maximum mass and maximum entropy. For higher central densities, the
temperature, m... | gr-qc hep-th | we study spherically symmetric equilibrium configurations of selfgravitating massless thermal radiation in asymptotically antide sitter space in d4 it was shown by page and phillips that there is a maximum redshifted temperature maximum mass and maximum entropy for higher central densities the temperature mass and entr... | [['we', 'study', 'spherically', 'symmetric', 'equilibrium', 'configurations', 'of', 'selfgravitating', 'massless', 'thermal', 'radiation', 'in', 'asymptotically', 'antide', 'sitter', 'space', 'in', 'd4', 'it', 'was', 'shown', 'by', 'page', 'and', 'phillips', 'that', 'there', 'is', 'a', 'maximum', 'redshifted', 'tempera... | [-0.13084393940492695, 0.19165194975640357, -0.05678820897909728, 0.09048575204258308, 0.008609952712970331, -0.13177057943299167, -0.009568248267385586, 0.3293854166130143, -0.12860714945526533, -0.24333718972480742, 0.10099394328041726, -0.33130852520188764, -0.08046921590450874, 0.111054721934921, -0.049567636502675... |
707.0865 | Spectral properties of singular Sturm-Liouville operators with
indefinite weight sgn x | We consider a singular Sturm-Liouville expression with the indefinite weight
sgn x. To this expression there is naturally a self-adjoint operator in some
Krein space associated. We characterize the local definitizability of this
operator in a neighbourhood of $\infty$. Moreover, in this situation, the point
$\infty$ ... | math.SP math.CA | we consider a singular sturmliouville expression with the indefinite weight sgn x to this expression there is naturally a selfadjoint operator in some krein space associated we characterize the local definitizability of this operator in a neighbourhood of infty moreover in this situation the point infty is a regular cr... | [['we', 'consider', 'a', 'singular', 'sturmliouville', 'expression', 'with', 'the', 'indefinite', 'weight', 'sgn', 'x', 'to', 'this', 'expression', 'there', 'is', 'naturally', 'a', 'selfadjoint', 'operator', 'in', 'some', 'krein', 'space', 'associated', 'we', 'characterize', 'the', 'local', 'definitizability', 'of', 't... | [-0.18083306857560938, 0.05886685270741362, -0.07729683452713731, 0.09003390019879097, -0.08076421435721018, -0.12766829688680936, 0.009738519573835907, 0.3583862999913509, -0.2932308225112187, -0.1215772872186593, 0.11672400514677016, -0.34228500989391597, -0.19695731413525505, 0.14462726958398078, -0.1084376808029373... |
707.0866 | Supersolidity, entropy and frustration | We study the properties of t-t'-V model of hard-core bosons on the triangular
lattice that can be realized in optical lattices. By mapping to the spin-1/2
XXZ model in a field, we determine the phase diagram of the t-V model where the
supersolid characterized by the ordering pattern (x,x,-2x') ("ferrimagnetic" or
SS ... | cond-mat.str-el cond-mat.supr-con | we study the properties of ttv model of hardcore bosons on the triangular lattice that can be realized in optical lattices by mapping to the spin12 xxz model in a field we determine the phase diagram of the tv model where the supersolid characterized by the ordering pattern xx2x ferrimagnetic or ss a is a ground state ... | [['we', 'study', 'the', 'properties', 'of', 'ttv', 'model', 'of', 'hardcore', 'bosons', 'on', 'the', 'triangular', 'lattice', 'that', 'can', 'be', 'realized', 'in', 'optical', 'lattices', 'by', 'mapping', 'to', 'the', 'spin12', 'xxz', 'model', 'in', 'a', 'field', 'we', 'determine', 'the', 'phase', 'diagram', 'of', 'the... | [-0.17996341262714585, 0.2633001970548387, -0.05144386058943211, 0.023177983277254618, -0.029784549737983532, -0.14926685620963143, 0.1289407029069717, 0.35681521224256174, -0.2824472401129163, -0.22500044637717362, 0.09448237458760243, -0.30028078804953373, -0.11883859260621872, 0.09397535358785071, 0.0647656904258073... |
707.0867 | Frame dragging and super-energy | We show that the vorticity appearing in stationary vacuum spacetimes is
always related to the existence of a flow of super-energy on the plane
orthogonal to the vorticity vector. This result, toghether with the previously
established link between vorticity and super--energy in radiative (Bondi-Sachs)
spacetimes stren... | gr-qc math-ph math.MP | we show that the vorticity appearing in stationary vacuum spacetimes is always related to the existence of a flow of superenergy on the plane orthogonal to the vorticity vector this result toghether with the previously established link between vorticity and superenergy in radiative bondisachs spacetimes strength furthe... | [['we', 'show', 'that', 'the', 'vorticity', 'appearing', 'in', 'stationary', 'vacuum', 'spacetimes', 'is', 'always', 'related', 'to', 'the', 'existence', 'of', 'a', 'flow', 'of', 'superenergy', 'on', 'the', 'plane', 'orthogonal', 'to', 'the', 'vorticity', 'vector', 'this', 'result', 'toghether', 'with', 'the', 'previou... | [-0.20505353702642656, 0.11259469586440314, -0.06192877510132394, 0.05862419678379734, -0.08945218847780409, -0.06805974691001287, -0.0486930582230374, 0.32151833345513725, -0.24848532038977592, -0.20766955879280122, 0.04410941533002434, -0.20893167377591637, -0.10931293476941221, 0.17707300793095412, -0.04412822875241... |
707.0868 | Light Nuclei as Quantized Skyrmions | We consider the rigid body quantization of Skyrmions with topological charges
1 to 8, as approximated by the rational map ansatz. Novel, general expressions
for the elements of the inertia tensors, in terms of the approximating rational
map, are presented and are used to determine the kinetic energy contribution to
t... | hep-th nucl-th | we consider the rigid body quantization of skyrmions with topological charges 1 to 8 as approximated by the rational map ansatz novel general expressions for the elements of the inertia tensors in terms of the approximating rational map are presented and are used to determine the kinetic energy contribution to the tota... | [['we', 'consider', 'the', 'rigid', 'body', 'quantization', 'of', 'skyrmions', 'with', 'topological', 'charges', '1', 'to', '8', 'as', 'approximated', 'by', 'the', 'rational', 'map', 'ansatz', 'novel', 'general', 'expressions', 'for', 'the', 'elements', 'of', 'the', 'inertia', 'tensors', 'in', 'terms', 'of', 'the', 'ap... | [-0.11865185449861891, 0.17501600657635788, -0.015651017637247897, 0.09154645464086271, -0.001790619767424497, -0.08016640288182177, 0.032109507564250586, 0.33382642834068654, -0.25154589719886145, -0.33681421115953514, 0.05044116094007392, -0.3032620731372755, -0.07769681625886933, 0.14695805028735937, 0.0040803037194... |
707.0869 | Convexity of the self-energy functional in the variational cluster
approximation | In the variational cluster approximation (VCA) (or variational cluster
perturbation theory), widely used to study the Hubbard model, a fundamental
problem that renders variational solutions difficult in practice is its known
lack of convexity at stationary points, i.e. the physical solutions can be
saddle points rath... | cond-mat.str-el cond-mat.supr-con | in the variational cluster approximation vca or variational cluster perturbation theory widely used to study the hubbard model a fundamental problem that renders variational solutions difficult in practice is its known lack of convexity at stationary points ie the physical solutions can be saddle points rather than ext... | [['in', 'the', 'variational', 'cluster', 'approximation', 'vca', 'or', 'variational', 'cluster', 'perturbation', 'theory', 'widely', 'used', 'to', 'study', 'the', 'hubbard', 'model', 'a', 'fundamental', 'problem', 'that', 'renders', 'variational', 'solutions', 'difficult', 'in', 'practice', 'is', 'its', 'known', 'lack'... | [-0.11502356460579194, 0.047237749311507954, -0.1387427081535684, 0.11621498290915042, -0.08367987485011903, -0.13427971323452345, 0.08839966471409198, 0.35014833980126353, -0.29791234619915485, -0.24777210945087463, 0.07373482556388963, -0.27582884056375806, -0.16598129684911905, 0.14514725224410252, -0.02141719374567... |
707.087 | Two-Dimensional Dynamics of Ultracold Atoms in Optical Lattices | We analyze the dynamics of ultracold atoms in optical lattices induced by a
sudden shift of the underlying harmonic trapping potential. In order to study
the effect of strong interactions, dimensionality and lattice topology on
transport properties, we consider bosonic atoms with arbitrarily strong
repulsive interact... | cond-mat.other | we analyze the dynamics of ultracold atoms in optical lattices induced by a sudden shift of the underlying harmonic trapping potential in order to study the effect of strong interactions dimensionality and lattice topology on transport properties we consider bosonic atoms with arbitrarily strong repulsive interactions ... | [['we', 'analyze', 'the', 'dynamics', 'of', 'ultracold', 'atoms', 'in', 'optical', 'lattices', 'induced', 'by', 'a', 'sudden', 'shift', 'of', 'the', 'underlying', 'harmonic', 'trapping', 'potential', 'in', 'order', 'to', 'study', 'the', 'effect', 'of', 'strong', 'interactions', 'dimensionality', 'and', 'lattice', 'topo... | [-0.18995384177945268, 0.24765997028085762, -0.002341626455465582, 0.030181352469998483, -0.00816229157275162, -0.16043926789783514, 0.07224780643278231, 0.4085995023129866, -0.2842166684209727, -0.18959836214064404, 0.04953494089176484, -0.31102357996412766, -0.12475855302405901, 0.09531824373138639, 0.086754377926319... |
707.0871 | Optimal Linear Precoding Strategies for Wideband Non-Cooperative Systems
based on Game Theory-Part II: Algorithms | In this two-part paper, we address the problem of finding the optimal
precoding/multiplexing scheme for a set of non-cooperative links sharing the
same physical resources, e.g., time and bandwidth. We consider two alternative
optimization problems: P.1) the maximization of mutual information on each
link, given const... | cs.IT cs.GT math.IT | in this twopart paper we address the problem of finding the optimal precodingmultiplexing scheme for a set of noncooperative links sharing the same physical resources eg time and bandwidth we consider two alternative optimization problems p1 the maximization of mutual information on each link given constraints on the t... | [['in', 'this', 'twopart', 'paper', 'we', 'address', 'the', 'problem', 'of', 'finding', 'the', 'optimal', 'precodingmultiplexing', 'scheme', 'for', 'a', 'set', 'of', 'noncooperative', 'links', 'sharing', 'the', 'same', 'physical', 'resources', 'eg', 'time', 'and', 'bandwidth', 'we', 'consider', 'two', 'alternative', 'o... | [-0.15712905069589256, -0.06318040557531417, -0.08485388214019342, 0.08759761493420229, -0.06188273491749827, -0.19706770815850738, 0.10921908332518517, 0.3731120037022405, -0.2859383463429717, -0.2848972513125493, 0.14950424683271335, -0.18988820924602737, -0.1546031604664257, 0.1336778797209263, -0.09342205871362239,... |
707.0872 | Hydrodynamics of fluid-solid coexistence in dense shear granular flow | We consider dense rapid shear flow of inelastically colliding hard disks.
Navier-Stokes granular hydrodynamics is applied accounting for the recent
finding \cite{Luding,Khain} that shear viscosity diverges at a lower density
than the rest of constitutive relations. New interpolation formulas for
constitutive relation... | cond-mat.soft | we consider dense rapid shear flow of inelastically colliding hard disks navierstokes granular hydrodynamics is applied accounting for the recent finding citeludingkhain that shear viscosity diverges at a lower density than the rest of constitutive relations new interpolation formulas for constitutive relations between... | [['we', 'consider', 'dense', 'rapid', 'shear', 'flow', 'of', 'inelastically', 'colliding', 'hard', 'disks', 'navierstokes', 'granular', 'hydrodynamics', 'is', 'applied', 'accounting', 'for', 'the', 'recent', 'finding', 'citeludingkhain', 'that', 'shear', 'viscosity', 'diverges', 'at', 'a', 'lower', 'density', 'than', '... | [-0.1685066536469385, 0.1761518377326429, -0.1317879159040749, 0.04256466373614967, -0.026908690337091683, -0.10633656564727426, -0.03845618800073862, 0.3565232127904892, -0.2578568051867187, -0.2387016371777281, 0.051432729231193665, -0.27698874977231025, -0.09658297948166727, 0.17318825036194174, 0.03343487792520318,... |
707.0873 | ExoPTF Science Uniquely Enabled by Far-IR Interferometry: Probing the
Formation of Planetary Systems, and Finding and Characterizing Exoplanets | By providing sensitive sub-arcsecond images and integral field spectroscopy
in the 25 - 400 micron wavelength range, a far-IR interferometer will
revolutionize our understanding of planetary system formation, reveal
otherwise-undetectable planets through the disk perturbations they induce, and
spectroscopically probe... | astro-ph | by providing sensitive subarcsecond images and integral field spectroscopy in the 25 400 micron wavelength range a farir interferometer will revolutionize our understanding of planetary system formation reveal otherwiseundetectable planets through the disk perturbations they induce and spectroscopically probe the atmos... | [['by', 'providing', 'sensitive', 'subarcsecond', 'images', 'and', 'integral', 'field', 'spectroscopy', 'in', 'the', '25', '400', 'micron', 'wavelength', 'range', 'a', 'farir', 'interferometer', 'will', 'revolutionize', 'our', 'understanding', 'of', 'planetary', 'system', 'formation', 'reveal', 'otherwiseundetectable',... | [-0.0975129202068757, 0.15194207019020348, -0.06612934295277474, 0.07494226675598993, -0.11451413893367106, -0.06633963992141416, 0.042462128849889515, 0.4005821389040915, -0.18052554299520845, -0.37339687328996124, 0.10568138673746337, -0.2733778222806036, -0.10198551996895192, 0.22641572220866585, -0.0859542603204605... |
707.0874 | Isometry theorem for the Segal-Bargmann transform on noncompact
symmetric spaces of the complex type | We consider the Segal-Bargmann transform for a noncompact symmetric space of
the complex type. We establish isometry and surjectivity theorems for the
transform, in a form as parallel as possible to the results in the compact
case. The isometry theorem involves integration over a tube of radius R in the
complexificat... | math-ph math.MP math.RT | we consider the segalbargmann transform for a noncompact symmetric space of the complex type we establish isometry and surjectivity theorems for the transform in a form as parallel as possible to the results in the compact case the isometry theorem involves integration over a tube of radius r in the complexification fo... | [['we', 'consider', 'the', 'segalbargmann', 'transform', 'for', 'a', 'noncompact', 'symmetric', 'space', 'of', 'the', 'complex', 'type', 'we', 'establish', 'isometry', 'and', 'surjectivity', 'theorems', 'for', 'the', 'transform', 'in', 'a', 'form', 'as', 'parallel', 'as', 'possible', 'to', 'the', 'results', 'in', 'the'... | [-0.16049306595092078, 0.019154857625309604, -0.10864303783928773, 0.08190396531339152, -0.11529522793120649, -0.11733367706435811, -0.021176047714326126, 0.35910659902785197, -0.2478489236210484, -0.183781855838536, 0.17534419703605889, -0.244199002691978, -0.13069796830370842, 0.2090344514293843, -0.08600846281645438... |
707.0875 | Theory and Numerics of Gravitational Waves from Preheating after
Inflation | Preheating after inflation involves large, time-dependent field
inhomogeneities, which act as a classical source of gravitational radiation.
The resulting spectrum might be probed by direct detection experiments if
inflation occurs at a low enough energy scale. In this paper, we develop a
theory and algorithm to calc... | astro-ph gr-qc hep-ph hep-th | preheating after inflation involves large timedependent field inhomogeneities which act as a classical source of gravitational radiation the resulting spectrum might be probed by direct detection experiments if inflation occurs at a low enough energy scale in this paper we develop a theory and algorithm to calculate an... | [['preheating', 'after', 'inflation', 'involves', 'large', 'timedependent', 'field', 'inhomogeneities', 'which', 'act', 'as', 'a', 'classical', 'source', 'of', 'gravitational', 'radiation', 'the', 'resulting', 'spectrum', 'might', 'be', 'probed', 'by', 'direct', 'detection', 'experiments', 'if', 'inflation', 'occurs', ... | [-0.11743914049458254, 0.17187583419506375, -0.10860179238287467, 0.0882392737819765, -0.06745770171381019, -0.09523729755189912, -0.00873181086407488, 0.36104215946268714, -0.23329145265536685, -0.2905316831328415, 0.09841992061360386, -0.219511983386273, -0.16632778793395603, 0.2327455762461782, 0.020921886752914693,... |
707.0876 | Quasi-Local Linear Momentum in Black-Hole Binaries | We propose a quasi-local formula for the linear momentum of black-hole
horizons inspired by the formalism of quasi-local horizons. We test this
formula using two complementary configurations: (i) by calculating the large
orbital linear momentum of the two black holes in an unequal-mass, zero-spin,
quasi-circular bina... | gr-qc astro-ph | we propose a quasilocal formula for the linear momentum of blackhole horizons inspired by the formalism of quasilocal horizons we test this formula using two complementary configurations i by calculating the large orbital linear momentum of the two black holes in an unequalmass zerospin quasicircular binary and ii by c... | [['we', 'propose', 'a', 'quasilocal', 'formula', 'for', 'the', 'linear', 'momentum', 'of', 'blackhole', 'horizons', 'inspired', 'by', 'the', 'formalism', 'of', 'quasilocal', 'horizons', 'we', 'test', 'this', 'formula', 'using', 'two', 'complementary', 'configurations', 'i', 'by', 'calculating', 'the', 'large', 'orbital... | [-0.17703906078129372, 0.15994828104003125, -0.08061725740628119, 0.1003537390943359, -0.07457186288152019, -0.09249173478778214, -0.0249547884611294, 0.2954791834023088, -0.15759043236996265, -0.2880370242005967, -0.0005765037804326795, -0.3045604961349609, -0.006163706881628233, 0.2168491401491647, -0.021544880857889... |
707.0877 | Signatures of Extra Gauge Bosons in the Littlest Higgs Model with
T-parity at Future Colliders | We study the collider signatures of a T-odd gauge boson $W_{H}$ pair
production in the Littlest Higgs Model with T-parity (LHT) at Large Hadron
Collider (LHC) and Linear Collider (LC). At the LHC, we search for the $W_{H}$
boson using its leptonic decay, i.e. $pp\to W_{H}^{+}W_{H}^{-}\to
A_{H}A_{H}\ell^{+}\nu_{\ell}\... | hep-ph | we study the collider signatures of a todd gauge boson w_h pair production in the littlest higgs model with tparity lht at large hadron collider lhc and linear collider lc at the lhc we search for the w_h boson using its leptonic decay ie ppto w_hw_hto a_ha_hellnu_ellellprimebarnu_ellprime which gives rise to a collide... | [['we', 'study', 'the', 'collider', 'signatures', 'of', 'a', 'todd', 'gauge', 'boson', 'w_h', 'pair', 'production', 'in', 'the', 'littlest', 'higgs', 'model', 'with', 'tparity', 'lht', 'at', 'large', 'hadron', 'collider', 'lhc', 'and', 'linear', 'collider', 'lc', 'at', 'the', 'lhc', 'we', 'search', 'for', 'the', 'w_h',... | [-0.05183158204010574, 0.25295662437077604, -0.11384729627894646, 0.1387338858043688, -0.08892604342815126, -0.22681151889832463, 0.0018680558253147798, 0.3292908870342483, -0.2766507871522818, -0.26579809217236755, 0.014373400289048554, -0.28325098676311716, 0.01795092659928586, 0.16318598431435685, 0.0737664973932579... |
707.0878 | Risk Analysis in Robust Control -- Making the Case for Probabilistic
Robust Control | This paper offers a critical view of the "worst-case" approach that is the
cornerstone of robust control design. It is our contention that a blind
acceptance of worst-case scenarios may lead to designs that are actually more
dangerous than designs based on probabilistic techniques with a built-in risk
factor. The rea... | math.OC cs.SY math.ST stat.TH | this paper offers a critical view of the worstcase approach that is the cornerstone of robust control design it is our contention that a blind acceptance of worstcase scenarios may lead to designs that are actually more dangerous than designs based on probabilistic techniques with a builtin risk factor the real issue i... | [['this', 'paper', 'offers', 'a', 'critical', 'view', 'of', 'the', 'worstcase', 'approach', 'that', 'is', 'the', 'cornerstone', 'of', 'robust', 'control', 'design', 'it', 'is', 'our', 'contention', 'that', 'a', 'blind', 'acceptance', 'of', 'worstcase', 'scenarios', 'may', 'lead', 'to', 'designs', 'that', 'are', 'actual... | [-0.08123929686012811, 0.031523502222608794, -0.12782962229989825, 0.10865488306264437, -0.11246517445847747, -0.1917965212415549, 0.08634608742459456, 0.400213502121291, -0.23107496640822361, -0.2731439552535968, 0.1425476064024094, -0.23660582772323063, -0.207404690268006, 0.2510086286136703, -0.16457392778801955, 0.... |
707.0879 | Escape of Ionizing Radiation from High Redshift Galaxies | We model the escape of ionizing radiation from high-redshift galaxies using
high-resolution Adaptive Mesh Refinement N-body + hydrodynamics simulations.
Our simulations include time-dependent and spatially-resolved transfer of
ionizing radiation in three dimensions, including effects of dust absorption.
For galaxies ... | astro-ph | we model the escape of ionizing radiation from highredshift galaxies using highresolution adaptive mesh refinement nbody hydrodynamics simulations our simulations include timedependent and spatiallyresolved transfer of ionizing radiation in three dimensions including effects of dust absorption for galaxies of total mas... | [['we', 'model', 'the', 'escape', 'of', 'ionizing', 'radiation', 'from', 'highredshift', 'galaxies', 'using', 'highresolution', 'adaptive', 'mesh', 'refinement', 'nbody', 'hydrodynamics', 'simulations', 'our', 'simulations', 'include', 'timedependent', 'and', 'spatiallyresolved', 'transfer', 'of', 'ionizing', 'radiatio... | [-0.039324441163796464, 0.1328698773035252, -0.006452046897679752, 0.0843003389969896, -0.02400547163749768, -0.013511842395690782, 0.08350179405769685, 0.43566750483335676, -0.13125601306721266, -0.3542650045474639, -0.018585224718392693, -0.3343704707505232, 0.02992623203999346, 0.21219991392095214, 0.013969160092004... |
707.088 | Defects Can Increase the Melting Temperature of DNA-Nanoparticle
Assemblies | DNA-gold nanoparticle assemblies have shown promise as an alternative
technology to DNA microarrays for DNA detection and RNA profiling.
Understanding the effect of DNA sequences on the melting temperature of the
system is central to developing reliable detection technology. We studied the
effects of DNA base-pairing... | physics.bio-ph | dnagold nanoparticle assemblies have shown promise as an alternative technology to dna microarrays for dna detection and rna profiling understanding the effect of dna sequences on the melting temperature of the system is central to developing reliable detection technology we studied the effects of dna basepairing defec... | [['dnagold', 'nanoparticle', 'assemblies', 'have', 'shown', 'promise', 'as', 'an', 'alternative', 'technology', 'to', 'dna', 'microarrays', 'for', 'dna', 'detection', 'and', 'rna', 'profiling', 'understanding', 'the', 'effect', 'of', 'dna', 'sequences', 'on', 'the', 'melting', 'temperature', 'of', 'the', 'system', 'is'... | [-0.11554195571766222, 0.1469769794732688, -0.04678790181101313, 0.062076856403506665, -0.007558268835541832, -0.12356807118360426, 0.08686545988443163, 0.38157846804865647, -0.23599473838891152, -0.2920621474876895, 0.0319772780021082, -0.29222270692239555, -0.19149755283822895, 0.17768209999505902, -0.048322522238841... |
707.0881 | SN 1993J VLBI (IV): A Geometric Determination of the Distance to M81
with the Expanding Shock Front Method | We compare the angular expansion velocities, determined with VLBI, with the
linear expansion velocities measured from optical spectra for supernova 1993J
in the galaxy M81, over the period from 7 d to ~9 yr after shock breakout. We
estimate the distance to SN 1993J using the Expanding Shock Front Method (ESM).
We fin... | astro-ph | we compare the angular expansion velocities determined with vlbi with the linear expansion velocities measured from optical spectra for supernova 1993j in the galaxy m81 over the period from 7 d to 9 yr after shock breakout we estimate the distance to sn 1993j using the expanding shock front method esm we find the best... | [['we', 'compare', 'the', 'angular', 'expansion', 'velocities', 'determined', 'with', 'vlbi', 'with', 'the', 'linear', 'expansion', 'velocities', 'measured', 'from', 'optical', 'spectra', 'for', 'supernova', '1993j', 'in', 'the', 'galaxy', 'm81', 'over', 'the', 'period', 'from', '7', 'd', 'to', '9', 'yr', 'after', 'sho... | [-0.04957728773993238, 0.057339814643978464, -0.08883169049437603, 0.05816821002059477, -0.0851731713982704, -0.0930993562127837, 0.09327418296395437, 0.39868010059988873, -0.23641290939480497, -0.3142230902317066, 0.08808280946855582, -0.29384347790141324, 0.023694681159753785, 0.22934179766562537, 0.02532923044884298... |
707.0882 | An algebraic theory of infinite classical lattices III: Theory of single
measurements | This is the third in a series of papers dealing with the algebraic theory of
infinite classical lattices. This paper presents a theory of single
measurements on a lattice which we represent as comprising a finite
subvolume--the system of measurement--immersed in an infinite surround or
``heat bath'' which determines ... | math-ph math.MP | this is the third in a series of papers dealing with the algebraic theory of infinite classical lattices this paper presents a theory of single measurements on a lattice which we represent as comprising a finite subvolumethe system of measurementimmersed in an infinite surround or heat bath which determines the systems... | [['this', 'is', 'the', 'third', 'in', 'a', 'series', 'of', 'papers', 'dealing', 'with', 'the', 'algebraic', 'theory', 'of', 'infinite', 'classical', 'lattices', 'this', 'paper', 'presents', 'a', 'theory', 'of', 'single', 'measurements', 'on', 'a', 'lattice', 'which', 'we', 'represent', 'as', 'comprising', 'a', 'finite'... | [-0.1702805239524151, 0.15851290407503504, -0.10325808527393855, 0.017161894724982925, -0.004454998613900354, -0.09381758904036804, 0.08409139104227288, 0.2908880384081704, -0.2608548796857094, -0.23448787688583128, 0.09796712564057711, -0.31251003770515895, -0.08521546589998671, 0.1698391419918969, -0.0526340884339605... |
707.0883 | The Space Infrared Interferometric Telescope (SPIRIT): High-resolution
imaging and spectroscopy in the far-infrared | We report results of a recently-completed pre-Formulation Phase study of
SPIRIT, a candidate NASA Origins Probe mission. SPIRIT is a spatial and
spectral interferometer with an operating wavelength range 25 - 400 microns.
SPIRIT will provide sub-arcsecond resolution images and spectra with resolution
R = 3000 in a 1 ... | astro-ph | we report results of a recentlycompleted preformulation phase study of spirit a candidate nasa origins probe mission spirit is a spatial and spectral interferometer with an operating wavelength range 25 400 microns spirit will provide subarcsecond resolution images and spectra with resolution r 3000 in a 1 arcmin field... | [['we', 'report', 'results', 'of', 'a', 'recentlycompleted', 'preformulation', 'phase', 'study', 'of', 'spirit', 'a', 'candidate', 'nasa', 'origins', 'probe', 'mission', 'spirit', 'is', 'a', 'spatial', 'and', 'spectral', 'interferometer', 'with', 'an', 'operating', 'wavelength', 'range', '25', '400', 'microns', 'spirit... | [-0.08418945325637593, 0.14826154084605783, -0.07570513495547922, 0.06286381478404877, -0.13469177844491623, -0.07086265909465704, -0.04149445847786488, 0.39552052142032496, -0.1912901453436055, -0.3973626663630947, 0.1112285698252129, -0.2721603792424954, -0.10221984481822091, 0.18538887253863381, -0.04404103373514211... |
707.0884 | The Effective Field Theory of Codimension-two Branes | Distributional sources of matter on codimension-two and higher branes are
only well-defined as regularized objects. Nevertheless, intuition from
effective field theory suggests that the low-energy physics on such branes
should be independent of any high-energy regularization scheme. In this paper,
we address this iss... | hep-th | distributional sources of matter on codimensiontwo and higher branes are only welldefined as regularized objects nevertheless intuition from effective field theory suggests that the lowenergy physics on such branes should be independent of any highenergy regularization scheme in this paper we address this issue in the ... | [['distributional', 'sources', 'of', 'matter', 'on', 'codimensiontwo', 'and', 'higher', 'branes', 'are', 'only', 'welldefined', 'as', 'regularized', 'objects', 'nevertheless', 'intuition', 'from', 'effective', 'field', 'theory', 'suggests', 'that', 'the', 'lowenergy', 'physics', 'on', 'such', 'branes', 'should', 'be', ... | [-0.11037057346087505, 0.1673972562612243, -0.10247218223816867, 0.1473831755262035, -0.08201226063503592, -0.15428801774005615, 0.01198551708088715, 0.309480807347807, -0.2211048258607512, -0.29593525298023177, 0.0711131503574425, -0.29040571903712603, -0.17468423185237586, 0.14241269926206945, -0.05629226776993653, 0... |
707.0885 | Observation of a uniform temperature dependence in the electrical
resistance across the structural phase transition in thin film vanadium oxide
($VO_{2}$) | An electrical study of thin $VO_{2}$ films in the vicinity of the structural
phase transition at $68^{0}C$ shows (a) that the electrical resistance $R$
follows $log (R)$ $\propto$ $-T$ over the $T$-range, $20 < T < 80 ^{0}C$
covering both sides of the structural transition, and (b) a history dependent
hysteresis loop... | cond-mat.mes-hall cond-mat.mtrl-sci | an electrical study of thin vo_2 films in the vicinity of the structural phase transition at 680c shows a that the electrical resistance r follows log r propto t over the trange 20 t 80 0c covering both sides of the structural transition and b a history dependent hysteresis loop in r upon thermal cycling these features... | [['an', 'electrical', 'study', 'of', 'thin', 'vo_2', 'films', 'in', 'the', 'vicinity', 'of', 'the', 'structural', 'phase', 'transition', 'at', '680c', 'shows', 'a', 'that', 'the', 'electrical', 'resistance', 'r', 'follows', 'log', 'r', 'propto', 't', 'over', 'the', 'trange', '20', 't', '80', '0c', 'covering', 'both', '... | [-0.1826438988558948, 0.1963383008029688, -0.0689687888424557, -0.08329455098853661, 0.013641186294933924, -0.14733954248949885, 0.11907068112005408, 0.403571912417045, -0.3112897293928724, -0.28371833714728173, 0.04938299464276777, -0.3311950269799966, -0.1102156695121756, 0.17720142518385099, 0.006109138356091884, -0... |
707.0886 | Radiative torques: Analytical Model and Basic Properties | We attempt to get a physical insight into grain alignment processes by
studying basic properties of radiative torques (RATs). For this purpose we
consider a simple toy model of a helical grain that reproduces well the basic
features of RATs. The model grain consists of a spheroidal body with a mirror
attached at an a... | astro-ph | we attempt to get a physical insight into grain alignment processes by studying basic properties of radiative torques rats for this purpose we consider a simple toy model of a helical grain that reproduces well the basic features of rats the model grain consists of a spheroidal body with a mirror attached at an angle t... | [['we', 'attempt', 'to', 'get', 'a', 'physical', 'insight', 'into', 'grain', 'alignment', 'processes', 'by', 'studying', 'basic', 'properties', 'of', 'radiative', 'torques', 'rats', 'for', 'this', 'purpose', 'we', 'consider', 'a', 'simple', 'toy', 'model', 'of', 'a', 'helical', 'grain', 'that', 'reproduces', 'well', 't... | [-0.1280052013163419, 0.10420548067311439, -0.10236712859414233, 0.03385400668593236, -0.07690437983904706, -0.11403963422718269, -0.01871589335098944, 0.4033189352062312, -0.25333671990649703, -0.29663104528327133, 0.015123181915307631, -0.21625720136399734, -0.12849428239303942, 0.1917958598828218, -0.006682952916214... |
707.0887 | Di-lepton ttH At The CMS | In keeping with the "find the Higgs" bandwagon, due to embark together with
the Large Hadron Collider (LHC), we investigate discovery prospects with Higgs
produced in conjunction with two top quarks decaying in the dilepton channel.
The following is a brief account of adventures along the way; the interested
reader m... | hep-ex | in keeping with the find the higgs bandwagon due to embark together with the large hadron collider lhc we investigate discovery prospects with higgs produced in conjunction with two top quarks decaying in the dilepton channel the following is a brief account of adventures along the way the interested reader may find mo... | [['in', 'keeping', 'with', 'the', 'find', 'the', 'higgs', 'bandwagon', 'due', 'to', 'embark', 'together', 'with', 'the', 'large', 'hadron', 'collider', 'lhc', 'we', 'investigate', 'discovery', 'prospects', 'with', 'higgs', 'produced', 'in', 'conjunction', 'with', 'two', 'top', 'quarks', 'decaying', 'in', 'the', 'dilept... | [-0.08210586902497564, 0.2184010173618924, -0.09217559899154462, 0.09516288403201063, -0.11044995714665244, -0.17930038513517693, -0.025235489925794434, 0.31772082473821284, -0.19608533818666873, -0.26866032722357075, 0.016783961519729673, -0.32885248328379374, -0.006393658291352422, 0.1441763198133885, -0.013428952593... |
707.0888 | Cosmic String Loops and Gravitational Radiation | Understanding of the signatures of cosmic string networks is limited by a
large uncertainty in the sizes at which cosmic string loops form. We review
cosmic string network evolution, and the gravitational signatures, with
emphasis on this uncertainty. We then review a recent analytic model of cosmic
string networks. ... | astro-ph gr-qc hep-ph hep-th | understanding of the signatures of cosmic string networks is limited by a large uncertainty in the sizes at which cosmic string loops form we review cosmic string network evolution and the gravitational signatures with emphasis on this uncertainty we then review a recent analytic model of cosmic string networks in comb... | [['understanding', 'of', 'the', 'signatures', 'of', 'cosmic', 'string', 'networks', 'is', 'limited', 'by', 'a', 'large', 'uncertainty', 'in', 'the', 'sizes', 'at', 'which', 'cosmic', 'string', 'loops', 'form', 'we', 'review', 'cosmic', 'string', 'network', 'evolution', 'and', 'the', 'gravitational', 'signatures', 'with... | [-0.14707280121026745, 0.17685505502746615, -0.04034720890519052, 0.16117103447063394, -0.07483691641009681, -0.020199744740851445, 0.023273270581802813, 0.3237285537294822, -0.25684099803024, -0.3219544946833855, 0.08440872759784175, -0.2824643473601946, -0.10988308371293663, 0.18204268432996873, 0.02639494070525069, ... |
707.0889 | Deformation theory of representations of prop(erad)s | We study the deformation theory of morphisms of properads and props thereby
extending to a non-linear framework Quillen's deformation theory for
commutative rings. The associated chain complex is endowed with a Lie algebra
up to homotopy structure. Its Maurer-Cartan elements correspond to deformed
structures, which a... | math.QA math.AT | we study the deformation theory of morphisms of properads and props thereby extending to a nonlinear framework quillens deformation theory for commutative rings the associated chain complex is endowed with a lie algebra up to homotopy structure its maurercartan elements correspond to deformed structures which allows us... | [['we', 'study', 'the', 'deformation', 'theory', 'of', 'morphisms', 'of', 'properads', 'and', 'props', 'thereby', 'extending', 'to', 'a', 'nonlinear', 'framework', 'quillens', 'deformation', 'theory', 'for', 'commutative', 'rings', 'the', 'associated', 'chain', 'complex', 'is', 'endowed', 'with', 'a', 'lie', 'algebra',... | [-0.15765257195205976, 0.015366760471125547, -0.08910364647859444, 0.10057635872612057, -0.1795064073362171, -0.13401262810428258, -0.04181365362479092, 0.36704430055961895, -0.3965720627286799, -0.2169081095476384, 0.08355272452657421, -0.1785970829464054, -0.20018393645003507, 0.14823349816437606, -0.1695789197527858... |
707.089 | Are there Hilbert-style Pure Type Systems? | For many a natural deduction style logic there is a Hilbert-style logic that
is equivalent to it in that it has the same theorems (i.e. valid judgements
with empty contexts). For intuitionistic logic, the axioms of the equivalent
Hilbert-style logic can be propositions which are also known as the types of
the combina... | cs.LO | for many a natural deduction style logic there is a hilbertstyle logic that is equivalent to it in that it has the same theorems ie valid judgements with empty contexts for intuitionistic logic the axioms of the equivalent hilbertstyle logic can be propositions which are also known as the types of the combinators i k a... | [['for', 'many', 'a', 'natural', 'deduction', 'style', 'logic', 'there', 'is', 'a', 'hilbertstyle', 'logic', 'that', 'is', 'equivalent', 'to', 'it', 'in', 'that', 'it', 'has', 'the', 'same', 'theorems', 'ie', 'valid', 'judgements', 'with', 'empty', 'contexts', 'for', 'intuitionistic', 'logic', 'the', 'axioms', 'of', 't... | [-0.0722087390142782, 0.07488806784720342, -0.09258121479538152, 0.13139617264447412, -0.12087766444491191, -0.22382462053859456, 0.02917715758901496, 0.3506619145601303, -0.2702259156918528, -0.26316117339542716, 0.10186991154988317, -0.2568120714705223, -0.10066958865279267, 0.20746644141270254, -0.13738212812004139,... |
707.0891 | The Nash Equilibrium Revisited: Chaos and Complexity Hidden in
Simplicity | The Nash Equilibrium is a much discussed, deceptively complex, method for the
analysis of non-cooperative games. If one reads many of the commonly available
definitions the description of the Nash Equilibrium is deceptively simple in
appearance. Modern research has discovered a number of new and important
complex pro... | cs.GT cs.CC | the nash equilibrium is a much discussed deceptively complex method for the analysis of noncooperative games if one reads many of the commonly available definitions the description of the nash equilibrium is deceptively simple in appearance modern research has discovered a number of new and important complex properties... | [['the', 'nash', 'equilibrium', 'is', 'a', 'much', 'discussed', 'deceptively', 'complex', 'method', 'for', 'the', 'analysis', 'of', 'noncooperative', 'games', 'if', 'one', 'reads', 'many', 'of', 'the', 'commonly', 'available', 'definitions', 'the', 'description', 'of', 'the', 'nash', 'equilibrium', 'is', 'deceptively',... | [-0.12766987477719297, 0.03731435649745838, -0.14682887075925508, 0.13933770418583155, -0.06492623654537696, -0.1938647750810888, 0.04854327102561985, 0.34731093568147203, -0.2850337836807441, -0.3143977465520262, 0.11554382594214509, -0.24493627701351633, -0.23477585388530717, 0.15200356070188897, -0.09554804340920976... |
707.0892 | Ground State of the Kagome Lattice Heisenberg Antiferromagnet | Using series expansions around the dimer limit, we show that the ground state
of the Heisenberg Antiferromagnet on the Kagome Lattice appears to be a Valence
Bond Crystal (VBC) with a 36-site unit cell, and an energy per site of
$E/J=-0.433\pm0.001$. It is a honeycomb lattice of `perfect hexagons' as
discussed by Nik... | cond-mat.str-el | using series expansions around the dimer limit we show that the ground state of the heisenberg antiferromagnet on the kagome lattice appears to be a valence bond crystal vbc with a 36site unit cell and an energy per site of ej0433pm0001 it is a honeycomb lattice of perfect hexagons as discussed by nikolic and senthil t... | [['using', 'series', 'expansions', 'around', 'the', 'dimer', 'limit', 'we', 'show', 'that', 'the', 'ground', 'state', 'of', 'the', 'heisenberg', 'antiferromagnet', 'on', 'the', 'kagome', 'lattice', 'appears', 'to', 'be', 'a', 'valence', 'bond', 'crystal', 'vbc', 'with', 'a', '36site', 'unit', 'cell', 'and', 'an', 'ener... | [-0.15982381186809888, 0.21676246339479716, -0.004470481366737728, 0.004707646976072329, -0.014436177480787894, -0.11106571008208072, 0.09666339868744894, 0.37239824150166934, -0.26138032141444123, -0.27121905244554684, 0.09196115517469752, -0.3407607349703551, -0.04607181235366341, 0.08449147234242231, 0.0464931529276... |
707.0893 | Unparticle physics and Higgs phenomenology | Recently, conceptually new physics beyond the Standard Model has been
proposed, where a hidden conformal sector provides ``unparticle'' which couples
to the Standard Model sector through higher dimensional operators in low energy
effective theory. Among several possibilities, we focus on operators involving
unparticl... | hep-ph hep-ex hep-th | recently conceptually new physics beyond the standard model has been proposed where a hidden conformal sector provides unparticle which couples to the standard model sector through higher dimensional operators in low energy effective theory among several possibilities we focus on operators involving unparticle the higg... | [['recently', 'conceptually', 'new', 'physics', 'beyond', 'the', 'standard', 'model', 'has', 'been', 'proposed', 'where', 'a', 'hidden', 'conformal', 'sector', 'provides', 'unparticle', 'which', 'couples', 'to', 'the', 'standard', 'model', 'sector', 'through', 'higher', 'dimensional', 'operators', 'in', 'low', 'energy'... | [-0.0817596846966651, 0.30992614884443326, -0.05264479275471692, 0.1875650859726914, -0.1236659021951772, -0.23812360653396825, 0.008383356094970528, 0.2934494321716243, -0.2129684778331811, -0.2827405971892435, 0.0009919228080403188, -0.2871020132868454, -0.06813043042182408, 0.10376908689223487, 0.09854123093637412, ... |
707.0894 | Hybrid compactifications and brane gravity in six dimensions | We consider a six-dimensional axisymmetric Einstein-Maxwell model of warped
braneworlds. The bulk is bounded by two branes, one of which is a conical
3-brane and the other is a 4-brane wrapped around the axis of symmetry. The
latter brane is assumed to be our universe. If the tension of the 3-brane is
fine-tuned, it ... | hep-th gr-qc | we consider a sixdimensional axisymmetric einsteinmaxwell model of warped braneworlds the bulk is bounded by two branes one of which is a conical 3brane and the other is a 4brane wrapped around the axis of symmetry the latter brane is assumed to be our universe if the tension of the 3brane is finetuned it folds the int... | [['we', 'consider', 'a', 'sixdimensional', 'axisymmetric', 'einsteinmaxwell', 'model', 'of', 'warped', 'braneworlds', 'the', 'bulk', 'is', 'bounded', 'by', 'two', 'branes', 'one', 'of', 'which', 'is', 'a', 'conical', '3brane', 'and', 'the', 'other', 'is', 'a', '4brane', 'wrapped', 'around', 'the', 'axis', 'of', 'symmet... | [-0.185981692150976, 0.165695197468267, -0.08609530970253135, 0.08501067769115749, -0.11641877836187962, -0.14854299748416946, -0.07123175385574788, 0.2939399050929668, -0.21499895751052958, -0.2374676091183739, 0.09373125375251137, -0.23496548559871205, -0.1124765237168917, 0.09890498565404084, -0.050096254076131365, ... |
707.0895 | Segmentation and Context of Literary and Musical Sequences | We test a segmentation algorithm, based on the calculation of the
Jensen-Shannon divergence between probability distributions, to two symbolic
sequences of literary and musical origin. The first sequence represents the
successive appearance of characters in a theatrical play, and the second
represents the succession ... | cs.CL physics.data-an | we test a segmentation algorithm based on the calculation of the jensenshannon divergence between probability distributions to two symbolic sequences of literary and musical origin the first sequence represents the successive appearance of characters in a theatrical play and the second represents the succession of tone... | [['we', 'test', 'a', 'segmentation', 'algorithm', 'based', 'on', 'the', 'calculation', 'of', 'the', 'jensenshannon', 'divergence', 'between', 'probability', 'distributions', 'to', 'two', 'symbolic', 'sequences', 'of', 'literary', 'and', 'musical', 'origin', 'the', 'first', 'sequence', 'represents', 'the', 'successive',... | [-0.1277735023151921, 0.0809814009580093, -0.10981886321837722, 0.082760899870292, -0.054360680881401766, -0.05152111004673592, 0.016399738746290297, 0.3753693262115121, -0.30197678187295146, -0.3179962430351778, 0.04202924967925672, -0.28369072539245954, -0.19291282475561553, 0.17757207977221065, -0.08874040099832675,... |
707.0896 | Shocked Molecular Hydrogen in the 3C 326 Radio Galaxy System | The Spitzer spectrum of the giant FR II radio galaxy 3C 326 is dominated by
very strong molecular hydrogen emission lines on a faint IR continuum. The H2
emission originates in the northern component of a double-galaxy system
associated with 3C 326. The integrated luminosity in H2 pure-rotational lines
is 8.0E41 erg/... | astro-ph | the spitzer spectrum of the giant fr ii radio galaxy 3c 326 is dominated by very strong molecular hydrogen emission lines on a faint ir continuum the h2 emission originates in the northern component of a doublegalaxy system associated with 3c 326 the integrated luminosity in h2 purerotational lines is 80e41 ergs which ... | [['the', 'spitzer', 'spectrum', 'of', 'the', 'giant', 'fr', 'ii', 'radio', 'galaxy', '3c', '326', 'is', 'dominated', 'by', 'very', 'strong', 'molecular', 'hydrogen', 'emission', 'lines', 'on', 'a', 'faint', 'ir', 'continuum', 'the', 'h2', 'emission', 'originates', 'in', 'the', 'northern', 'component', 'of', 'a', 'doubl... | [-0.061522678368271806, 0.08733107570865818, 0.0024506176511446633, 0.09649606228298466, -0.08040377674288712, -0.07751550805452909, -0.007660215732070978, 0.4828005613408341, -0.1284008950544605, -0.2942104322357556, 0.04821356921823829, -0.27787199026175047, 0.030288117755254782, 0.16025305559019584, -0.0153754707866... |
707.0897 | Orbital Solution & Fundamental Parameters of sigma Scorpii | The first orbital solution for the spectroscopic pair in the multiple star
system sigma Scorpii, determined from measurements with the Sydney University
Stellar Interferometer (SUSI), is presented. The primary component is of beta
Cephei variable type and has been one of the most intensively studied examples
of its c... | astro-ph | the first orbital solution for the spectroscopic pair in the multiple star system sigma scorpii determined from measurements with the sydney university stellar interferometer susi is presented the primary component is of beta cephei variable type and has been one of the most intensively studied examples of its class th... | [['the', 'first', 'orbital', 'solution', 'for', 'the', 'spectroscopic', 'pair', 'in', 'the', 'multiple', 'star', 'system', 'sigma', 'scorpii', 'determined', 'from', 'measurements', 'with', 'the', 'sydney', 'university', 'stellar', 'interferometer', 'susi', 'is', 'presented', 'the', 'primary', 'component', 'is', 'of', '... | [-0.07995536223519593, 0.07994177796691657, -0.05788824060559273, 0.035768980596214535, -0.08951989109255373, -0.10507778760418296, 0.021291204899549485, 0.3789048141539097, -0.16070393924135715, -0.35144611418247224, 0.09643773592077196, -0.3005556779205799, -0.012954307571053505, 0.23994909316580743, -0.0517415734678... |
707.0898 | Entanglement and Irreversibility in the Approach to Thermal Equilibrium | When a physical system is put in contact with a very large thermal bath, it
undergoes a dissipative (i.e., an apparently irreversible) process that leads
to thermal equilibrium. This dynamical process can be described fully within
quantum physics, involving only unitary, therefore reversible, maps. The
information, i... | quant-ph | when a physical system is put in contact with a very large thermal bath it undergoes a dissipative ie an apparently irreversible process that leads to thermal equilibrium this dynamical process can be described fully within quantum physics involving only unitary therefore reversible maps the information initially prese... | [['when', 'a', 'physical', 'system', 'is', 'put', 'in', 'contact', 'with', 'a', 'very', 'large', 'thermal', 'bath', 'it', 'undergoes', 'a', 'dissipative', 'ie', 'an', 'apparently', 'irreversible', 'process', 'that', 'leads', 'to', 'thermal', 'equilibrium', 'this', 'dynamical', 'process', 'can', 'be', 'described', 'full... | [-0.12370307120545476, 0.22224690898394783, -0.1361797729623504, 0.04741663390828421, -0.019097175587376114, -0.1980210041774626, 0.036081619229662465, 0.31838147473172285, -0.2905168380602845, -0.244053222835646, 0.09846607708186639, -0.3042930607916787, -0.11211226719751721, 0.16722468098669196, -0.061918430445984995... |
707.0899 | Broken SU(3) Flavor Symmetry and Tribimaximal Neutrino Mixing | Recent work on a lepton mass matrix model based on an SU(3) flavor symmetry
which is broken into S_4 is reviewed. The flavor structures of the masses and
mixing are caused by VEVs of SU(2)_L-singlet scalars \phi which are nonets
({\bf 8}+{\bf 1}) of the SU(3) flavor symmetry, and which are broken into {\bf
2}+{\bf 3}... | hep-ph | recent work on a lepton mass matrix model based on an su3 flavor symmetry which is broken into s_4 is reviewed the flavor structures of the masses and mixing are caused by vevs of su2_lsinglet scalars phi which are nonets bf 8bf 1 of the su3 flavor symmetry and which are broken into bf 2bf 3bf 3 and bf 1 of s_4 if we r... | [['recent', 'work', 'on', 'a', 'lepton', 'mass', 'matrix', 'model', 'based', 'on', 'an', 'su3', 'flavor', 'symmetry', 'which', 'is', 'broken', 'into', 's_4', 'is', 'reviewed', 'the', 'flavor', 'structures', 'of', 'the', 'masses', 'and', 'mixing', 'are', 'caused', 'by', 'vevs', 'of', 'su2_lsinglet', 'scalars', 'phi', 'w... | [-0.14134991068858654, 0.33937727262673434, 0.001243013018657538, 0.1328950352448208, -0.09360167870128697, -0.17941562861034815, 0.007042722443161024, 0.3456527231769128, -0.17446063057180833, -0.25969617002304984, 0.029684316396543925, -0.24531505832617934, -0.038035076738081194, 0.01468477031501772, 0.05490586943924... |
707.09 | Traversable Wormholes Construction in (2+1) Gravity | Wormholes have been always an interesting object in gravity theories. In this
paper we make a little review of the principal properties of these objects and
the exotic matter they need to exist. Then, we obtain two specific solutions in
the formalism of (2+1)-dimensional gravity with negative cosmological constant.
T... | gr-qc | wormholes have been always an interesting object in gravity theories in this paper we make a little review of the principal properties of these objects and the exotic matter they need to exist then we obtain two specific solutions in the formalism of 21dimensional gravity with negative cosmological constant the obtaine... | [['wormholes', 'have', 'been', 'always', 'an', 'interesting', 'object', 'in', 'gravity', 'theories', 'in', 'this', 'paper', 'we', 'make', 'a', 'little', 'review', 'of', 'the', 'principal', 'properties', 'of', 'these', 'objects', 'and', 'the', 'exotic', 'matter', 'they', 'need', 'to', 'exist', 'then', 'we', 'obtain', 't... | [-0.14701947165012824, 0.07139587569727154, -0.13583228839561343, 0.1429647504526656, -0.1466666805325076, -0.17530691252904945, -0.06381785092962673, 0.3607757463818416, -0.17300584679469466, -0.3392782268463634, 0.09852679059404182, -0.2837179092573933, -0.15491317196283488, 0.12568790074437858, -0.08888253693003208,... |
707.0901 | Effect of time delay on feedback control of a flashing ratchet | It was recently shown that the use of feedback control can improve the
performance of a flashing ratchet. We investigate the effect of a time delay in
the implementation of feedback control in a closed-loop collective flashing
ratchet, using Langevin dynamics simulations. Surprisingly, for a large
ensemble, a well-ch... | cond-mat.stat-mech | it was recently shown that the use of feedback control can improve the performance of a flashing ratchet we investigate the effect of a time delay in the implementation of feedback control in a closedloop collective flashing ratchet using langevin dynamics simulations surprisingly for a large ensemble a wellchosen dela... | [['it', 'was', 'recently', 'shown', 'that', 'the', 'use', 'of', 'feedback', 'control', 'can', 'improve', 'the', 'performance', 'of', 'a', 'flashing', 'ratchet', 'we', 'investigate', 'the', 'effect', 'of', 'a', 'time', 'delay', 'in', 'the', 'implementation', 'of', 'feedback', 'control', 'in', 'a', 'closedloop', 'collect... | [-0.160930276707452, 0.14108598300542935, -0.09380537006807954, 0.031171165706932936, -0.0566079986134642, -0.1573217710168486, 0.105485531201243, 0.36927711341838193, -0.24883894830998174, -0.287174878361866, 0.10125478468240148, -0.21849153573883878, -0.14346855204496392, 0.2729459456833346, -0.06839919257628962, 0.0... |
707.0902 | Flow Representation of the Bose-Hubbard Hamiltonian : General Case | In this paper the explicit flow representation to the Bose-Hubbard
Hamiltonian is given in the general case. This representation may be useful in
creating cat states for the system of atoms trapped in the optical ring.
| quant-ph math-ph math.MP | in this paper the explicit flow representation to the bosehubbard hamiltonian is given in the general case this representation may be useful in creating cat states for the system of atoms trapped in the optical ring | [['in', 'this', 'paper', 'the', 'explicit', 'flow', 'representation', 'to', 'the', 'bosehubbard', 'hamiltonian', 'is', 'given', 'in', 'the', 'general', 'case', 'this', 'representation', 'may', 'be', 'useful', 'in', 'creating', 'cat', 'states', 'for', 'the', 'system', 'of', 'atoms', 'trapped', 'in', 'the', 'optical', 'r... | [-0.12439511592189471, 0.13937081039572755, -0.06776605502495335, 0.02239149491651915, 0.02009408944286406, -0.14729469067727527, -0.03136802376441968, 0.36485039277209175, -0.28026559286647373, -0.2032438400718901, 0.055626515868223377, -0.238523249165155, -0.13636365129301944, 0.1689852396440175, -0.09116824990875709... |
707.0903 | Loss-tolerant operations in parity-code linear optics quantum computing | A heavy focus for optical quantum computing is the introduction of
error-correction, and the minimisation of resource requirements. We detail a
complete encoding and manipulation scheme designed for linear optics quantum
computing, incorporating scalable operations and loss-tolerant architecture.
| quant-ph | a heavy focus for optical quantum computing is the introduction of errorcorrection and the minimisation of resource requirements we detail a complete encoding and manipulation scheme designed for linear optics quantum computing incorporating scalable operations and losstolerant architecture | [['a', 'heavy', 'focus', 'for', 'optical', 'quantum', 'computing', 'is', 'the', 'introduction', 'of', 'errorcorrection', 'and', 'the', 'minimisation', 'of', 'resource', 'requirements', 'we', 'detail', 'a', 'complete', 'encoding', 'and', 'manipulation', 'scheme', 'designed', 'for', 'linear', 'optics', 'quantum', 'comput... | [-0.18332760862540454, 0.09060446441626961, -0.08662259500277669, 0.03784285310815137, -0.04689910752992881, -0.31112907755825864, 0.07458240280270968, 0.3864261874634969, -0.2603465282162161, -0.3035189146911235, 0.11345347059939645, -0.1741438969038427, -0.15900189683337598, 0.22772951031986036, -0.09778896561137547,... |
707.0904 | Brown representability for space-valued functors | In this paper we prove two theorems which resemble the classical
cohomological and homological Brown representability theorems. The main
difference is that our results classify small contravariant functors from
spaces to spaces up to weak equivalence of functors.
In more detail, we show that every small contravaria... | math.AT | in this paper we prove two theorems which resemble the classical cohomological and homological brown representability theorems the main difference is that our results classify small contravariant functors from spaces to spaces up to weak equivalence of functors in more detail we show that every small contravariant func... | [['in', 'this', 'paper', 'we', 'prove', 'two', 'theorems', 'which', 'resemble', 'the', 'classical', 'cohomological', 'and', 'homological', 'brown', 'representability', 'theorems', 'the', 'main', 'difference', 'is', 'that', 'our', 'results', 'classify', 'small', 'contravariant', 'functors', 'from', 'spaces', 'to', 'spac... | [-0.13410083157472283, 0.03125761883829029, -0.13143924263591367, 0.17800028319188935, -0.13866959327471354, -0.13584953751189693, -0.0056491641678862396, 0.3533628003882064, -0.4919270650754052, -0.14244127933183806, 0.0353400312625097, -0.1894721025281826, -0.10899794262443338, 0.1516000614670526, -0.2963742746355673... |
707.0905 | Muon Identification at ATLAS and CMS | Muonic final states will provide clean signatures formany physics processes
at the LHC. The two LHC experiments ATLAS and CMS will be able to identify
muons with a high reconstruction efficiency above 96% and a high transverse
momentum resolution better than 2% for transverse momenta below 400 GeV/c and
about 10% at ... | hep-ex | muonic final states will provide clean signatures formany physics processes at the lhc the two lhc experiments atlas and cms will be able to identify muons with a high reconstruction efficiency above 96 and a high transverse momentum resolution better than 2 for transverse momenta below 400 gevc and about 10 at 1 tevc ... | [['muonic', 'final', 'states', 'will', 'provide', 'clean', 'signatures', 'formany', 'physics', 'processes', 'at', 'the', 'lhc', 'the', 'two', 'lhc', 'experiments', 'atlas', 'and', 'cms', 'will', 'be', 'able', 'to', 'identify', 'muons', 'with', 'a', 'high', 'reconstruction', 'efficiency', 'above', '96', 'and', 'a', 'hig... | [-0.025505369378796477, 0.2514181122695752, -0.037965866077075326, 0.07298797667191517, -0.061138275211427624, -0.15454716455396705, -0.046991477379443376, 0.3472980402087367, -0.1704980259665882, -0.41795289674847147, 0.057564177092505754, -0.39489075993224393, 0.13275727566595621, 0.223183849520292, -0.00615295768150... |
707.0906 | A spectral sequence to compute L2-Betti numbers of groups and groupoids | We construct a spectral sequence for L2-type cohomology groups of discrete
measured groupoids. Based on the spectral sequence, we prove the Hopf-Singer
conjecture for aspherical manifolds with poly-surface fundamental groups. More
generally, we obtain a permanence result for the Hopf-Singer conjecture under
taking fi... | math.DS math.AT | we construct a spectral sequence for l2type cohomology groups of discrete measured groupoids based on the spectral sequence we prove the hopfsinger conjecture for aspherical manifolds with polysurface fundamental groups more generally we obtain a permanence result for the hopfsinger conjecture under taking fiber bundle... | [['we', 'construct', 'a', 'spectral', 'sequence', 'for', 'l2type', 'cohomology', 'groups', 'of', 'discrete', 'measured', 'groupoids', 'based', 'on', 'the', 'spectral', 'sequence', 'we', 'prove', 'the', 'hopfsinger', 'conjecture', 'for', 'aspherical', 'manifolds', 'with', 'polysurface', 'fundamental', 'groups', 'more', ... | [-0.18652338490034615, 0.06834624311435117, -0.13747050494340987, 0.12435888816554357, -0.08271039013975653, -0.11202553253963418, 0.04349334664835498, 0.39664134462417544, -0.2809365878802264, -0.2760298339671445, 0.129036991079552, -0.1797377715829289, -0.13685325782574798, 0.2410938368639213, -0.15071445992537613, -... |
707.0907 | The concrete theory of numbers : Problem of simplicity of Fermat
number-twins | The problem of simplicity of Fermat number-twins $f_{n}^{\pm}=2^{2^n}\pm3$ is
studied. The question for what $n$ numbers $f_{n}^{\pm}$ are composite is
investigated. The factor-identities for numbers of a kind $x^2 \pm k $ are
found.
| math.GM | the problem of simplicity of fermat numbertwins f_npm22npm3 is studied the question for what n numbers f_npm are composite is investigated the factoridentities for numbers of a kind x2 pm k are found | [['the', 'problem', 'of', 'simplicity', 'of', 'fermat', 'numbertwins', 'f_npm22npm3', 'is', 'studied', 'the', 'question', 'for', 'what', 'n', 'numbers', 'f_npm', 'are', 'composite', 'is', 'investigated', 'the', 'factoridentities', 'for', 'numbers', 'of', 'a', 'kind', 'x2', 'pm', 'k', 'are', 'found']] | [-0.25137334670229206, 0.13598651747251378, -0.03697117563770634, 0.11230383110874943, -0.03925206464040896, -0.14467886981457986, -0.006238151036588283, 0.3119934160133888, -0.27949951935944883, -0.3453655146576207, 0.08058518315825997, -0.3076746382204623, -0.09945566657577352, 0.23669772559841132, -0.016784809304979... |
707.0908 | Reheating and Cosmic String Production | We compute the string production rate at the end of inflation, using the
string spectrum obtained in \lss in a near-de Sitter space. Our result shows
that highly excited strings are hardly produced, thus the simple slow-roll
inflation alone does not offer a cosmic string production mechanism.
| hep-th | we compute the string production rate at the end of inflation using the string spectrum obtained in lss in a nearde sitter space our result shows that highly excited strings are hardly produced thus the simple slowroll inflation alone does not offer a cosmic string production mechanism | [['we', 'compute', 'the', 'string', 'production', 'rate', 'at', 'the', 'end', 'of', 'inflation', 'using', 'the', 'string', 'spectrum', 'obtained', 'in', 'lss', 'in', 'a', 'nearde', 'sitter', 'space', 'our', 'result', 'shows', 'that', 'highly', 'excited', 'strings', 'are', 'hardly', 'produced', 'thus', 'the', 'simple', ... | [-0.16172859630488018, 0.21228666383614567, -0.14169869802773316, 0.18539444092621513, -0.07719661840336754, -0.11203705435222451, 0.011927684016050176, 0.31005488819581395, -0.23962996355158853, -0.22876657006588388, 0.03243526816863487, -0.21951024909999142, -0.06068583191471531, 0.1945611484982866, -0.00677506360126... |
707.0909 | Spectrum Sensing in Cognitive Radios Based on Multiple Cyclic
Frequencies | Cognitive radios sense the radio spectrum in order to find unused frequency
bands and use them in an agile manner. Transmission by the primary user must be
detected reliably even in the low signal-to-noise ratio (SNR) regime and in the
face of shadowing and fading. Communication signals are typically
cyclostationary,... | cs.IT math.IT | cognitive radios sense the radio spectrum in order to find unused frequency bands and use them in an agile manner transmission by the primary user must be detected reliably even in the low signaltonoise ratio snr regime and in the face of shadowing and fading communication signals are typically cyclostationary and have... | [['cognitive', 'radios', 'sense', 'the', 'radio', 'spectrum', 'in', 'order', 'to', 'find', 'unused', 'frequency', 'bands', 'and', 'use', 'them', 'in', 'an', 'agile', 'manner', 'transmission', 'by', 'the', 'primary', 'user', 'must', 'be', 'detected', 'reliably', 'even', 'in', 'the', 'low', 'signaltonoise', 'ratio', 'snr... | [-0.18812362312110598, 0.05863991751857339, -0.04002328884570363, 0.0752952117451974, -0.06610915439710868, -0.19481383455069567, 0.078119786090251, 0.39865513081232945, -0.26815548981958165, -0.30820695134604764, 0.0957317532341325, -0.24000563619692858, -0.1863701047939053, 0.19354280726259163, -0.09498354366249935, ... |
707.091 | Cosmic-Ray Heating of Molecular Gas in the Nuclear Disk: Low Star
Formation Efficiency | Understanding the processes occurring in the nuclear disk of our Galaxy is
interesting in its own right, as part of the Milky Way Galaxy, but also because
it is the closest galactic nucleus. It has been more than two decades since it
was recognized that the general phenomenon of higher gas temperature in the
inner fe... | astro-ph | understanding the processes occurring in the nuclear disk of our galaxy is interesting in its own right as part of the milky way galaxy but also because it is the closest galactic nucleus it has been more than two decades since it was recognized that the general phenomenon of higher gas temperature in the inner few hun... | [['understanding', 'the', 'processes', 'occurring', 'in', 'the', 'nuclear', 'disk', 'of', 'our', 'galaxy', 'is', 'interesting', 'in', 'its', 'own', 'right', 'as', 'part', 'of', 'the', 'milky', 'way', 'galaxy', 'but', 'also', 'because', 'it', 'is', 'the', 'closest', 'galactic', 'nucleus', 'it', 'has', 'been', 'more', 't... | [-0.04999780678837043, 0.12828072315533798, -0.0418286256543878, 0.07113448167431423, -0.05597773807198562, -0.02268657168006581, 0.0289071539929607, 0.3982913409914784, -0.1852811034792338, -0.3198826963780448, 0.05131464545271651, -0.2814033363894042, -0.016473856950978364, 0.2113073656257275, 0.029169642769733346, -... |
707.0911 | A Complete Survey of the Central Molecular Zone in NH3 | We present a map of the major part of the central molecular zone (CMZ) of
simultaneous observations in the NH3 (J,K) = (1,1) and (2,2) lines using the
Kagoshima 6-m telescope. The mapped area is -1.000 < l < 1.625 deg, -0.375 < b
< +0.250 deg. The kinetic temperatures derived from the (2,2) to (1,1)
intensity ratios ... | astro-ph | we present a map of the major part of the central molecular zone cmz of simultaneous observations in the nh3 jk 11 and 22 lines using the kagoshima 6m telescope the mapped area is 1000 l 1625 deg 0375 b 0250 deg the kinetic temperatures derived from the 22 to 11 intensity ratios are 2080 k or exceed 80 k the gases corr... | [['we', 'present', 'a', 'map', 'of', 'the', 'major', 'part', 'of', 'the', 'central', 'molecular', 'zone', 'cmz', 'of', 'simultaneous', 'observations', 'in', 'the', 'nh3', 'jk', '11', 'and', '22', 'lines', 'using', 'the', 'kagoshima', '6m', 'telescope', 'the', 'mapped', 'area', 'is', '1000', 'l', '1625', 'deg', '0375', ... | [-0.08069230454099159, 0.14669431340588318, 0.014395161286218587, 0.002153728607456721, -0.009657206156914797, -0.043536398371835365, 0.0903177611981604, 0.40738904657517344, -0.16847135381636405, -0.32669562904523053, 0.07542306761558536, -0.30152771952177543, 0.013700400093578896, 0.15620106352608515, 0.0179766120335... |
707.0912 | An SU(3) symmetry for light neutrinos | It is proposed that light neutrinos form a triplet in a global SU(3) symmetry
in mass eigenstate basis. Assuming that the SU(3)symmetry is broken in the
direction (-alambda_{3}+frac{b}/{sqrt{3}}lambda_{8}), and after going to the
flavor basis we predict atmospheric mixing angle, sin ^{2}theta_{23}=0.5 and
sin theta_{... | hep-ph | it is proposed that light neutrinos form a triplet in a global su3 symmetry in mass eigenstate basis assuming that the su3symmetry is broken in the direction alambda_3fracbsqrt3lambda_8 and after going to the flavor basis we predict atmospheric mixing angle sin 2theta_2305 and sin theta_130 if nu_munu_tau symmetry is a... | [['it', 'is', 'proposed', 'that', 'light', 'neutrinos', 'form', 'a', 'triplet', 'in', 'a', 'global', 'su3', 'symmetry', 'in', 'mass', 'eigenstate', 'basis', 'assuming', 'that', 'the', 'su3symmetry', 'is', 'broken', 'in', 'the', 'direction', 'alambda_3fracbsqrt3lambda_8', 'and', 'after', 'going', 'to', 'the', 'flavor', ... | [-0.12215081815131355, 0.270325985542217, -0.01848889630136275, 0.08812313886944118, -0.073473691431329, -0.15557305892214698, 0.04703998802836205, 0.351759992713152, -0.2521351025937948, -0.19712804789589936, 0.09439147406171054, -0.26029263273271364, -0.09853222406317674, 0.1005795351554488, 0.03501655298913287, 0.04... |
707.0913 | A vanishing theorem for sheaves of small differential operators in
positive characteristic | Let $X$ be a smooth variety over an algebraically closed field $k$ of
positive characteristic, ${\rm D}_X$ the sheaf of PD-differential operators,
and ${\bar D}_X$ its central reduction, the sheaf of small differential
operators. In this paper we show that if $X$ is a line-hyperplane incidence
variety (a partial flag... | math.AG math.RT | let x be a smooth variety over an algebraically closed field k of positive characteristic rm d_x the sheaf of pddifferential operators and bar d_x its central reduction the sheaf of small differential operators in this paper we show that if x is a linehyperplane incidence variety a partial flag variety of type 1nn1 or ... | [['let', 'x', 'be', 'a', 'smooth', 'variety', 'over', 'an', 'algebraically', 'closed', 'field', 'k', 'of', 'positive', 'characteristic', 'rm', 'd_x', 'the', 'sheaf', 'of', 'pddifferential', 'operators', 'and', 'bar', 'd_x', 'its', 'central', 'reduction', 'the', 'sheaf', 'of', 'small', 'differential', 'operators', 'in',... | [-0.2327982724361521, 0.0644110818311674, -0.06674328701670415, 0.03239085260013651, -0.07119260049616319, -0.12525234785529651, -0.04486335116234841, 0.3187873243753399, -0.36665476085285525, -0.16413510120141186, 0.0804347596401515, -0.21463420834541985, -0.138581284249085, 0.20333491056849848, -0.12630272632564551, ... |
707.0914 | Method of characteristics and solution of DGLAP evolution equation in
leading order (LO) and next to leading order (NLO) at small-x | In this paper the singlet and non-singlet structure functions have been
obtained by solving Dokshitzer, Gribove, Lipatov, Alterelli, Parisi (DGLAP)
evolution equations in leading order (LO) and next to leading order (NLO) at
the small x limit. Here we have used a Taylor Series expansion and then the
method of charact... | hep-ph | in this paper the singlet and nonsinglet structure functions have been obtained by solving dokshitzer gribove lipatov alterelli parisi dglap evolution equations in leading order lo and next to leading order nlo at the small x limit here we have used a taylor series expansion and then the method of characteristics to so... | [['in', 'this', 'paper', 'the', 'singlet', 'and', 'nonsinglet', 'structure', 'functions', 'have', 'been', 'obtained', 'by', 'solving', 'dokshitzer', 'gribove', 'lipatov', 'alterelli', 'parisi', 'dglap', 'evolution', 'equations', 'in', 'leading', 'order', 'lo', 'and', 'next', 'to', 'leading', 'order', 'nlo', 'at', 'the'... | [-0.051479949869892815, 0.0944609680067893, -0.13582349948996267, 0.089991043822223, -0.05754254060470826, -0.02050061748278412, -0.017420661144333518, 0.3425128322892955, -0.21315697663427366, -0.2884157544921164, 0.06618422577339043, -0.3108913195258998, -0.088987455812174, 0.10811558939734256, 0.08329564734519303, 0... |
707.0915 | D-affinity and Frobenius morphism on quadrics | We compute decomposition of Frobenius push-forwards of line bundles on
quadrics into a direct sum of line bundles and spinor bundles. As an
application we show when the Frobenius push-forward gives a tilting bundle and
we apply it to study D-modules on quadrics.
| math.AG math.RT | we compute decomposition of frobenius pushforwards of line bundles on quadrics into a direct sum of line bundles and spinor bundles as an application we show when the frobenius pushforward gives a tilting bundle and we apply it to study dmodules on quadrics | [['we', 'compute', 'decomposition', 'of', 'frobenius', 'pushforwards', 'of', 'line', 'bundles', 'on', 'quadrics', 'into', 'a', 'direct', 'sum', 'of', 'line', 'bundles', 'and', 'spinor', 'bundles', 'as', 'an', 'application', 'we', 'show', 'when', 'the', 'frobenius', 'pushforward', 'gives', 'a', 'tilting', 'bundle', 'and... | [-0.23049740397999452, -0.07951670894392517, -0.06906513895752818, 0.0634288020258726, -0.13609528931420903, -0.10589589042112578, -0.02421177694097508, 0.43336925300401313, -0.33243088892032935, -0.11333997362444914, 0.06836400691116619, -0.19086293419173292, -0.2036921924933098, 0.1918355134250813, -0.153529923517516... |
707.0916 | Local Tunneling Spectroscopy across a Metamagnetic Critical Point in the
Bi-layer Ruthenate Sr3Ru2O7 | The local spectroscopic signatures of metamagnetic criticality in Sr3Ru2O7
were explored using scanning tunneling microscopy (STM). Singular features in
the tunneling spectrum were found close to the Fermi level, as would be
expected in a Stoner picture of itinerant electron metamagnetism. These
features showed a pro... | cond-mat.str-el | the local spectroscopic signatures of metamagnetic criticality in sr3ru2o7 were explored using scanning tunneling microscopy stm singular features in the tunneling spectrum were found close to the fermi level as would be expected in a stoner picture of itinerant electron metamagnetism these features showed a pronounced... | [['the', 'local', 'spectroscopic', 'signatures', 'of', 'metamagnetic', 'criticality', 'in', 'sr3ru2o7', 'were', 'explored', 'using', 'scanning', 'tunneling', 'microscopy', 'stm', 'singular', 'features', 'in', 'the', 'tunneling', 'spectrum', 'were', 'found', 'close', 'to', 'the', 'fermi', 'level', 'as', 'would', 'be', '... | [-0.17640226100159523, 0.17708112851071817, -0.09670545008982746, 0.11159307180451623, -0.025188371614394082, -0.1300316258611229, 0.09198570624273718, 0.3556283437826026, -0.279967164235691, -0.3193554393678474, -0.04299074557694929, -0.32996098639873356, -0.161392913128321, 0.18367375136473968, 0.004020230289405355, ... |
707.0917 | Toroidal embeddings and polyhedral divisors | Given an effective action of an (n-1)-dimensional torus on an n-dimensional
normal affine variety, Mumford constructs a toroidal embedding, while Altmann
and Hausen give a description in terms of a polyhedral divisor on a curve. We
compare the fan of the toroidal embedding with this polyhedral divisor.
| math.AG | given an effective action of an n1dimensional torus on an ndimensional normal affine variety mumford constructs a toroidal embedding while altmann and hausen give a description in terms of a polyhedral divisor on a curve we compare the fan of the toroidal embedding with this polyhedral divisor | [['given', 'an', 'effective', 'action', 'of', 'an', 'n1dimensional', 'torus', 'on', 'an', 'ndimensional', 'normal', 'affine', 'variety', 'mumford', 'constructs', 'a', 'toroidal', 'embedding', 'while', 'altmann', 'and', 'hausen', 'give', 'a', 'description', 'in', 'terms', 'of', 'a', 'polyhedral', 'divisor', 'on', 'a', '... | [-0.17873470962760932, -0.007549497399521259, -0.10983304637781482, 0.020952250003477835, -0.14781880426280042, -0.0966035793040027, -0.014616024858774022, 0.3051350266533963, -0.27955051996012, -0.18840107706157452, 0.05776042634611355, -0.22325985188140196, -0.17520964958090732, 0.21418835593268593, -0.23592023139304... |
707.0918 | Improved VLBI astrometry of OH maser stars | Aims: Accurate distances to evolved stars with high mass loss rates are
needed for studies of many of their fundamental properties. However, as these
stars are heavily obscured and variable, optical and infrared astrometry is
unable to provide enough accuracy.
Methods: Astrometry using masers in the circumstellar e... | astro-ph | aims accurate distances to evolved stars with high mass loss rates are needed for studies of many of their fundamental properties however as these stars are heavily obscured and variable optical and infrared astrometry is unable to provide enough accuracy methods astrometry using masers in the circumstellar envelopes c... | [['aims', 'accurate', 'distances', 'to', 'evolved', 'stars', 'with', 'high', 'mass', 'loss', 'rates', 'are', 'needed', 'for', 'studies', 'of', 'many', 'of', 'their', 'fundamental', 'properties', 'however', 'as', 'these', 'stars', 'are', 'heavily', 'obscured', 'and', 'variable', 'optical', 'and', 'infrared', 'astrometry... | [-0.06011805375665222, 0.08494948613735144, -0.07188682978882928, 0.04107853963311451, -0.12713599469504533, -0.12613040713946694, 0.12230715373931289, 0.4913919608827615, -0.1575010326175783, -0.3689221764400013, 0.09417158478601395, -0.2812904398765807, 0.0005843497142849261, 0.20732364720989657, -0.09294321403528254... |
707.0919 | Effects of hadronic loops on the direct CP violation of $B_{c}$ | It is well known that the final state interaction plays an important role in
the decays of $B$-meson. The contribution of the final state interaction which
is supposed to be long-distance effects, to the concerned processes can
interfere with that of the short-distance effects produced via the tree and/or
loop diagra... | hep-ph | it is well known that the final state interaction plays an important role in the decays of bmeson the contribution of the final state interaction which is supposed to be longdistance effects to the concerned processes can interfere with that of the shortdistance effects produced via the tree andor loop diagrams at quar... | [['it', 'is', 'well', 'known', 'that', 'the', 'final', 'state', 'interaction', 'plays', 'an', 'important', 'role', 'in', 'the', 'decays', 'of', 'bmeson', 'the', 'contribution', 'of', 'the', 'final', 'state', 'interaction', 'which', 'is', 'supposed', 'to', 'be', 'longdistance', 'effects', 'to', 'the', 'concerned', 'proc... | [-0.09552253462724238, 0.21019434369250822, -0.11549155801165874, 0.10479918993107716, -0.07348408503770429, -0.10923906105676753, 0.04749181250738443, 0.2892079078561108, -0.2819648815956492, -0.28666771728632934, 0.0866383116273522, -0.30595426210171023, -0.0636914754755195, 0.1511435169264074, 0.06008962632138157, 0... |
707.092 | Spatial Topology and its Structural Analysis based on the Concept of
Simplicial Complex | This paper introduces a model that identifies spatial relationships for a
structural analysis based on the concept of simplicial complex. The spatial
relationships are identified through overlapping two map layers, namely a
primary layer and a contextual layer. The identified spatial relationships are
represented as ... | physics.data-an physics.space-ph | this paper introduces a model that identifies spatial relationships for a structural analysis based on the concept of simplicial complex the spatial relationships are identified through overlapping two map layers namely a primary layer and a contextual layer the identified spatial relationships are represented as a sim... | [['this', 'paper', 'introduces', 'a', 'model', 'that', 'identifies', 'spatial', 'relationships', 'for', 'a', 'structural', 'analysis', 'based', 'on', 'the', 'concept', 'of', 'simplicial', 'complex', 'the', 'spatial', 'relationships', 'are', 'identified', 'through', 'overlapping', 'two', 'map', 'layers', 'namely', 'a', ... | [-0.1318987876018685, 0.06430789956366482, -0.05466797012607304, 0.07685517942834552, -0.05812882041740202, -0.10623936752536856, 0.04661525587431219, 0.373227484336814, -0.3138077500153263, -0.3261285953622007, 0.0806788627209095, -0.2895096350906405, -0.20726793324545542, 0.12333336509412753, -0.035862095064612444, 0... |
707.0921 | Astrophysics in Southern Africa | The government of South Africa has identified astronomy as a field in which
their country has a strategic advantage and is consequently investing very
significantly in astronomical infrastructure. South Africa now operates a 10-m
class optical telescope, the Southern African Large Telescope (SALT), and is
one of two ... | astro-ph | the government of south africa has identified astronomy as a field in which their country has a strategic advantage and is consequently investing very significantly in astronomical infrastructure south africa now operates a 10m class optical telescope the southern african large telescope salt and is one of two countrie... | [['the', 'government', 'of', 'south', 'africa', 'has', 'identified', 'astronomy', 'as', 'a', 'field', 'in', 'which', 'their', 'country', 'has', 'a', 'strategic', 'advantage', 'and', 'is', 'consequently', 'investing', 'very', 'significantly', 'in', 'astronomical', 'infrastructure', 'south', 'africa', 'now', 'operates', ... | [-0.0728997669875531, 0.1300711216244963, -0.05159087776399513, 0.08396278974094723, -0.16763368366490594, -0.12165426731211837, 0.04317095388002444, 0.38027683698867515, -0.20495667621470626, -0.3369800470394605, 0.20296039254824835, -0.30373126563968184, -0.12586627450591328, 0.23370031856863602, -0.05262843439378208... |
707.0922 | B-type defects in Landau-Ginzburg models | We consider Landau-Ginzburg models with possibly different superpotentials
glued together along one-dimensional defect lines. Defects preserving B-type
supersymmetry can be represented by matrix factorisations of the difference of
the superpotentials. The composition of these defects and their action on
B-type bounda... | hep-th | we consider landauginzburg models with possibly different superpotentials glued together along onedimensional defect lines defects preserving btype supersymmetry can be represented by matrix factorisations of the difference of the superpotentials the composition of these defects and their action on btype boundary condi... | [['we', 'consider', 'landauginzburg', 'models', 'with', 'possibly', 'different', 'superpotentials', 'glued', 'together', 'along', 'onedimensional', 'defect', 'lines', 'defects', 'preserving', 'btype', 'supersymmetry', 'can', 'be', 'represented', 'by', 'matrix', 'factorisations', 'of', 'the', 'difference', 'of', 'the', ... | [-0.08537450164467805, 0.12443370265065737, -0.026760415218415715, 0.06772070412989706, 0.008109186978323297, -0.18027947521546767, -0.05478491760524256, 0.40916822365640354, -0.20058965303247706, -0.280438947890486, 0.08605973749598932, -0.29671084644672063, -0.14810131124353834, 0.0664260560380561, -0.134293353013206... |
707.0923 | Quark-gluon plasma paradox | Based on simple physics arguments it is shown that the concept of quark-gluon
plasma, a state of matter consisting of uncorrelated quarks, antiquarks, and
gluons, has a fundamental problem.
| hep-ph | based on simple physics arguments it is shown that the concept of quarkgluon plasma a state of matter consisting of uncorrelated quarks antiquarks and gluons has a fundamental problem | [['based', 'on', 'simple', 'physics', 'arguments', 'it', 'is', 'shown', 'that', 'the', 'concept', 'of', 'quarkgluon', 'plasma', 'a', 'state', 'of', 'matter', 'consisting', 'of', 'uncorrelated', 'quarks', 'antiquarks', 'and', 'gluons', 'has', 'a', 'fundamental', 'problem']] | [-0.05808700968366887, 0.3327435164166422, -0.23141557164490223, 0.08421003382155222, -0.06849233382220926, -0.12164148158425915, 0.026224250808872026, 0.30668072942002067, -0.16569654405887785, -0.20011046348974623, -0.04000450009158973, -0.28703892423674976, -0.04508623416567671, 0.11614089895939005, 0.02661142228492... |
707.0924 | How to define the boundaries of a convective zone and how extended is
overshooting? | Under nonlocal convection theory, convection extends without limit therefore
no apparent boundary can be defined clearly as in the local theory. From the
requirement of a similar structure for both local and non-local models having
the same depth of convection zone, and taking into account the driving
mechanism of tu... | astro-ph | under nonlocal convection theory convection extends without limit therefore no apparent boundary can be defined clearly as in the local theory from the requirement of a similar structure for both local and nonlocal models having the same depth of convection zone and taking into account the driving mechanism of turbulen... | [['under', 'nonlocal', 'convection', 'theory', 'convection', 'extends', 'without', 'limit', 'therefore', 'no', 'apparent', 'boundary', 'can', 'be', 'defined', 'clearly', 'as', 'in', 'the', 'local', 'theory', 'from', 'the', 'requirement', 'of', 'a', 'similar', 'structure', 'for', 'both', 'local', 'and', 'nonlocal', 'mod... | [-0.12132003917195015, 0.22638207917972164, -0.07955300221079259, 0.090240539644199, -0.0846859022960928, -0.08008239944067658, 0.09606609246564851, 0.31985226976474623, -0.30083445999677755, -0.29044586098542313, 0.10154273544424143, -0.21684911984472943, -0.05921467110612921, 0.16819932773222576, -0.05478458683402511... |
707.0925 | The braid groups of the projective plane and the Fadell-Neuwirth short
exact sequence | We study the pure braid groups $P_n(RP^2)$ of the real projective plane
$RP^2$, and in particular the possible splitting of the Fadell-Neuwirth short
exact sequence $1 \to P_m(RP^2 {x_1,...,x_n} \to P_{n+m}(RP^2)
\stackrel{p_{\ast}}{\to} P_n(RP^2) \to 1$, where $n\geq 2$ and $m\geq 1$, and
$p_{\ast}$ is the homomorph... | math.GT math.GR | we study the pure braid groups p_nrp2 of the real projective plane rp2 and in particular the possible splitting of the fadellneuwirth short exact sequence 1 to p_mrp2 x_1x_n to p_nmrp2 stackrelp_astto p_nrp2 to 1 where ngeq 2 and mgeq 1 and p_ast is the homomorphism which corresponds geometrically to forgetting the las... | [['we', 'study', 'the', 'pure', 'braid', 'groups', 'p_nrp2', 'of', 'the', 'real', 'projective', 'plane', 'rp2', 'and', 'in', 'particular', 'the', 'possible', 'splitting', 'of', 'the', 'fadellneuwirth', 'short', 'exact', 'sequence', '1', 'to', 'p_mrp2', 'x_1x_n', 'to', 'p_nmrp2', 'stackrelp_astto', 'p_nrp2', 'to', '1', ... | [-0.1511270915839396, 0.08673871329504272, -0.07250371566604848, 0.052085250844997696, -0.039177186040195246, -0.12711034623918518, -0.00798299177018488, 0.3444258588797494, -0.26670403153660566, -0.25688320847428187, 0.11720851162486029, -0.26667418711562485, -0.14458424457030108, 0.17357104146640573, -0.0912088694069... |
707.0926 | Theorem proving support in programming language semantics | We describe several views of the semantics of a simple programming language
as formal documents in the calculus of inductive constructions that can be
verified by the Coq proof system. Covered aspects are natural semantics,
denotational semantics, axiomatic semantics, and abstract interpretation.
Descriptions as recu... | cs.LO cs.PL | we describe several views of the semantics of a simple programming language as formal documents in the calculus of inductive constructions that can be verified by the coq proof system covered aspects are natural semantics denotational semantics axiomatic semantics and abstract interpretation descriptions as recursive f... | [['we', 'describe', 'several', 'views', 'of', 'the', 'semantics', 'of', 'a', 'simple', 'programming', 'language', 'as', 'formal', 'documents', 'in', 'the', 'calculus', 'of', 'inductive', 'constructions', 'that', 'can', 'be', 'verified', 'by', 'the', 'coq', 'proof', 'system', 'covered', 'aspects', 'are', 'natural', 'sem... | [-0.07123492568149231, 0.017740867455868285, -0.14712394658476113, 0.1465194795106072, -0.18969845475949115, -0.199814011817798, 0.013830468214582652, 0.3589692461490631, -0.32148764315992595, -0.2881736868788721, 0.07733332897303626, -0.22413644568994642, -0.09417151670437306, 0.20806295538321137, -0.17381516737863423... |
707.0927 | Huge Transverse Magnetization in the Field-Induced Phase of the
Antiferromagnetic Molecular Wheel CsFe8 | The 1H-NMR spectrum and nuclear relaxation rate 1/T_1 in the
antiferromagnetic wheel CsFe8 were measured to characterize the previously
observed magnetic field-induced low-temperature phase around the level crossing
at 8 T. The data show that the phase is characterized by a huge staggered
transverse polarization of t... | cond-mat.str-el | the 1hnmr spectrum and nuclear relaxation rate 1t_1 in the antiferromagnetic wheel csfe8 were measured to characterize the previously observed magnetic fieldinduced lowtemperature phase around the level crossing at 8 t the data show that the phase is characterized by a huge staggered transverse polarization of the elec... | [['the', '1hnmr', 'spectrum', 'and', 'nuclear', 'relaxation', 'rate', '1t_1', 'in', 'the', 'antiferromagnetic', 'wheel', 'csfe8', 'were', 'measured', 'to', 'characterize', 'the', 'previously', 'observed', 'magnetic', 'fieldinduced', 'lowtemperature', 'phase', 'around', 'the', 'level', 'crossing', 'at', '8', 't', 'the',... | [-0.20783714742224285, 0.24873774621696415, -0.04231243787765287, 0.034074842425373696, -0.03932019674043725, -0.07633837499399332, 0.10268871682912004, 0.3601584845371004, -0.2739765398487773, -0.33332314007524133, 0.03451612758267995, -0.29807070070418756, -0.05810910768375017, 0.15834783346972603, 0.1142967288395848... |
707.0928 | Tau tagging at Atlas and CMS | The tau identification and reconstruction algorithms developed for the LHC
experiments Atlas and CMS are presented. Reconstruction methods suitable for
use at High Level Trigger and off-line are described in detail
| hep-ex | the tau identification and reconstruction algorithms developed for the lhc experiments atlas and cms are presented reconstruction methods suitable for use at high level trigger and offline are described in detail | [['the', 'tau', 'identification', 'and', 'reconstruction', 'algorithms', 'developed', 'for', 'the', 'lhc', 'experiments', 'atlas', 'and', 'cms', 'are', 'presented', 'reconstruction', 'methods', 'suitable', 'for', 'use', 'at', 'high', 'level', 'trigger', 'and', 'offline', 'are', 'described', 'in', 'detail']] | [0.005011986220075238, 0.08901676589683179, -0.03372962065341492, 0.14844350444693719, 0.0027537855109380136, -0.20046100753449625, -0.08126534790461583, 0.41150998588531246, -0.19828250944133727, -0.3792512057529342, 0.16365655170257895, -0.28454980416403663, -0.039134210636538845, 0.23642515084676205, 0.0033161797590... |
707.0929 | Phase Structure of Thermal QCD/QED:A Gauge Invariant Solution of the HTL
Resummed Improved Ladder Dyson-Schwinger Equation | Based on the hard-thermal-loop resummed improved ladder Dyson-Schwinger
quation for the fermion mass function, we propose a procedure how we can get
the gauge invariant solution in the sense it satisfies the Ward-Takahashi
identity. Results of the numerical analysis are shown and properties of the
``gauge-invariant''... | hep-ph | based on the hardthermalloop resummed improved ladder dysonschwinger quation for the fermion mass function we propose a procedure how we can get the gauge invariant solution in the sense it satisfies the wardtakahashi identity results of the numerical analysis are shown and properties of the gaugeinvariant solutions ar... | [['based', 'on', 'the', 'hardthermalloop', 'resummed', 'improved', 'ladder', 'dysonschwinger', 'quation', 'for', 'the', 'fermion', 'mass', 'function', 'we', 'propose', 'a', 'procedure', 'how', 'we', 'can', 'get', 'the', 'gauge', 'invariant', 'solution', 'in', 'the', 'sense', 'it', 'satisfies', 'the', 'wardtakahashi', '... | [-0.13895393681607912, 0.1004852543832088, -0.16375760475591739, 0.1255172168912024, -0.09685177751341645, -0.07611723527150722, 0.009422992261088625, 0.35441905196889173, -0.1931500905478487, -0.23361486727751943, 0.07362730970026507, -0.3081201032678388, -0.18081772922329148, 0.1246784677614971, -0.004000352486511882... |
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