id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.2435 | Generalized second law in modified theory of gravity | In the context of modified theory of gravity (f(R) gravity) we try to study
the conditions required for validity of the generalized second law.
| gr-qc astro-ph | in the context of modified theory of gravity fr gravity we try to study the conditions required for validity of the generalized second law | [['in', 'the', 'context', 'of', 'modified', 'theory', 'of', 'gravity', 'fr', 'gravity', 'we', 'try', 'to', 'study', 'the', 'conditions', 'required', 'for', 'validity', 'of', 'the', 'generalized', 'second', 'law']] | [-0.12003378520118228, 0.015830770794612665, -0.13143512179764608, 0.15264389167229334, -0.11372969143364269, -0.13030621657768884, -0.011405631768866442, 0.19151179205315808, -0.2051701865469416, -0.3160775477687518, 0.036616958144198485, -0.15905521534538516, -0.1670351019129157, 0.13933221390470862, -0.1279261218539... |
709.2436 | A Note on Singular Cardinals in Set Theory Without Choice | We discuss how singular can cardinals be in absence of the axiom of choice.
We show that, contrasting with known negative consistency results (of Gitik and
others), certain positive results are provable. Then we pose some problems.
| math.LO | we discuss how singular can cardinals be in absence of the axiom of choice we show that contrasting with known negative consistency results of gitik and others certain positive results are provable then we pose some problems | [['we', 'discuss', 'how', 'singular', 'can', 'cardinals', 'be', 'in', 'absence', 'of', 'the', 'axiom', 'of', 'choice', 'we', 'show', 'that', 'contrasting', 'with', 'known', 'negative', 'consistency', 'results', 'of', 'gitik', 'and', 'others', 'certain', 'positive', 'results', 'are', 'provable', 'then', 'we', 'pose', 's... | [-0.15312565752380602, 0.10929498962453894, -0.06009969782285594, 0.11717050077041259, -0.1517047626847351, -0.19405157667760914, 0.012710381903358409, 0.40042159343893463, -0.27932722020793604, -0.2437216028118053, 0.13365005658675186, -0.2990829696677424, -0.20058961494548902, 0.1888065120658359, -0.20354166259435383... |
709.2437 | On Cauchy surfaces in conformally stationary spacetimes | This paper has been withdrawn by the authors because it has been merged with
paper arXiv:0903.3501v1 [math.DG]
| gr-qc math.DG | this paper has been withdrawn by the authors because it has been merged with paper arxiv09033501v1 mathdg | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'because', 'it', 'has', 'been', 'merged', 'with', 'paper', 'arxiv09033501v1', 'mathdg']] | [-0.029607543256133795, -0.016487155691720545, -0.19224902661517262, -0.12260523686563829, -0.15811534435488284, -0.08797323750331998, -0.11817580815113615, 0.40517787728458643, -0.17007693485356867, -0.3511813855729997, 0.1553890355862677, -0.3310900020878762, -0.18741409783251584, 0.04126482142601162, -0.281149961403... |
709.2438 | KAON 2007: Conference Summary | A concise overview of the interesting recent developments in kaon phyiscs
discussed at KAON 2007 is presented.
| hep-ph | a concise overview of the interesting recent developments in kaon phyiscs discussed at kaon 2007 is presented | [['a', 'concise', 'overview', 'of', 'the', 'interesting', 'recent', 'developments', 'in', 'kaon', 'phyiscs', 'discussed', 'at', 'kaon', '2007', 'is', 'presented']] | [-0.04353322576293174, 0.20466537707868745, -0.06616910155314733, 0.1411313290009275, -0.1330548477742602, -0.12046539824565544, -0.012816308394950978, 0.2847304041771328, -0.041053284069194514, -0.19036302222486803, 0.03090982310994364, -0.304856654640068, -0.12829621618284898, 0.2226675050880979, -0.05823894940754946... |
709.2439 | Soft-photon corrections in multi-body meson decays | The effects due to soft-photon emission (and the related virtual corrections)
in multi-body decays of B, D, and K mesons are analysed. We present analytic
expressions for the universal O(alpha) correction factors which can be applied
to all multi-body decay modes where a tight soft-photon energy cut in the
decaying-p... | hep-ph | the effects due to softphoton emission and the related virtual corrections in multibody decays of b d and k mesons are analysed we present analytic expressions for the universal oalpha correction factors which can be applied to all multibody decay modes where a tight softphoton energy cut in the decayingparticle restfr... | [['the', 'effects', 'due', 'to', 'softphoton', 'emission', 'and', 'the', 'related', 'virtual', 'corrections', 'in', 'multibody', 'decays', 'of', 'b', 'd', 'and', 'k', 'mesons', 'are', 'analysed', 'we', 'present', 'analytic', 'expressions', 'for', 'the', 'universal', 'oalpha', 'correction', 'factors', 'which', 'can', 'b... | [-0.114126664090001, 0.20459489951135365, -0.09809828278925883, 0.1742826994920436, -0.014442936988076666, -0.11608092350230276, 0.02797717473643658, 0.3287778704703509, -0.2122384443607918, -0.22842150509029954, -0.007889267561220369, -0.30788656613779264, -0.026542648304622253, 0.1424066637652916, 0.05229051790844936... |
709.244 | Time-Dependent Multi-Centre Solutions from New Metrics with Holonomy
Sim(n-2) | The classifications of holonomy groups in Lorentzian and in Euclidean
signature are quite different. A group of interest in Lorentzian signature in n
dimensions is the maximal proper subgroup of the Lorentz group, SIM(n-2).
Ricci-flat metrics with SIM(2) holonomy were constructed by Kerr and Goldberg,
and a single fo... | hep-th gr-qc math.DG | the classifications of holonomy groups in lorentzian and in euclidean signature are quite different a group of interest in lorentzian signature in n dimensions is the maximal proper subgroup of the lorentz group simn2 ricciflat metrics with sim2 holonomy were constructed by kerr and goldberg and a single fourdimensiona... | [['the', 'classifications', 'of', 'holonomy', 'groups', 'in', 'lorentzian', 'and', 'in', 'euclidean', 'signature', 'are', 'quite', 'different', 'a', 'group', 'of', 'interest', 'in', 'lorentzian', 'signature', 'in', 'n', 'dimensions', 'is', 'the', 'maximal', 'proper', 'subgroup', 'of', 'the', 'lorentz', 'group', 'simn2'... | [-0.17399379669481682, 0.10112549649062136, -0.049786580029737064, 0.08419051515024707, -0.1336062511705138, -0.15069909450011673, -0.04195674440081887, 0.338157501740864, -0.15537299115935133, -0.2749264882049627, 0.0954969058106481, -0.27769963591945945, -0.14130538073713306, 0.18937886230371617, -0.10005769066995493... |
709.2441 | A characterization of Weingarten surfaces in hyperbolic 3-space | We study 2-dimensional submanifolds of the space
${\mathbb{L}}({\mathbb{H}}^3)$ of oriented geodesics of hyperbolic 3-space,
endowed with the canonical neutral K\"ahler structure. Such a surface is
Lagrangian iff there exists a surface in ${\mathbb{H}}^3$ orthogonal to the
geodesics of $\Sigma$.
We prove that the i... | math.DG | we study 2dimensional submanifolds of the space mathbblmathbbh3 of oriented geodesics of hyperbolic 3space endowed with the canonical neutral kahler structure such a surface is lagrangian iff there exists a surface in mathbbh3 orthogonal to the geodesics of sigma we prove that the induced metric on a lagrangian surface... | [['we', 'study', '2dimensional', 'submanifolds', 'of', 'the', 'space', 'mathbblmathbbh3', 'of', 'oriented', 'geodesics', 'of', 'hyperbolic', '3space', 'endowed', 'with', 'the', 'canonical', 'neutral', 'kahler', 'structure', 'such', 'a', 'surface', 'is', 'lagrangian', 'iff', 'there', 'exists', 'a', 'surface', 'in', 'mat... | [-0.25132441657963983, 0.12120154029253172, -0.06881720047870961, 0.0707388517682072, -0.09922011718542005, -0.1277419823842744, -0.07741817571756353, 0.3773824577898874, -0.2498563726840075, -0.15696755080110356, 0.056624165448738495, -0.312466258755497, -0.2128331486795408, 0.15368478722909154, -0.14448785398174854, ... |
709.2442 | Complete intersection dimensions and Foxby classes | Let $R$ be a local ring and $M$ a finitely generated $R$-module. The complete
intersection dimension of $M$--defined by Avramov, Gasharov and Peeva, and
denoted $\cidim_R(M)$--is a homological invariant whose finiteness implies that
$M$ is similar to a module over a complete intersection. It is related to the
classic... | math.AC math.RA | let r be a local ring and m a finitely generated rmodule the complete intersection dimension of mdefined by avramov gasharov and peeva and denoted cidim_rmis a homological invariant whose finiteness implies that m is similar to a module over a complete intersection it is related to the classical projective dimension an... | [['let', 'r', 'be', 'a', 'local', 'ring', 'and', 'm', 'a', 'finitely', 'generated', 'rmodule', 'the', 'complete', 'intersection', 'dimension', 'of', 'mdefined', 'by', 'avramov', 'gasharov', 'and', 'peeva', 'and', 'denoted', 'cidim_rmis', 'a', 'homological', 'invariant', 'whose', 'finiteness', 'implies', 'that', 'm', 'i... | [-0.168214576397013, 0.0679291118900259, -0.10827827951512657, 0.02977528824825882, -0.053533335379162036, -0.22557315942212627, -0.06528145948773367, 0.2969570156264972, -0.36192759663075, -0.13954509685297947, 0.10239172270488958, -0.25744842302210474, -0.08399005247918251, 0.14804540000452132, -0.1837805651773054, -... |
709.2443 | Fractional Dynamical Systems on Fractional Leibniz Algebroids | The theory of derivative of noninteger order goes back to Leibniz, Liouville
and Riemann. Derivatives of fractional order have found many applications in
recent studies in mechanics, physics, economics. In this paper we define the
fractional tangent bundle on a manifold, using a method of Radu Miron. The
fractional L... | math.DG math.DS | the theory of derivative of noninteger order goes back to leibniz liouville and riemann derivatives of fractional order have found many applications in recent studies in mechanics physics economics in this paper we define the fractional tangent bundle on a manifold using a method of radu miron the fractional leibniz al... | [['the', 'theory', 'of', 'derivative', 'of', 'noninteger', 'order', 'goes', 'back', 'to', 'leibniz', 'liouville', 'and', 'riemann', 'derivatives', 'of', 'fractional', 'order', 'have', 'found', 'many', 'applications', 'in', 'recent', 'studies', 'in', 'mechanics', 'physics', 'economics', 'in', 'this', 'paper', 'we', 'def... | [-0.1762556694382408, 0.011208382561601187, -0.09570893016151927, 0.11109017346441273, -0.18247340013548521, -0.09575344909566232, -0.04333956963317075, 0.3268130940818031, -0.32248830370290177, -0.23722591463633827, 0.13915613009823932, -0.2807562590681646, -0.2317040053943933, 0.16895285170708954, -0.1718651771866782... |
709.2444 | Unitary and Euclidean representations of a quiver | A unitary (Euclidean) representation of a quiver is given by assigning to
each vertex a unitary (Euclidean) vector space and to each arrow a linear
mapping of the corresponding vector spaces. We recall an algorithm for reducing
the matrices of a unitary representation to canonical form, give a certain
description of ... | math.RT | a unitary euclidean representation of a quiver is given by assigning to each vertex a unitary euclidean vector space and to each arrow a linear mapping of the corresponding vector spaces we recall an algorithm for reducing the matrices of a unitary representation to canonical form give a certain description of the repr... | [['a', 'unitary', 'euclidean', 'representation', 'of', 'a', 'quiver', 'is', 'given', 'by', 'assigning', 'to', 'each', 'vertex', 'a', 'unitary', 'euclidean', 'vector', 'space', 'and', 'to', 'each', 'arrow', 'a', 'linear', 'mapping', 'of', 'the', 'corresponding', 'vector', 'spaces', 'we', 'recall', 'an', 'algorithm', 'fo... | [-0.11520676550400608, 0.13694282342347672, -0.07781430330200523, 0.028404816707787925, -0.08826339358518667, -0.10642658799484957, 0.01608858086789648, 0.33467716774811934, -0.32677631990016237, -0.18925626443096383, 0.05833099023941174, -0.23176685131757574, -0.18267607449339338, 0.11174856465967263, -0.1020405818525... |
709.2445 | A Simple Characterization of Strategic Behaviors in Broadcast Channels | In this paper, we consider the problem of resource allocation among two
competing users sharing a binary symmetric broadcast channel. We model the
interaction between autonomous selfish users in the resource allocation and
analyze their strategic behavior in manipulating the allocation outcome. We
analytically show t... | cs.IT cs.GT math.IT | in this paper we consider the problem of resource allocation among two competing users sharing a binary symmetric broadcast channel we model the interaction between autonomous selfish users in the resource allocation and analyze their strategic behavior in manipulating the allocation outcome we analytically show that u... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'problem', 'of', 'resource', 'allocation', 'among', 'two', 'competing', 'users', 'sharing', 'a', 'binary', 'symmetric', 'broadcast', 'channel', 'we', 'model', 'the', 'interaction', 'between', 'autonomous', 'selfish', 'users', 'in', 'the', 'resource', 'allocation', 'and'... | [-0.2446682484844453, 0.03627841902540668, -0.06619181664770141, 0.09045925931422971, -0.12827357886057786, -0.25142552946721586, 0.16816900488543873, 0.45017552748322487, -0.29977465560659766, -0.30199734314673526, 0.048608565944424996, -0.28068225966896587, -0.16012966238400517, 0.07727536052013473, -0.11555559759076... |
709.2446 | Learning for Dynamic Bidding in Cognitive Radio Resources | In this paper, we model the various wireless users in a cognitive radio
network as a collection of selfish, autonomous agents that strategically
interact in order to acquire the dynamically available spectrum opportunities.
Our main focus is on developing solutions for wireless users to successfully
compete with each... | cs.LG cs.GT | in this paper we model the various wireless users in a cognitive radio network as a collection of selfish autonomous agents that strategically interact in order to acquire the dynamically available spectrum opportunities our main focus is on developing solutions for wireless users to successfully compete with each othe... | [['in', 'this', 'paper', 'we', 'model', 'the', 'various', 'wireless', 'users', 'in', 'a', 'cognitive', 'radio', 'network', 'as', 'a', 'collection', 'of', 'selfish', 'autonomous', 'agents', 'that', 'strategically', 'interact', 'in', 'order', 'to', 'acquire', 'the', 'dynamically', 'available', 'spectrum', 'opportunities'... | [-0.1624559140010617, 0.03720269390406991, -0.037618196790862084, 0.037850285530538604, -0.1195322551747158, -0.1946322245743605, 0.1262195156737428, 0.4213776169383427, -0.29403870511610214, -0.3189611441254832, 0.07983111642992811, -0.28095312574221387, -0.15597893358729933, 0.13928788960949978, -0.12435517891955512,... |
709.2447 | Testing Lorentz Symmetry with Gravity | In this talk, results from the gravitational sector of the Standard-Model
Extension (SME) are discussed. The weak-field phenomenology of the resulting
modified gravitational field equations is explored. The application of the
results to a variety of modern gravity experiments, including lunar laser
ranging, Gravity P... | gr-qc | in this talk results from the gravitational sector of the standardmodel extension sme are discussed the weakfield phenomenology of the resulting modified gravitational field equations is explored the application of the results to a variety of modern gravity experiments including lunar laser ranging gravity probe b bina... | [['in', 'this', 'talk', 'results', 'from', 'the', 'gravitational', 'sector', 'of', 'the', 'standardmodel', 'extension', 'sme', 'are', 'discussed', 'the', 'weakfield', 'phenomenology', 'of', 'the', 'resulting', 'modified', 'gravitational', 'field', 'equations', 'is', 'explored', 'the', 'application', 'of', 'the', 'resul... | [-0.14011859958390555, 0.1370804345295314, -0.06447205028962344, 0.0886205324720997, -0.13521225086503452, -0.10283160890873161, -0.04223544975262015, 0.22531927254561696, -0.21054548077705887, -0.3139610415504825, 0.04641773733085081, -0.2634207957664565, -0.11990120364052634, 0.2933073354013745, -0.000339190592058002... |
709.2448 | Symmetric symplectic homotopy K3 surfaces | A study on the relation between the smooth structure of a symplectic homotopy
K3 surface and its symplectic symmetries is initiated. A measurement of
exoticness of a symplectic homotopy K3 surface is introduced, and the influence
of an effective action of a K3 group via symplectic symmetries is investigated.
It is sh... | math.GT math.SG | a study on the relation between the smooth structure of a symplectic homotopy k3 surface and its symplectic symmetries is initiated a measurement of exoticness of a symplectic homotopy k3 surface is introduced and the influence of an effective action of a k3 group via symplectic symmetries is investigated it is shown t... | [['a', 'study', 'on', 'the', 'relation', 'between', 'the', 'smooth', 'structure', 'of', 'a', 'symplectic', 'homotopy', 'k3', 'surface', 'and', 'its', 'symplectic', 'symmetries', 'is', 'initiated', 'a', 'measurement', 'of', 'exoticness', 'of', 'a', 'symplectic', 'homotopy', 'k3', 'surface', 'is', 'introduced', 'and', 't... | [-0.20901817697301603, 0.15537677707384395, -0.13405137710367976, 0.11207661398694362, -0.13242919946294593, -0.17674225001098684, -0.01508051223689848, 0.3347363459830314, -0.3041247290922171, -0.2698549104689707, 0.07468172519515126, -0.25611856087284574, -0.19117893638499714, 0.1768445901777911, -0.151748726787677, ... |
709.2449 | Some classes of rational functions and related Banach spaces | For positive integers d, r, and M, we consider the class of rational
functions on real d-dimensional space whose denominators are products of at
most r functions of the form 1+Q(x) where each Q is a quadratic form with
eigenvalues bounded above by M and below by 1/M. Each numerator is a monic
monomial of the same deg... | math.FA | for positive integers d r and m we consider the class of rational functions on real ddimensional space whose denominators are products of at most r functions of the form 1qx where each q is a quadratic form with eigenvalues bounded above by m and below by 1m each numerator is a monic monomial of the same degree as the ... | [['for', 'positive', 'integers', 'd', 'r', 'and', 'm', 'we', 'consider', 'the', 'class', 'of', 'rational', 'functions', 'on', 'real', 'ddimensional', 'space', 'whose', 'denominators', 'are', 'products', 'of', 'at', 'most', 'r', 'functions', 'of', 'the', 'form', '1qx', 'where', 'each', 'q', 'is', 'a', 'quadratic', 'form... | [-0.16723259797868048, 0.11734904105129142, -0.015131930951517256, 0.04142798488704307, -0.04142173499229454, -0.13565528279530906, 0.00286283437312851, 0.33593472790934387, -0.32594323267694564, -0.18971869852393866, 0.10336239160969854, -0.3121652343821141, -0.1529870212829161, 0.20189547157102836, -0.020027729586487... |
709.245 | Numerical methods comparison for protostellar collapse calculations | The development of parallel supercomputers allows today the detailed study of
the collapse and the fragmentation of prestellar cores with increasingly
accurate numerical simulations. Thanks to the advances in sub-millimeter
observations, a wide range of observed initial conditions enable us to study
the different mod... | astro-ph | the development of parallel supercomputers allows today the detailed study of the collapse and the fragmentation of prestellar cores with increasingly accurate numerical simulations thanks to the advances in submillimeter observations a wide range of observed initial conditions enable us to study the different modes of... | [['the', 'development', 'of', 'parallel', 'supercomputers', 'allows', 'today', 'the', 'detailed', 'study', 'of', 'the', 'collapse', 'and', 'the', 'fragmentation', 'of', 'prestellar', 'cores', 'with', 'increasingly', 'accurate', 'numerical', 'simulations', 'thanks', 'to', 'the', 'advances', 'in', 'submillimeter', 'obser... | [-0.08539640075704526, 0.051002405268012634, -0.08160874570852944, 0.06649880467282077, -0.0622683131701446, -0.028767200652509928, -0.024852595827542245, 0.37953022766326155, -0.1845325308741026, -0.34235693624997066, 0.09147326201643972, -0.19994861744462036, -0.0543644323045945, 0.20492582489581157, 0.00290899499142... |
709.2451 | Cooling, Gravity and Geometry: Flow-driven Massive Core Formation | We study numerically the formation of molecular clouds in large-scale
colliding flows including self-gravity. The models emphasize the competition
between the effects of gravity on global and local scales in an isolated cloud.
Global gravity builds up large-scale filaments, while local gravity --
triggered by a combi... | astro-ph | we study numerically the formation of molecular clouds in largescale colliding flows including selfgravity the models emphasize the competition between the effects of gravity on global and local scales in an isolated cloud global gravity builds up largescale filaments while local gravity triggered by a combination of s... | [['we', 'study', 'numerically', 'the', 'formation', 'of', 'molecular', 'clouds', 'in', 'largescale', 'colliding', 'flows', 'including', 'selfgravity', 'the', 'models', 'emphasize', 'the', 'competition', 'between', 'the', 'effects', 'of', 'gravity', 'on', 'global', 'and', 'local', 'scales', 'in', 'an', 'isolated', 'clou... | [-0.16603750484408547, 0.1390132850290581, -0.0891291031377836, 0.0871197532081771, -0.021879604142028053, -0.011757969812811417, 0.014734972940600465, 0.30900848575566014, -0.24805483657499433, -0.3339378676626464, 0.07846862395641617, -0.211283863085145, -0.037839157319903165, 0.14420238478374864, 0.05922900424109326... |
709.2452 | Besov Spaces and Frames on Compact Manifolds | We show that one can characterize the Besov spaces on a smooth compact
oriented Riemannian manifold, for the full range of indices, through a
knowledge of the size of frame coefficients, using the frames we have
constructed in [8].
| math.FA | we show that one can characterize the besov spaces on a smooth compact oriented riemannian manifold for the full range of indices through a knowledge of the size of frame coefficients using the frames we have constructed in 8 | [['we', 'show', 'that', 'one', 'can', 'characterize', 'the', 'besov', 'spaces', 'on', 'a', 'smooth', 'compact', 'oriented', 'riemannian', 'manifold', 'for', 'the', 'full', 'range', 'of', 'indices', 'through', 'a', 'knowledge', 'of', 'the', 'size', 'of', 'frame', 'coefficients', 'using', 'the', 'frames', 'we', 'have', '... | [-0.12105597130572185, 0.06764099133224824, -0.06659083431795573, 0.0718082553969744, -0.06279906549323828, -0.021780759024505433, -0.02786336972927436, 0.4566939585866072, -0.24377152094474205, -0.24593261390542373, 0.13070854519267017, -0.22326406752929473, -0.09911333937914325, 0.23648579596416452, -0.11833761957211... |
709.2453 | About Superluminal motions and Special Relativity: A Discussion of some
recent Experiments, and the solution of the Causal Paradoxes | Some experiments, performed at Berkeley, Cologne, Florence, Vienna, Orsay,
Rennes, etc., led to the claim that something seems to travel with a group
velocity larger than the speed c of light in vacuum. Various other experimental
results seem to point in the same direction: For instance, localized wavelet-
type solut... | physics.class-ph physics.gen-ph physics.optics | some experiments performed at berkeley cologne florence vienna orsay rennes etc led to the claim that something seems to travel with a group velocity larger than the speed c of light in vacuum various other experimental results seem to point in the same direction for instance localized wavelet type solutions to maxwell... | [['some', 'experiments', 'performed', 'at', 'berkeley', 'cologne', 'florence', 'vienna', 'orsay', 'rennes', 'etc', 'led', 'to', 'the', 'claim', 'that', 'something', 'seems', 'to', 'travel', 'with', 'a', 'group', 'velocity', 'larger', 'than', 'the', 'speed', 'c', 'of', 'light', 'in', 'vacuum', 'various', 'other', 'exper... | [-0.08237229866924911, 0.14189937487961007, -0.1113133778482174, 0.12331196818088826, -0.13797764751451233, -0.176561711778721, 0.0017815197703524833, 0.3738279290461483, -0.22370118285224844, -0.30353164206115674, 0.08569259774969676, -0.2832197264374162, -0.14666075833732836, 0.20549869885659203, -0.08309428150980519... |
709.2454 | Gravitational Fugacity as the seed of self-organized violent relaxaton
process toward Local Virial relation | We propose the self-organized relaxation process which drives a collisionless
self-gravitating system (SGS) to the equilibrium state satisfying local virial
(LV) relation. During the violent relaxation process, particles can move widely
within the time interval as short as a few free fall times, because of the
effect... | astro-ph cond-mat.dis-nn cond-mat.stat-mech | we propose the selforganized relaxation process which drives a collisionless selfgravitating system sgs to the equilibrium state satisfying local virial lv relation during the violent relaxation process particles can move widely within the time interval as short as a few free fall times because of the effective potenti... | [['we', 'propose', 'the', 'selforganized', 'relaxation', 'process', 'which', 'drives', 'a', 'collisionless', 'selfgravitating', 'system', 'sgs', 'to', 'the', 'equilibrium', 'state', 'satisfying', 'local', 'virial', 'lv', 'relation', 'during', 'the', 'violent', 'relaxation', 'process', 'particles', 'can', 'move', 'widel... | [-0.12116530490190988, 0.18254476353260024, -0.07688794688188604, 0.0731404859923454, -0.04695158011413046, -0.10889284071246429, 0.04800523539872042, 0.28046133374529225, -0.2764745192070093, -0.29255298255809714, 0.10279452583286912, -0.24047187363462788, -0.12714563445986382, 0.15547895516601523, 0.00248070052991222... |
709.2455 | Existence of a multiplicative basis for a finitely spaced module over an
aggregate | By [R. Bautista, P. Gabriel, A.V Roiter., L. Salmeron, Representation-finite
algebras and multiplicative basis. Invent. Math. 81 (1985) 217-285.], a
finite-dimensional algebra having finitely many isoclasses of indecomposable
representations admits a multiplicative basis. In Sections 4.10-4.12 of [P.
Gabriel, A. V. R... | math.RT | by r bautista p gabriel av roiter l salmeron representationfinite algebras and multiplicative basis invent math 81 1985 217285 a finitedimensional algebra having finitely many isoclasses of indecomposable representations admits a multiplicative basis in sections 410412 of p gabriel a v roiter representations of finited... | [['by', 'r', 'bautista', 'p', 'gabriel', 'av', 'roiter', 'l', 'salmeron', 'representationfinite', 'algebras', 'and', 'multiplicative', 'basis', 'invent', 'math', '81', '1985', '217285', 'a', 'finitedimensional', 'algebra', 'having', 'finitely', 'many', 'isoclasses', 'of', 'indecomposable', 'representations', 'admits', ... | [-0.15461553264395805, 0.024862396791054314, -0.07635956253532482, -0.0009166157966398674, -0.08498781807450713, -0.18077625573167336, -0.03547083154536676, 0.3410603627562523, -0.35531850789160724, -0.25381501423923863, 0.03682892915516066, -0.22460711541909562, -0.15611630436319832, 0.16960501079650028, -0.2269706259... |
709.2456 | Holographic Cosmological Constant and Dark Energy | A general holographic relation between UV and IR cutoff of an effective field
theory is proposed. Taking the IR cutoff relevant to the dark energy as the
Hubble scale, we find that the cosmological constant is highly suppressed by a
numerical factor and the fine tuning problem seems alleviative. We also use
different... | hep-th astro-ph | a general holographic relation between uv and ir cutoff of an effective field theory is proposed taking the ir cutoff relevant to the dark energy as the hubble scale we find that the cosmological constant is highly suppressed by a numerical factor and the fine tuning problem seems alleviative we also use different ir c... | [['a', 'general', 'holographic', 'relation', 'between', 'uv', 'and', 'ir', 'cutoff', 'of', 'an', 'effective', 'field', 'theory', 'is', 'proposed', 'taking', 'the', 'ir', 'cutoff', 'relevant', 'to', 'the', 'dark', 'energy', 'as', 'the', 'hubble', 'scale', 'we', 'find', 'that', 'the', 'cosmological', 'constant', 'is', 'h... | [-0.09552028330474877, 0.14463868801523358, -0.11115454519302517, 0.14411803988058228, -0.1027836250613673, -0.09445642944141898, -0.0038263688380222607, 0.3873733740731858, -0.2311562428628837, -0.36073112053175765, 0.043441183198634804, -0.23603729293614195, -0.07811514518318186, 0.14817711575955583, 0.00352033036018... |
709.2457 | Global analysis of hadron-production data in e^+ e^- annihilation for
determining fragmentation functions | Fragmentation functions of pion, kaon, and nucleon are determined by global
analyses of hadron-production data in $e^+e^-$ annihilation. It is particularly
important that uncertainties of the fragmentation functions are estimated for
the first time. We found that light-quark and gluon fragmentation functions
have lar... | hep-ph hep-ex nucl-ex nucl-th | fragmentation functions of pion kaon and nucleon are determined by global analyses of hadronproduction data in ee annihilation it is particularly important that uncertainties of the fragmentation functions are estimated for the first time we found that lightquark and gluon fragmentation functions have large uncertainti... | [['fragmentation', 'functions', 'of', 'pion', 'kaon', 'and', 'nucleon', 'are', 'determined', 'by', 'global', 'analyses', 'of', 'hadronproduction', 'data', 'in', 'ee', 'annihilation', 'it', 'is', 'particularly', 'important', 'that', 'uncertainties', 'of', 'the', 'fragmentation', 'functions', 'are', 'estimated', 'for', '... | [-0.056609310673151926, 0.251736477469501, -0.12880318297199833, 0.2065125289621754, -0.023552513997820976, -0.05970338696740495, 0.020916001077795638, 0.38488399456209926, -0.1987421679473256, -0.2138513763191052, -0.0006525545433000888, -0.27090911106522947, -0.022772654739561155, 0.1367967364839414, 0.13036504574572... |
709.2458 | Positivity criteria generalizing the leading principal minors criterion | For each Hermitian matrix, we prove that instead of the leading principal
minors some of their sums can be used in the leading principal minors criterion
and in other inertia problems.
| math.RT | for each hermitian matrix we prove that instead of the leading principal minors some of their sums can be used in the leading principal minors criterion and in other inertia problems | [['for', 'each', 'hermitian', 'matrix', 'we', 'prove', 'that', 'instead', 'of', 'the', 'leading', 'principal', 'minors', 'some', 'of', 'their', 'sums', 'can', 'be', 'used', 'in', 'the', 'leading', 'principal', 'minors', 'criterion', 'and', 'in', 'other', 'inertia', 'problems']] | [-0.1461769642248269, 0.09156738597178651, -0.07524064255337562, 0.03776560315201359, -0.056651891960251714, -0.12580977230062407, -0.04622518325284604, 0.32656213148467, -0.34316128384201755, -0.18505821491201077, 0.20046914880344224, -0.2719643504448956, -0.17928828046687187, 0.15448377653956413, -0.07607157321106042... |
709.2459 | Quantum theory of the low-frequency linear susceptibility of
interferometer-type superconducting qubits | We use the density matrix formalism to analyze the interaction of
interferometer-type superconducting qubits with a high quality tank circuit,
which frequency is well below the gap frequency of a qubit. We start with the
ground state characterization of the superconducting flux and charge qubits.
Then, by making use ... | cond-mat.supr-con cond-mat.mes-hall | we use the density matrix formalism to analyze the interaction of interferometertype superconducting qubits with a high quality tank circuit which frequency is well below the gap frequency of a qubit we start with the ground state characterization of the superconducting flux and charge qubits then by making use of a dr... | [['we', 'use', 'the', 'density', 'matrix', 'formalism', 'to', 'analyze', 'the', 'interaction', 'of', 'interferometertype', 'superconducting', 'qubits', 'with', 'a', 'high', 'quality', 'tank', 'circuit', 'which', 'frequency', 'is', 'well', 'below', 'the', 'gap', 'frequency', 'of', 'a', 'qubit', 'we', 'start', 'with', 't... | [-0.16815229699246048, 0.19585315789067254, 0.0023930315648388, -0.03695752438080987, -0.013960921762453527, -0.1544755359813955, 0.12610880653349893, 0.3936217008638628, -0.19406166712071785, -0.3074725423411457, 0.0546518456582076, -0.27004329793001575, -0.05488657511617105, 0.20791407726397834, -0.0087675261455252, ... |
709.246 | The problems of classifying pairs of forms and local algebras with zero
cube radical are wild | We prove that over an algebraically closed field of characteristic not two
the problems of classifying pairs of sesquilinear forms in which the second is
Hermitian, pairs of bilinear forms in which the second is symmetric
(skew-symmetric), and local algebras with zero cube radical and square radical
of dimension 2 ar... | math.RT | we prove that over an algebraically closed field of characteristic not two the problems of classifying pairs of sesquilinear forms in which the second is hermitian pairs of bilinear forms in which the second is symmetric skewsymmetric and local algebras with zero cube radical and square radical of dimension 2 are hopel... | [['we', 'prove', 'that', 'over', 'an', 'algebraically', 'closed', 'field', 'of', 'characteristic', 'not', 'two', 'the', 'problems', 'of', 'classifying', 'pairs', 'of', 'sesquilinear', 'forms', 'in', 'which', 'the', 'second', 'is', 'hermitian', 'pairs', 'of', 'bilinear', 'forms', 'in', 'which', 'the', 'second', 'is', 's... | [-0.19717997826103653, 0.08267070625297493, -0.0013173206576279231, 0.02582707845805479, -0.06176179162492709, -0.15516965642039265, -0.036529778063829454, 0.34397862779774835, -0.35687040223607, -0.19110725365712175, 0.07335255783649959, -0.27017246490743546, -0.13629125861584077, 0.17539289534158473, -0.0321297125624... |
709.2461 | A Logic of Injectivity | Injectivity of objects with respect to a set $\ch$ of morphisms is an
important concept of algebra, model theory and homotopy theory. Here we study
the logic of injectivity consequences of $\ch$, by which we understand
morphisms $h$ such that injectivity with respect to $\ch$ implies injectivity
with respect to $h$. ... | math.CT | injectivity of objects with respect to a set ch of morphisms is an important concept of algebra model theory and homotopy theory here we study the logic of injectivity consequences of ch by which we understand morphisms h such that injectivity with respect to ch implies injectivity with respect to h we formulate three ... | [['injectivity', 'of', 'objects', 'with', 'respect', 'to', 'a', 'set', 'ch', 'of', 'morphisms', 'is', 'an', 'important', 'concept', 'of', 'algebra', 'model', 'theory', 'and', 'homotopy', 'theory', 'here', 'we', 'study', 'the', 'logic', 'of', 'injectivity', 'consequences', 'of', 'ch', 'by', 'which', 'we', 'understand', ... | [-0.10234649757762532, 0.06385273314071538, -0.03484568759225882, 0.09704173692619776, -0.09594523835579281, -0.16384123728845965, 0.012105343011361394, 0.3985084589611698, -0.33826796913130597, -0.25591801717342644, 0.10466718926237753, -0.24041096857943378, -0.09076267737731501, 0.1583512502717325, -0.178674358598232... |
709.2462 | Plasma mechanisms of resonant terahertz detection in two-dimensional
electron channel with split gates | We analyze the operation of a resonant detector of terahertz (THz) radiation
based on a two-dimensional electron gas (2DEG) channel with split gates. The
side gates are used for the excitation of plasma oscillations by incoming THz
radiation and control of the resonant plasma frequencies. The central gate
provides th... | cond-mat.other | we analyze the operation of a resonant detector of terahertz thz radiation based on a twodimensional electron gas 2deg channel with split gates the side gates are used for the excitation of plasma oscillations by incoming thz radiation and control of the resonant plasma frequencies the central gate provides the potenti... | [['we', 'analyze', 'the', 'operation', 'of', 'a', 'resonant', 'detector', 'of', 'terahertz', 'thz', 'radiation', 'based', 'on', 'a', 'twodimensional', 'electron', 'gas', '2deg', 'channel', 'with', 'split', 'gates', 'the', 'side', 'gates', 'are', 'used', 'for', 'the', 'excitation', 'of', 'plasma', 'oscillations', 'by', ... | [-0.16890460026098897, 0.17993984256328674, -0.011114375576352245, -0.005993945338294552, 0.009262820827583505, -0.183365273647109, 0.08561245717157591, 0.4031470569208363, -0.2514597968316316, -0.3134093451874935, 0.02204772831165904, -0.2887793196309728, -0.04829836728988795, 0.26573903688433154, 0.03817279322307236,... |
709.2463 | Problems of classifying associative or Lie algebras and triples of
symmetric or skew-symmetric matrices are wild | We prove that the problems of classifying triples of symmetric or
skew-symmetric matrices up to congruence, local commutative associative
algebras with zero cube radical and square radical of dimension 3, and Lie
algebras with central commutator subalgebra of dimension 3 are hopeless since
each of them reduces to the... | math.RT | we prove that the problems of classifying triples of symmetric or skewsymmetric matrices up to congruence local commutative associative algebras with zero cube radical and square radical of dimension 3 and lie algebras with central commutator subalgebra of dimension 3 are hopeless since each of them reduces to the prob... | [['we', 'prove', 'that', 'the', 'problems', 'of', 'classifying', 'triples', 'of', 'symmetric', 'or', 'skewsymmetric', 'matrices', 'up', 'to', 'congruence', 'local', 'commutative', 'associative', 'algebras', 'with', 'zero', 'cube', 'radical', 'and', 'square', 'radical', 'of', 'dimension', '3', 'and', 'lie', 'algebras', ... | [-0.1659214329129706, 0.05633360841311515, 0.04850345387433966, 0.026189664906511704, -0.09009944605641067, -0.20742474347352982, -0.01815350060351193, 0.3680215335140626, -0.39508672927816707, -0.2027971451325963, 0.11759893272537739, -0.2956374051049352, -0.08997771599097178, 0.11700409507999818, -0.09284025762851039... |
709.2464 | An ultrametric version of the Maillet-Malgrange theorem for nonlinear
q-difference equations | We prove an ultrametric q-difference version of the Maillet-Malgrange
theorem, on the Gevrey nature of formal solutions of nonlinear analytic
q-difference equations. Since \deg_q and \ord_q define two valuations on
{\mathbb C}(q), we obtain, in particular, a result on the growth of the degree
in q and the order at q ... | math.CA math.NT math.QA | we prove an ultrametric qdifference version of the mailletmalgrange theorem on the gevrey nature of formal solutions of nonlinear analytic qdifference equations since deg_q and ord_q define two valuations on mathbb cq we obtain in particular a result on the growth of the degree in q and the order at q of formal solutio... | [['we', 'prove', 'an', 'ultrametric', 'qdifference', 'version', 'of', 'the', 'mailletmalgrange', 'theorem', 'on', 'the', 'gevrey', 'nature', 'of', 'formal', 'solutions', 'of', 'nonlinear', 'analytic', 'qdifference', 'equations', 'since', 'deg_q', 'and', 'ord_q', 'define', 'two', 'valuations', 'on', 'mathbb', 'cq', 'we'... | [-0.2032412862819102, 0.01023582839658798, -0.09500698037704246, 0.07196952674504635, -0.07680754112966713, -0.14086031272918695, -0.007139145477955777, 0.23370830168104953, -0.3072525893471071, -0.21022512953698871, 0.08672706339700473, -0.2602654427201265, -0.18827339289857756, 0.22513489923920363, -0.096409417807109... |
709.2465 | Biquandle longitude invariant of long virtual knots | It is known that the number of biquandle colorings of a long virtual knot
diagram, with a fixed color of the initial arc, is a knot invariant. In this
paper we describe a more subtle invariant: a family of biquandle endomorphisms
obtained from the set of colorings and longitudinal information.
| math.GT | it is known that the number of biquandle colorings of a long virtual knot diagram with a fixed color of the initial arc is a knot invariant in this paper we describe a more subtle invariant a family of biquandle endomorphisms obtained from the set of colorings and longitudinal information | [['it', 'is', 'known', 'that', 'the', 'number', 'of', 'biquandle', 'colorings', 'of', 'a', 'long', 'virtual', 'knot', 'diagram', 'with', 'a', 'fixed', 'color', 'of', 'the', 'initial', 'arc', 'is', 'a', 'knot', 'invariant', 'in', 'this', 'paper', 'we', 'describe', 'a', 'more', 'subtle', 'invariant', 'a', 'family', 'of',... | [-0.2591662640008144, 0.16695068715140224, -0.15512860851362348, 0.09404603907139972, -0.10468272012192756, -0.1252471339609474, 0.06167636065045372, 0.3636868938058615, -0.3126799264550209, -0.31035508431494235, 0.059641149442177264, -0.24342247180640697, -0.18008133228868245, 0.14430033084005117, -0.1620965797547251,... |
709.2466 | Littlewood's algorithm and quaternion matrices | A strengthened form of Schur's triangularization theorem is given for
quaternion matrices with real spectrum (for complex matrices it was given by
Littlewood). Littlewood's algorithm for reducing a complex matrix to a
canonical form under unitary similarity is extended to quaternion matrices
whose eigenvalues have ge... | math.RT | a strengthened form of schurs triangularization theorem is given for quaternion matrices with real spectrum for complex matrices it was given by littlewood littlewoods algorithm for reducing a complex matrix to a canonical form under unitary similarity is extended to quaternion matrices whose eigenvalues have geometric... | [['a', 'strengthened', 'form', 'of', 'schurs', 'triangularization', 'theorem', 'is', 'given', 'for', 'quaternion', 'matrices', 'with', 'real', 'spectrum', 'for', 'complex', 'matrices', 'it', 'was', 'given', 'by', 'littlewood', 'littlewoods', 'algorithm', 'for', 'reducing', 'a', 'complex', 'matrix', 'to', 'a', 'canonica... | [-0.1261315915811186, 0.08772143286963303, -0.10375016438774765, 0.10371219815472917, -0.09242059344736238, -0.1818731170593916, -0.02162897423598527, 0.34344249513621133, -0.2712895907073592, -0.23063449442270212, 0.09853141642330836, -0.23280676260280112, -0.23386844360114387, 0.16174918199734142, -0.0968321567052044... |
709.2467 | Resonant Excitation of Disk Oscillations in Deformed Disks II: A Model
of High Frequency QPOs | The amplification of disk oscillations resulting from nonlinear resonant
couplings between the oscillations and a disk deformation is examined. The disk
is geometrically thin and general relativistic with a non-rotating central
source. A Lagrangian formulation is adopted. The author examined the same
problem a few ye... | astro-ph | the amplification of disk oscillations resulting from nonlinear resonant couplings between the oscillations and a disk deformation is examined the disk is geometrically thin and general relativistic with a nonrotating central source a lagrangian formulation is adopted the author examined the same problem a few years ag... | [['the', 'amplification', 'of', 'disk', 'oscillations', 'resulting', 'from', 'nonlinear', 'resonant', 'couplings', 'between', 'the', 'oscillations', 'and', 'a', 'disk', 'deformation', 'is', 'examined', 'the', 'disk', 'is', 'geometrically', 'thin', 'and', 'general', 'relativistic', 'with', 'a', 'nonrotating', 'central',... | [-0.1779770583147183, 0.16689317213824473, -0.04936004394816386, 0.05648015554415414, -0.09572154778383068, -0.09617260675373915, -0.021023381113804675, 0.3580395619510799, -0.25484506608289037, -0.2518192043546839, 0.0992669061625477, -0.2664914895453163, -0.13303071976312109, 0.1917754577132999, -0.038269226971818636... |
709.2468 | Adjoint cohomology of graded Lie algebras of maximal class | We compute explicitly the adjoint cohomology of two N-graded Lie algebras of
maximal class (infinite dimensional filiform Lie algebras) m_0 and m_2. It is
known that up to an isomorphism there are only three N-graded Lie algebras of
the maximal class. The third algebra from this list is the "positive" part L_1
of the... | math.RA math.RT | we compute explicitly the adjoint cohomology of two ngraded lie algebras of maximal class infinite dimensional filiform lie algebras m_0 and m_2 it is known that up to an isomorphism there are only three ngraded lie algebras of the maximal class the third algebra from this list is the positive part l_1 of the witt or v... | [['we', 'compute', 'explicitly', 'the', 'adjoint', 'cohomology', 'of', 'two', 'ngraded', 'lie', 'algebras', 'of', 'maximal', 'class', 'infinite', 'dimensional', 'filiform', 'lie', 'algebras', 'm_0', 'and', 'm_2', 'it', 'is', 'known', 'that', 'up', 'to', 'an', 'isomorphism', 'there', 'are', 'only', 'three', 'ngraded', '... | [-0.21495905603476606, 0.09739650702657265, -0.016461702964299326, 0.0553606950203315, -0.16134818936032908, -0.11836445493787363, -0.08088275734437528, 0.36593105445441965, -0.3763704138633969, -0.21443339214138277, 0.17676289805855888, -0.242718899115961, -0.12658144148056405, 0.14370526634105532, -0.1225132394152192... |
709.2469 | Estimate of the number of one-parameter families of modules over a tame
algebra | The problem of classifying modules over a tame algebra A reduces to a block
matrix problem of tame type whose indecomposable canonical matrices are zero-
or one-parameter. Respectively, the set of nonisomorphic indecomposable modules
of dimension at most d divides into a finite number f(d,A) of modules and
one-parame... | math.RT | the problem of classifying modules over a tame algebra a reduces to a block matrix problem of tame type whose indecomposable canonical matrices are zero or oneparameter respectively the set of nonisomorphic indecomposable modules of dimension at most d divides into a finite number fda of modules and oneparameter series... | [['the', 'problem', 'of', 'classifying', 'modules', 'over', 'a', 'tame', 'algebra', 'a', 'reduces', 'to', 'a', 'block', 'matrix', 'problem', 'of', 'tame', 'type', 'whose', 'indecomposable', 'canonical', 'matrices', 'are', 'zero', 'or', 'oneparameter', 'respectively', 'the', 'set', 'of', 'nonisomorphic', 'indecomposable... | [-0.15778962611783665, 0.12502613293447093, 0.01286371242111692, -0.01406108240141523, -0.052300039919318406, -0.1701423488403824, -0.011103984484049891, 0.27984990814066196, -0.34158193921046026, -0.20701539883860848, 0.10833598612961205, -0.29173849539442376, -0.12433229447380834, 0.16641354893723115, -0.067187372175... |
709.247 | Computation of the canonical form for the matrices of chains and cycles
of linear mappings | Paul Van Dooren [Linear Algebra Appl. 27 (1979) 103-140] constructed an
algorithm for the computation of all irregular summands in Kronecker's
canonical form of a matrix pencil. The algorithm is numerically stable since it
uses only unitary transformations. We extend Paul Van Dooren's algorithm to the
matrices of a c... | math.RT | paul van dooren linear algebra appl 27 1979 103140 constructed an algorithm for the computation of all irregular summands in kroneckers canonical form of a matrix pencil the algorithm is numerically stable since it uses only unitary transformations we extend paul van doorens algorithm to the matrices of a cycle of line... | [['paul', 'van', 'dooren', 'linear', 'algebra', 'appl', '27', '1979', '103140', 'constructed', 'an', 'algorithm', 'for', 'the', 'computation', 'of', 'all', 'irregular', 'summands', 'in', 'kroneckers', 'canonical', 'form', 'of', 'a', 'matrix', 'pencil', 'the', 'algorithm', 'is', 'numerically', 'stable', 'since', 'it', '... | [-0.13235953953299745, 0.023014947254149078, -0.08274069214787554, 0.013314912271430241, -0.03727930337738465, -0.1923363761538092, 0.025668169303304133, 0.3302329182624817, -0.30257994925384135, -0.2428763827363796, 0.08551854212704461, -0.23137709768671616, -0.25331114499154045, 0.18197020952242846, -0.10467798999617... |
709.2471 | Q-Curvature, Spectral Invariants, and Representation Theory | We give an introductory account of functional determinants of elliptic
operators on manifolds and Polyakov-type formulas for their infinitesimal and
finite conformal variations. We relate this to extremal problems and to the
Q-curvature on even-dimensional conformal manifolds. The exposition is
self-contained, in the... | math.DG math-ph math.MP | we give an introductory account of functional determinants of elliptic operators on manifolds and polyakovtype formulas for their infinitesimal and finite conformal variations we relate this to extremal problems and to the qcurvature on evendimensional conformal manifolds the exposition is selfcontained in the sense of... | [['we', 'give', 'an', 'introductory', 'account', 'of', 'functional', 'determinants', 'of', 'elliptic', 'operators', 'on', 'manifolds', 'and', 'polyakovtype', 'formulas', 'for', 'their', 'infinitesimal', 'and', 'finite', 'conformal', 'variations', 'we', 'relate', 'this', 'to', 'extremal', 'problems', 'and', 'to', 'the',... | [-0.12101130046996109, 0.047815716645952, -0.0902339846157191, 0.13199189114139268, -0.20131788206319406, -0.12787799171494776, -0.044599804234805335, 0.3405157898536377, -0.18545536549042976, -0.263573986233065, 0.12845700689011433, -0.31263531767354724, -0.1726716813026813, 0.16437468104669006, -0.17706327361596969, ... |
709.2472 | Formation of molecular hydrogen on amorphous silicate surfaces | Experimental results on the formation of molecular hydrogen on amorphous
silicate surfaces are presented and analyzed using a rate equation model. The
energy barriers for the relevant diffusion and desorption processes are
obtained. They turn out to be significantly higher than those obtained for
polycrystalline sili... | astro-ph | experimental results on the formation of molecular hydrogen on amorphous silicate surfaces are presented and analyzed using a rate equation model the energy barriers for the relevant diffusion and desorption processes are obtained they turn out to be significantly higher than those obtained for polycrystalline silicate... | [['experimental', 'results', 'on', 'the', 'formation', 'of', 'molecular', 'hydrogen', 'on', 'amorphous', 'silicate', 'surfaces', 'are', 'presented', 'and', 'analyzed', 'using', 'a', 'rate', 'equation', 'model', 'the', 'energy', 'barriers', 'for', 'the', 'relevant', 'diffusion', 'and', 'desorption', 'processes', 'are', ... | [0.0005037459234396616, 0.1397113112681028, -0.041818862568794024, 0.043047048983215874, 0.048661191225983204, -0.05604432075698343, 0.03450824669044879, 0.4977046801812119, -0.21606821703414122, -0.2719781930040982, 0.019569623365532605, -0.27071277025517904, -0.06434199081526862, 0.15673316427144326, 0.02535243017805... |
709.2473 | Canonical forms for complex matrix congruence and *congruence | Canonical forms for congruence and *congruence of square complex matrices
were given by Horn and Sergeichuk in [Linear Algebra Appl. 389 (2004) 347-353],
based on Sergeichuk's paper [Math. USSR, Izvestiya 31 (3) (1988) 481-501],
which employed the theory of representations of quivers with involution. We use
standard ... | math.RT | canonical forms for congruence and congruence of square complex matrices were given by horn and sergeichuk in linear algebra appl 389 2004 347353 based on sergeichuks paper math ussr izvestiya 31 3 1988 481501 which employed the theory of representations of quivers with involution we use standard methods of matrix anal... | [['canonical', 'forms', 'for', 'congruence', 'and', 'congruence', 'of', 'square', 'complex', 'matrices', 'were', 'given', 'by', 'horn', 'and', 'sergeichuk', 'in', 'linear', 'algebra', 'appl', '389', '2004', '347353', 'based', 'on', 'sergeichuks', 'paper', 'math', 'ussr', 'izvestiya', '31', '3', '1988', '481501', 'which... | [-0.11601229339293292, 0.028094298294130363, -0.0323052536893882, 0.059567060956362425, -0.11058939476980705, -0.11756702470329572, -0.006395622450893499, 0.33177057443239355, -0.26578682578247886, -0.28639943125868605, 0.07837468331771956, -0.2524541866359354, -0.21368311846382776, 0.18397155718851554, -0.051458213276... |
709.2474 | The Camera of the MAGIC-II Telescope | The MAGIC 17m diameter Cherenkov telescope will be upgraded with a second
telescope within the year 2007. The camera of MAGIC-II will include several new
features compared to the MAGIC-I camera. Photomultipliers with the highest
available photon collection efficiency have been selected. A modular design
allows easier... | astro-ph | the magic 17m diameter cherenkov telescope will be upgraded with a second telescope within the year 2007 the camera of magicii will include several new features compared to the magici camera photomultipliers with the highest available photon collection efficiency have been selected a modular design allows easier access... | [['the', 'magic', '17m', 'diameter', 'cherenkov', 'telescope', 'will', 'be', 'upgraded', 'with', 'a', 'second', 'telescope', 'within', 'the', 'year', '2007', 'the', 'camera', 'of', 'magicii', 'will', 'include', 'several', 'new', 'features', 'compared', 'to', 'the', 'magici', 'camera', 'photomultipliers', 'with', 'the',... | [-0.0856369767908848, 0.1319909139340105, -0.0732190739864143, 0.005694109675792416, -0.15213381113504532, -0.1893892385396025, -0.010435072579971885, 0.4376363237037934, -0.20406001702111254, -0.3921785487102405, 0.1350132378058568, -0.3098363142553842, -0.05481420629607734, 0.23689046743456074, -0.11836289266444823, ... |
709.2475 | Sparse Representations for Structured Noise Filtering | The role of sparse representations in the context of structured noise
filtering is discussed. A strategy, especially conceived so as to address
problems of an ill posed nature, is presented. The proposed approach revises
and extends the Oblique Matching Pursuit technique. It is shown that, by
working with an orthogon... | math.FA | the role of sparse representations in the context of structured noise filtering is discussed a strategy especially conceived so as to address problems of an ill posed nature is presented the proposed approach revises and extends the oblique matching pursuit technique it is shown that by working with an orthogonal proje... | [['the', 'role', 'of', 'sparse', 'representations', 'in', 'the', 'context', 'of', 'structured', 'noise', 'filtering', 'is', 'discussed', 'a', 'strategy', 'especially', 'conceived', 'so', 'as', 'to', 'address', 'problems', 'of', 'an', 'ill', 'posed', 'nature', 'is', 'presented', 'the', 'proposed', 'approach', 'revises',... | [-0.06850914022419602, 0.05266616857649448, -0.1008022572635673, 0.05801566164319714, -0.12340617624732356, -0.13663857935617368, -0.021004471629858017, 0.40043617178996405, -0.3059324307988087, -0.28590910223002236, 0.16480065360820542, -0.1950967102094243, -0.20147268479069075, 0.15402998765309653, -0.128929067986706... |
709.2476 | Cross Comparison of Synonym Graphs in A Multi Linguistic Context | Language is one of the most important aspects of human cognition; it
represents the way we think, act and communicate with each other. Each language
has its own history, background, and form. A language represents a lot of
important cultural aspects of the nation speaking it. Languages differ and so
do cultures. In t... | nlin.AO | language is one of the most important aspects of human cognition it represents the way we think act and communicate with each other each language has its own history background and form a language represents a lot of important cultural aspects of the nation speaking it languages differ and so do cultures in this paper ... | [['language', 'is', 'one', 'of', 'the', 'most', 'important', 'aspects', 'of', 'human', 'cognition', 'it', 'represents', 'the', 'way', 'we', 'think', 'act', 'and', 'communicate', 'with', 'each', 'other', 'each', 'language', 'has', 'its', 'own', 'history', 'background', 'and', 'form', 'a', 'language', 'represents', 'a', ... | [-0.0460157188004, 0.04200596558060367, -0.08528177739752756, 0.09107623626624553, -0.14680351785846524, -0.11115597197264954, 0.04969378921017702, 0.4352628548557942, -0.2287844670032822, -0.29080096418420637, 0.05456542598256203, -0.32320900532739383, -0.2273446069037138, 0.17369386394202083, -0.1167171517374007, -0.... |
709.2477 | Source radii at target rapidity from two-proton and two-deuteron
correlations in central Pb+Pb collisions at 158 A GeV | Two-proton and two-deuteron correlations have been studied in the target
fragmentation region of central Pb+Pb collisions at 158 A GeV. Protons and
deuterons were measured with the Plastic Ball spectrometer of the WA98
experiment at the CERN SPS. The results of one-dimensional and
multi-dimensional analyses using bot... | nucl-ex | twoproton and twodeuteron correlations have been studied in the target fragmentation region of central pbpb collisions at 158 a gev protons and deuterons were measured with the plastic ball spectrometer of the wa98 experiment at the cern sps the results of onedimensional and multidimensional analyses using both the ber... | [['twoproton', 'and', 'twodeuteron', 'correlations', 'have', 'been', 'studied', 'in', 'the', 'target', 'fragmentation', 'region', 'of', 'central', 'pbpb', 'collisions', 'at', '158', 'a', 'gev', 'protons', 'and', 'deuterons', 'were', 'measured', 'with', 'the', 'plastic', 'ball', 'spectrometer', 'of', 'the', 'wa98', 'exp... | [-0.06532957392392588, 0.22948206489829226, -0.1153327518966326, 0.107787094533074, 0.02935214553890396, -0.11414638465397399, -0.06044512104689459, 0.38446976724734977, -0.16230021540675899, -0.25902558625906646, 0.005176081066212255, -0.36899676401753073, 0.08645846867118, 0.1521470060202578, 0.10532718150821622, 0.0... |
709.2478 | Unparticle physics in diphoton production at the CERN LHC | We have considered the di-photon production with unparticle at LHC. The
contributions of spin-0 and spin-2 unparticle to the di-photon production are
studied in the invariant mass and other kinematical distributions, along with
their dependencies on the model dependent parameters. The signal corresponding
to the unpa... | hep-ph | we have considered the diphoton production with unparticle at lhc the contributions of spin0 and spin2 unparticle to the diphoton production are studied in the invariant mass and other kinematical distributions along with their dependencies on the model dependent parameters the signal corresponding to the unparticle is... | [['we', 'have', 'considered', 'the', 'diphoton', 'production', 'with', 'unparticle', 'at', 'lhc', 'the', 'contributions', 'of', 'spin0', 'and', 'spin2', 'unparticle', 'to', 'the', 'diphoton', 'production', 'are', 'studied', 'in', 'the', 'invariant', 'mass', 'and', 'other', 'kinematical', 'distributions', 'along', 'with... | [-0.10296575577472741, 0.26064912061742945, -0.0638447793042463, 0.17965173817301205, -0.10880324486115912, -0.17187517886665069, -0.0599364179476463, 0.34235212530167597, -0.20506625383530022, -0.30520750473271, -0.035093139165151374, -0.3286659660626133, -0.011066277634422734, 0.10997381693472699, 0.10511584019393853... |
709.2479 | Electron/Photon identification in ATLAS and CMS | Recent studies in ATLAS and CMS experiments for the reconstruction and
identification of electrons and photons using full Monte Carlo and testbeam
data are reported
| physics.data-an | recent studies in atlas and cms experiments for the reconstruction and identification of electrons and photons using full monte carlo and testbeam data are reported | [['recent', 'studies', 'in', 'atlas', 'and', 'cms', 'experiments', 'for', 'the', 'reconstruction', 'and', 'identification', 'of', 'electrons', 'and', 'photons', 'using', 'full', 'monte', 'carlo', 'and', 'testbeam', 'data', 'are', 'reported']] | [0.01796282347291708, 0.1429625464230776, -0.048628323450684546, 0.0682455886527896, 0.0118658547103405, -0.08505054432898759, -0.014489052891731262, 0.43039336025714875, -0.1365757641941309, -0.45182682693004605, 0.10445080707082526, -0.4728437773883343, 0.04687680542469025, 0.27573031529784203, 0.07152902156114578, 0... |
709.248 | Aharonov-Bohm differential conductance modulation in defective metallic
single-wall carbon nanotubes | Using a perturbative approach, the effects of the energy gap induced by the
Aharonov-Bohm (AB) flux on the transport properties of defective metallic
single-walled carbon nanotubes (MSWCNTs) are investigated. The electronic waves
scattered back and forth by a pair of impurities give rise to Fabry-Perot
oscillations w... | cond-mat.mes-hall | using a perturbative approach the effects of the energy gap induced by the aharonovbohm ab flux on the transport properties of defective metallic singlewalled carbon nanotubes mswcnts are investigated the electronic waves scattered back and forth by a pair of impurities give rise to fabryperot oscillations which consti... | [['using', 'a', 'perturbative', 'approach', 'the', 'effects', 'of', 'the', 'energy', 'gap', 'induced', 'by', 'the', 'aharonovbohm', 'ab', 'flux', 'on', 'the', 'transport', 'properties', 'of', 'defective', 'metallic', 'singlewalled', 'carbon', 'nanotubes', 'mswcnts', 'are', 'investigated', 'the', 'electronic', 'waves', ... | [-0.2024653437502363, 0.19982839213725687, -0.04601577761742538, 0.025266093371734435, -0.021157686581554726, -0.1332619700655444, 0.0633886304506466, 0.41887004358066215, -0.2592757742399175, -0.279553518474915, 0.020476904094414734, -0.29321211874124836, -0.14488171718407483, 0.18764263795153624, 0.001914442576035774... |
709.2481 | Next-nearest-neighbor spin-spin and chiral-spin correlation functions in
generalized XXX chain | We develop a simple technique for calculation of next to nearest neighbor
spin-spin and chiral-spin correlation functions in inhomogeneous XXX model.
Exact expression of the chiral-spin order parameter as a function of the model
parameter, $\omega$, is analytically found. Using the same method we also
calculate the n... | cond-mat.str-el cond-mat.stat-mech | we develop a simple technique for calculation of next to nearest neighbor spinspin and chiralspin correlation functions in inhomogeneous xxx model exact expression of the chiralspin order parameter as a function of the model parameter omega is analytically found using the same method we also calculate the next to neare... | [['we', 'develop', 'a', 'simple', 'technique', 'for', 'calculation', 'of', 'next', 'to', 'nearest', 'neighbor', 'spinspin', 'and', 'chiralspin', 'correlation', 'functions', 'in', 'inhomogeneous', 'xxx', 'model', 'exact', 'expression', 'of', 'the', 'chiralspin', 'order', 'parameter', 'as', 'a', 'function', 'of', 'the', ... | [-0.10522522566108299, 0.06915806654641139, 0.0043399293333225486, 0.15566715005011897, -0.045918963117791076, -0.14200212637661025, 0.05035360109260572, 0.4175578716344067, -0.26967288140856127, -0.24649047541398822, 0.05393425833192721, -0.30548543967285824, -0.1314630351262167, 0.15620522822220145, 0.170836787525331... |
709.2482 | Normal form of m-by-n-by-2 matrices for equivalence | We give a canonical form of m-by-2-by-2 spatial matrices for equivalence over
any field.
| math.RT | we give a canonical form of mby2by2 spatial matrices for equivalence over any field | [['we', 'give', 'a', 'canonical', 'form', 'of', 'mby2by2', 'spatial', 'matrices', 'for', 'equivalence', 'over', 'any', 'field']] | [-0.19374565615390354, 0.08399596631240386, -0.10651576031859104, 0.08101866422937466, -0.03442268517728035, -0.09671822688184105, -0.011459179437504364, 0.380961421590585, -0.23358856299175665, -0.22000157163263515, 0.017418452431089602, -0.13336564084658256, -0.1323042596475436, 0.1772001855648481, -0.014798385807527... |
709.2483 | Quantum Thetas on Noncommutative T^d with General Embeddings | In this paper we construct quantum theta functions over noncommutative T^d
with general embeddings. Manin has constructed quantum theta functions from the
lattice embedding into vector space x finite group. We extend Manin's
construction of quantum thetas to the case of general embedding of vector space
x lattice x t... | math-ph math.MP | in this paper we construct quantum theta functions over noncommutative td with general embeddings manin has constructed quantum theta functions from the lattice embedding into vector space x finite group we extend manins construction of quantum thetas to the case of general embedding of vector space x lattice x torus i... | [['in', 'this', 'paper', 'we', 'construct', 'quantum', 'theta', 'functions', 'over', 'noncommutative', 'td', 'with', 'general', 'embeddings', 'manin', 'has', 'constructed', 'quantum', 'theta', 'functions', 'from', 'the', 'lattice', 'embedding', 'into', 'vector', 'space', 'x', 'finite', 'group', 'we', 'extend', 'manins'... | [-0.13474582661545337, 0.14520877236594457, -0.05968151207674633, 0.05665824193897836, -0.10174949047616635, -0.1302437885109373, 0.040294177191698866, 0.3806476549085493, -0.33715040966717885, -0.13642631032776953, 0.07459541700305324, -0.2795388404646832, -0.1798403720263241, 0.17195195594633167, -0.04020725648774944... |
709.2484 | Effect of Motion of the Reference Frame on Geometrical Form of the Line
of Monopole Singularity | The monopole singularity string, infinite direct line in the rest reference
frame, is considered as a rigid physical line, and behavior of its geometrical
form under the Lorentz transformations is studied. The method to test the form
of any rigid line or surface in relativistical terms is based on the use of
light si... | physics.class-ph | the monopole singularity string infinite direct line in the rest reference frame is considered as a rigid physical line and behavior of its geometrical form under the lorentz transformations is studied the method to test the form of any rigid line or surface in relativistical terms is based on the use of light signals ... | [['the', 'monopole', 'singularity', 'string', 'infinite', 'direct', 'line', 'in', 'the', 'rest', 'reference', 'frame', 'is', 'considered', 'as', 'a', 'rigid', 'physical', 'line', 'and', 'behavior', 'of', 'its', 'geometrical', 'form', 'under', 'the', 'lorentz', 'transformations', 'is', 'studied', 'the', 'method', 'to', ... | [-0.12669118567579754, 0.04491985456126047, -0.07298158503442505, 0.025590196519747414, -0.0817755299003821, -0.1205602778961331, 0.02342024524032112, 0.37897569091964356, -0.233305074307333, -0.22334894181137355, 0.07229939422038921, -0.2689075302349036, -0.06890587087779661, 0.1392165179393897, -0.031340450901065915,... |
709.2485 | Canonical matrices for linear matrix problems | We consider a large class of matrix problems, which includes the problem of
classifying arbitrary systems of linear mappings. For every matrix problem from
this class, we construct Belitskii's algorithm for reducing a matrix to a
canonical form, which is the generalization of the Jordan normal form, and
study the set... | math.RT | we consider a large class of matrix problems which includes the problem of classifying arbitrary systems of linear mappings for every matrix problem from this class we construct belitskiis algorithm for reducing a matrix to a canonical form which is the generalization of the jordan normal form and study the set cmn of ... | [['we', 'consider', 'a', 'large', 'class', 'of', 'matrix', 'problems', 'which', 'includes', 'the', 'problem', 'of', 'classifying', 'arbitrary', 'systems', 'of', 'linear', 'mappings', 'for', 'every', 'matrix', 'problem', 'from', 'this', 'class', 'we', 'construct', 'belitskiis', 'algorithm', 'for', 'reducing', 'a', 'matr... | [-0.16846453151713633, 0.07576190599794835, 0.037556044085277726, 0.0016445568618700676, -0.03528757792772706, -0.13449655875045152, 0.03755137561964467, 0.32359462488711493, -0.30024503555494486, -0.2003853182241167, 0.10792008170872427, -0.2927175424512975, -0.17913663416642445, 0.1626065312428688, -0.053032189598018... |
709.2486 | Field equations of electromagnetic and gravitational fields | The paper studies the validity of Maxwell equation in the case for
coexistence of electromagnetic field and gravitational field. With the algebra
of quaternions, the Newton's law of gravitation is the same as that in
classical theory of gravitational field. Meanwhile the Maxwell equation is
identical with that in cla... | physics.gen-ph | the paper studies the validity of maxwell equation in the case for coexistence of electromagnetic field and gravitational field with the algebra of quaternions the newtons law of gravitation is the same as that in classical theory of gravitational field meanwhile the maxwell equation is identical with that in classical... | [['the', 'paper', 'studies', 'the', 'validity', 'of', 'maxwell', 'equation', 'in', 'the', 'case', 'for', 'coexistence', 'of', 'electromagnetic', 'field', 'and', 'gravitational', 'field', 'with', 'the', 'algebra', 'of', 'quaternions', 'the', 'newtons', 'law', 'of', 'gravitation', 'is', 'the', 'same', 'as', 'that', 'in',... | [-0.19279918449510394, 0.12337816432480095, -0.07289640857720549, 0.026311984360308467, -0.1120826793310133, -0.07078997298026259, -0.057548617872915875, 0.27121381120738186, -0.2325117644826764, -0.2911958240008759, 0.057599089734563694, -0.23119186403826603, -0.16688035670848725, 0.19834104383780252, 0.00703724920387... |
709.2487 | Exploring the QCD phase structure with density fluctuations | We briefly summarize the properties of conserved charge fluctuations as a
sensitive probe for the QCD phase transitions. We discuss the density
fluctuations which play a significant role to search for the critical end
point. The importance of spinodal instabilities to distinguish the first-order
phase transition is a... | hep-ph nucl-th | we briefly summarize the properties of conserved charge fluctuations as a sensitive probe for the qcd phase transitions we discuss the density fluctuations which play a significant role to search for the critical end point the importance of spinodal instabilities to distinguish the firstorder phase transition is also i... | [['we', 'briefly', 'summarize', 'the', 'properties', 'of', 'conserved', 'charge', 'fluctuations', 'as', 'a', 'sensitive', 'probe', 'for', 'the', 'qcd', 'phase', 'transitions', 'we', 'discuss', 'the', 'density', 'fluctuations', 'which', 'play', 'a', 'significant', 'role', 'to', 'search', 'for', 'the', 'critical', 'end',... | [-0.16454121394425023, 0.23931743081050869, -0.12209043727845562, 0.13842448538254795, -0.020886962682160795, -0.0498806112873539, 0.08076292640833678, 0.2904283586813479, -0.23795898393632806, -0.23253555383001054, 0.11143536949340178, -0.30437004397034034, -0.16478974079447134, 0.0762372466840078, 0.06752343445408102... |
709.2488 | Complexity of matrix problems | In representation theory, the problem of classifying pairs of matrices up to
simultaneous similarity is used as a measure of complexity; classification
problems containing it are called wild problems. We show in an explicit form
that this problem contains all classification matrix problems given by quivers
or posets.... | math.RT | in representation theory the problem of classifying pairs of matrices up to simultaneous similarity is used as a measure of complexity classification problems containing it are called wild problems we show in an explicit form that this problem contains all classification matrix problems given by quivers or posets then ... | [['in', 'representation', 'theory', 'the', 'problem', 'of', 'classifying', 'pairs', 'of', 'matrices', 'up', 'to', 'simultaneous', 'similarity', 'is', 'used', 'as', 'a', 'measure', 'of', 'complexity', 'classification', 'problems', 'containing', 'it', 'are', 'called', 'wild', 'problems', 'we', 'show', 'in', 'an', 'explic... | [-0.11587098012085266, 0.0457996720815229, -0.02989871976545678, 0.08511044742442879, -0.08100983909252188, -0.1461186410534143, -0.004499489148279195, 0.3501723464754111, -0.3274753171739713, -0.2655940208153553, 0.14147594255803786, -0.28488191075289165, -0.1961319087960599, 0.1787192363045969, -0.15488434462579634, ... |
709.2489 | Congruences of a square matrix and its transpose | It is known that any square matrix over any field F is congruent to its
transpose. We show that they are also *congruent with respect to any
nonidentity involution on F.
| math.RT | it is known that any square matrix over any field f is congruent to its transpose we show that they are also congruent with respect to any nonidentity involution on f | [['it', 'is', 'known', 'that', 'any', 'square', 'matrix', 'over', 'any', 'field', 'f', 'is', 'congruent', 'to', 'its', 'transpose', 'we', 'show', 'that', 'they', 'are', 'also', 'congruent', 'with', 'respect', 'to', 'any', 'nonidentity', 'involution', 'on', 'f']] | [-0.16764741144593684, 0.11667757018679573, -0.039950006310978246, -0.02756852803060845, -0.07624011065420364, -0.21041149560422187, -0.038703873723505006, 0.47312799865199673, -0.33068351405522517, -0.20595236260241137, 0.11069718037822074, -0.3476197851761695, -0.2020891653674264, 0.1560825463985243, -0.1619040944403... |
709.249 | Semiclassical limit of the scattering cross section as a distribution | We consider quantum scattering from a compactly supported potential $q$. The
semiclassical limit amounts to letting the wavenumber $k \to \infty$ while
rescaling the potential as $k^2 q$ (alternatively, one can scale Planck's
constant $\hbar \searrow 0$). It is well-known that, under appropriate
conditions, for $\om ... | math-ph math.MP | we consider quantum scattering from a compactly supported potential q the semiclassical limit amounts to letting the wavenumber k to infty while rescaling the potential as k2 q alternatively one can scale plancks constant hbar searrow 0 it is wellknown that under appropriate conditions for om in bbs_n1 such that there ... | [['we', 'consider', 'quantum', 'scattering', 'from', 'a', 'compactly', 'supported', 'potential', 'q', 'the', 'semiclassical', 'limit', 'amounts', 'to', 'letting', 'the', 'wavenumber', 'k', 'to', 'infty', 'while', 'rescaling', 'the', 'potential', 'as', 'k2', 'q', 'alternatively', 'one', 'can', 'scale', 'plancks', 'const... | [-0.13362495956322606, 0.15796546924330696, -0.07723036020635501, 0.06166759882880551, -0.100154678634607, -0.16821466460414985, 0.005050680171415159, 0.3662113663237038, -0.3176650620351555, -0.22732022557583814, 0.037273327377939446, -0.3146708956510584, -0.07227264641865937, 0.19867261514111698, -0.01809486988428476... |
709.2491 | Supersymmetry Breaking Vacua from M Theory Fivebranes | We consider intersecting brane configurations realizing N=2 supersymmetric
gauge theories broken to N=1 by multitrace superpotentials, and softly to N=0.
We analyze, in the framework of M5-brane wrapping a curve, the supersymmetric
vacua and the analogs of spontaneous supersymmetry breaking and soft
supersymmetry bre... | hep-th | we consider intersecting brane configurations realizing n2 supersymmetric gauge theories broken to n1 by multitrace superpotentials and softly to n0 we analyze in the framework of m5brane wrapping a curve the supersymmetric vacua and the analogs of spontaneous supersymmetry breaking and soft supersymmetry breaking in g... | [['we', 'consider', 'intersecting', 'brane', 'configurations', 'realizing', 'n2', 'supersymmetric', 'gauge', 'theories', 'broken', 'to', 'n1', 'by', 'multitrace', 'superpotentials', 'and', 'softly', 'to', 'n0', 'we', 'analyze', 'in', 'the', 'framework', 'of', 'm5brane', 'wrapping', 'a', 'curve', 'the', 'supersymmetric'... | [-0.18746204278431833, 0.22816799692156023, -0.05781723977793662, 0.1550897961122948, -0.10882535376667715, -0.18716469224084886, -0.0016915419286018924, 0.3520495710677974, -0.1563921601576894, -0.26460906538883583, 0.12400158593255471, -0.22907295462005495, -0.19192432313177146, 0.007477650516911557, -0.1258413061957... |
709.2492 | A Gauge field Induced by the Global Gauge Invariance of Action Integral | As a general rule, it is considered that the global gauge invariance of an
action integral does not cause the occurrence of gauge field. However, in this
paper we demonstrate that when the so-called localized assumption is excluded,
the gauge field will be induced by the global gauge invariance of the action
integral... | math-ph math.MP | as a general rule it is considered that the global gauge invariance of an action integral does not cause the occurrence of gauge field however in this paper we demonstrate that when the socalled localized assumption is excluded the gauge field will be induced by the global gauge invariance of the action integral an exa... | [['as', 'a', 'general', 'rule', 'it', 'is', 'considered', 'that', 'the', 'global', 'gauge', 'invariance', 'of', 'an', 'action', 'integral', 'does', 'not', 'cause', 'the', 'occurrence', 'of', 'gauge', 'field', 'however', 'in', 'this', 'paper', 'we', 'demonstrate', 'that', 'when', 'the', 'socalled', 'localized', 'assumpt... | [-0.17059262823141713, 0.1737923649961289, -0.10862499151806362, 0.0914295152398437, -0.13132495787300047, -0.06591868323472436, -0.0028488970510508927, 0.3599012185071335, -0.24711302735033583, -0.24976658277579997, 0.13000815063829488, -0.1667786777996626, -0.2016809651109039, 0.11047703733087563, -0.0908696195110678... |
709.2493 | Infraparticle Scattering States in Non-Relativistic QED: I. The
Bloch-Nordsieck Paradigm | We construct infraparticle scattering states for Compton scattering in the
standard model of non-relativistic QED. In our construction, an infrared cutoff
initially introduced to regularize the model is removed completely. We
rigorously establish the properties of infraparticle scattering theory
predicted in the clas... | math-ph math.MP | we construct infraparticle scattering states for compton scattering in the standard model of nonrelativistic qed in our construction an infrared cutoff initially introduced to regularize the model is removed completely we rigorously establish the properties of infraparticle scattering theory predicted in the classic wo... | [['we', 'construct', 'infraparticle', 'scattering', 'states', 'for', 'compton', 'scattering', 'in', 'the', 'standard', 'model', 'of', 'nonrelativistic', 'qed', 'in', 'our', 'construction', 'an', 'infrared', 'cutoff', 'initially', 'introduced', 'to', 'regularize', 'the', 'model', 'is', 'removed', 'completely', 'we', 'ri... | [-0.023603011634466903, 0.12869364038363398, -0.13263943892504487, 0.09161047735417793, -0.026286863216332026, -0.09686272127686867, 0.0057278944495400145, 0.32381659859259215, -0.25705041037872434, -0.24405343581124075, -0.005964368668251804, -0.28987921326687294, -0.14489547209481576, 0.14112263421661086, -0.02334968... |
709.2494 | Exact solution of one class of Maryland model | The Hamiltonian H of one-body Maryland model is defined as the sum of a
linear unperturbed Hamiltonian H_0 and the interaction V, which is a Toeplitz
matrix. Maryland model with a doubly infinite Hilbert space are exactly solved.
Special cases of one-body Maryland model include the original Maryland model
(Phys. Rev.... | quant-ph | the hamiltonian h of onebody maryland model is defined as the sum of a linear unperturbed hamiltonian h_0 and the interaction v which is a toeplitz matrix maryland model with a doubly infinite hilbert space are exactly solved special cases of onebody maryland model include the original maryland model phys rev lett 49 8... | [['the', 'hamiltonian', 'h', 'of', 'onebody', 'maryland', 'model', 'is', 'defined', 'as', 'the', 'sum', 'of', 'a', 'linear', 'unperturbed', 'hamiltonian', 'h_0', 'and', 'the', 'interaction', 'v', 'which', 'is', 'a', 'toeplitz', 'matrix', 'maryland', 'model', 'with', 'a', 'doubly', 'infinite', 'hilbert', 'space', 'are',... | [-0.12184843044087756, 0.14188998124639815, -0.012083791759020338, -0.011978993445760958, -0.046117395269296445, -0.22630887254975582, -0.008688191022277655, 0.26876861383304157, -0.19635410562720304, -0.27258733444614336, 0.007275401268998394, -0.3235465032776119, -0.15619281188507253, 0.15548381535578906, -0.02296170... |
709.2495 | Reentrant temperature dependence of critical current in superconductor -
ferromagnet - superconductor junctions based on PdFe alloys | The magnetic and transport properties of $Pd_{0.99}Fe_{0.01}$ thin films have
been studied. We have found that the Curie temperature of the films is about 20
K and the magnetic properties strongly depend on temperature below $T_{Curie}$.
We have also fabricated the set of superconductor-ferromagnet-superconductor
jos... | cond-mat.supr-con | the magnetic and transport properties of pd_099fe_001 thin films have been studied we have found that the curie temperature of the films is about 20 k and the magnetic properties strongly depend on temperature below t_curie we have also fabricated the set of superconductorferromagnetsuperconductor josephson junctions n... | [['the', 'magnetic', 'and', 'transport', 'properties', 'of', 'pd_099fe_001', 'thin', 'films', 'have', 'been', 'studied', 'we', 'have', 'found', 'that', 'the', 'curie', 'temperature', 'of', 'the', 'films', 'is', 'about', '20', 'k', 'and', 'the', 'magnetic', 'properties', 'strongly', 'depend', 'on', 'temperature', 'below... | [-0.19104457428291827, 0.18209871927929389, -0.0576989846666912, -0.06616643343011958, -0.015828942226899134, -0.11082024149016126, 0.06681975202223697, 0.42943910131980845, -0.2087764763938529, -0.31810229939299745, 0.034116786668778626, -0.3413325184351438, -0.06023087408151719, 0.2231620204477728, 0.0899010623575418... |
709.2496 | Resolution of singularities, asymptotic expansions of oscillatory
integrals, and related phenomena | The elementary resolution of singularities algorithm of the author's earlier
paper (math.CA/0609217) is developed further, replacing the quasibump functions
in the blown up coordinates with the characteristic function of a rectangle
times a smooth function. Such functions are easier to deal with, and as
application t... | math.CA | the elementary resolution of singularities algorithm of the authors earlier paper mathca0609217 is developed further replacing the quasibump functions in the blown up coordinates with the characteristic function of a rectangle times a smooth function such functions are easier to deal with and as application the existen... | [['the', 'elementary', 'resolution', 'of', 'singularities', 'algorithm', 'of', 'the', 'authors', 'earlier', 'paper', 'mathca0609217', 'is', 'developed', 'further', 'replacing', 'the', 'quasibump', 'functions', 'in', 'the', 'blown', 'up', 'coordinates', 'with', 'the', 'characteristic', 'function', 'of', 'a', 'rectangle'... | [-0.1272029038102898, 0.05249440623634395, -0.13027457975383316, 0.08552252220355773, -0.09738878309726715, -0.07411862716877035, 0.006822448132360088, 0.34835478165852174, -0.2479282146053655, -0.26683180219094665, 0.13864875951715347, -0.28142268200005804, -0.1663905964116566, 0.20530175734976572, -0.0718363032875848... |
709.2497 | Comment on ``Method to analyze electromechanical stability of dielectric
elastomers" [Appl. Phys. Lett. 91, 061921 (2007)] | The model of Zhao and Suo can be readily generalized to predict the critical
breakdown electric field $E_c$ value of elastomers with arbitrary elastic
strain energy function. An explicit expression for $E_c$ is presented for
elastomeric thin films under biaxial strain and comparisons are made with
experimental data u... | cond-mat.mtrl-sci | the model of zhao and suo can be readily generalized to predict the critical breakdown electric field e_c value of elastomers with arbitrary elastic strain energy function an explicit expression for e_c is presented for elastomeric thin films under biaxial strain and comparisons are made with experimental data using a ... | [['the', 'model', 'of', 'zhao', 'and', 'suo', 'can', 'be', 'readily', 'generalized', 'to', 'predict', 'the', 'critical', 'breakdown', 'electric', 'field', 'e_c', 'value', 'of', 'elastomers', 'with', 'arbitrary', 'elastic', 'strain', 'energy', 'function', 'an', 'explicit', 'expression', 'for', 'e_c', 'is', 'presented', ... | [-0.1052833711539672, 0.13791777212286802, -0.07798228942084352, -0.011497240228817571, -0.08079028104406756, -0.17377794445240619, 0.015306040506205848, 0.39562387078547395, -0.25801231213719455, -0.3052863329082627, 0.05943535385351326, -0.2496056090474028, -0.1457436248043401, 0.2178729112524338, -0.0036159665890138... |
709.2498 | Four-Probe Measurements of Carbon Nanotubes with Narrow Metal Contacts | We find that electrons in single-wall carbon nanotubes may propagate
substantial distances (tens of nanometers) under the metal contacts. We perform
four-probe transport measurements of the nanotube conductance and observe
significant deviations from the standard Kirchhoff's circuit rules. Most
noticeably, injecting ... | cond-mat.mes-hall | we find that electrons in singlewall carbon nanotubes may propagate substantial distances tens of nanometers under the metal contacts we perform fourprobe transport measurements of the nanotube conductance and observe significant deviations from the standard kirchhoffs circuit rules most noticeably injecting current be... | [['we', 'find', 'that', 'electrons', 'in', 'singlewall', 'carbon', 'nanotubes', 'may', 'propagate', 'substantial', 'distances', 'tens', 'of', 'nanometers', 'under', 'the', 'metal', 'contacts', 'we', 'perform', 'fourprobe', 'transport', 'measurements', 'of', 'the', 'nanotube', 'conductance', 'and', 'observe', 'significa... | [-0.20713878204696812, 0.1694304643679061, -0.004861191933741793, -0.03587313519528834, 0.02189578936054204, -0.22436736051895423, 0.15117468481548713, 0.45507238066056743, -0.2812953385819128, -0.332610623765504, -0.06423148848443816, -0.40677120303735137, -0.09535238839453086, 0.20690457158343634, 0.01893249635759275... |
709.2499 | Our Search for an H-R Diagram of Quasars | The 4D Eigenvector 1 parameter space was introduced seven years ago as an
attempt at multiwavelength spectroscopic representation of quasars. It appears
to be the most effective diagnostic space for unifying the diversity of broad
line AGN. This progress report shows that the diagnostic power of 4DE1 is
confirmed usi... | astro-ph | the 4d eigenvector 1 parameter space was introduced seven years ago as an attempt at multiwavelength spectroscopic representation of quasars it appears to be the most effective diagnostic space for unifying the diversity of broad line agn this progress report shows that the diagnostic power of 4de1 is confirmed using o... | [['the', '4d', 'eigenvector', '1', 'parameter', 'space', 'was', 'introduced', 'seven', 'years', 'ago', 'as', 'an', 'attempt', 'at', 'multiwavelength', 'spectroscopic', 'representation', 'of', 'quasars', 'it', 'appears', 'to', 'be', 'the', 'most', 'effective', 'diagnostic', 'space', 'for', 'unifying', 'the', 'diversity'... | [0.028531605188513724, 0.0732559807735316, -0.0033544652907700418, 0.17074572189757936, -0.1745346977388848, -0.1420474955778596, 0.05749850528207507, 0.5101383626595032, -0.11681005101912259, -0.3239718760219704, 0.02382867505000033, -0.35957361011357186, 0.015034707388740113, 0.20302715593791507, -0.01455067703165382... |
709.25 | The Pierre Auger Observatory: status, results and perspective | While the completion of the Pierre Auger Observatory (or simply ``Auger'') is
still underway, the 5165 km^2.sr.yr integrated acceptance accumulated since the
January 1st, 2004 is now significantly larger than what was gathered by the
previous experiments dedicated to the detection of ultra-high-energy cosmic
rays (UH... | astro-ph | while the completion of the pierre auger observatory or simply auger is still underway the 5165 km2sryr integrated acceptance accumulated since the january 1st 2004 is now significantly larger than what was gathered by the previous experiments dedicated to the detection of ultrahighenergy cosmic rays uhecrs we report o... | [['while', 'the', 'completion', 'of', 'the', 'pierre', 'auger', 'observatory', 'or', 'simply', 'auger', 'is', 'still', 'underway', 'the', '5165', 'km2sryr', 'integrated', 'acceptance', 'accumulated', 'since', 'the', 'january', '1st', '2004', 'is', 'now', 'significantly', 'larger', 'than', 'what', 'was', 'gathered', 'by... | [-0.058923387788236144, 0.20748321073595435, -0.010883894506841898, 0.1460856055712793, -0.08020298754796386, 0.025262141982093454, 0.014754434616770595, 0.3959562055766582, -0.20578958021942526, -0.3988469600910321, 0.05748924117535353, -0.35853975240141156, -0.04381418943637982, 0.2241530400677584, 0.0349499695675331... |
709.2501 | Generalized vorticity in transitional quantum turbulence | Transition to condensate state in the degenerate gas of bosons is studied
using the Gross-Pitaevskii equation. It is shown that adiabatic invariance of
an enstrophy (mean squared vorticity) based on a generalized vorticity $curl
(|\psi|^2 {\bf v})/|\psi|^2$, controls dynamics of the transitional turbulence
just befor... | cond-mat.other nlin.CD | transition to condensate state in the degenerate gas of bosons is studied using the grosspitaevskii equation it is shown that adiabatic invariance of an enstrophy mean squared vorticity based on a generalized vorticity curl psi2 bf vpsi2 controls dynamics of the transitional turbulence just before formation of the cond... | [['transition', 'to', 'condensate', 'state', 'in', 'the', 'degenerate', 'gas', 'of', 'bosons', 'is', 'studied', 'using', 'the', 'grosspitaevskii', 'equation', 'it', 'is', 'shown', 'that', 'adiabatic', 'invariance', 'of', 'an', 'enstrophy', 'mean', 'squared', 'vorticity', 'based', 'on', 'a', 'generalized', 'vorticity', ... | [-0.18510522119062703, 0.19028085877770146, -0.09325182047489632, 0.05985632289853778, -0.03130441937953167, -0.09585233121677968, -0.06429573067829811, 0.2920789045248447, -0.256116376283379, -0.20277732224868877, 0.0299255708138974, -0.2412832067324676, -0.07547325233047429, 0.16002696310169995, 0.045900365337729454,... |
709.2502 | Ultrahigh-energy cosmic-ray bounds on nonbirefringent modified-Maxwell
theory | A particularly simple Lorentz-violating modification of the Maxwell theory of
photons maintains gauge invariance, CPT, and renormalization. This
modified-Maxwell theory, coupled to standard Dirac particles, involves nineteen
dimensionless "deformation parameters." Ten of these parameters lead to
birefringence and are... | hep-ph astro-ph hep-th | a particularly simple lorentzviolating modification of the maxwell theory of photons maintains gauge invariance cpt and renormalization this modifiedmaxwell theory coupled to standard dirac particles involves nineteen dimensionless deformation parameters ten of these parameters lead to birefringence and are already tig... | [['a', 'particularly', 'simple', 'lorentzviolating', 'modification', 'of', 'the', 'maxwell', 'theory', 'of', 'photons', 'maintains', 'gauge', 'invariance', 'cpt', 'and', 'renormalization', 'this', 'modifiedmaxwell', 'theory', 'coupled', 'to', 'standard', 'dirac', 'particles', 'involves', 'nineteen', 'dimensionless', 'd... | [-0.08960551975871481, 0.2734741005384306, -0.005795559254548852, 0.08675360693577824, -0.11645111483004358, -0.09778458865669866, 0.007052829523297352, 0.3236603395096839, -0.16975705695545507, -0.4142459842952944, 0.00731100375387108, -0.33117337740490227, -0.03574304966374286, 0.24002649370462648, 0.0025285419385274... |
709.2503 | Decohering d-dimensional quantum resistance | The Landauer scattering approach to 4-probe resistance is revisited for the
case of a d-dimensional disordered resistor in the presence of decoherence. Our
treatment is based on an invariant-embedding equation for the evolution of the
coherent reflection amplitude coefficient in the length of a 1-dimensional
disorder... | cond-mat.mes-hall cond-mat.dis-nn | the landauer scattering approach to 4probe resistance is revisited for the case of a ddimensional disordered resistor in the presence of decoherence our treatment is based on an invariantembedding equation for the evolution of the coherent reflection amplitude coefficient in the length of a 1dimensional disordered cond... | [['the', 'landauer', 'scattering', 'approach', 'to', '4probe', 'resistance', 'is', 'revisited', 'for', 'the', 'case', 'of', 'a', 'ddimensional', 'disordered', 'resistor', 'in', 'the', 'presence', 'of', 'decoherence', 'our', 'treatment', 'is', 'based', 'on', 'an', 'invariantembedding', 'equation', 'for', 'the', 'evoluti... | [-0.1560198016420096, 0.18921838245104683, -0.09023551186992826, 0.018266609076600143, -0.02385325893107244, -0.14106626392336574, 0.02758201369792669, 0.30893357417652173, -0.26773252935444347, -0.18722739031616442, 0.035369799190067025, -0.2994003843426883, -0.12027056517586959, 0.17806160964579237, -0.01134049275703... |
709.2504 | Rigidity, boundary interpolation and reproducing kernels | We use reproducing kernel methods to study various rigidity problems. The
methods and setting allow us to also consider the non-positive case.
| math.CV | we use reproducing kernel methods to study various rigidity problems the methods and setting allow us to also consider the nonpositive case | [['we', 'use', 'reproducing', 'kernel', 'methods', 'to', 'study', 'various', 'rigidity', 'problems', 'the', 'methods', 'and', 'setting', 'allow', 'us', 'to', 'also', 'consider', 'the', 'nonpositive', 'case']] | [-0.004712099463424899, -0.053624600637704134, -0.08707353519275784, 0.16997516121376643, -0.13545953651720827, -0.18184050172567368, -0.013502679606476291, 0.44832008941607043, -0.2521264255893501, -0.21365481022406707, 0.13499741203320975, -0.24977696568451144, -0.2163212839514017, 0.24915858019482007, -0.09571733274... |
709.2505 | Dark Energy-Dark Matter Interaction from the Abell Cluster A586 and
violation of the Equivalence Principle | We find that the Abell Cluster A586 exhibits evidence of the interaction
between dark matter and dark energy and argue that this interaction suggests
evidence of violation of the Equivalence Principle. This violation is found in
the context of two different models of dark energy-dark matter interaction.
| astro-ph gr-qc hep-th | we find that the abell cluster a586 exhibits evidence of the interaction between dark matter and dark energy and argue that this interaction suggests evidence of violation of the equivalence principle this violation is found in the context of two different models of dark energydark matter interaction | [['we', 'find', 'that', 'the', 'abell', 'cluster', 'a586', 'exhibits', 'evidence', 'of', 'the', 'interaction', 'between', 'dark', 'matter', 'and', 'dark', 'energy', 'and', 'argue', 'that', 'this', 'interaction', 'suggests', 'evidence', 'of', 'violation', 'of', 'the', 'equivalence', 'principle', 'this', 'violation', 'is... | [-0.19180985961228292, 0.13698027576716182, -0.17679051003676463, 0.1727546454937336, -0.06567073335989992, -0.09271852656247768, -0.014022261062835125, 0.2865956013903339, -0.2060571156362904, -0.42267081474370144, -0.06448305006129072, -0.24625040757212233, -0.09703809633216959, 0.1011976143147083, 0.1114041084384030... |
709.2506 | Autoencoder, Principal Component Analysis and Support Vector Regression
for Data Imputation | Data collection often results in records that have missing values or
variables. This investigation compares 3 different data imputation models and
identifies their merits by using accuracy measures. Autoencoder Neural
Networks, Principal components and Support Vector regression are used for
prediction and combined wi... | cs.AI cs.DB | data collection often results in records that have missing values or variables this investigation compares 3 different data imputation models and identifies their merits by using accuracy measures autoencoder neural networks principal components and support vector regression are used for prediction and combined with a ... | [['data', 'collection', 'often', 'results', 'in', 'records', 'that', 'have', 'missing', 'values', 'or', 'variables', 'this', 'investigation', 'compares', '3', 'different', 'data', 'imputation', 'models', 'and', 'identifies', 'their', 'merits', 'by', 'using', 'accuracy', 'measures', 'autoencoder', 'neural', 'networks', ... | [-0.05814324677563631, -0.038198255959406985, -0.06006509303319994, 0.08632317448487752, -0.09157275805341919, -0.17764471486661132, 0.0833803390531422, 0.43723596460544145, -0.23340848972509196, -0.3238363283338373, 0.12293869926169473, -0.3056630506129055, -0.14707422433779216, 0.17824024675096703, -0.098366483861764... |
709.2507 | Scattering Theory for Jacobi Operators with General Steplike
Quasi-Periodic Background | We develop direct and inverse scattering theory for Jacobi operators with
steplike coefficients which are asymptotically close to different finite-gap
quasi-periodic coefficients on different sides. We give a complete
characterization of the scattering data, which allow unique solvability of the
inverse scattering pr... | math.SP math-ph math.MP | we develop direct and inverse scattering theory for jacobi operators with steplike coefficients which are asymptotically close to different finitegap quasiperiodic coefficients on different sides we give a complete characterization of the scattering data which allow unique solvability of the inverse scattering problem ... | [['we', 'develop', 'direct', 'and', 'inverse', 'scattering', 'theory', 'for', 'jacobi', 'operators', 'with', 'steplike', 'coefficients', 'which', 'are', 'asymptotically', 'close', 'to', 'different', 'finitegap', 'quasiperiodic', 'coefficients', 'on', 'different', 'sides', 'we', 'give', 'a', 'complete', 'characterizatio... | [-0.13187997803414384, 0.09722830039950517, -0.05966161087585183, 0.06857411538322385, -0.1393469016900501, -0.12517079312461787, -0.03481175072262816, 0.353612267662986, -0.3236771712724406, -0.20975690288469195, 0.13034832375594235, -0.3057420128383316, -0.14964352587524515, 0.19013491275612837, 0.02880228027844658, ... |
709.2508 | Some aspects of calculus on non-smooth sets | Sets in R^n in which every pair of elements x, y can be connected by a path
in the set of length bounded by a constant multiple of the distance between x
and y are considered.
| math.CA | sets in rn in which every pair of elements x y can be connected by a path in the set of length bounded by a constant multiple of the distance between x and y are considered | [['sets', 'in', 'rn', 'in', 'which', 'every', 'pair', 'of', 'elements', 'x', 'y', 'can', 'be', 'connected', 'by', 'a', 'path', 'in', 'the', 'set', 'of', 'length', 'bounded', 'by', 'a', 'constant', 'multiple', 'of', 'the', 'distance', 'between', 'x', 'and', 'y', 'are', 'considered']] | [-0.22053535114456382, 0.17904149311491185, -0.009721666315777434, -0.02904427858690421, 0.04477269457937735, -0.12570795817818078, 0.07078396497915189, 0.40913170524355436, -0.37259366135630345, -0.21517149111928624, 0.034151726108070254, -0.30563725810498, -0.06290300071446432, 0.20464064284331268, -0.064150331231455... |
709.2509 | Measurement of Rashba and Dresselhaus spin-orbit magnetic fields | Spin-orbit coupling is a manifestation of special relativity. In the
reference frame of a moving electron, electric fields transform into magnetic
fields, which interact with the electron spin and lift the degeneracy of
spin-up and spin-down states. In solid-state systems, the resulting spin-orbit
fields are referred... | cond-mat.mes-hall | spinorbit coupling is a manifestation of special relativity in the reference frame of a moving electron electric fields transform into magnetic fields which interact with the electron spin and lift the degeneracy of spinup and spindown states in solidstate systems the resulting spinorbit fields are referred to as dress... | [['spinorbit', 'coupling', 'is', 'a', 'manifestation', 'of', 'special', 'relativity', 'in', 'the', 'reference', 'frame', 'of', 'a', 'moving', 'electron', 'electric', 'fields', 'transform', 'into', 'magnetic', 'fields', 'which', 'interact', 'with', 'the', 'electron', 'spin', 'and', 'lift', 'the', 'degeneracy', 'of', 'sp... | [-0.17931715052730093, 0.20056318175047635, -0.02135038654319942, 0.04264064602321014, -0.08436564452325304, -0.1328863303984205, 0.013524316866532899, 0.42975787112799785, -0.2938276292422476, -0.3386548886219195, 0.0014148125968252618, -0.25041485897731036, -0.07705734670317421, 0.21742979829510053, 0.024203838380053... |
709.251 | The Rise and Fall of Debris Disks: MIPS Observations of h and chi Persei
and the Evolution of Mid-IR Emission from Planet Formation | We describe Spitzer/MIPS observations of the double cluster, h and $\chi$
Persei, covering a $\sim$ 0.6 square-degree area surrounding the cores of both
clusters. The data are combined with IRAC and 2MASS data to investigate $\sim$
616 sources from 1.25-24 $\mu m$. We use the long-baseline $K_{s}$-[24] color
to ident... | astro-ph | we describe spitzermips observations of the double cluster h and chi persei covering a sim 06 squaredegree area surrounding the cores of both clusters the data are combined with irac and 2mass data to investigate sim 616 sources from 12524 mu m we use the longbaseline k_s24 color to identify two populations with ir exc... | [['we', 'describe', 'spitzermips', 'observations', 'of', 'the', 'double', 'cluster', 'h', 'and', 'chi', 'persei', 'covering', 'a', 'sim', '06', 'squaredegree', 'area', 'surrounding', 'the', 'cores', 'of', 'both', 'clusters', 'the', 'data', 'are', 'combined', 'with', 'irac', 'and', '2mass', 'data', 'to', 'investigate', ... | [-0.03029610619138358, 0.1637912965360746, -0.0131980153800404, 0.059865632602578045, -0.06327571834590139, -0.06939491338364906, 0.11183795283448561, 0.43711931561514483, -0.18582689642280045, -0.40761282990060455, 0.04987846728148581, -0.3914819796448626, 0.034556948324654904, 0.14416416015247105, -0.0520630949226176... |
709.2511 | Hamiltonian vector fields of homogeneous polynomials in two variables | Let $g:\mathbb{R}^2\to\mathbb{R}$ be a homogeneous polynomial of degree
$p>1$, $G=(-g'_{y}, g'_{x})$ be its Hamiltonian vector field, and $G_t$ be the
local flow generated by $G$. Denote by $E(G,O)$ the space of germs of
$C^{\infty}$ diffeomorphisms $(\mathbb{R}^2,O)\to(\mathbb{R}^2,O)$ that
preserve orbits of $G$. L... | math.DS | let gmathbbr2tomathbbr be a homogeneous polynomial of degree p1 gg_y g_x be its hamiltonian vector field and g_t be the local flow generated by g denote by ego the space of germs of cinfty diffeomorphisms mathbbr2otomathbbr2o that preserve orbits of g let also e_mathrmidgo be the identity component of ego with respect ... | [['let', 'gmathbbr2tomathbbr', 'be', 'a', 'homogeneous', 'polynomial', 'of', 'degree', 'p1', 'gg_y', 'g_x', 'be', 'its', 'hamiltonian', 'vector', 'field', 'and', 'g_t', 'be', 'the', 'local', 'flow', 'generated', 'by', 'g', 'denote', 'by', 'ego', 'the', 'space', 'of', 'germs', 'of', 'cinfty', 'diffeomorphisms', 'mathbbr... | [-0.22081020286657496, 0.1087972563600724, -0.10285476465141039, -0.044833294527193944, -0.07264718543375273, -0.1466399538875013, -0.061088172730977656, 0.3825636085413106, -0.33104312809353525, -0.1755806168022735, 0.04304925564301575, -0.2752807474779812, -0.13695162560113452, 0.1619135489106759, -0.0584379126100087... |
709.2512 | Quantifying Homology Classes II: Localization and Stability | In the companion paper, we measured homology classes and computed the optimal
homology basis. This paper addresses two related problems, namely, localization
and stability. We localize a class with the cycle minimizing a certain
objective function. We explore three different objective functions, namely,
volume, diame... | cs.CG cs.CC math.AT | in the companion paper we measured homology classes and computed the optimal homology basis this paper addresses two related problems namely localization and stability we localize a class with the cycle minimizing a certain objective function we explore three different objective functions namely volume diameter and rad... | [['in', 'the', 'companion', 'paper', 'we', 'measured', 'homology', 'classes', 'and', 'computed', 'the', 'optimal', 'homology', 'basis', 'this', 'paper', 'addresses', 'two', 'related', 'problems', 'namely', 'localization', 'and', 'stability', 'we', 'localize', 'a', 'class', 'with', 'the', 'cycle', 'minimizing', 'a', 'ce... | [-0.18687045815850384, 0.06653889804950049, -0.029605626760200524, 0.09884973618217968, -0.03353004685292641, -0.0952966580295871, 0.005771001887871702, 0.37993097981844826, -0.3193557703246673, -0.2789960926420045, 0.12460066144750721, -0.24711589997998257, -0.22147688072645802, 0.14766757736175223, -0.150519160489583... |
709.2513 | Extension of the Weil-Petersson connection | Convexity properties of Weil-Petersson geodesics on the Teichm\"{u}ller space
of punctured Riemann surfaces are investigated. A normal form is presented for
the Weil-Petersson Levi-Civita connection for pinched hyperbolic metrics. The
normal form is used to establish approximation of geodesics in boundary spaces.
Con... | math.DG | convexity properties of weilpetersson geodesics on the teichmuller space of punctured riemann surfaces are investigated a normal form is presented for the weilpetersson levicivita connection for pinched hyperbolic metrics the normal form is used to establish approximation of geodesics in boundary spaces considerations ... | [['convexity', 'properties', 'of', 'weilpetersson', 'geodesics', 'on', 'the', 'teichmuller', 'space', 'of', 'punctured', 'riemann', 'surfaces', 'are', 'investigated', 'a', 'normal', 'form', 'is', 'presented', 'for', 'the', 'weilpetersson', 'levicivita', 'connection', 'for', 'pinched', 'hyperbolic', 'metrics', 'the', 'n... | [-0.2760477692880217, 0.06732200141320185, -0.14628435295796202, 0.18312859532588552, -0.18549704003418166, -0.10093432018953946, -0.02099438562178083, 0.38652616402795237, -0.29437683273347154, -0.13812032061058185, 0.06490718210378903, -0.3238992520247496, -0.1679882876755249, 0.23329136532641226, -0.1502558514475822... |
709.2514 | Time Optimal Attitude Control for a Rigid Body | A time optimal attitude control problem is studied for the dynamics of a
rigid body. The objective is to minimize the time to rotate the rigid body to a
desired attitude and angular velocity while subject to constraints on the
control input. Necessary conditions for optimality are developed directly on
the special or... | math.OC | a time optimal attitude control problem is studied for the dynamics of a rigid body the objective is to minimize the time to rotate the rigid body to a desired attitude and angular velocity while subject to constraints on the control input necessary conditions for optimality are developed directly on the special orthog... | [['a', 'time', 'optimal', 'attitude', 'control', 'problem', 'is', 'studied', 'for', 'the', 'dynamics', 'of', 'a', 'rigid', 'body', 'the', 'objective', 'is', 'to', 'minimize', 'the', 'time', 'to', 'rotate', 'the', 'rigid', 'body', 'to', 'a', 'desired', 'attitude', 'and', 'angular', 'velocity', 'while', 'subject', 'to', ... | [-0.155903731768792, 0.05328540517436431, -0.11067975319690945, 0.053700177465536625, -0.14125244496859496, -0.14819514181450472, -0.012575789688645984, 0.4016703799251438, -0.2993597465516754, -0.29027472937826154, 0.1508056643886434, -0.19140051732691685, -0.14425226846753164, 0.20380117841310394, -0.1262270562718947... |
709.2515 | Hanle effect in the CN violet system with LTE modeling | Weak entangled magnetic fields with mixed polarity occupy the main part of
the quiet Sun. The Zeeman effect diagnostics fails to measure such fields
because of cancellation in circular polarization. However, the Hanle effect
diagnostics, accessible through the second solar spectrum, provides us with a
very sensitive ... | astro-ph | weak entangled magnetic fields with mixed polarity occupy the main part of the quiet sun the zeeman effect diagnostics fails to measure such fields because of cancellation in circular polarization however the hanle effect diagnostics accessible through the second solar spectrum provides us with a very sensitive tool fo... | [['weak', 'entangled', 'magnetic', 'fields', 'with', 'mixed', 'polarity', 'occupy', 'the', 'main', 'part', 'of', 'the', 'quiet', 'sun', 'the', 'zeeman', 'effect', 'diagnostics', 'fails', 'to', 'measure', 'such', 'fields', 'because', 'of', 'cancellation', 'in', 'circular', 'polarization', 'however', 'the', 'hanle', 'eff... | [-0.1262646417971275, 0.11357820456584153, -0.011767685160994504, 0.09161613638949746, -0.04361911335977041, -0.10541298946995101, 0.007836379817278725, 0.3813811287317918, -0.22689002226096192, -0.3305062890503572, 0.05621401545991398, -0.22784801072241168, -0.0877367422499239, 0.21355725296126618, 0.02248345764625507... |
709.2516 | Calice Si-W EM Calorimeter: Preliminary Results of the Testbeams 2006 | The CALICE Si-W electromagnetic calorimeter has been tested with electron
beams (1 to 6 GeV) at DESY in May 2006, as well as electrons (6 to 45 GeV) and
hadrons (6 to 80 GeV) at CERN in August and October 2006. Several millions of
events have been taken at different incident angles and three beam impact
positions. Th... | physics.ins-det | the calice siw electromagnetic calorimeter has been tested with electron beams 1 to 6 gev at desy in may 2006 as well as electrons 6 to 45 gev and hadrons 6 to 80 gev at cern in august and october 2006 several millions of events have been taken at different incident angles and three beam impact positions the ecal calib... | [['the', 'calice', 'siw', 'electromagnetic', 'calorimeter', 'has', 'been', 'tested', 'with', 'electron', 'beams', '1', 'to', '6', 'gev', 'at', 'desy', 'in', 'may', '2006', 'as', 'well', 'as', 'electrons', '6', 'to', '45', 'gev', 'and', 'hadrons', '6', 'to', '80', 'gev', 'at', 'cern', 'in', 'august', 'and', 'october', '... | [-0.0608485341815159, 0.21114449332805074, -0.06116540872917927, 0.10132886552217199, -0.034039170506033806, -0.16250368655025166, -0.0387354626399564, 0.437213119396821, -0.15942072940920976, -0.47059537767571336, 0.03558224444327123, -0.35313493551632535, 0.06565235867264106, 0.218124396674226, 0.011384768312440273, ... |
709.2517 | Compact Stellar Systems around NGC 1399 | We have obtained spectroscopic redshifts of colour-selected point sources in
four wide area VLT-FLAMES fields around the Fornax Cluster giant elliptical
galaxy NGC 1399, identifying as cluster members 30 previously unknown faint
(-10.5<M_g'<-8.8) compact stellar systems (CSS), and improving redshift
accuracy for 23 p... | astro-ph | we have obtained spectroscopic redshifts of colourselected point sources in four wide area vltflames fields around the fornax cluster giant elliptical galaxy ngc 1399 identifying as cluster members 30 previously unknown faint 105m_g88 compact stellar systems css and improving redshift accuracy for 23 previously catalog... | [['we', 'have', 'obtained', 'spectroscopic', 'redshifts', 'of', 'colourselected', 'point', 'sources', 'in', 'four', 'wide', 'area', 'vltflames', 'fields', 'around', 'the', 'fornax', 'cluster', 'giant', 'elliptical', 'galaxy', 'ngc', '1399', 'identifying', 'as', 'cluster', 'members', '30', 'previously', 'unknown', 'fain... | [-0.08144804906272175, 0.03686555054135868, -0.1337327020931371, 0.10874956207773626, -0.11921054830937977, -0.10336548014504227, 0.023108575953517143, 0.5124413085686511, -0.06916506032865512, -0.36255837535988805, -0.013183304206335749, -0.30646218778344836, -0.013156244018163656, 0.21355931934132572, -0.075785398289... |
709.2518 | Contact Interactions at the LHC | Contact interactions offer a general framework for describing a new
interaction with a scale above the energy scale probed. These interactions can
occur if the Standard Model particles are composite or if new heavy particles
are exchanged. The discovery potential of contact interactions at the LHC in
dimuon and dijet... | hep-ex hep-ph | contact interactions offer a general framework for describing a new interaction with a scale above the energy scale probed these interactions can occur if the standard model particles are composite or if new heavy particles are exchanged the discovery potential of contact interactions at the lhc in dimuon and dijet fin... | [['contact', 'interactions', 'offer', 'a', 'general', 'framework', 'for', 'describing', 'a', 'new', 'interaction', 'with', 'a', 'scale', 'above', 'the', 'energy', 'scale', 'probed', 'these', 'interactions', 'can', 'occur', 'if', 'the', 'standard', 'model', 'particles', 'are', 'composite', 'or', 'if', 'new', 'heavy', 'p... | [-0.12618394264330465, 0.28848973928640287, -0.09386241489458674, 0.13736136133472124, -0.020340924244374038, -0.2012407461957385, -0.006238619996778046, 0.3058782539019982, -0.2653969047901531, -0.34870220814676334, 0.02701901469651299, -0.32613806766457853, -0.024138539241782078, 0.12112936409345518, 0.09702734534318... |
709.2519 | A photometric search for transients in galaxy clusters | We have begun a program to search for supernovae and other transients in the
fields of galaxy clusters with the 2.3m Bok Telescope on Kitt Peak. We present
our automated photometric methods for data reduction, efficiency
characterization, and initial spectroscopy. With this program, we aim to
ultimately identify $\si... | astro-ph | we have begun a program to search for supernovae and other transients in the fields of galaxy clusters with the 23m bok telescope on kitt peak we present our automated photometric methods for data reduction efficiency characterization and initial spectroscopy with this program we aim to ultimately identify sim2535 clus... | [['we', 'have', 'begun', 'a', 'program', 'to', 'search', 'for', 'supernovae', 'and', 'other', 'transients', 'in', 'the', 'fields', 'of', 'galaxy', 'clusters', 'with', 'the', '23m', 'bok', 'telescope', 'on', 'kitt', 'peak', 'we', 'present', 'our', 'automated', 'photometric', 'methods', 'for', 'data', 'reduction', 'effic... | [-0.04453937107284074, 0.08757032610498666, -0.06651784379276833, 0.10478110766042195, -0.10941646910256951, -0.08033064408113334, 0.12407789633511448, 0.4216881429457016, -0.17973711989064034, -0.3096466208282063, 0.052304708192350974, -0.3477606562450411, 0.0015941594430697481, 0.21506444668050498, -0.015860285158972... |
709.252 | Orbital-quenching-induced magnetism in Ba_2NaOsO_6 | The double perovskite \bnoo with heptavalent Os ($d^1$) is observed to remain
in the ideal cubic structure ({\it i.e.} without orbital ordering) despite
single occupation of the $t_{2g}$ orbitals, even in the ferromagnetically
ordered phase below 6.8 K. Analysis based on the {\it ab initio} dispersion
expressed in te... | cond-mat.str-el cond-mat.mtrl-sci | the double perovskite bnoo with heptavalent os d1 is observed to remain in the ideal cubic structure it ie without orbital ordering despite single occupation of the t_2g orbitals even in the ferromagnetically ordered phase below 68 k analysis based on the it ab initio dispersion expressed in terms of an os t_2gbased wa... | [['the', 'double', 'perovskite', 'bnoo', 'with', 'heptavalent', 'os', 'd1', 'is', 'observed', 'to', 'remain', 'in', 'the', 'ideal', 'cubic', 'structure', 'it', 'ie', 'without', 'orbital', 'ordering', 'despite', 'single', 'occupation', 'of', 'the', 't_2g', 'orbitals', 'even', 'in', 'the', 'ferromagnetically', 'ordered',... | [-0.2226116888129335, 0.20189728110794208, -0.0046755454294105, 0.08313900577535452, -0.02693438946017038, -0.13629646636719736, 0.10942619737231164, 0.3695081410500891, -0.2615109556920339, -0.2927030087231058, -0.057233580876637914, -0.32950397668771936, -0.12160979465485733, 0.07070478878776047, 0.06834666108142445,... |
709.2521 | A Logical Analysis of the Time-Warp Effect of General Relativity | Several versions of the Gravitational Time Dilation effect of General
Relativity are formulated by the use of Einstein's Equivalence Principle. It is
shown that all of them are logical consequence of a first-order axiom system of
Special Relativity extended to accelerated observers.
| gr-qc math-ph math.LO math.MP | several versions of the gravitational time dilation effect of general relativity are formulated by the use of einsteins equivalence principle it is shown that all of them are logical consequence of a firstorder axiom system of special relativity extended to accelerated observers | [['several', 'versions', 'of', 'the', 'gravitational', 'time', 'dilation', 'effect', 'of', 'general', 'relativity', 'are', 'formulated', 'by', 'the', 'use', 'of', 'einsteins', 'equivalence', 'principle', 'it', 'is', 'shown', 'that', 'all', 'of', 'them', 'are', 'logical', 'consequence', 'of', 'a', 'firstorder', 'axiom',... | [-0.1698911180470272, 0.09781360111775853, -0.09631156670816597, 0.15144260212851113, -0.12140603096313066, -0.15623197273262554, -0.04745089901345117, 0.30790712611217586, -0.28603792616299223, -0.2864538249337957, 0.07073101037669749, -0.18074681051629818, -0.11835404148414022, 0.21499671038916512, -0.086673399278273... |
709.2522 | Activating Mg acceptors in AlN by oxygen: first principles calculations | First principles calculations based on density functional theory (DFT) are
performed to study the electronic properties of Mg acceptors in AlN at the
presence of oxygen. It is found that Mg and O tend to form complexes like Mg-O,
Mg$_2$-O, Mg$_3$-O and Mg$_4$-O which have activation energies about 0.23 eV
lower than ... | physics.comp-ph | first principles calculations based on density functional theory dft are performed to study the electronic properties of mg acceptors in aln at the presence of oxygen it is found that mg and o tend to form complexes like mgo mg_2o mg_3o and mg_4o which have activation energies about 023 ev lower than that of mg except ... | [['first', 'principles', 'calculations', 'based', 'on', 'density', 'functional', 'theory', 'dft', 'are', 'performed', 'to', 'study', 'the', 'electronic', 'properties', 'of', 'mg', 'acceptors', 'in', 'aln', 'at', 'the', 'presence', 'of', 'oxygen', 'it', 'is', 'found', 'that', 'mg', 'and', 'o', 'tend', 'to', 'form', 'com... | [-0.00881692021680267, 0.128380353299334, 0.04948546453379095, 0.021726259791656682, 0.04527425553811633, -0.17860928850005503, 0.1299512486267106, 0.48426940277542757, -0.18088379728243403, -0.39142786081394426, -0.04792074241432483, -0.32852382139181313, -0.10050537536001723, 0.13711856463114205, 0.041504178609213106... |
709.2523 | A Generalization of the Poincar\'e-Cartan Integral Invariant for a
Nonlinear Nonholonomic Dynamical System | Based on the d'Alembert-Lagrange-Poincar\'{e} variational principle, we
formulate general equations of motion for mechanical systems subject to
nonlinear nonholonomic constraints, that do not involve Lagrangian undetermined
multipliers. We write these equations in a canonical form called the
Poincar\'{e}-Hamilton equ... | math-ph math.MP | based on the dalembertlagrangepoincare variational principle we formulate general equations of motion for mechanical systems subject to nonlinear nonholonomic constraints that do not involve lagrangian undetermined multipliers we write these equations in a canonical form called the poincarehamilton equations and study ... | [['based', 'on', 'the', 'dalembertlagrangepoincare', 'variational', 'principle', 'we', 'formulate', 'general', 'equations', 'of', 'motion', 'for', 'mechanical', 'systems', 'subject', 'to', 'nonlinear', 'nonholonomic', 'constraints', 'that', 'do', 'not', 'involve', 'lagrangian', 'undetermined', 'multipliers', 'we', 'wri... | [-0.18856811833968035, 0.06254212573738553, -0.10894577614884793, 0.07786355330021817, -0.11639532231248352, -0.10466108163192618, -0.027089769599818382, 0.2691865040785672, -0.315100754540758, -0.25922427594098224, 0.12459095001921151, -0.18643746049409465, -0.1897294248665581, 0.20084213472593637, -0.0757952176206627... |
709.2524 | Cheon's anholonomies in Floquet operators | Anholonomies in the parametric dependences of the eigenvalues and the
eigenvectors of Floquet operators that describe unit time evolutions of
periodically driven systems, e.g., kicked rotors, are studied. First, an
example of the anholonomies induced by a periodically pulsed rank-1
perturbation is given. As a functio... | quant-ph | anholonomies in the parametric dependences of the eigenvalues and the eigenvectors of floquet operators that describe unit time evolutions of periodically driven systems eg kicked rotors are studied first an example of the anholonomies induced by a periodically pulsed rank1 perturbation is given as a function of the st... | [['anholonomies', 'in', 'the', 'parametric', 'dependences', 'of', 'the', 'eigenvalues', 'and', 'the', 'eigenvectors', 'of', 'floquet', 'operators', 'that', 'describe', 'unit', 'time', 'evolutions', 'of', 'periodically', 'driven', 'systems', 'eg', 'kicked', 'rotors', 'are', 'studied', 'first', 'an', 'example', 'of', 'th... | [-0.20597111921784, 0.2028710708269274, -0.059653042608128926, 0.004897650864477139, -0.008468036174320572, -0.12047538521260487, 0.023107711361465406, 0.34445691202318424, -0.28105781986643535, -0.2431496095631291, 0.1056336620454604, -0.28937003487441204, -0.19244839778469172, 0.208729806981035, -0.045291524900996895... |
709.2525 | H-Decompositions | We show that for all graphs H of size n, the complete graph $K_{2n+1}$ has an
$H$-decomposition.
| cs.DM | we show that for all graphs h of size n the complete graph k_2n1 has an hdecomposition | [['we', 'show', 'that', 'for', 'all', 'graphs', 'h', 'of', 'size', 'n', 'the', 'complete', 'graph', 'k_2n1', 'has', 'an', 'hdecomposition']] | [-0.15527572992312558, 0.11219245050982435, -0.0029526535859879326, -0.029071245835546183, -0.051931888166376776, -0.0626780676710255, -0.04087505884030286, 0.4377082831719342, -0.202456185265499, -0.27741037780309424, 0.05964360799749985, -0.3176422557410072, -0.10349446558393538, 0.14313988908029654, -0.0687864636454... |
709.2526 | Many body generalization of the Landau Zener problem | We formulate and approximately solve a specific many-body generalization of
the Landau-Zener problem. Unlike with the single particle Landau-Zener problem,
our system does not abide in the adiabatic ground state, even at very slow
driving rates. The structure of the theory suggests that this finding reflects
a more g... | cond-mat.mes-hall | we formulate and approximately solve a specific manybody generalization of the landauzener problem unlike with the single particle landauzener problem our system does not abide in the adiabatic ground state even at very slow driving rates the structure of the theory suggests that this finding reflects a more general ph... | [['we', 'formulate', 'and', 'approximately', 'solve', 'a', 'specific', 'manybody', 'generalization', 'of', 'the', 'landauzener', 'problem', 'unlike', 'with', 'the', 'single', 'particle', 'landauzener', 'problem', 'our', 'system', 'does', 'not', 'abide', 'in', 'the', 'adiabatic', 'ground', 'state', 'even', 'at', 'very',... | [-0.13259329671979816, 0.13982842475542429, -0.06519296865666374, 0.07456946811344962, -0.021761510482714845, -0.17551192480494224, 0.028541430329260903, 0.3221345816494986, -0.288793837629436, -0.3148912138200276, 0.0433072388086224, -0.22923999471545575, -0.15966690268500575, 0.25045200145991875, -0.03320766920002088... |
709.2527 | Formation Process of a Light Bridge Revealed with the Hinode Solar
Optical Telescope | The Solar Optical Telescope (SOT) aboard HINODE successfully and continuously
observed a formation process of a light bridge in a matured sunspot of the NOAA
active region 10923 for several days with high spatial resolution. During its
formation, many umbral dots were observed emerging from the leading edges of
penum... | astro-ph | the solar optical telescope sot aboard hinode successfully and continuously observed a formation process of a light bridge in a matured sunspot of the noaa active region 10923 for several days with high spatial resolution during its formation many umbral dots were observed emerging from the leading edges of penumbral f... | [['the', 'solar', 'optical', 'telescope', 'sot', 'aboard', 'hinode', 'successfully', 'and', 'continuously', 'observed', 'a', 'formation', 'process', 'of', 'a', 'light', 'bridge', 'in', 'a', 'matured', 'sunspot', 'of', 'the', 'noaa', 'active', 'region', '10923', 'for', 'several', 'days', 'with', 'high', 'spatial', 'reso... | [-0.11440974990635332, 0.2386676248885235, -0.04426194327926187, 0.08244740396976712, -0.07866906672027152, -0.06901473181167195, 0.014449903931544751, 0.4368778416145669, -0.2623343316039869, -0.35367353611663743, 0.0957024786395629, -0.2626553648341523, -0.12354245820386829, 0.21593295278179706, -0.04008775279154569,... |
709.2528 | Confinement Induced Polarization effects in Valence and Inner-shell
Spectra of Atactic Polystyrene | Vacuum ultraviolet (VUV) transmission spectra show a clear polarization
effect in pi electronic transition in spin coated atactic polystyrene (aPS)
films of thickness below 4Rg, where Rg (~20.4nm) is the radius of gyration of
the polymer. This transition associated with pendant benzene rings in
polystyrene. The polar... | cond-mat.soft cond-mat.mtrl-sci | vacuum ultraviolet vuv transmission spectra show a clear polarization effect in pi electronic transition in spin coated atactic polystyrene aps films of thickness below 4rg where rg 204nm is the radius of gyration of the polymer this transition associated with pendant benzene rings in polystyrene the polarization effec... | [['vacuum', 'ultraviolet', 'vuv', 'transmission', 'spectra', 'show', 'a', 'clear', 'polarization', 'effect', 'in', 'pi', 'electronic', 'transition', 'in', 'spin', 'coated', 'atactic', 'polystyrene', 'aps', 'films', 'of', 'thickness', 'below', '4rg', 'where', 'rg', '204nm', 'is', 'the', 'radius', 'of', 'gyration', 'of',... | [-0.17299942659552803, 0.21780976331645047, -0.055890165996088675, -0.07555828207070149, -0.000609746220465185, -0.1449788388898455, 0.006889657656288226, 0.4859293072491489, -0.2732830150421113, -0.272156465375288, -0.005075384957969866, -0.33974882917633903, -0.08761547865861123, 0.09694847643064956, 0.03974239404580... |
709.2529 | A New Family of Somos-like Recurrences | We exhibit a three parameter infinite family of quadratic recurrence
relations inspired by the well known Somos sequences. For one infinite
subfamily we prove that the recurrence generates an infinite sequence of
integers by showing that the same sequence is generated by a linear recurrence
(with suitable initial con... | math.CO | we exhibit a three parameter infinite family of quadratic recurrence relations inspired by the well known somos sequences for one infinite subfamily we prove that the recurrence generates an infinite sequence of integers by showing that the same sequence is generated by a linear recurrence with suitable initial conditi... | [['we', 'exhibit', 'a', 'three', 'parameter', 'infinite', 'family', 'of', 'quadratic', 'recurrence', 'relations', 'inspired', 'by', 'the', 'well', 'known', 'somos', 'sequences', 'for', 'one', 'infinite', 'subfamily', 'we', 'prove', 'that', 'the', 'recurrence', 'generates', 'an', 'infinite', 'sequence', 'of', 'integers'... | [-0.22105531261038425, 0.18947355625234413, -0.09104875458487824, 0.13056846622745993, -0.06895283840026763, -0.14417374612235312, -0.011960523776404226, 0.31750891168615714, -0.3444675323900892, -0.2500582414943336, 0.08925964312850317, -0.2631885157759065, -0.2314166943612161, 0.25431572387356366, -0.0271082252312674... |
709.253 | Three-boson problem at low energy and Implications for dilute
Bose-Einstein condensates | It is shown that the effective interaction strength of three bosons at small
collision energies can be extracted from their wave function at zero energy. An
asymptotic expansion of this wave function at large interparticle distances is
derived, from which is defined a quantity $D$ named three-body scattering
hypervol... | cond-mat.stat-mech hep-lat nucl-th | it is shown that the effective interaction strength of three bosons at small collision energies can be extracted from their wave function at zero energy an asymptotic expansion of this wave function at large interparticle distances is derived from which is defined a quantity d named threebody scattering hypervolume whi... | [['it', 'is', 'shown', 'that', 'the', 'effective', 'interaction', 'strength', 'of', 'three', 'bosons', 'at', 'small', 'collision', 'energies', 'can', 'be', 'extracted', 'from', 'their', 'wave', 'function', 'at', 'zero', 'energy', 'an', 'asymptotic', 'expansion', 'of', 'this', 'wave', 'function', 'at', 'large', 'interpa... | [-0.15638302754632605, 0.2195061973581384, -0.10445046983538002, 0.08849538151055943, 0.0035821433242138787, -0.12406778754120751, -0.0057285009297629585, 0.28676712385761977, -0.25305857899123413, -0.2649281168160087, -0.01737800208441816, -0.31132724896694225, -0.0689284660196184, 0.12142706897733054, 0.0897042803020... |
709.2531 | The total charm cross section | We assess the theoretical uncertainties on the total charm cross section. We
discuss the importance of the quark mass, the scale choice and the parton
densities on the estimate of the uncertainty. We conclude that due to the small
charm quark mass, which amplifies the effect of the other parameters in the
calculation... | hep-ph | we assess the theoretical uncertainties on the total charm cross section we discuss the importance of the quark mass the scale choice and the parton densities on the estimate of the uncertainty we conclude that due to the small charm quark mass which amplifies the effect of the other parameters in the calculation the u... | [['we', 'assess', 'the', 'theoretical', 'uncertainties', 'on', 'the', 'total', 'charm', 'cross', 'section', 'we', 'discuss', 'the', 'importance', 'of', 'the', 'quark', 'mass', 'the', 'scale', 'choice', 'and', 'the', 'parton', 'densities', 'on', 'the', 'estimate', 'of', 'the', 'uncertainty', 'we', 'conclude', 'that', 'd... | [-0.04784745499491692, 0.175845481068469, -0.06647989460482047, 0.1736228094669059, -0.04880380252232919, 0.04733852889890281, 0.10011934379402261, 0.3128102397116331, -0.2106498713676746, -0.3031812481009043, 0.007231520286474663, -0.31136700222985103, 0.03599047360207456, 0.15067568260889788, -0.021988749804978187, 0... |
709.2532 | On Weak Fields in Finsler Spaces | It is shown that in the weak field approximation the new geometrical approach
can lead to the linear field equations for the several independent fields. For
the stronger fields and in the second order approximation the field equations
become non-linear, and the fields become dependent. This breaks the
superposition p... | math-ph math.MP | it is shown that in the weak field approximation the new geometrical approach can lead to the linear field equations for the several independent fields for the stronger fields and in the second order approximation the field equations become nonlinear and the fields become dependent this breaks the superposition princip... | [['it', 'is', 'shown', 'that', 'in', 'the', 'weak', 'field', 'approximation', 'the', 'new', 'geometrical', 'approach', 'can', 'lead', 'to', 'the', 'linear', 'field', 'equations', 'for', 'the', 'several', 'independent', 'fields', 'for', 'the', 'stronger', 'fields', 'and', 'in', 'the', 'second', 'order', 'approximation',... | [-0.16143097899806558, 0.1567071904216639, -0.10065842988181183, 0.11014430553901051, -0.0872631558555771, -0.08095146645791829, -0.07984710331815718, 0.3370526910823008, -0.2711874437306754, -0.2848457402697849, 0.0485831696463389, -0.19182478661373767, -0.14040650459620255, 0.19025814745427025, 0.016412172297185116, ... |
709.2533 | Host galaxy subtraction of TeV candidate BL Lacertae objects | We have derived R-band host galaxy fluxes of 20 TeV candidate BL Lacertae
objects as a function of aperture radius and FWHM. The results are given as
correction tables, that list the fluxes (in mJy) of all ``contaminating''
sources (host galaxy + significant nearby objects) as a function of aperture
radius and FWHM. ... | astro-ph | we have derived rband host galaxy fluxes of 20 tev candidate bl lacertae objects as a function of aperture radius and fwhm the results are given as correction tables that list the fluxes in mjy of all contaminating sources host galaxy significant nearby objects as a function of aperture radius and fwhm we found that th... | [['we', 'have', 'derived', 'rband', 'host', 'galaxy', 'fluxes', 'of', '20', 'tev', 'candidate', 'bl', 'lacertae', 'objects', 'as', 'a', 'function', 'of', 'aperture', 'radius', 'and', 'fwhm', 'the', 'results', 'are', 'given', 'as', 'correction', 'tables', 'that', 'list', 'the', 'fluxes', 'in', 'mjy', 'of', 'all', 'conta... | [-0.0635101166812496, 0.03510122885927558, -0.031494123375632316, 0.10179990047139204, -0.07540465976135471, -0.10241682668670248, 0.06743009519986172, 0.48611210853370845, -0.12506264468463948, -0.416731761306779, 0.11548646587719763, -0.2941279997412338, -0.04832902247420488, 0.25030840169160795, -0.0875725516030549,... |
709.2534 | Properties of the angular gap in a one dimensional photonic band gap
structure containing single negative materials | The linear properties of the angular gap in a one dimensional photonic band
gap structure containing single negative material layers are investigated. This
gap forms at oblique incidence due to total internal reflection into air when
the Snell's law breaks down and its lower edge occurs at the frequency where
the ref... | cond-mat.other | the linear properties of the angular gap in a one dimensional photonic band gap structure containing single negative material layers are investigated this gap forms at oblique incidence due to total internal reflection into air when the snells law breaks down and its lower edge occurs at the frequency where the refract... | [['the', 'linear', 'properties', 'of', 'the', 'angular', 'gap', 'in', 'a', 'one', 'dimensional', 'photonic', 'band', 'gap', 'structure', 'containing', 'single', 'negative', 'material', 'layers', 'are', 'investigated', 'this', 'gap', 'forms', 'at', 'oblique', 'incidence', 'due', 'to', 'total', 'internal', 'reflection', ... | [-0.15975481080315676, 0.20579311314448265, -0.03710453449973777, 0.01738150843659476, -0.08151943153972106, -0.1333721420998054, 0.04487998152880238, 0.4294014895755437, -0.33628986884028683, -0.3470985763255627, 0.07464930781204585, -0.2551396956682325, -0.10505236418084091, 0.16541922226690897, 0.01165379108785982, ... |
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