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710.4253 | There are non homotopic framed homotopies of long knots | Let $\mathcal {M}$ be the space of all, including singular, long knots in
3-space and for which a fixed projection into the plane is an immersion. Let
$cl(\Sigma^{(1)}_{iness})$ be the closure of the union of all singular knots in
$\mathcal {M}$ with exactly one ordinary double point and such that the two
resolutions... | math.GT | let mathcal m be the space of all including singular long knots in 3space and for which a fixed projection into the plane is an immersion let clsigma1_iness be the closure of the union of all singular knots in mathcal m with exactly one ordinary double point and such that the two resolutions represent the same non sing... | [['let', 'mathcal', 'm', 'be', 'the', 'space', 'of', 'all', 'including', 'singular', 'long', 'knots', 'in', '3space', 'and', 'for', 'which', 'a', 'fixed', 'projection', 'into', 'the', 'plane', 'is', 'an', 'immersion', 'let', 'clsigma1_iness', 'be', 'the', 'closure', 'of', 'the', 'union', 'of', 'all', 'singular', 'knots... | [-0.2344755313652974, 0.11642243008573865, -0.0679193493103821, 0.033551110229736204, -0.08636713158745543, -0.16284930555074906, -0.024638326644066146, 0.3174218319062669, -0.299420470559357, -0.21470325482359168, 0.06785330670454458, -0.24941114339846243, -0.1375083992056136, 0.17589394969321887, -0.12336400661448754... |
710.4254 | Study of the Dynamics of Large Reflector Antennas with Accelerometers | The Atacama Large Millimeter Array (ALMA) will consist of up to 64
state-of-the-art sub-mm telescopes, subject to stringent performance
specifications which will push the boundaries of the technology, and makes
testing of antenna performance a likewise challenging task. Two antenna
prototypes were evaluated at the AL... | astro-ph | the atacama large millimeter array alma will consist of up to 64 stateoftheart submm telescopes subject to stringent performance specifications which will push the boundaries of the technology and makes testing of antenna performance a likewise challenging task two antenna prototypes were evaluated at the alma test fac... | [['the', 'atacama', 'large', 'millimeter', 'array', 'alma', 'will', 'consist', 'of', 'up', 'to', '64', 'stateoftheart', 'submm', 'telescopes', 'subject', 'to', 'stringent', 'performance', 'specifications', 'which', 'will', 'push', 'the', 'boundaries', 'of', 'the', 'technology', 'and', 'makes', 'testing', 'of', 'antenna... | [-0.19078948203757218, 0.08724359106325877, 0.0061935727054229645, -0.003260379649044451, -0.07751191302078858, -0.14043154248516843, 0.0004487992949559813, 0.389328485484459, -0.20663573703716828, -0.3530582038662102, 0.14710678203072683, -0.2558512336565653, -0.11303810934430059, 0.2337499845513626, -0.06301807210768... |
710.4255 | Analysis of a Mixed Strategy for Multiple Relay Networks | In their landmark paper Cover and El Gamal proposed different coding
strategies for the relay channel with a single relay supporting a communication
pair. These strategies are the decode-and-forward and compress-and-forward
approach, as well as a general lower bound on the capacity of a relay network
which relies on ... | cs.IT math.IT | in their landmark paper cover and el gamal proposed different coding strategies for the relay channel with a single relay supporting a communication pair these strategies are the decodeandforward and compressandforward approach as well as a general lower bound on the capacity of a relay network which relies on the mixe... | [['in', 'their', 'landmark', 'paper', 'cover', 'and', 'el', 'gamal', 'proposed', 'different', 'coding', 'strategies', 'for', 'the', 'relay', 'channel', 'with', 'a', 'single', 'relay', 'supporting', 'a', 'communication', 'pair', 'these', 'strategies', 'are', 'the', 'decodeandforward', 'and', 'compressandforward', 'appro... | [-0.2183158288764603, 0.003766790698008502, -0.06651013703085482, -0.006805222093209843, -0.0609211992513498, -0.35784852385575716, 0.17133338129805292, 0.4047867365756675, -0.28387553885798245, -0.2304717293173513, 0.08654277109992964, -0.2364867854740142, -0.16598047900342328, 0.11389576208722942, -0.0811361038893023... |
710.4256 | (1+1)-dimensional separation of variables | In this paper we explore general conditions which guarantee that the geodesic
flow on a 2-dimensional manifold with indefinite signature is locally
separable. This is equivalent to showing that a 2-dimensional natural
Hamiltonian system on the hyperbolic plane possesses a second integral of
motion which is a quadrati... | nlin.SI math-ph math.MP | in this paper we explore general conditions which guarantee that the geodesic flow on a 2dimensional manifold with indefinite signature is locally separable this is equivalent to showing that a 2dimensional natural hamiltonian system on the hyperbolic plane possesses a second integral of motion which is a quadratic pol... | [['in', 'this', 'paper', 'we', 'explore', 'general', 'conditions', 'which', 'guarantee', 'that', 'the', 'geodesic', 'flow', 'on', 'a', '2dimensional', 'manifold', 'with', 'indefinite', 'signature', 'is', 'locally', 'separable', 'this', 'is', 'equivalent', 'to', 'showing', 'that', 'a', '2dimensional', 'natural', 'hamilt... | [-0.21082562324360454, 0.10322346049130406, -0.059816133000399216, 0.06729887927810911, -0.1009606515174953, -0.13586022795897235, -0.07259649637392676, 0.3280325969127883, -0.27892876806609, -0.21674023308021265, 0.10083960420996675, -0.24987794536553176, -0.16282136645629117, 0.13262003147628823, -0.02717745148733553... |
710.4257 | Pairing mean-field theory for the dynamics of dissociation of molecular
Bose-Einstein condensates | We develop a pairing mean-field theory to describe the quantum dynamics of
the dissociation of molecular Bose-Einstein condensates into their constituent
bosonic or fermionic atoms. We apply the theory to one, two, and
three-dimensional geometries and analyze the role of dimensionality on the atom
production rate as ... | cond-mat.other cond-mat.stat-mech | we develop a pairing meanfield theory to describe the quantum dynamics of the dissociation of molecular boseeinstein condensates into their constituent bosonic or fermionic atoms we apply the theory to one two and threedimensional geometries and analyze the role of dimensionality on the atom production rate as a functi... | [['we', 'develop', 'a', 'pairing', 'meanfield', 'theory', 'to', 'describe', 'the', 'quantum', 'dynamics', 'of', 'the', 'dissociation', 'of', 'molecular', 'boseeinstein', 'condensates', 'into', 'their', 'constituent', 'bosonic', 'or', 'fermionic', 'atoms', 'we', 'apply', 'the', 'theory', 'to', 'one', 'two', 'and', 'thre... | [-0.10531636387663516, 0.17277376147339474, -0.05890131375525851, 0.10878338212512333, 0.039658111233163526, -0.10050813156507306, 0.05281210192164557, 0.3425922474647696, -0.19062611182107012, -0.2576298933602064, 0.0007614018408128539, -0.2903003949420275, -0.09583816981679331, 0.14619918576366192, 0.0602941027968316... |
710.4258 | The Double Chooz reactor neutrino experiment | The Double Chooz reactor neutrino experiment will be the next detector to
search for a non vanishing theta13 mixing angle with unprecedented sensitivity,
which might open the way to unveiling CP violation in the leptonic sector. The
measurement of this angle will be based in a precise comparison of the
antineutrino s... | hep-ex | the double chooz reactor neutrino experiment will be the next detector to search for a non vanishing theta13 mixing angle with unprecedented sensitivity which might open the way to unveiling cp violation in the leptonic sector the measurement of this angle will be based in a precise comparison of the antineutrino spect... | [['the', 'double', 'chooz', 'reactor', 'neutrino', 'experiment', 'will', 'be', 'the', 'next', 'detector', 'to', 'search', 'for', 'a', 'non', 'vanishing', 'theta13', 'mixing', 'angle', 'with', 'unprecedented', 'sensitivity', 'which', 'might', 'open', 'the', 'way', 'to', 'unveiling', 'cp', 'violation', 'in', 'the', 'lept... | [-0.08278908516513184, 0.211803606335338, -0.033018840942531824, 0.08869754426130974, -0.033403209637145735, -0.15722851409904054, 0.10210928937571274, 0.29734768775115544, -0.2233812833374769, -0.36185310204588883, 0.11750858970697516, -0.3682718601556042, -0.0019078863410253984, 0.20548837476667972, -0.00160230139295... |
710.4259 | Ergodicity of Langevin Processes with Degenerate Diffusion in Momentums | This paper introduces a geometric method for proving ergodicity of degenerate
noise driven stochastic processes. The driving noise is assumed to be an
arbitrary Levy process with non-degenerate diffusion component (but that may be
applied to a single degree of freedom of the system). The geometric conditions
are the ... | math.PR | this paper introduces a geometric method for proving ergodicity of degenerate noise driven stochastic processes the driving noise is assumed to be an arbitrary levy process with nondegenerate diffusion component but that may be applied to a single degree of freedom of the system the geometric conditions are the approxi... | [['this', 'paper', 'introduces', 'a', 'geometric', 'method', 'for', 'proving', 'ergodicity', 'of', 'degenerate', 'noise', 'driven', 'stochastic', 'processes', 'the', 'driving', 'noise', 'is', 'assumed', 'to', 'be', 'an', 'arbitrary', 'levy', 'process', 'with', 'nondegenerate', 'diffusion', 'component', 'but', 'that', '... | [-0.15994330849465485, 0.13208337825095917, -0.12024457469014517, 0.02528858456758529, -0.04040577419016325, -0.1388270689821835, 0.024557587569282252, 0.33638303145660575, -0.3404177455429701, -0.20786779579138448, 0.12283616184326325, -0.22214013671647784, -0.1679545173897071, 0.16672903549005377, -0.0996890652104089... |
710.426 | Carter's constant revealed | A new formulation of Carter's constant for geodesic motion in Kerr black
holes is given. It is shown that Carter's constant corresponds to the total
angular momentum plus a precisely defined part which is quadratic in the linear
momenta. The characterization is exact in the weak field limit obtained by
letting the gr... | gr-qc astro-ph | a new formulation of carters constant for geodesic motion in kerr black holes is given it is shown that carters constant corresponds to the total angular momentum plus a precisely defined part which is quadratic in the linear momenta the characterization is exact in the weak field limit obtained by letting the gravitat... | [['a', 'new', 'formulation', 'of', 'carters', 'constant', 'for', 'geodesic', 'motion', 'in', 'kerr', 'black', 'holes', 'is', 'given', 'it', 'is', 'shown', 'that', 'carters', 'constant', 'corresponds', 'to', 'the', 'total', 'angular', 'momentum', 'plus', 'a', 'precisely', 'defined', 'part', 'which', 'is', 'quadratic', '... | [-0.1841635688541861, 0.14221340548022685, -0.061600958524518704, 0.09121935145441352, -0.1261030258723052, -0.09612699970602989, -0.023749329149723053, 0.2769423724791731, -0.22898464658892298, -0.2754937783669097, 0.05702368372557572, -0.25494846145072614, -0.09698620537879417, 0.22494172744722252, -0.044787820277129... |
710.4261 | Survivable MPLS Over Optical Transport Networks: Cost and Resource Usage
Analysis | In this paper we study different options for the survivability implementation
in MPLS over Optical Transport Networks (OTN) in terms of network resource
usage and configuration cost. We investigate two approaches to the
survivability deployment: single layer and multilayer survivability and present
various methods fo... | cs.NI cs.PF | in this paper we study different options for the survivability implementation in mpls over optical transport networks otn in terms of network resource usage and configuration cost we investigate two approaches to the survivability deployment single layer and multilayer survivability and present various methods for spar... | [['in', 'this', 'paper', 'we', 'study', 'different', 'options', 'for', 'the', 'survivability', 'implementation', 'in', 'mpls', 'over', 'optical', 'transport', 'networks', 'otn', 'in', 'terms', 'of', 'network', 'resource', 'usage', 'and', 'configuration', 'cost', 'we', 'investigate', 'two', 'approaches', 'to', 'the', 's... | [-0.1537296949771957, 0.017676265090703965, 0.012784626152780322, 0.005818444378415329, -0.03986813712451193, -0.14654566003216637, 0.14528098905614267, 0.43985213017505076, -0.2924250663092567, -0.33681093767285347, 0.1201314306202241, -0.26531497560855416, -0.11869456117972732, 0.17923712085829013, -0.082378055407769... |
710.4262 | Crowded-Field Astrometry with the Space Interferometry Mission - I.
Estimating the Single-Measurement Astrometric Bias Arising from Confusion | The accuracy of position measurements on stellar targets with the future
Space Interferometry Mission (SIM) will be limited not only by photon noise and
by the properties of the instrument (design, stability, etc.) and the overall
measurement program (observing strategy, reduction methods, etc.), but also by
the pres... | astro-ph | the accuracy of position measurements on stellar targets with the future space interferometry mission sim will be limited not only by photon noise and by the properties of the instrument design stability etc and the overall measurement program observing strategy reduction methods etc but also by the presence of other c... | [['the', 'accuracy', 'of', 'position', 'measurements', 'on', 'stellar', 'targets', 'with', 'the', 'future', 'space', 'interferometry', 'mission', 'sim', 'will', 'be', 'limited', 'not', 'only', 'by', 'photon', 'noise', 'and', 'by', 'the', 'properties', 'of', 'the', 'instrument', 'design', 'stability', 'etc', 'and', 'the... | [-0.09592620152690058, 0.07373584443020512, -0.07387198427060432, 0.07910752480939856, -0.08713303906134101, -0.10780622307404515, 0.06817978212310188, 0.39323939506776606, -0.21913264038896826, -0.37251090370666456, 0.11906954614771047, -0.2537514299321855, -0.10324078921235093, 0.21498331353213368, -0.100532852125331... |
710.4263 | Silicon in the Quantum Limit: Quantum Computing and Decoherence in
Silicon Architectures | Semiconductor architectures hold promise for quantum information processing
(QIP) applications due to their large industrial base and perceived scalability
potential. Electron spins in silicon in particular may be an excellent
architecture for QIP and also for spin electronics (spintronics) applications.
While the ch... | cond-mat.mtrl-sci cond-mat.mes-hall | semiconductor architectures hold promise for quantum information processing qip applications due to their large industrial base and perceived scalability potential electron spins in silicon in particular may be an excellent architecture for qip and also for spin electronics spintronics applications while the charge of ... | [['semiconductor', 'architectures', 'hold', 'promise', 'for', 'quantum', 'information', 'processing', 'qip', 'applications', 'due', 'to', 'their', 'large', 'industrial', 'base', 'and', 'perceived', 'scalability', 'potential', 'electron', 'spins', 'in', 'silicon', 'in', 'particular', 'may', 'be', 'an', 'excellent', 'arc... | [-0.12167861808576795, 0.1711807419020353, -0.0090987777408465, 0.029954309987646165, -0.01293982652714476, -0.2331358471557782, 0.017695246533672247, 0.4178161884310766, -0.25517512242293966, -0.31028411747351037, 0.04439523534985433, -0.28878442520646663, -0.12315526706071854, 0.23973545448270517, -0.0342314183234505... |
710.4264 | Diophantine approximation, Khintchine's theorem, torus geometry and
Hausdorff dimension | A general form of the Borel-Cantelli Lemma and its connection with the proof
of Khintchine's Theorem on Diophantine approximation and the more general
Khintchine-Groshev theorem are discussed. The torus geometry in the planar case
allows a relatively direct proof of the planar Groshev theorem for the set of
$\psi$-ap... | math.NT | a general form of the borelcantelli lemma and its connection with the proof of khintchines theorem on diophantine approximation and the more general khintchinegroshev theorem are discussed the torus geometry in the planar case allows a relatively direct proof of the planar groshev theorem for the set of psiapproximable... | [['a', 'general', 'form', 'of', 'the', 'borelcantelli', 'lemma', 'and', 'its', 'connection', 'with', 'the', 'proof', 'of', 'khintchines', 'theorem', 'on', 'diophantine', 'approximation', 'and', 'the', 'more', 'general', 'khintchinegroshev', 'theorem', 'are', 'discussed', 'the', 'torus', 'geometry', 'in', 'the', 'planar... | [-0.1515406922085926, 0.0456042030763066, -0.07729187014878594, 0.10162140165318435, -0.047585261786090474, -0.10284298381884582, 0.07357852441990483, 0.26547010511525776, -0.25049288171742645, -0.23251976593175122, 0.1236510136430817, -0.2603643727448538, -0.1218575382538672, 0.2551166957543631, -0.10544457215915568, ... |
710.4265 | Searches for Higgs and BSM at the Tevatron | This paper presents an overview of recent experimental direct searches for
Higgs-boson and beyond-the-standard-model (BSM) physics shown in the plenary
session at the SUSY07 conference. The results reported correspond to an
integrated luminosity of up to 2 fb-1 of Run II data from $p\bar{p}$ collisions
collected by t... | hep-ex | this paper presents an overview of recent experimental direct searches for higgsboson and beyondthestandardmodel bsm physics shown in the plenary session at the susy07 conference the results reported correspond to an integrated luminosity of up to 2 fb1 of run ii data from pbarp collisions collected by the cdf and d0 e... | [['this', 'paper', 'presents', 'an', 'overview', 'of', 'recent', 'experimental', 'direct', 'searches', 'for', 'higgsboson', 'and', 'beyondthestandardmodel', 'bsm', 'physics', 'shown', 'in', 'the', 'plenary', 'session', 'at', 'the', 'susy07', 'conference', 'the', 'results', 'reported', 'correspond', 'to', 'an', 'integra... | [-0.03379432545028109, 0.23411982393201397, -0.03368880635509822, 0.18695392582483825, -0.10437673486966566, -0.22556787451408458, -0.012360973289768006, 0.2822277886756011, -0.16437934509891744, -0.3198651210065709, 0.03420909680349025, -0.3624217141487494, 0.03312650100722761, 0.14502293134990166, 0.05872686946184825... |
710.4266 | Expansions for the Bollobas-Riordan polynomial of separable ribbon
graphs | We define 2-decompositions of ribbon graphs, which generalise 2-sums and
tensor products of graphs. We give formulae for the Bollobas-Riordan polynomial
of such a 2-decomposition, and derive the classical Brylawski formula for the
Tutte polynomial of a tensor product as a (very) special case. This study was
initially... | math.CO | we define 2decompositions of ribbon graphs which generalise 2sums and tensor products of graphs we give formulae for the bollobasriordan polynomial of such a 2decomposition and derive the classical brylawski formula for the tutte polynomial of a tensor product as a very special case this study was initially motivated f... | [['we', 'define', '2decompositions', 'of', 'ribbon', 'graphs', 'which', 'generalise', '2sums', 'and', 'tensor', 'products', 'of', 'graphs', 'we', 'give', 'formulae', 'for', 'the', 'bollobasriordan', 'polynomial', 'of', 'such', 'a', '2decomposition', 'and', 'derive', 'the', 'classical', 'brylawski', 'formula', 'for', 't... | [-0.1423928454387351, 0.06241116339469954, -0.10073567667859606, 0.09600366584163567, -0.10145939711946994, -0.12223776391329011, 0.015427805532226557, 0.3227408316161018, -0.28114798178648925, -0.2674520415166626, 0.10774301144556375, -0.19106351331356564, -0.23993100921506993, 0.19734268384127063, -0.1038020997584681... |
710.4267 | Topics on String Phenomenology | These lectures present some topics of string phenomenology and contain two
parts. In the first part, I review the possibility of lowering the string scale
in the TeV region, that provides a theoretical framework for solving the mass
hierarchy problem and unifying all interactions. The apparent weakness of
gravity can... | hep-th gr-qc hep-ph | these lectures present some topics of string phenomenology and contain two parts in the first part i review the possibility of lowering the string scale in the tev region that provides a theoretical framework for solving the mass hierarchy problem and unifying all interactions the apparent weakness of gravity can then ... | [['these', 'lectures', 'present', 'some', 'topics', 'of', 'string', 'phenomenology', 'and', 'contain', 'two', 'parts', 'in', 'the', 'first', 'part', 'i', 'review', 'the', 'possibility', 'of', 'lowering', 'the', 'string', 'scale', 'in', 'the', 'tev', 'region', 'that', 'provides', 'a', 'theoretical', 'framework', 'for', ... | [-0.09402428297433636, 0.19439375184821583, -0.0725898004175336, 0.13496866424075418, -0.09606531887002978, -0.15449680690653622, -0.022258660328746745, 0.3076258014222725, -0.20891065416437699, -0.32836799129622996, 0.07917358266321586, -0.23251401776221792, -0.090327001989663, 0.12112715504484822, -0.0157383312602430... |
710.4268 | Finite Field Experiments (with an Appendix by Stefan Wiedmann) | We explain how to use computer experiments over finite fields to gain
heuristic information about the solution set of polynomial equations in
characteristic zero. These are notes of a tutorial I gave at the NATO Advanced
Study Institute on Higher-Dimensional Geometry over Finite Fields in G"ottingen
2007.
| math.AG | we explain how to use computer experiments over finite fields to gain heuristic information about the solution set of polynomial equations in characteristic zero these are notes of a tutorial i gave at the nato advanced study institute on higherdimensional geometry over finite fields in gottingen 2007 | [['we', 'explain', 'how', 'to', 'use', 'computer', 'experiments', 'over', 'finite', 'fields', 'to', 'gain', 'heuristic', 'information', 'about', 'the', 'solution', 'set', 'of', 'polynomial', 'equations', 'in', 'characteristic', 'zero', 'these', 'are', 'notes', 'of', 'a', 'tutorial', 'i', 'gave', 'at', 'the', 'nato', 'a... | [-0.08453653422877827, 0.07452221841432471, -0.14136647774857727, 0.05115053844340938, -0.14648540211009217, -0.12300892615135997, -0.02838758866679161, 0.31834758584328154, -0.23448468146330498, -0.30439680258921803, 0.13787992714230526, -0.26681303412237384, -0.16026038042408355, 0.24593713823111452, -0.0973820104759... |
710.4269 | Shape, size and robustness: feasible regions in the parameter space of
biochemical networks | The concept of robustness of regulatory networks has been closely related to
the nature of the interactions among genes, and the capability of pattern
maintenance or reproducibility. Defining this robustness property is a
challenging task, but mathematical models have often associated it to the
volume of the space of... | q-bio.MN | the concept of robustness of regulatory networks has been closely related to the nature of the interactions among genes and the capability of pattern maintenance or reproducibility defining this robustness property is a challenging task but mathematical models have often associated it to the volume of the space of admi... | [['the', 'concept', 'of', 'robustness', 'of', 'regulatory', 'networks', 'has', 'been', 'closely', 'related', 'to', 'the', 'nature', 'of', 'the', 'interactions', 'among', 'genes', 'and', 'the', 'capability', 'of', 'pattern', 'maintenance', 'or', 'reproducibility', 'defining', 'this', 'robustness', 'property', 'is', 'a',... | [-0.12219140459083255, 0.05458578782351899, -0.04350256149026555, 0.07980711813576494, -0.0918737667241505, -0.09895023859555384, 0.06165532265965651, 0.3768745853884758, -0.2878844554021538, -0.3063705487346107, 0.11721899758672694, -0.21292113421901643, -0.22291699123171554, 0.19711797443785137, -0.07793394937603311,... |
710.427 | Spin-c Prequantization and Symplectic Cutting | We define spin-c prequantization of a symplectic manifold to be a spin-c
structure and a connection which are compatible with the symplectic form. We
describe the cutting of an S^1-equivariant spin-c prequantization. The cutting
process involves a choice of a spin-c prequantization for the complex plane. We
prove tha... | math.DG math.SG | we define spinc prequantization of a symplectic manifold to be a spinc structure and a connection which are compatible with the symplectic form we describe the cutting of an s1equivariant spinc prequantization the cutting process involves a choice of a spinc prequantization for the complex plane we prove that the cutti... | [['we', 'define', 'spinc', 'prequantization', 'of', 'a', 'symplectic', 'manifold', 'to', 'be', 'a', 'spinc', 'structure', 'and', 'a', 'connection', 'which', 'are', 'compatible', 'with', 'the', 'symplectic', 'form', 'we', 'describe', 'the', 'cutting', 'of', 'an', 's1equivariant', 'spinc', 'prequantization', 'the', 'cutt... | [-0.21200724017538436, 0.05734315967009473, -0.0913635506358457, 0.07721568011987834, -0.17463295355643313, -0.12224395779178363, 0.030727040945163174, 0.4091671651152715, -0.3178022639085985, -0.21716459871154942, 0.0907493212247548, -0.2099432672743928, -0.18373116146620005, 0.15310933160251133, -0.12813094990608626,... |
710.4271 | Asymptotics of the quantum Hamming bound for subsystem codes | Ashikhmin and Litsyn showed that all binary stabilizer codes - pure or impure
- of sufficiently large length obey the quantum Hamming bound, ruling out the
possibility that impure codes of large length can outperform pure codes with
respect to sphere packing. In contrast we show that impure subsystem codes do
not obe... | quant-ph | ashikhmin and litsyn showed that all binary stabilizer codes pure or impure of sufficiently large length obey the quantum hamming bound ruling out the possibility that impure codes of large length can outperform pure codes with respect to sphere packing in contrast we show that impure subsystem codes do not obey the qu... | [['ashikhmin', 'and', 'litsyn', 'showed', 'that', 'all', 'binary', 'stabilizer', 'codes', 'pure', 'or', 'impure', 'of', 'sufficiently', 'large', 'length', 'obey', 'the', 'quantum', 'hamming', 'bound', 'ruling', 'out', 'the', 'possibility', 'that', 'impure', 'codes', 'of', 'large', 'length', 'can', 'outperform', 'pure',... | [-0.17582592666874847, 0.22969220374263338, -0.06826367327798304, 0.136526978363029, 0.04830253381257901, -0.3402992341086849, 0.04622901364398951, 0.3501755485867525, -0.2651062398399045, -0.23976661687998052, 0.0711652056129601, -0.28419495209470974, -0.12862266386351126, 0.19182516698417096, -0.07311062433215633, 0.... |
710.4272 | An approximation trichotomy for Boolean #CSP | We give a trichotomy theorem for the complexity of approximately counting the
number of satisfying assignments of a Boolean CSP instance. Such problems are
parameterised by a constraint language specifying the relations that may be
used in constraints. If every relation in the constraint language is affine
then the n... | cs.CC | we give a trichotomy theorem for the complexity of approximately counting the number of satisfying assignments of a boolean csp instance such problems are parameterised by a constraint language specifying the relations that may be used in constraints if every relation in the constraint language is affine then the numbe... | [['we', 'give', 'a', 'trichotomy', 'theorem', 'for', 'the', 'complexity', 'of', 'approximately', 'counting', 'the', 'number', 'of', 'satisfying', 'assignments', 'of', 'a', 'boolean', 'csp', 'instance', 'such', 'problems', 'are', 'parameterised', 'by', 'a', 'constraint', 'language', 'specifying', 'the', 'relations', 'th... | [-0.13025222144125406, 0.06794523134692965, -0.0469643646985831, 0.09545750567669901, -0.11743951569934073, -0.16928818141648838, 0.08513821038720479, 0.3239139994404402, -0.324532058796879, -0.3690761281100259, 0.08688258267069482, -0.2689630847076425, -0.08574396697243294, 0.19792759873489119, -0.09711512786908502, 0... |
710.4273 | Supergravity and Two-Field Inflation Effects in Right-Handed
Sneutrino-Modified D-term Inflation | We extend previous work on the minimal D-term inflation model modified by
Right-Handed (RH) sneutrino fields to include additional inflaton-sector SUGRA
corrections and two-field inflation effects. We show that SUGRA corrections
simultaneously allow n_{s} to be within 3-year WMAP limits and the cosmic
string contribu... | hep-ph astro-ph hep-th | we extend previous work on the minimal dterm inflation model modified by righthanded rh sneutrino fields to include additional inflatonsector sugra corrections and twofield inflation effects we show that sugra corrections simultaneously allow n_s to be within 3year wmap limits and the cosmic string contribution to the ... | [['we', 'extend', 'previous', 'work', 'on', 'the', 'minimal', 'dterm', 'inflation', 'model', 'modified', 'by', 'righthanded', 'rh', 'sneutrino', 'fields', 'to', 'include', 'additional', 'inflatonsector', 'sugra', 'corrections', 'and', 'twofield', 'inflation', 'effects', 'we', 'show', 'that', 'sugra', 'corrections', 'si... | [-0.08100789042983529, 0.2644020347080925, -0.0021471417471516452, 0.16161364404368997, -0.0877582707798621, -0.1935357880909871, -0.027563008102205515, 0.3225317956198432, -0.2130432160549341, -0.3657657250874495, 0.04163461330428019, -0.3332255104769196, -0.021110734289774558, 0.1808245132252224, -0.00582567521920990... |
710.4274 | Large-scale Propagation of Very Light Jets in Galaxy Clusters | We performed MHD simulations of very light bipolar jets with density
contrasts down to 10^-4 in axisymmetry, which were injected into a medium of
constant density and evolved up to 200 kpc (200 r_j) full length. These jets
show weak and roundish bow shocks as well as broad cocoons and thermalize their
kinetic energy ... | astro-ph | we performed mhd simulations of very light bipolar jets with density contrasts down to 104 in axisymmetry which were injected into a medium of constant density and evolved up to 200 kpc 200 r_j full length these jets show weak and roundish bow shocks as well as broad cocoons and thermalize their kinetic energy very eff... | [['we', 'performed', 'mhd', 'simulations', 'of', 'very', 'light', 'bipolar', 'jets', 'with', 'density', 'contrasts', 'down', 'to', '104', 'in', 'axisymmetry', 'which', 'were', 'injected', 'into', 'a', 'medium', 'of', 'constant', 'density', 'and', 'evolved', 'up', 'to', '200', 'kpc', '200', 'r_j', 'full', 'length', 'the... | [-0.10997099859420867, 0.18384119178004124, -0.0455273234764602, 0.16786311182430855, -0.09859014669542804, -0.08335103186796985, -0.01141236110033431, 0.44959764845450134, -0.2540977090944116, -0.3512048450225562, 0.07606696686593305, -0.2338980636102896, 0.011282395133200814, 0.16737307771565577, 0.04070204182861227,... |
710.4275 | Cosmological Unparticle Correlators | We introduce and study an extension of the correlator of unparticle matter
operators in a cosmological environment. Starting from FRW spaces we specialize
to a de Sitter spacetime and derive its inflationary power spectrum which we
find to be almost flat. We finally investigate some consequences of requiring
the exis... | hep-th gr-qc hep-ph | we introduce and study an extension of the correlator of unparticle matter operators in a cosmological environment starting from frw spaces we specialize to a de sitter spacetime and derive its inflationary power spectrum which we find to be almost flat we finally investigate some consequences of requiring the existenc... | [['we', 'introduce', 'and', 'study', 'an', 'extension', 'of', 'the', 'correlator', 'of', 'unparticle', 'matter', 'operators', 'in', 'a', 'cosmological', 'environment', 'starting', 'from', 'frw', 'spaces', 'we', 'specialize', 'to', 'a', 'de', 'sitter', 'spacetime', 'and', 'derive', 'its', 'inflationary', 'power', 'spect... | [-0.16724488237377955, 0.09886659204698844, -0.1825985281757312, 0.11462077949363447, -0.09926105584963807, -0.11130719840002712, -0.049242459530432825, 0.3302042813738808, -0.20106234293416492, -0.21476749267276318, 0.08972519725284656, -0.21804735848127166, -0.17002453256282024, 0.11480011831736192, -0.04813523474149... |
710.4276 | On the Euclidean Version of the Photon Number Integral | We reconsider the Euclidean version of the photon number integral introduced
in ref 1. This integral is well defined for any smooth non-self-intersecting
curve in $\R^N$. Besides studying general features of this integral (including
it s conformal invariance), we evaluate it explicitly for the ellipse. The
result is ... | math-ph math.MP | we reconsider the euclidean version of the photon number integral introduced in ref 1 this integral is well defined for any smooth nonselfintersecting curve in rn besides studying general features of this integral including it s conformal invariance we evaluate it explicitly for the ellipse the result is n_ellipsexi1xi... | [['we', 'reconsider', 'the', 'euclidean', 'version', 'of', 'the', 'photon', 'number', 'integral', 'introduced', 'in', 'ref', '1', 'this', 'integral', 'is', 'well', 'defined', 'for', 'any', 'smooth', 'nonselfintersecting', 'curve', 'in', 'rn', 'besides', 'studying', 'general', 'features', 'of', 'this', 'integral', 'incl... | [-0.16848282936180747, 0.07063566117958966, -0.06353519253735972, 0.039995047248910766, -0.043897332098378344, -0.10743553771875626, -0.020271230521503578, 0.3385883163915254, -0.232164315359537, -0.27528777627577616, 0.1026718953399659, -0.2745591950640732, -0.1503583556988688, 0.1985269742422239, -0.08689747941355373... |
710.4277 | Inelastic Scattering and Spin Polarization in Dilute Magnetic
Semiconductor (Ga,Mn)Sb | The Point Contact Andreev Reflection (PCAR) technique has already been used
to measure the spin polarization of some of the dilute magnetic semiconductors,
such as narrow-band (In,Mn)Sb, as well as wider gap (Ga,Mn)As. While in
(In,Mn)Sb conventional Andreev reflection has been demonstrated, in (Ga,Mn)As
quasiparticl... | cond-mat.supr-con cond-mat.mtrl-sci | the point contact andreev reflection pcar technique has already been used to measure the spin polarization of some of the dilute magnetic semiconductors such as narrowband inmnsb as well as wider gap gamnas while in inmnsb conventional andreev reflection has been demonstrated in gamnas quasiparticle density of states d... | [['the', 'point', 'contact', 'andreev', 'reflection', 'pcar', 'technique', 'has', 'already', 'been', 'used', 'to', 'measure', 'the', 'spin', 'polarization', 'of', 'some', 'of', 'the', 'dilute', 'magnetic', 'semiconductors', 'such', 'as', 'narrowband', 'inmnsb', 'as', 'well', 'as', 'wider', 'gap', 'gamnas', 'while', 'in... | [-0.13194895568253692, 0.18245222159255778, -0.09108322159817783, 0.018183933240511724, -0.049039952957662204, -0.12321155468222275, 0.03898215433081952, 0.45874937487545836, -0.2454724448923302, -0.3412258951431541, -0.01488418327719574, -0.3295171289474413, -0.05760057969519528, 0.2020113565258041, 0.0499898816248582... |
710.4278 | Shape reconstruction from gradient data | We present a novel method for reconstructing the shape of an object from
measured gradient data. A certain class of optical sensors does not measure the
shape of an object, but its local slope. These sensors display several
advantages, including high information efficiency, sensitivity, and robustness.
For many appli... | physics.optics | we present a novel method for reconstructing the shape of an object from measured gradient data a certain class of optical sensors does not measure the shape of an object but its local slope these sensors display several advantages including high information efficiency sensitivity and robustness for many applications h... | [['we', 'present', 'a', 'novel', 'method', 'for', 'reconstructing', 'the', 'shape', 'of', 'an', 'object', 'from', 'measured', 'gradient', 'data', 'a', 'certain', 'class', 'of', 'optical', 'sensors', 'does', 'not', 'measure', 'the', 'shape', 'of', 'an', 'object', 'but', 'its', 'local', 'slope', 'these', 'sensors', 'disp... | [-0.04013800609076547, 0.02334027790054385, -0.11577532495799903, 0.047488120376124036, -0.08500555855943612, -0.14138001754779267, -0.0018797730397735093, 0.4635446008865361, -0.29441544474448655, -0.33715643035667436, 0.15549794135317374, -0.2533487181288299, -0.15747994192884313, 0.26199975973079065, -0.116440664017... |
710.4279 | The SuperNEMO double beta decay experiment | The SuperNEMO project studies the feasibility of employing a technique of
tracking plus calorimetry to search for neutrinoless double beta decay in 100
kg of enriched isotopes. It aims to reach an effective neutrino mass
sensitivity of 50 meV. The current status of the SuperNEMO R&D programme is
described, focusing o... | physics.ins-det hep-ex | the supernemo project studies the feasibility of employing a technique of tracking plus calorimetry to search for neutrinoless double beta decay in 100 kg of enriched isotopes it aims to reach an effective neutrino mass sensitivity of 50 mev the current status of the supernemo rd programme is described focusing on the ... | [['the', 'supernemo', 'project', 'studies', 'the', 'feasibility', 'of', 'employing', 'a', 'technique', 'of', 'tracking', 'plus', 'calorimetry', 'to', 'search', 'for', 'neutrinoless', 'double', 'beta', 'decay', 'in', '100', 'kg', 'of', 'enriched', 'isotopes', 'it', 'aims', 'to', 'reach', 'an', 'effective', 'neutrino', '... | [-0.0362361960911325, 0.1692213992129317, 0.008176394921195294, 0.06064495706440149, 0.009342713125079172, -0.1033693240606226, 0.08139069897255727, 0.28907598009599106, -0.17235981237276324, -0.3521227678616664, 0.08133698172709306, -0.3169219695763396, 0.01649885667783175, 0.2383339402357316, 0.04456397653224745, 0.0... |
710.428 | Gamma Ray Bursts from the early Universe: predictions for present-day
and future instruments | Long Gamma Ray Bursts (GRBs) constitute an important tool to study the
Universe near and beyond the epoch of reionization. We delineate here the
characteristics of an 'ideal' instrument for the search of GRBs at z>6-10. We
find that the detection of these objects requires soft band detectors with a
high sensitivity a... | astro-ph | long gamma ray bursts grbs constitute an important tool to study the universe near and beyond the epoch of reionization we delineate here the characteristics of an ideal instrument for the search of grbs at z610 we find that the detection of these objects requires soft band detectors with a high sensitivity and moderat... | [['long', 'gamma', 'ray', 'bursts', 'grbs', 'constitute', 'an', 'important', 'tool', 'to', 'study', 'the', 'universe', 'near', 'and', 'beyond', 'the', 'epoch', 'of', 'reionization', 'we', 'delineate', 'here', 'the', 'characteristics', 'of', 'an', 'ideal', 'instrument', 'for', 'the', 'search', 'of', 'grbs', 'at', 'z610'... | [-0.06376270995398609, 0.16545643721328002, -0.03663537759000862, 0.1436865432298477, -0.10003806838073752, -0.10621856156653366, 0.06828893474745434, 0.4486919161993698, -0.17869875955463038, -0.3578676578703248, 0.08647008932536394, -0.33226808070532937, -0.03884539727444172, 0.26461313491005595, -0.00499665037099292... |
710.4281 | Tan(beta) enhanced Yukawa couplings for supersymmetric Higgs singlets at
one loop | Extensions of the MSSM generically feature gauge singlet Higgs bosons. These
singlet Higgs bosons have tan(beta)-enhanced Yukawa couplings to down-type
quarks and leptons at the one-loop level. We present an effective Lagrangian
incorporating these Yukawa couplings and use it to study their effect on
singlet Higgs bo... | hep-ph | extensions of the mssm generically feature gauge singlet higgs bosons these singlet higgs bosons have tanbetaenhanced yukawa couplings to downtype quarks and leptons at the oneloop level we present an effective lagrangian incorporating these yukawa couplings and use it to study their effect on singlet higgs boson pheno... | [['extensions', 'of', 'the', 'mssm', 'generically', 'feature', 'gauge', 'singlet', 'higgs', 'bosons', 'these', 'singlet', 'higgs', 'bosons', 'have', 'tanbetaenhanced', 'yukawa', 'couplings', 'to', 'downtype', 'quarks', 'and', 'leptons', 'at', 'the', 'oneloop', 'level', 'we', 'present', 'an', 'effective', 'lagrangian', ... | [-0.10198725716222122, 0.3555692643048494, -0.00671160786064813, 0.23506826454779156, -0.11200536886252553, -0.22463107685255537, 0.01122678152891437, 0.34484159986836366, -0.18370781953906618, -0.2461583588878254, -0.07292056251990509, -0.2915061166094818, -0.0462981129839388, 0.03671857049262308, 0.12165452902070639,... |
710.4282 | Broad Lyman-Alpha Emission from Supernova Remnants in Young Galaxies | Charge transfer (or exchange) reactions between hydrogen atoms and protons in
collisionless shocks of supernova remnants (SNRs) are a natural way of
producing broad Balmer, Lyman and other lines of hydrogen. We wish to quantify
the importance of shock-induced, non-thermal hydrogen emission from SNRs in
young galaxies... | astro-ph | charge transfer or exchange reactions between hydrogen atoms and protons in collisionless shocks of supernova remnants snrs are a natural way of producing broad balmer lyman and other lines of hydrogen we wish to quantify the importance of shockinduced nonthermal hydrogen emission from snrs in young galaxies we present... | [['charge', 'transfer', 'or', 'exchange', 'reactions', 'between', 'hydrogen', 'atoms', 'and', 'protons', 'in', 'collisionless', 'shocks', 'of', 'supernova', 'remnants', 'snrs', 'are', 'a', 'natural', 'way', 'of', 'producing', 'broad', 'balmer', 'lyman', 'and', 'other', 'lines', 'of', 'hydrogen', 'we', 'wish', 'to', 'qu... | [0.021119543750835367, 0.13415461119784172, 0.050687229769780885, 0.1552394685080968, -0.06908934220758288, -0.0970577989445003, 0.03638592573142675, 0.5021407821020761, -0.16145362218592835, -0.32575511057796175, -0.03435797686038842, -0.32826914762479775, 0.05725946637103334, 0.22078624835865962, 0.05225687027299035,... |
710.4283 | Crossing the phantom divide in an interacting generalized Chaplygin gas | Unified generalized Chaplygin gas models assuming an interaction between dark
energy and dark matter fluids have been previously proposed. Following these
ideas, we consider a particular relation between dark densities, which allows
the possibility of a time varying equation of state for dark energy that
crosses the ... | hep-th | unified generalized chaplygin gas models assuming an interaction between dark energy and dark matter fluids have been previously proposed following these ideas we consider a particular relation between dark densities which allows the possibility of a time varying equation of state for dark energy that crosses the phant... | [['unified', 'generalized', 'chaplygin', 'gas', 'models', 'assuming', 'an', 'interaction', 'between', 'dark', 'energy', 'and', 'dark', 'matter', 'fluids', 'have', 'been', 'previously', 'proposed', 'following', 'these', 'ideas', 'we', 'consider', 'a', 'particular', 'relation', 'between', 'dark', 'densities', 'which', 'a... | [-0.11452191238071385, 0.1346821918156385, -0.15152099412238307, 0.09523007126889475, -0.06381212319146194, -0.13235178074050372, -0.020455246750751267, 0.3091035433943667, -0.24950846507335486, -0.34142761562606727, 0.040022306530179616, -0.2654266715096879, -0.05014508966680454, 0.11710342305266987, 0.038856519842975... |
710.4284 | Numerical obstructions to abelian surfaces in toric Fano 4-folds | Some of the 124 toric Fano 4-folds contain abelian surfaces but most do not:
in a few cases it is not known whether they do or not. By elementary methods,
with a little computer help, we exclude some more possibilities.
| math.AG | some of the 124 toric fano 4folds contain abelian surfaces but most do not in a few cases it is not known whether they do or not by elementary methods with a little computer help we exclude some more possibilities | [['some', 'of', 'the', '124', 'toric', 'fano', '4folds', 'contain', 'abelian', 'surfaces', 'but', 'most', 'do', 'not', 'in', 'a', 'few', 'cases', 'it', 'is', 'not', 'known', 'whether', 'they', 'do', 'or', 'not', 'by', 'elementary', 'methods', 'with', 'a', 'little', 'computer', 'help', 'we', 'exclude', 'some', 'more', '... | [-0.10206224269641098, 0.10100195748964325, -0.07422654372639954, 0.19464601573126855, -0.19281195742078125, -0.282601093663834, 0.03718371232971549, 0.4474121376872063, -0.19361080709204542, -0.3178674592170864, 0.16327440035238397, -0.25910343090072274, -0.1833330375913647, 0.27259221496060493, -0.16979904621839523, ... |
710.4285 | Experimental validation and physical modelling of vocal folds
pathologies | Voiced sounds involve self-sustained vocal folds oscillations due to the
interaction between the airflow and the vocal folds. Common vocal folds
pathologies like polyps and anatomical asymmetry degrade the mechanical vocal
fold properties and consequently disturb the normal oscillation pattern
resulting in an abnorma... | physics.class-ph | voiced sounds involve selfsustained vocal folds oscillations due to the interaction between the airflow and the vocal folds common vocal folds pathologies like polyps and anatomical asymmetry degrade the mechanical vocal fold properties and consequently disturb the normal oscillation pattern resulting in an abnormal so... | [['voiced', 'sounds', 'involve', 'selfsustained', 'vocal', 'folds', 'oscillations', 'due', 'to', 'the', 'interaction', 'between', 'the', 'airflow', 'and', 'the', 'vocal', 'folds', 'common', 'vocal', 'folds', 'pathologies', 'like', 'polyps', 'and', 'anatomical', 'asymmetry', 'degrade', 'the', 'mechanical', 'vocal', 'fol... | [-0.10343725658154493, 0.09739230023934639, -0.09323844183170048, 0.06765929454365815, -0.09603158557121465, -0.14287115656770766, 0.012033425206672164, 0.3278106140515095, -0.24606734720836806, -0.30959485704668716, 0.011414339993579336, -0.2992961485663877, -0.23589964681069214, 0.21605906059782765, -0.11333465620453... |
710.4286 | A mechanical experimental setup to simulate vocal folds vibrations.
Preliminary results | This paper contributes to the understanding of vocal folds oscillation during
phonation. In order to test theoretical models of phonation, a new experimental
set-up using a deformable vocal folds replica is presented. The replica is
shown to be able to produce self sustained oscillations under controlled
experimental... | physics.class-ph | this paper contributes to the understanding of vocal folds oscillation during phonation in order to test theoretical models of phonation a new experimental setup using a deformable vocal folds replica is presented the replica is shown to be able to produce self sustained oscillations under controlled experimental condi... | [['this', 'paper', 'contributes', 'to', 'the', 'understanding', 'of', 'vocal', 'folds', 'oscillation', 'during', 'phonation', 'in', 'order', 'to', 'test', 'theoretical', 'models', 'of', 'phonation', 'a', 'new', 'experimental', 'setup', 'using', 'a', 'deformable', 'vocal', 'folds', 'replica', 'is', 'presented', 'the', '... | [-0.10287076838873327, 0.1492796790684806, -0.089574412740767, 0.050349756605923175, -0.10749477647058665, -0.12393496000766754, 0.034920552962459626, 0.3720392979979515, -0.2692993500418961, -0.3003624891638756, 0.08373818017821759, -0.23580245944485068, -0.17223310337774456, 0.21253631731495262, -0.07432949841488153,... |
710.4287 | Diffractive photoproduction of Z^0 bosons in coherent interactions at
CERN-LHC | The exclusive $Z^0$ photoproduction at high energies in $\gamma p (A)$, $p p$
and $AA$ collisions is investigate within the color dipole formalism. We
generalize the description of the deeply virtual compton scattering (DVCS)
process, which describe quite well the HERA data, for the production of $Z^0$
bosons and est... | hep-ph | the exclusive z0 photoproduction at high energies in gamma p a p p and aa collisions is investigate within the color dipole formalism we generalize the description of the deeply virtual compton scattering dvcs process which describe quite well the hera data for the production of z0 bosons and estimate the total cross s... | [['the', 'exclusive', 'z0', 'photoproduction', 'at', 'high', 'energies', 'in', 'gamma', 'p', 'a', 'p', 'p', 'and', 'aa', 'collisions', 'is', 'investigate', 'within', 'the', 'color', 'dipole', 'formalism', 'we', 'generalize', 'the', 'description', 'of', 'the', 'deeply', 'virtual', 'compton', 'scattering', 'dvcs', 'proce... | [-0.034072555355385115, 0.22008259038055508, -0.12139058055726801, 0.16922702057776218, 0.0013251666878831797, -0.10398510832743633, 0.0034577376764513895, 0.38687193679928394, -0.22374429377919897, -0.24910224982719312, -0.07908863984128653, -0.33984774143713387, 0.06904778191913455, 0.1535335100609167, 0.103387651942... |
710.4288 | Controllable switching of vortex chirality in magnetic nanodisks by a
field pulse | We propose a way of fast switching the chirality in a magnetic nanodisk by
applying a field pulse. To break the symmetry with respect to clockwise or
counterclockwise chirality a mask is added by which an inhomogeneous field
influences the vortex state of a nanodisk. Using numerical spin--lattice
simulations we demon... | cond-mat.str-el | we propose a way of fast switching the chirality in a magnetic nanodisk by applying a field pulse to break the symmetry with respect to clockwise or counterclockwise chirality a mask is added by which an inhomogeneous field influences the vortex state of a nanodisk using numerical spinlattice simulations we demonstrate... | [['we', 'propose', 'a', 'way', 'of', 'fast', 'switching', 'the', 'chirality', 'in', 'a', 'magnetic', 'nanodisk', 'by', 'applying', 'a', 'field', 'pulse', 'to', 'break', 'the', 'symmetry', 'with', 'respect', 'to', 'clockwise', 'or', 'counterclockwise', 'chirality', 'a', 'mask', 'is', 'added', 'by', 'which', 'an', 'inhom... | [-0.19999257217586777, 0.2293171934171919, -0.08939635355807381, -0.034830570705292496, -0.11172503355982495, -0.13467205212922928, 0.030375317269418802, 0.4646873134360821, -0.2816793527684094, -0.29928732014700976, 0.07048858950966624, -0.19210910896000302, -0.12331551314262604, 0.15323649834766753, -0.01919838759105... |
710.4289 | Finite groups with an automorphism cubing a large fraction of elements | We investigate the possible structures imposed on a finite group by its
possession of an automorphism sending a large fraction of the group elements to
their cubes, the philosophy being that this should force the group to be, in
some sense, close to abelian. We prove two theorems. In the first, we
completely classify... | math.GR math.NT | we investigate the possible structures imposed on a finite group by its possession of an automorphism sending a large fraction of the group elements to their cubes the philosophy being that this should force the group to be in some sense close to abelian we prove two theorems in the first we completely classify all fin... | [['we', 'investigate', 'the', 'possible', 'structures', 'imposed', 'on', 'a', 'finite', 'group', 'by', 'its', 'possession', 'of', 'an', 'automorphism', 'sending', 'a', 'large', 'fraction', 'of', 'the', 'group', 'elements', 'to', 'their', 'cubes', 'the', 'philosophy', 'being', 'that', 'this', 'should', 'force', 'the', '... | [-0.1492334976530555, 0.12432726986421994, -0.10897532019019804, 0.04538744018553564, -0.13370167567990918, -0.123684648155831, 0.03300678850922773, 0.37981750825962063, -0.32943775131374536, -0.26042320777873984, 0.14147902666110665, -0.29873917157214785, -0.11946094293571102, 0.2020669188966393, -0.12008834588119671,... |
710.429 | Bounding dissipation in stochastic models | We generalize to stochastic dynamics the exact expression for average
dissipation along an arbitrary non-equilibrium process, given in Phys. Rev.
Lett. 98, 080602 (2007). We then derive lower bounds by various coarse-graining
procedures and illustrate how, when and where the information on the
dissipation is captured... | cond-mat.stat-mech | we generalize to stochastic dynamics the exact expression for average dissipation along an arbitrary nonequilibrium process given in phys rev lett 98 080602 2007 we then derive lower bounds by various coarsegraining procedures and illustrate how when and where the information on the dissipation is captured in models of... | [['we', 'generalize', 'to', 'stochastic', 'dynamics', 'the', 'exact', 'expression', 'for', 'average', 'dissipation', 'along', 'an', 'arbitrary', 'nonequilibrium', 'process', 'given', 'in', 'phys', 'rev', 'lett', '98', '080602', '2007', 'we', 'then', 'derive', 'lower', 'bounds', 'by', 'various', 'coarsegraining', 'proce... | [-0.05402277268607308, 0.1378786838163419, -0.06063926280303686, -0.009600519565740089, -0.022766630432602984, -0.11260263325163612, 0.08483078430786177, 0.32153867224783256, -0.17345110569752892, -0.34026851872396136, 0.01083759788889438, -0.2402366053795925, -0.2075406037253776, 0.24521280946296262, -0.14393025244741... |
710.4291 | A Class of Monotonic Quantities along the Ricci Flow | We construct a class of monotonic quantities along the normalized Ricci flow
on closed n-dimensional manifolds.
| math.DG math.AP | we construct a class of monotonic quantities along the normalized ricci flow on closed ndimensional manifolds | [['we', 'construct', 'a', 'class', 'of', 'monotonic', 'quantities', 'along', 'the', 'normalized', 'ricci', 'flow', 'on', 'closed', 'ndimensional', 'manifolds']] | [-0.27193521661683917, 0.09769010992022231, -0.07175872894003987, 0.07916425389703363, -0.09977535391226411, -0.14564629687811248, -0.12553407135419548, 0.4063993003219366, -0.2668120698072016, -0.0967416763305664, 0.10008143926097546, -0.3445807747775689, -0.11203092096548062, 0.2176247527822852, -0.13654269208200276,... |
710.4292 | Mesons in marginally deformed AdS/CFT | We study the embedding of spacetime filling D7-branes in beta-deformed
backgrounds which, according to the AdS/CFT dictionary, corresponds to
flavoring beta-deformed N=4 super Yang-Mills. We consider supersymmetric and
more general non-supersymmetric three parameter deformations. The equations of
motion for quadratic... | hep-th | we study the embedding of spacetime filling d7branes in betadeformed backgrounds which according to the adscft dictionary corresponds to flavoring betadeformed n4 super yangmills we consider supersymmetric and more general nonsupersymmetric three parameter deformations the equations of motion for quadratic fluctuations... | [['we', 'study', 'the', 'embedding', 'of', 'spacetime', 'filling', 'd7branes', 'in', 'betadeformed', 'backgrounds', 'which', 'according', 'to', 'the', 'adscft', 'dictionary', 'corresponds', 'to', 'flavoring', 'betadeformed', 'n4', 'super', 'yangmills', 'we', 'consider', 'supersymmetric', 'and', 'more', 'general', 'nons... | [-0.14136078897030563, 0.2032119314188411, -0.07589789030543707, 0.1128904616103482, -0.0886115413928114, -0.16019593775186927, -0.026353188385597404, 0.3209344682480217, -0.1846128862624595, -0.2622541922524811, 0.06515509446489053, -0.25138331271618297, -0.197348930390227, 0.0685479751694093, -0.05200905891331853, 0.... |
710.4293 | On the flavor structure of the littlest Higgs model | We investigate the Yukawa sector for up-like quarks in the Lee's version of
the Littlest Higgs model. We derive general quark mass and mixing formulae and
study leading order contributions due to non-zero light quark masses. Relying
on the unitarity of the generalized quark mixing matrix we obtain corrections
to the ... | hep-ph | we investigate the yukawa sector for uplike quarks in the lees version of the littlest higgs model we derive general quark mass and mixing formulae and study leading order contributions due to nonzero light quark masses relying on the unitarity of the generalized quark mixing matrix we obtain corrections to the ckm mat... | [['we', 'investigate', 'the', 'yukawa', 'sector', 'for', 'uplike', 'quarks', 'in', 'the', 'lees', 'version', 'of', 'the', 'littlest', 'higgs', 'model', 'we', 'derive', 'general', 'quark', 'mass', 'and', 'mixing', 'formulae', 'and', 'study', 'leading', 'order', 'contributions', 'due', 'to', 'nonzero', 'light', 'quark', ... | [-0.07279423734727354, 0.24181685334559547, -0.01764101659386488, 0.13588857265431742, -0.04278872389931324, -0.14223132434893737, 0.13660452474093387, 0.301287014406821, -0.20370210263270053, -0.2290163362044687, 0.020656236519552153, -0.31686478905564497, -0.046041316387420594, 0.08083625377756197, 0.0500557131984478... |
710.4294 | Long-Term Collisional Evolution of Debris Disks | We simulated the long-term collisional depletion of debris disks around
solar-type (G2V) stars with our code. The numerical results were supplemented
by, and interpreted through, a new analytic model. A few general scaling rules
for the disk evolution are suggested. The timescale of the collisional
evolution is inver... | astro-ph | we simulated the longterm collisional depletion of debris disks around solartype g2v stars with our code the numerical results were supplemented by and interpreted through a new analytic model a few general scaling rules for the disk evolution are suggested the timescale of the collisional evolution is inversely propor... | [['we', 'simulated', 'the', 'longterm', 'collisional', 'depletion', 'of', 'debris', 'disks', 'around', 'solartype', 'g2v', 'stars', 'with', 'our', 'code', 'the', 'numerical', 'results', 'were', 'supplemented', 'by', 'and', 'interpreted', 'through', 'a', 'new', 'analytic', 'model', 'a', 'few', 'general', 'scaling', 'rul... | [-0.06831329501138124, 0.18570373609134763, -0.05993609286687227, 0.08952360723025563, -0.028704516967991367, -0.045543016672394625, 0.00855663441517904, 0.35514958241016276, -0.2240838724109755, -0.36507459009846893, 0.07229153746319593, -0.26061860547291443, -0.0022736383107258007, 0.1882462892073604, -0.024440970806... |
710.4295 | Partial Differential system in two variables with
$W(D_6^{(1)})$-symmetry and the Garnier system in two variables | In this note, we will compare the Garnier system in two variables with
four-dimensional partial differential system in two variables with
$W(D_6^{(1)})$-symmetry. Both systems are different in each compactification in
the variables $q_1,q_2$, however, has same five holomorphy conditions in the
variables $p_1,p_2$.
| math.AG math.CA | in this note we will compare the garnier system in two variables with fourdimensional partial differential system in two variables with wd_61symmetry both systems are different in each compactification in the variables q_1q_2 however has same five holomorphy conditions in the variables p_1p_2 | [['in', 'this', 'note', 'we', 'will', 'compare', 'the', 'garnier', 'system', 'in', 'two', 'variables', 'with', 'fourdimensional', 'partial', 'differential', 'system', 'in', 'two', 'variables', 'with', 'wd_61symmetry', 'both', 'systems', 'are', 'different', 'in', 'each', 'compactification', 'in', 'the', 'variables', 'q_... | [-0.23832433369188083, 0.11358486785597745, -0.07789521059021354, 0.04216875298602861, -0.018708555155345016, -0.12118365562387876, -0.05024335903692104, 0.33645364535706385, -0.2505365163087845, -0.2568706854279818, 0.1472690392762334, -0.30663208033712136, -0.12801432325726464, 0.14992560064863591, -0.148205132179317... |
710.4296 | Determining the WIMP Mass from Direct Dark Matter Detection Data | Weakly interacting massive particles (WIMPs) are one of the leading
candidates for Dark Matter. So far we can use direct Dark Matter detection to
estimate the mass of halo WIMPs only by fitting predicted recoil spectra to
future experimental data. Here we develop a model-independent method for
determining the WIMP ma... | hep-ph astro-ph | weakly interacting massive particles wimps are one of the leading candidates for dark matter so far we can use direct dark matter detection to estimate the mass of halo wimps only by fitting predicted recoil spectra to future experimental data here we develop a modelindependent method for determining the wimp mass by u... | [['weakly', 'interacting', 'massive', 'particles', 'wimps', 'are', 'one', 'of', 'the', 'leading', 'candidates', 'for', 'dark', 'matter', 'so', 'far', 'we', 'can', 'use', 'direct', 'dark', 'matter', 'detection', 'to', 'estimate', 'the', 'mass', 'of', 'halo', 'wimps', 'only', 'by', 'fitting', 'predicted', 'recoil', 'spec... | [-0.024127842570593642, 0.18601345290829027, -0.11766392573878005, 0.1526331253411187, -0.12278870174886433, -0.09154360806364771, 0.020030449543680464, 0.3343337351394879, -0.18796855165715237, -0.4152081249599028, 0.03778162344798937, -0.3283319506221093, -0.01605121880209401, 0.2019220525910566, 0.04858907687754094,... |
710.4297 | Asymptotics and singularities in cosmological models with positive
cosmological constant | This thesis is concerned with global properties of those cosmological
solutions of Einstein's field equations which obey accelerated expansion into
the future driven by a non-vanishing cosmological constant, as suggested by
current cosmological observations. In particular, the strong cosmic censorship
and BKL conject... | gr-qc | this thesis is concerned with global properties of those cosmological solutions of einsteins field equations which obey accelerated expansion into the future driven by a nonvanishing cosmological constant as suggested by current cosmological observations in particular the strong cosmic censorship and bkl conjecture are... | [['this', 'thesis', 'is', 'concerned', 'with', 'global', 'properties', 'of', 'those', 'cosmological', 'solutions', 'of', 'einsteins', 'field', 'equations', 'which', 'obey', 'accelerated', 'expansion', 'into', 'the', 'future', 'driven', 'by', 'a', 'nonvanishing', 'cosmological', 'constant', 'as', 'suggested', 'by', 'cur... | [-0.1501116289433254, 0.03627485536493148, -0.1027398094393151, 0.08429395733350564, -0.11101227885557581, -0.1473082542743372, -0.03727393646258861, 0.34073710478842256, -0.23533390009087388, -0.2574400683439782, 0.1364768394324726, -0.2478963716684476, -0.13936166259581628, 0.18103145648694963, -0.05735058971559224, ... |
710.4298 | Two-Parameter Scaling of Microwave Rectification vs Microwave Power at
the Boundary between Two-Dimensional Electron Systems | We report measurements of the rectification of microwave radiation (0.7-20
GHz) at the boundary between two-dimensional electron systems separated by a
narrow gap on a silicon surface for different temperatures, electron densities
and microwave power. For frequencies above 4 GHz and different temperatures,
the rectif... | cond-mat.str-el | we report measurements of the rectification of microwave radiation 0720 ghz at the boundary between twodimensional electron systems separated by a narrow gap on a silicon surface for different temperatures electron densities and microwave power for frequencies above 4 ghz and different temperatures the rectified voltag... | [['we', 'report', 'measurements', 'of', 'the', 'rectification', 'of', 'microwave', 'radiation', '0720', 'ghz', 'at', 'the', 'boundary', 'between', 'twodimensional', 'electron', 'systems', 'separated', 'by', 'a', 'narrow', 'gap', 'on', 'a', 'silicon', 'surface', 'for', 'different', 'temperatures', 'electron', 'densities... | [-0.14571967491259177, 0.1645343196898466, -0.02129036720143631, -0.003505654913412097, -0.001404367561917752, -0.19403835512542475, 0.050620935587600495, 0.3751723572301368, -0.26994205615483224, -0.31366893555969, 0.007712051408210148, -0.326332236515979, -0.060900550646086536, 0.2814775115364076, 0.01082262447259078... |
710.4299 | Stationary untrapped boundary conditions in general relativity | A class of boundary conditions for canonical general relativity are proposed
and studied at the quasi-local level. It is shown that for untrapped or
marginal surfaces, fixing the area element on the 2-surface (rather than the
induced 2-metric) and the angular momentum surface density is enough to have a
functionally ... | gr-qc | a class of boundary conditions for canonical general relativity are proposed and studied at the quasilocal level it is shown that for untrapped or marginal surfaces fixing the area element on the 2surface rather than the induced 2metric and the angular momentum surface density is enough to have a functionally different... | [['a', 'class', 'of', 'boundary', 'conditions', 'for', 'canonical', 'general', 'relativity', 'are', 'proposed', 'and', 'studied', 'at', 'the', 'quasilocal', 'level', 'it', 'is', 'shown', 'that', 'for', 'untrapped', 'or', 'marginal', 'surfaces', 'fixing', 'the', 'area', 'element', 'on', 'the', '2surface', 'rather', 'tha... | [-0.16242066243397807, 0.16715860700654522, -0.07525546984537176, 0.09925426215730267, -0.10451300931655028, -0.12156617416488663, -0.030299592494282504, 0.3069992242610528, -0.21606600669894735, -0.21666520864138722, 0.0949370695200575, -0.2591093301086057, -0.08262217881872883, 0.15030028042219526, -0.049031103023288... |
710.43 | Odd Khovanov homology | We describe an invariant of links in the three-sphere which is closely
related to Khovanov's Jones polynomial homology. Our construction replaces the
symmetric algebra appearing in Khovanov's definition with an exterior algebra.
The two invariants have the same reduction modulo 2, but differ over the
rationals. There... | math.QA math.GT | we describe an invariant of links in the threesphere which is closely related to khovanovs jones polynomial homology our construction replaces the symmetric algebra appearing in khovanovs definition with an exterior algebra the two invariants have the same reduction modulo 2 but differ over the rationals there is a red... | [['we', 'describe', 'an', 'invariant', 'of', 'links', 'in', 'the', 'threesphere', 'which', 'is', 'closely', 'related', 'to', 'khovanovs', 'jones', 'polynomial', 'homology', 'our', 'construction', 'replaces', 'the', 'symmetric', 'algebra', 'appearing', 'in', 'khovanovs', 'definition', 'with', 'an', 'exterior', 'algebra'... | [-0.22970963343619727, 0.08239851009790213, -0.15308564483129886, 0.05924147330940916, -0.11807419235030046, -0.1500318745151162, -0.15344184810976283, 0.26372462986753537, -0.3915406874739207, -0.2572686261139237, 0.08968789692466649, -0.21743833986827388, -0.20537916836328804, 0.17343042947781773, -0.1819937996996136... |
710.4301 | Interaction of massive black hole binaries with their stellar
environment: III. Scattering of bound stars | We develop a formalism for studying the dynamics of massive black hole
binaries embedded in gravitationally-bound stellar cusps, and study the binary
orbital decay by three-body interactions, the impact of stellar slingshots on
the density profile of the inner cusp, and the properties of the ejected
hypervelocity sta... | astro-ph | we develop a formalism for studying the dynamics of massive black hole binaries embedded in gravitationallybound stellar cusps and study the binary orbital decay by threebody interactions the impact of stellar slingshots on the density profile of the inner cusp and the properties of the ejected hypervelocity stars hvss... | [['we', 'develop', 'a', 'formalism', 'for', 'studying', 'the', 'dynamics', 'of', 'massive', 'black', 'hole', 'binaries', 'embedded', 'in', 'gravitationallybound', 'stellar', 'cusps', 'and', 'study', 'the', 'binary', 'orbital', 'decay', 'by', 'threebody', 'interactions', 'the', 'impact', 'of', 'stellar', 'slingshots', '... | [-0.15567284876995377, 0.19412344434855863, -0.10572198755497728, 0.1381884667254833, -0.10664046350777434, -0.02956375089010589, 0.05240496018741048, 0.3231127954769933, -0.15675137299089303, -0.3430526143733109, 0.00027926062160220583, -0.29207807128723157, -0.016654720456388435, 0.20935323394993186, 0.00277756569176... |
710.4302 | Theory of NMR in semiconductor quantum point contact devices | We describe how a local non-equilibrium nuclear polarisation can be generated
and detected by electrical means in a semiconductor quantum point contact
device. We show that measurements of the nuclear spin relaxation rate will
provide clear signatures of the interaction mechanism underlying the "0.7"
conductance anom... | cond-mat.mes-hall cond-mat.str-el | we describe how a local nonequilibrium nuclear polarisation can be generated and detected by electrical means in a semiconductor quantum point contact device we show that measurements of the nuclear spin relaxation rate will provide clear signatures of the interaction mechanism underlying the 07 conductance anomaly our... | [['we', 'describe', 'how', 'a', 'local', 'nonequilibrium', 'nuclear', 'polarisation', 'can', 'be', 'generated', 'and', 'detected', 'by', 'electrical', 'means', 'in', 'a', 'semiconductor', 'quantum', 'point', 'contact', 'device', 'we', 'show', 'that', 'measurements', 'of', 'the', 'nuclear', 'spin', 'relaxation', 'rate',... | [-0.13792269941880547, 0.17605147353158548, -0.12621087951582666, 0.08709530371169631, -0.039618644651431494, -0.15364744734520522, 0.013014457400482243, 0.406996048700351, -0.28085190669942395, -0.3024292602800788, 0.03938622577026343, -0.26986627896817833, -0.1878241807108936, 0.22751071914218557, 0.04425096071253602... |
710.4303 | Theorie homotopique des DG-categories | In this thesis we present several original contributions to the study of:
- DG categories and their invariants;
- Neeman's well-generated (algebraic) triangulated categories;
- Fomin-Zelevinsky's cluster algebras approach via representation theory.
| math.KT math.AG | in this thesis we present several original contributions to the study of dg categories and their invariants neemans wellgenerated algebraic triangulated categories fominzelevinskys cluster algebras approach via representation theory | [['in', 'this', 'thesis', 'we', 'present', 'several', 'original', 'contributions', 'to', 'the', 'study', 'of', 'dg', 'categories', 'and', 'their', 'invariants', 'neemans', 'wellgenerated', 'algebraic', 'triangulated', 'categories', 'fominzelevinskys', 'cluster', 'algebras', 'approach', 'via', 'representation', 'theory'... | [-0.13282545069874874, -0.05211207277045168, -0.17205263125100012, 0.12851190447791255, -0.10749943278216083, -0.1156274445098022, -0.018505797653202097, 0.36156786779134437, -0.4229084949555068, -0.26425968547319545, 0.06547812693190344, -0.17917054663572846, -0.2076259683817625, 0.10404106595649801, -0.23988675403183... |
710.4304 | Belief propagation algorithm for computing correlation functions in
finite-temperature quantum many-body systems on loopy graphs | Belief propagation -- a powerful heuristic method to solve inference problems
involving a large number of random variables -- was recently generalized to
quantum theory. Like its classical counterpart, this algorithm is exact on
trees when the appropriate independence conditions are met and is expected to
provide rel... | quant-ph cond-mat.stat-mech | belief propagation a powerful heuristic method to solve inference problems involving a large number of random variables was recently generalized to quantum theory like its classical counterpart this algorithm is exact on trees when the appropriate independence conditions are met and is expected to provide reliable appr... | [['belief', 'propagation', 'a', 'powerful', 'heuristic', 'method', 'to', 'solve', 'inference', 'problems', 'involving', 'a', 'large', 'number', 'of', 'random', 'variables', 'was', 'recently', 'generalized', 'to', 'quantum', 'theory', 'like', 'its', 'classical', 'counterpart', 'this', 'algorithm', 'is', 'exact', 'on', '... | [-0.11251194363382334, 0.11312158664610858, -0.08688141930421504, 0.14119498963506583, -0.08643245713901707, -0.15647796451036508, 0.04907912847944924, 0.3817900259513408, -0.25733267741743476, -0.2851206582970917, 0.10512333924610479, -0.2412922768193918, -0.19384708663759131, 0.21883399214517946, -0.05035651083259532... |
710.4305 | Bound-free pair production cross section in heavy-ion colliders from the
equivalent photon approach | Exact calculations of the electron-positron pair production by a single
photon in the Coulomb field of a nucleus with simultaneous capture of the
electron into the K-shell are discussed for different nuclear charges. Using
the equivalent photon method of Weizsaecker and Williams, a simple expression
for the bound-fre... | nucl-th | exact calculations of the electronpositron pair production by a single photon in the coulomb field of a nucleus with simultaneous capture of the electron into the kshell are discussed for different nuclear charges using the equivalent photon method of weizsaecker and williams a simple expression for the boundfree produ... | [['exact', 'calculations', 'of', 'the', 'electronpositron', 'pair', 'production', 'by', 'a', 'single', 'photon', 'in', 'the', 'coulomb', 'field', 'of', 'a', 'nucleus', 'with', 'simultaneous', 'capture', 'of', 'the', 'electron', 'into', 'the', 'kshell', 'are', 'discussed', 'for', 'different', 'nuclear', 'charges', 'usin... | [-0.03390012711822761, 0.20685748603533616, -0.026930979029698807, 0.1336284104512412, 0.045492835409911066, -0.13369268521130312, 0.021890092979777943, 0.35394523755619023, -0.17611841123664018, -0.26288624009766587, -0.12377443434988064, -0.3326925012057252, 0.07646991536162343, 0.20060699579489388, 0.086309467879773... |
710.4306 | Unifying dark components and crossing the phantom divide with a
classical Dirac field | In this paper we consider a spatially flat Friedmann-Robertson-Walker (FRW)
cosmological model whit cosmological constant, containing a stiff fluid and a
classical Dirac field. The proposed cosmological scenario describes the
evolution of effective dark matter and dark energy components reproducing, with
the help of ... | astro-ph | in this paper we consider a spatially flat friedmannrobertsonwalker frw cosmological model whit cosmological constant containing a stiff fluid and a classical dirac field the proposed cosmological scenario describes the evolution of effective dark matter and dark energy components reproducing with the help of that effe... | [['in', 'this', 'paper', 'we', 'consider', 'a', 'spatially', 'flat', 'friedmannrobertsonwalker', 'frw', 'cosmological', 'model', 'whit', 'cosmological', 'constant', 'containing', 'a', 'stiff', 'fluid', 'and', 'a', 'classical', 'dirac', 'field', 'the', 'proposed', 'cosmological', 'scenario', 'describes', 'the', 'evoluti... | [-0.1389409415285555, 0.13384025197909535, -0.09883835043131124, 0.08211449439646584, -0.11994035882958312, -0.1598719633899002, -0.06752776126676968, 0.2830383463550617, -0.23972138989772093, -0.3652444785624503, 0.05096735104936922, -0.20893870176065085, -0.06369772078100555, 0.113755128895034, 0.029909735859030544, ... |
710.4307 | The quermassintegral inequalities for starshaped domains | We give a simple proof of the insoperimetric inequality for quermassintegrals
of non-convex starshaped domains, using a reslut of Gerhardt \cite{G} and Urbas
\cite{U} on an expanding geometric curvature flow.
| math.DG math.AP | we give a simple proof of the insoperimetric inequality for quermassintegrals of nonconvex starshaped domains using a reslut of gerhardt citeg and urbas citeu on an expanding geometric curvature flow | [['we', 'give', 'a', 'simple', 'proof', 'of', 'the', 'insoperimetric', 'inequality', 'for', 'quermassintegrals', 'of', 'nonconvex', 'starshaped', 'domains', 'using', 'a', 'reslut', 'of', 'gerhardt', 'citeg', 'and', 'urbas', 'citeu', 'on', 'an', 'expanding', 'geometric', 'curvature', 'flow']] | [-0.15822668125232062, -0.0031821926127627697, -0.14646946099000396, 0.049748048945157615, -0.11549938490821256, -0.131350290271695, -0.01976353744113887, 0.3115861901530513, -0.2677752897143364, -0.17691705672553293, 0.1554558530829295, -0.23382287955394498, -0.15860850032832888, 0.22555713445224143, -0.19038810236034... |
710.4308 | Aharanov-Bohm excitons at elevated temperatures in type-II ZnTe/ZnSe
quantum dots | Optical emission from type-II ZnTe/ZnSe quantum dots demonstrates large and
persistent oscillations in both the peak energy and intensity indicating the
formation of coherently rotating states. Furthermore, the Aharanov-Bohm (AB)
effect is shown to be remarkably robust and persists until 180K. This is at
least one or... | cond-mat.mes-hall | optical emission from typeii znteznse quantum dots demonstrates large and persistent oscillations in both the peak energy and intensity indicating the formation of coherently rotating states furthermore the aharanovbohm ab effect is shown to be remarkably robust and persists until 180k this is at least one order of mag... | [['optical', 'emission', 'from', 'typeii', 'znteznse', 'quantum', 'dots', 'demonstrates', 'large', 'and', 'persistent', 'oscillations', 'in', 'both', 'the', 'peak', 'energy', 'and', 'intensity', 'indicating', 'the', 'formation', 'of', 'coherently', 'rotating', 'states', 'furthermore', 'the', 'aharanovbohm', 'ab', 'effe... | [-0.13207794735545145, 0.1796843941242275, -0.04889616943087036, 0.04415034902998932, 0.006347561965843565, -0.11806930535423912, 0.01646581603716569, 0.42608694148887144, -0.2592032241120346, -0.3257533315520145, 0.047274475802336575, -0.3061815328025994, -0.07778248091007729, 0.1960168360842784, 0.02355188703605611, ... |
710.4309 | Twisting on associative algebras and Rota-Baxter type operators | We will introduce an operation "twisting" on Hochschild complex by analogy
with Drinfeld's twisting operations. By using the twisting and derived bracket
construction, we will study differential graded Lie algebra structures
associated with bi-graded Hochschild complex. We will show that Rota-Baxter
type operators ar... | math.QA math.SG | we will introduce an operation twisting on hochschild complex by analogy with drinfelds twisting operations by using the twisting and derived bracket construction we will study differential graded lie algebra structures associated with bigraded hochschild complex we will show that rotabaxter type operators are solution... | [['we', 'will', 'introduce', 'an', 'operation', 'twisting', 'on', 'hochschild', 'complex', 'by', 'analogy', 'with', 'drinfelds', 'twisting', 'operations', 'by', 'using', 'the', 'twisting', 'and', 'derived', 'bracket', 'construction', 'we', 'will', 'study', 'differential', 'graded', 'lie', 'algebra', 'structures', 'asso... | [-0.2744387216084907, 0.09535403677774969, -0.021662849392141064, 0.07365112819318329, -0.21553846374304303, -0.12720599265078142, -0.1328413350687873, 0.3930400493404558, -0.4205162241574257, -0.20201133378601122, 0.1255635407212521, -0.18097688811981388, -0.2893777349963784, 0.21231367789028632, -0.2021883906901724, ... |
710.431 | On two-Dimensional Holonomy | We define the thin fundamental categorical group ${\mathcal P}_2(M,*)$ of a
based smooth manifold $(M,*)$ as the categorical group whose objects are rank-1
homotopy classes of based loops on $M$, and whose morphisms are rank-2 homotopy
classes of homotopies between based loops on $M$. Here two maps are rank-$n$
homot... | math.DG hep-th math.CT | we define the thin fundamental categorical group mathcal p_2m of a based smooth manifold m as the categorical group whose objects are rank1 homotopy classes of based loops on m and whose morphisms are rank2 homotopy classes of homotopies between based loops on m here two maps are rankn homotopic when the rank of the di... | [['we', 'define', 'the', 'thin', 'fundamental', 'categorical', 'group', 'mathcal', 'p_2m', 'of', 'a', 'based', 'smooth', 'manifold', 'm', 'as', 'the', 'categorical', 'group', 'whose', 'objects', 'are', 'rank1', 'homotopy', 'classes', 'of', 'based', 'loops', 'on', 'm', 'and', 'whose', 'morphisms', 'are', 'rank2', 'homot... | [-0.18139803264770776, 0.1082811648987474, -0.09989403832343317, 0.02729356056154375, -0.12016189886827863, -0.17158608343752643, 0.00011998809002820523, 0.38698521723910684, -0.3004670729530194, -0.23967508034360024, 0.04583178268775584, -0.22483985715671517, -0.12202864256987889, 0.1471433075122355, -0.15351420321591... |
710.4311 | Enhanced symmetry points and metastable supersymmetry breaking along
pseudo-runaway directions | We construct a model with long-lived metastable vacua in which all the
relevant parameters, including the supersymmetry breaking scale, are generated
dynamically by dimensional transmutation. The metastable vacua appear along a
pseudo-runaway direction near a point of enhanced symmetry as a result of a
balance betwee... | hep-th | we construct a model with longlived metastable vacua in which all the relevant parameters including the supersymmetry breaking scale are generated dynamically by dimensional transmutation the metastable vacua appear along a pseudorunaway direction near a point of enhanced symmetry as a result of a balance between nonpe... | [['we', 'construct', 'a', 'model', 'with', 'longlived', 'metastable', 'vacua', 'in', 'which', 'all', 'the', 'relevant', 'parameters', 'including', 'the', 'supersymmetry', 'breaking', 'scale', 'are', 'generated', 'dynamically', 'by', 'dimensional', 'transmutation', 'the', 'metastable', 'vacua', 'appear', 'along', 'a', '... | [-0.17941592547806426, 0.28939624038905326, -0.0908293309031238, 0.13703946091897104, -0.04248023992010825, -0.1521775192731965, 0.060478846308066915, 0.3317618594491776, -0.2640648807963015, -0.24092420122363198, 0.09543727302733598, -0.2212473982551568, -0.1369604810188577, 0.08668850115369219, 0.0005635852518845612,... |
710.4312 | Bulk thermodynamics and charge fluctuations at non-vanishing baryon
density | We present results on bulk thermodynamic quantities as well as net baryon
number, strangeness and electric charge fluctuations in QCD at non-zero density
and temperature obtained from lattice calculations with almost physical quark
masses for two values of the lattice cut-off $aT=1/4$ and 1/6 . We show that
with our ... | hep-lat | we present results on bulk thermodynamic quantities as well as net baryon number strangeness and electric charge fluctuations in qcd at nonzero density and temperature obtained from lattice calculations with almost physical quark masses for two values of the lattice cutoff at14 and 16 we show that with our improved p4f... | [['we', 'present', 'results', 'on', 'bulk', 'thermodynamic', 'quantities', 'as', 'well', 'as', 'net', 'baryon', 'number', 'strangeness', 'and', 'electric', 'charge', 'fluctuations', 'in', 'qcd', 'at', 'nonzero', 'density', 'and', 'temperature', 'obtained', 'from', 'lattice', 'calculations', 'with', 'almost', 'physical'... | [-0.11952581724950245, 0.3018022756917136, -0.057761806196400096, 0.06504488708118775, 0.005434247909912041, -0.09080500637048057, 0.06182703369030995, 0.31073988465326174, -0.2016899953356811, -0.3017628432597433, 0.04049477959051728, -0.3534149268083274, 0.0010663178842514754, 0.12370696355987873, 0.03718542152134303... |
710.4313 | Superconductivity-induced macroscopic resonant tunneling | We show analytically and by numerical simulations that the conductance
through $\pi$-biased chaotic Josephson junctions is enhanced by several orders
of magnitude in the short-wavelength regime. We identify the mechanism behind
this effect as {\it macroscopic resonant tunneling} through a macroscopic
number of low-en... | cond-mat.mes-hall cond-mat.supr-con | we show analytically and by numerical simulations that the conductance through pibiased chaotic josephson junctions is enhanced by several orders of magnitude in the shortwavelength regime we identify the mechanism behind this effect as it macroscopic resonant tunneling through a macroscopic number of lowenergy quaside... | [['we', 'show', 'analytically', 'and', 'by', 'numerical', 'simulations', 'that', 'the', 'conductance', 'through', 'pibiased', 'chaotic', 'josephson', 'junctions', 'is', 'enhanced', 'by', 'several', 'orders', 'of', 'magnitude', 'in', 'the', 'shortwavelength', 'regime', 'we', 'identify', 'the', 'mechanism', 'behind', 'th... | [-0.2346363603744818, 0.21772265845261837, -0.03706868606336091, 0.09282944372693158, 0.01639066087891874, -0.11642809134260144, 0.12058041252843711, 0.3184840229704328, -0.2853313151989942, -0.31408327961664484, -0.038593125339779676, -0.2835043709315157, -0.2200844437795003, 0.24943668982418982, 0.05440565856659542, ... |
710.4314 | Substrate Adhesion of a Nongrafted Flexible Polymer in a Cavity | In a contact density chain-growth study we investigate the
solubility-temperature pseudo-phase diagram of a lattice polymer in a cavity
with an attractive surface. In addition to the main phases of adsorbed and
desorbed conformations we find numerous subphases of collapsed and expanded
structures.
| cond-mat.soft | in a contact density chaingrowth study we investigate the solubilitytemperature pseudophase diagram of a lattice polymer in a cavity with an attractive surface in addition to the main phases of adsorbed and desorbed conformations we find numerous subphases of collapsed and expanded structures | [['in', 'a', 'contact', 'density', 'chaingrowth', 'study', 'we', 'investigate', 'the', 'solubilitytemperature', 'pseudophase', 'diagram', 'of', 'a', 'lattice', 'polymer', 'in', 'a', 'cavity', 'with', 'an', 'attractive', 'surface', 'in', 'addition', 'to', 'the', 'main', 'phases', 'of', 'adsorbed', 'and', 'desorbed', 'co... | [-0.17753227475250877, 0.17957914437926753, -0.1167325004068918, 0.007438512843881928, 0.04861678105107574, -0.11296209248681661, 0.08499460429397174, 0.42611451057154076, -0.22178625300266716, -0.24138345027905564, 0.02773791833423338, -0.23828773161526337, -0.17482658211401728, 0.08104860727393697, 0.0168491541732882... |
710.4315 | Critical Collapse of Einstein Cluster | We observe critical phenomena in spherically symmetric gravitational collapse
of Einstein Cluster. We show analytically that the collapse evolution ends
either in formation of a black hole or in dispersal depending on the values of
initial parameters which characterize initial density and angular momentum of
the coll... | gr-qc | we observe critical phenomena in spherically symmetric gravitational collapse of einstein cluster we show analytically that the collapse evolution ends either in formation of a black hole or in dispersal depending on the values of initial parameters which characterize initial density and angular momentum of the collaps... | [['we', 'observe', 'critical', 'phenomena', 'in', 'spherically', 'symmetric', 'gravitational', 'collapse', 'of', 'einstein', 'cluster', 'we', 'show', 'analytically', 'that', 'the', 'collapse', 'evolution', 'ends', 'either', 'in', 'formation', 'of', 'a', 'black', 'hole', 'or', 'in', 'dispersal', 'depending', 'on', 'the'... | [-0.17301452981441148, 0.12717879266116996, -0.07410746841805474, 0.10257170226767051, -0.008611792254817615, -0.09950596362599456, 0.04716192788625022, 0.318547233521026, -0.1753025109242952, -0.30416929800709597, 0.10266833207023578, -0.22958885614489377, -0.0738655298316319, 0.17141167286840475, 0.04827208645945909,... |
710.4316 | Can the new Neutrino Telescopes reveal the Gravitational Properties of
Antimatter? | We argue that the hypothesis of the gravitational repulsion between matter
and antimatter can be tested at the Ice Cube, a neutrino telescope, recently
constructed at the South Pole. If there is such a gravitational repulsion, the
gravitational field, deep inside the horizon of a black hole, might create
neutrino-ant... | gr-qc astro-ph.GA | we argue that the hypothesis of the gravitational repulsion between matter and antimatter can be tested at the ice cube a neutrino telescope recently constructed at the south pole if there is such a gravitational repulsion the gravitational field deep inside the horizon of a black hole might create neutrinoantineutrino... | [['we', 'argue', 'that', 'the', 'hypothesis', 'of', 'the', 'gravitational', 'repulsion', 'between', 'matter', 'and', 'antimatter', 'can', 'be', 'tested', 'at', 'the', 'ice', 'cube', 'a', 'neutrino', 'telescope', 'recently', 'constructed', 'at', 'the', 'south', 'pole', 'if', 'there', 'is', 'such', 'a', 'gravitational', ... | [-0.10927046072500726, 0.23388233986193444, -0.098111279059908, 0.19421525421559385, -0.09041777728446598, -0.09271815134581693, 0.011523647159578857, 0.3131317163271637, -0.198011269026179, -0.3105345195287774, 0.022247493229926852, -0.34362282799877997, -0.01978977190346682, 0.20016703798821003, 0.03635523594707122, ... |
710.4317 | One dimensional conformal metric flow II | In this paper we continue our studies of the one dimensional conformal metric
flows, which were introduced in [8]. In this part we mainly focus on evolution
equations involving fourth order derivatives. The global existence and
exponential convergence of metrics for the 1-Q and 4-Q flows are obtained.
| math.AP math.DG | in this paper we continue our studies of the one dimensional conformal metric flows which were introduced in 8 in this part we mainly focus on evolution equations involving fourth order derivatives the global existence and exponential convergence of metrics for the 1q and 4q flows are obtained | [['in', 'this', 'paper', 'we', 'continue', 'our', 'studies', 'of', 'the', 'one', 'dimensional', 'conformal', 'metric', 'flows', 'which', 'were', 'introduced', 'in', '8', 'in', 'this', 'part', 'we', 'mainly', 'focus', 'on', 'evolution', 'equations', 'involving', 'fourth', 'order', 'derivatives', 'the', 'global', 'existe... | [-0.1569131933307896, 0.07503690450782112, -0.05544188952383896, 0.05788159432025471, -0.025623639308226604, -0.03242872936728721, -0.04782005582577161, 0.30982225803503144, -0.21237504637489715, -0.23872115094369897, 0.18892715584418815, -0.313289836825182, -0.16848362931826463, 0.13377075269818306, -0.036053819421795... |
710.4318 | Differential invariants of a Lie group action: syzygies on a generating
set | Given a group action, known by its infinitesimal generators, we exhibit a
complete set of syzygies on a generating set of differential invariants. For
that we elaborate on the reinterpretation of Cartan's moving frame by Fels and
Olver (1999). This provides constructive tools for exploring algebras of
differential in... | cs.SC math.DG | given a group action known by its infinitesimal generators we exhibit a complete set of syzygies on a generating set of differential invariants for that we elaborate on the reinterpretation of cartans moving frame by fels and olver 1999 this provides constructive tools for exploring algebras of differential invariants | [['given', 'a', 'group', 'action', 'known', 'by', 'its', 'infinitesimal', 'generators', 'we', 'exhibit', 'a', 'complete', 'set', 'of', 'syzygies', 'on', 'a', 'generating', 'set', 'of', 'differential', 'invariants', 'for', 'that', 'we', 'elaborate', 'on', 'the', 'reinterpretation', 'of', 'cartans', 'moving', 'frame', 'b... | [-0.18108810885448237, 0.026329846254416873, -0.12139641600352123, 0.08433896419829784, -0.1421538154613607, -0.09976083321534858, 0.030781370380356415, 0.31388454116424735, -0.26959700365455785, -0.2745187410286495, 0.08602273017073012, -0.25266741562102524, -0.1416933450809851, 0.2553196995500095, -0.1687054689023263... |
710.4319 | Supersymmetric codimension-two branes in six-dimensional gauged
supergravity | We consider the six-dimensional Salam-Sezgin supergravity in the presence of
codimension-2 branes. In the case that the branes carry only tension, we
provide a way to supersymmetrise them by adding appropriate localised
Fayet-Iliopoulos terms and localised corrections to the Chern-Simons term and
modifying accordingl... | hep-th hep-ph | we consider the sixdimensional salamsezgin supergravity in the presence of codimension2 branes in the case that the branes carry only tension we provide a way to supersymmetrise them by adding appropriate localised fayetiliopoulos terms and localised corrections to the chernsimons term and modifying accordingly the fer... | [['we', 'consider', 'the', 'sixdimensional', 'salamsezgin', 'supergravity', 'in', 'the', 'presence', 'of', 'codimension2', 'branes', 'in', 'the', 'case', 'that', 'the', 'branes', 'carry', 'only', 'tension', 'we', 'provide', 'a', 'way', 'to', 'supersymmetrise', 'them', 'by', 'adding', 'appropriate', 'localised', 'fayeti... | [-0.17031864002938307, 0.1882421865704514, -0.0423233629174767, 0.10135417803660006, -0.07442357438424277, -0.18993486491371953, -0.017059601283454823, 0.28276755858863156, -0.140426079158686, -0.2783729969657817, 0.10255193645097611, -0.28009546804611407, -0.13619972394025398, 0.04189445815485207, -0.07344466278750804... |
710.432 | Liouville energy on a topological two sphere | In this paper we shall give an analytic proof of the fact that the Liouville
energy on a topological two sphere is bounded from below. Our proof does not
rely on the uniformization theorem and the Onofri inequality, thus it is
essentially needed in the alternative proof of the uniformization theorem via
the Calabi fl... | math.AP math.DG | in this paper we shall give an analytic proof of the fact that the liouville energy on a topological two sphere is bounded from below our proof does not rely on the uniformization theorem and the onofri inequality thus it is essentially needed in the alternative proof of the uniformization theorem via the calabi flow s... | [['in', 'this', 'paper', 'we', 'shall', 'give', 'an', 'analytic', 'proof', 'of', 'the', 'fact', 'that', 'the', 'liouville', 'energy', 'on', 'a', 'topological', 'two', 'sphere', 'is', 'bounded', 'from', 'below', 'our', 'proof', 'does', 'not', 'rely', 'on', 'the', 'uniformization', 'theorem', 'and', 'the', 'onofri', 'ine... | [-0.11096457344217178, 0.0513816847953235, -0.1830336518275241, 0.11612906639661211, -0.11882296469635688, -0.10225155497662342, 0.03557087506245201, 0.2851295546503164, -0.25860457862607944, -0.23970241884056193, 0.12205061999012311, -0.2512093302555, -0.17094887532771397, 0.2713665137103257, -0.14997584710064799, -0.... |
710.4321 | Coarse Grained Liouville Dynamics of piecewise linear discontinuous maps | We compute the spectrum of the classical and quantum mechanical
coarse-grained propagators for a piecewise linear discontinuous map. We analyze
the quantum - classical correspondence and the evolution of the spectrum with
increasing resolution. Our results are compared to the ones obtained for a
mixed system.
| quant-ph nlin.CD | we compute the spectrum of the classical and quantum mechanical coarsegrained propagators for a piecewise linear discontinuous map we analyze the quantum classical correspondence and the evolution of the spectrum with increasing resolution our results are compared to the ones obtained for a mixed system | [['we', 'compute', 'the', 'spectrum', 'of', 'the', 'classical', 'and', 'quantum', 'mechanical', 'coarsegrained', 'propagators', 'for', 'a', 'piecewise', 'linear', 'discontinuous', 'map', 'we', 'analyze', 'the', 'quantum', 'classical', 'correspondence', 'and', 'the', 'evolution', 'of', 'the', 'spectrum', 'with', 'increa... | [-0.09974385609643327, 0.08367308197129104, -0.11885096557024452, 0.06048795487731695, -0.004967414548931023, -0.1205207902731167, 0.0028347365040746, 0.3350112497806549, -0.3125494288073646, -0.24577539306547908, 0.09995313560486668, -0.2987799475590388, -0.14727263429926502, 0.2127740694416894, -0.02647130336198542, ... |
710.4322 | Exotic strange multibaryon states searches with $\Lambda$- hyperon and
$K^0_s$- meson systems in p+A collisions at momentum 10 GeV/c | Review for exotic strange multibaryon states were obseved in the effective
mass spectra of: 1)$\Lambda \pi^+$, $\Lambda \pi^-$, $\Lambda p$, $\Lambda p
p$, and $\Lambda K^0_S$, $K^0_S\pi^{\pm}$ and $K^0_Sp$ subsystems.The invariant
mass of $\Lambda \pi^+$ and $K^0_S\pi^{\pm}$ spectra has observed well known
$\Sigma^{... | hep-ex | review for exotic strange multibaryon states were obseved in the effective mass spectra of 1lambda pi lambda pi lambda p lambda p p and lambda k0_s k0_spipm and k0_sp subsystemsthe invariant mass of lambda pi and k0_spipm spectra has observed well known sigma1385 and kpm892 resonances the width of sigma1385 for pa reac... | [['review', 'for', 'exotic', 'strange', 'multibaryon', 'states', 'were', 'obseved', 'in', 'the', 'effective', 'mass', 'spectra', 'of', '1lambda', 'pi', 'lambda', 'pi', 'lambda', 'p', 'lambda', 'p', 'p', 'and', 'lambda', 'k0_s', 'k0_spipm', 'and', 'k0_sp', 'subsystemsthe', 'invariant', 'mass', 'of', 'lambda', 'pi', 'and... | [-0.1158205429045013, 0.23600004617162426, -0.07808012868050777, 0.13954197560117176, -0.006187411486124149, -0.16170544595448205, -0.0014143416827375238, 0.32487601706889846, -0.17228773626207253, -0.26893168192526157, -0.07860681188241062, -0.3866567833706586, 0.04000718647030869, 0.12988972670934867, 0.0831910255412... |
710.4323 | Chain-Growth Simulations of Lattice-Peptide Adsorption to Attractive
Substrates | Based on a newly developed contact-density chain-growth algorithm, we have
simulated a nongrafted peptide in the vicinity of different attractive
substrates. We analyzed the specificity of the peptide adsorption by focussing
on the conformational transitions the peptide experiences in the
binding/unbinding processes.... | cond-mat.soft | based on a newly developed contactdensity chaingrowth algorithm we have simulated a nongrafted peptide in the vicinity of different attractive substrates we analyzed the specificity of the peptide adsorption by focussing on the conformational transitions the peptide experiences in the bindingunbinding processes in a si... | [['based', 'on', 'a', 'newly', 'developed', 'contactdensity', 'chaingrowth', 'algorithm', 'we', 'have', 'simulated', 'a', 'nongrafted', 'peptide', 'in', 'the', 'vicinity', 'of', 'different', 'attractive', 'substrates', 'we', 'analyzed', 'the', 'specificity', 'of', 'the', 'peptide', 'adsorption', 'by', 'focussing', 'on'... | [-0.11395788537807387, 0.1311458510693444, -0.10739588630285195, 0.043810865584687206, -0.0038259202252617845, -0.12363478085009394, 0.09519446044892287, 0.41921031359824346, -0.20680541184160475, -0.2810166512997888, 0.025235834643713755, -0.25454074365981744, -0.14871920640546854, 0.16065983707127127, 0.0199348210439... |
710.4324 | A sharp inequality and its applications | We establish an analog Hardy inequality with sharp constant involving
exponential weight function. The special case of this inequality (for n=2)
leads to a direct proof of Onofri inequality on S^2.
| math.AP math.DG | we establish an analog hardy inequality with sharp constant involving exponential weight function the special case of this inequality for n2 leads to a direct proof of onofri inequality on s2 | [['we', 'establish', 'an', 'analog', 'hardy', 'inequality', 'with', 'sharp', 'constant', 'involving', 'exponential', 'weight', 'function', 'the', 'special', 'case', 'of', 'this', 'inequality', 'for', 'n2', 'leads', 'to', 'a', 'direct', 'proof', 'of', 'onofri', 'inequality', 'on', 's2']] | [-0.14288165766535507, 0.014228834579567305, -0.03577700840129006, 0.08031489445842922, -0.07656293116029232, -0.23944029390751834, 0.05501694426376132, 0.25049789377578324, -0.2688460586772811, -0.23122051316163234, 0.11270031613868571, -0.25234267428787727, -0.1470347416677302, 0.2464003130312889, -0.1004342290482694... |
710.4325 | Three-electron anisotropic quantum dots in variable magnetic fields:
exact results for excitation spectra, spin structures, and entanglement | Exact-diagonalization calculations for N=3 electrons in anisotropic quantum
dots, covering a broad range of confinement anisotropies and strength of
inter-electron repulsion, are presented for zero and low magnetic fields. The
excitation spectra are analyzed as a function of the strength of the magnetic
field and for... | cond-mat.mes-hall cond-mat.str-el physics.comp-ph quant-ph | exactdiagonalization calculations for n3 electrons in anisotropic quantum dots covering a broad range of confinement anisotropies and strength of interelectron repulsion are presented for zero and low magnetic fields the excitation spectra are analyzed as a function of the strength of the magnetic field and for increas... | [['exactdiagonalization', 'calculations', 'for', 'n3', 'electrons', 'in', 'anisotropic', 'quantum', 'dots', 'covering', 'a', 'broad', 'range', 'of', 'confinement', 'anisotropies', 'and', 'strength', 'of', 'interelectron', 'repulsion', 'are', 'presented', 'for', 'zero', 'and', 'low', 'magnetic', 'fields', 'the', 'excita... | [-0.16639734521821334, 0.22928879289406462, -0.038691040991883106, 0.07326266281346887, 0.007019792587413378, -0.1389024001010961, -0.014587276779789606, 0.39194881073440074, -0.27727762960839547, -0.2618698805527783, -0.0016643616147392869, -0.2933931310511269, -0.07766781732220546, 0.17678892534178006, 0.079052851583... |
710.4326 | Some Asymptotic Behavior of the first Eigenvalue along the Ricci Flow | We study some asymptotic behavior of the first nonzero eigenvalue of the
Lalacian along the normalized Ricci flow and give a direct short proof for an
asymptotic upper limit estimate.
| math.DG math.AP | we study some asymptotic behavior of the first nonzero eigenvalue of the lalacian along the normalized ricci flow and give a direct short proof for an asymptotic upper limit estimate | [['we', 'study', 'some', 'asymptotic', 'behavior', 'of', 'the', 'first', 'nonzero', 'eigenvalue', 'of', 'the', 'lalacian', 'along', 'the', 'normalized', 'ricci', 'flow', 'and', 'give', 'a', 'direct', 'short', 'proof', 'for', 'an', 'asymptotic', 'upper', 'limit', 'estimate']] | [-0.21763925575490656, 0.05447001198501374, -0.17396445423043494, 0.08225267213480227, -0.09717016410211037, -0.07487105075591083, 0.02180797979235649, 0.2653919470271674, -0.2162960503121902, -0.20441622910057677, 0.18743392161960745, -0.2921259942753562, -0.11900419876148025, 0.18898295855213856, -0.00730351215742271... |
710.4327 | Single photon Mach-Zehnder interferometer for quantum networks based on
the Single Photon Faraday Effect: principle and applications | Combining the recent progress in semiconductor nanostructures along with the
versatility of photonic crystals in confining and manipulating light, quantum
networks allow for the prospect of an integrated and low power quantum
technology. Within quantum networks, which consist of a system of waveguides
and nanocavitie... | cond-mat.mes-hall | combining the recent progress in semiconductor nanostructures along with the versatility of photonic crystals in confining and manipulating light quantum networks allow for the prospect of an integrated and low power quantum technology within quantum networks which consist of a system of waveguides and nanocavities wit... | [['combining', 'the', 'recent', 'progress', 'in', 'semiconductor', 'nanostructures', 'along', 'with', 'the', 'versatility', 'of', 'photonic', 'crystals', 'in', 'confining', 'and', 'manipulating', 'light', 'quantum', 'networks', 'allow', 'for', 'the', 'prospect', 'of', 'an', 'integrated', 'and', 'low', 'power', 'quantum... | [-0.11990895577047708, 0.17472169451850597, -0.07285423060838024, -0.01782828226885827, 0.0035108464713523384, -0.23243878615903668, 0.05946099870427989, 0.42624953455593, -0.26197940618251725, -0.30847213633002385, 0.03625576834276538, -0.2578669412229347, -0.13053412296850345, 0.27005015883375616, -0.0454244001773665... |
710.4328 | How Very Massive Metal Free Stars Start Cosmological Reionization | (Abridged) Using ab initio cosmological Eulerian adaptive mesh refinement
radiation hydrodynamical calculations, we discuss how very massive stars start
the process of cosmological reionization. The models include non-equilibrium
primordial gas chemistry and cooling processes and accurate radiation transport
in the C... | astro-ph | abridged using ab initio cosmological eulerian adaptive mesh refinement radiation hydrodynamical calculations we discuss how very massive stars start the process of cosmological reionization the models include nonequilibrium primordial gas chemistry and cooling processes and accurate radiation transport in the case b a... | [['abridged', 'using', 'ab', 'initio', 'cosmological', 'eulerian', 'adaptive', 'mesh', 'refinement', 'radiation', 'hydrodynamical', 'calculations', 'we', 'discuss', 'how', 'very', 'massive', 'stars', 'start', 'the', 'process', 'of', 'cosmological', 'reionization', 'the', 'models', 'include', 'nonequilibrium', 'primordi... | [-0.08328258155846775, 0.19733748093955086, -0.012812166755575033, 0.122532949831134, -0.05629046078717943, -0.05625664961848101, 0.02707745199922913, 0.4045785301127955, -0.17709407071402716, -0.37104739409647747, -0.0008399581038443151, -0.3181427295768707, 0.035104459677372246, 0.17988601640074625, 0.048332205253324... |
710.4329 | On tilting modules over cluster-tilted algebras | In this paper, we show that the tilting modules over a cluster-tilted algebra
$A$ lift to tilting objects in the associated cluster category $\mathcal{C}_H$.
As a first application, we describe the induced exchange relation for tilting
$A$-modules arising from the exchange relation for tilting object in
$\mathcal{C}_... | math.RT math.RA | in this paper we show that the tilting modules over a clustertilted algebra a lift to tilting objects in the associated cluster category mathcalc_h as a first application we describe the induced exchange relation for tilting amodules arising from the exchange relation for tilting object in mathcalc_h as a second applic... | [['in', 'this', 'paper', 'we', 'show', 'that', 'the', 'tilting', 'modules', 'over', 'a', 'clustertilted', 'algebra', 'a', 'lift', 'to', 'tilting', 'objects', 'in', 'the', 'associated', 'cluster', 'category', 'mathcalc_h', 'as', 'a', 'first', 'application', 'we', 'describe', 'the', 'induced', 'exchange', 'relation', 'fo... | [-0.2070903225675604, 0.051920168038647053, -0.04224010935779345, 0.07035670460249155, -0.145668580338864, -0.10372882478444254, -0.03637188148755833, 0.44207113468230275, -0.49532895484718226, -0.17655484051585701, 0.047257589044096736, -0.18195982258451188, -0.17580371280595408, 0.17376890382334842, -0.17879695246406... |
710.433 | NLO evolution of color dipoles | The small-$x$ deep inelastic scattering in the saturation region is governed
by the non-linear evolution of Wilson-line operators. In the leading
logarithmic approximation it is given by the BK equation for the evolution of
color dipoles. In the next-to-leading order the BK equation gets contributions
from quark and ... | hep-ph | the smallx deep inelastic scattering in the saturation region is governed by the nonlinear evolution of wilsonline operators in the leading logarithmic approximation it is given by the bk equation for the evolution of color dipoles in the nexttoleading order the bk equation gets contributions from quark and gluon loops... | [['the', 'smallx', 'deep', 'inelastic', 'scattering', 'in', 'the', 'saturation', 'region', 'is', 'governed', 'by', 'the', 'nonlinear', 'evolution', 'of', 'wilsonline', 'operators', 'in', 'the', 'leading', 'logarithmic', 'approximation', 'it', 'is', 'given', 'by', 'the', 'bk', 'equation', 'for', 'the', 'evolution', 'of'... | [-0.060313132515875625, 0.19368438592064194, -0.14165726818609983, 0.13438974394230171, -0.06639484658662695, -0.013813896139618009, -0.008313386233567144, 0.31744461914058775, -0.22614712406648324, -0.2102100834483281, 0.01435351076797815, -0.3317162823746912, -0.07713806238607504, 0.07692775802570395, 0.0804612174670... |
710.4331 | SUSY QCD Corrections to Higgs Pair Production from Bottom Quark Fusion | We present a complete next-to-leading order (NLO) calculation for the total
cross section for inclusive Higgs pair production via bottom-quark fusion at
the CERN Large Hadron Collider (LHC) in the minimal supersymmetric standard
model (MSSM) and the minimal supergravity model (mSUGRA). We emphasize the
contributions ... | hep-ph | we present a complete nexttoleading order nlo calculation for the total cross section for inclusive higgs pair production via bottomquark fusion at the cern large hadron collider lhc in the minimal supersymmetric standard model mssm and the minimal supergravity model msugra we emphasize the contributions of squark and ... | [['we', 'present', 'a', 'complete', 'nexttoleading', 'order', 'nlo', 'calculation', 'for', 'the', 'total', 'cross', 'section', 'for', 'inclusive', 'higgs', 'pair', 'production', 'via', 'bottomquark', 'fusion', 'at', 'the', 'cern', 'large', 'hadron', 'collider', 'lhc', 'in', 'the', 'minimal', 'supersymmetric', 'standard... | [-0.04543805012034009, 0.2885133774151378, -0.011450551343960282, 0.2182662512185862, -0.04321979118116281, -0.14706167240080464, 0.027115871610990522, 0.2970974135830108, -0.11211817286422719, -0.23617332465136828, -0.03304735118012025, -0.3506040381338528, 0.07424598180122026, 0.08361284906024356, 0.065106414673526, ... |
710.4332 | Unzipping of two random heteropolymers: Ground state energy and finite
size effects | We have analyzed the dependence of average ground state energy per monomer,
$e$, of the complex of two random heteropolymers with quenched sequences, on
chain length, $n$, in the ensemble of chains with uniform distribution of
primary sequences. Every chain monomer is randomly and independently chosen
with the unifor... | cond-mat.stat-mech | we have analyzed the dependence of average ground state energy per monomer e of the complex of two random heteropolymers with quenched sequences on chain length n in the ensemble of chains with uniform distribution of primary sequences every chain monomer is randomly and independently chosen with the uniform probabilit... | [['we', 'have', 'analyzed', 'the', 'dependence', 'of', 'average', 'ground', 'state', 'energy', 'per', 'monomer', 'e', 'of', 'the', 'complex', 'of', 'two', 'random', 'heteropolymers', 'with', 'quenched', 'sequences', 'on', 'chain', 'length', 'n', 'in', 'the', 'ensemble', 'of', 'chains', 'with', 'uniform', 'distribution'... | [-0.16572276517800097, 0.211708896055416, -0.02086999426182539, 0.041507632805380563, 0.057756091138014755, -0.18481861173875902, 0.07025164116116309, 0.395969651096902, -0.26954411920224136, -0.26520508703873963, 0.015144813499827827, -0.31248281911180253, -0.02051036894575633, 0.10150234517534562, 0.06736259871611582... |
710.4333 | Minimal Walking Technicolor | I report on our construction and analysis of the effective low energy
Lagrangian for the Minimal Walking Technicolor (MWT) model. The parameters of
the effective Lagrangian are constrained by imposing modified Weinberg sum
rules and by imposing a value for the S parameter estimated from the underlying
Technicolor the... | hep-ph | i report on our construction and analysis of the effective low energy lagrangian for the minimal walking technicolor mwt model the parameters of the effective lagrangian are constrained by imposing modified weinberg sum rules and by imposing a value for the s parameter estimated from the underlying technicolor theory t... | [['i', 'report', 'on', 'our', 'construction', 'and', 'analysis', 'of', 'the', 'effective', 'low', 'energy', 'lagrangian', 'for', 'the', 'minimal', 'walking', 'technicolor', 'mwt', 'model', 'the', 'parameters', 'of', 'the', 'effective', 'lagrangian', 'are', 'constrained', 'by', 'imposing', 'modified', 'weinberg', 'sum',... | [-0.10752552331957434, 0.19192106784508464, -0.056586160743609074, 0.11124597077390977, -0.11832902175041714, -0.15311236329642788, 0.09008626927721447, 0.27830472245945465, -0.21107751264103822, -0.3581298573740891, 0.09427805613293978, -0.21305791899649193, -0.10359925547880786, 0.091706359975173, -0.0030726370933864... |
710.4334 | Local bulk operators in AdS/CFT and the fate of the BTZ singularity | This paper has two parts. First we review the description of local bulk
operators in Lorentzian AdS in terms of non-local operators in the boundary
CFT. We discuss how bulk locality arises in pure AdS backgrounds and how it is
modified at finite N. Next we present some new results on BTZ black holes:
local operators ... | hep-th | this paper has two parts first we review the description of local bulk operators in lorentzian ads in terms of nonlocal operators in the boundary cft we discuss how bulk locality arises in pure ads backgrounds and how it is modified at finite n next we present some new results on btz black holes local operators can be ... | [['this', 'paper', 'has', 'two', 'parts', 'first', 'we', 'review', 'the', 'description', 'of', 'local', 'bulk', 'operators', 'in', 'lorentzian', 'ads', 'in', 'terms', 'of', 'nonlocal', 'operators', 'in', 'the', 'boundary', 'cft', 'we', 'discuss', 'how', 'bulk', 'locality', 'arises', 'in', 'pure', 'ads', 'backgrounds', ... | [-0.15733422835752287, 0.13276810252057697, -0.09141479199752212, 0.10576149539860047, -0.06967006514162716, -0.13790490319344983, -0.015057395421140625, 0.2832206108242921, -0.16347232609278645, -0.23540954646128026, 0.06940252361085225, -0.3637559712236828, -0.1353799048735274, 0.13538522880686366, -0.114520943095988... |
710.4335 | Denominators of cluster variables | Associated to any acyclic cluster algebra is a corresponding triangulated
category known as the cluster category. It is known that there is a one-to-one
correspondence between cluster variables in the cluster algebra and exceptional
indecomposable objects in the cluster category inducing a correspondence
between clus... | math.RT math.RA | associated to any acyclic cluster algebra is a corresponding triangulated category known as the cluster category it is known that there is a onetoone correspondence between cluster variables in the cluster algebra and exceptional indecomposable objects in the cluster category inducing a correspondence between clusters ... | [['associated', 'to', 'any', 'acyclic', 'cluster', 'algebra', 'is', 'a', 'corresponding', 'triangulated', 'category', 'known', 'as', 'the', 'cluster', 'category', 'it', 'is', 'known', 'that', 'there', 'is', 'a', 'onetoone', 'correspondence', 'between', 'cluster', 'variables', 'in', 'the', 'cluster', 'algebra', 'and', '... | [-0.1551309922694141, 0.0682362029259292, -0.11242672751068623, 0.061638248885352895, -0.10494381612421483, -0.11751622141490126, 0.014471844929214725, 0.37724543660262233, -0.37914059058022803, -0.23947175489499783, 0.09447169742789756, -0.18560221902707702, -0.11984627263503085, 0.15069450569561976, -0.12392569930316... |
710.4336 | Highly Anisotropic Vorticity Aligned Structures in a Shear Thickening
Attractive Colloidal System | Vorticity aligned cylindrical flocs of carbon black particles are coincident
with a primary shear thickening transition in steady flow and also appear as
transient structures in the flow response of gels produced by a secondary shear
thickening at high shear rates.
| cond-mat.soft | vorticity aligned cylindrical flocs of carbon black particles are coincident with a primary shear thickening transition in steady flow and also appear as transient structures in the flow response of gels produced by a secondary shear thickening at high shear rates | [['vorticity', 'aligned', 'cylindrical', 'flocs', 'of', 'carbon', 'black', 'particles', 'are', 'coincident', 'with', 'a', 'primary', 'shear', 'thickening', 'transition', 'in', 'steady', 'flow', 'and', 'also', 'appear', 'as', 'transient', 'structures', 'in', 'the', 'flow', 'response', 'of', 'gels', 'produced', 'by', 'a'... | [-0.1985568672236873, 0.27955098936288825, -0.07196864282439758, -0.025344270781227727, 0.01985146468732415, -0.10813626196099127, -0.08059157063139648, 0.3796908966061182, -0.3036308502778411, -0.20714727153706297, 0.07218022721183555, -0.2706752524870198, -0.12453407021920855, 0.1316526848822832, 0.002720167088072474... |
710.4337 | Parametrically Shielding Electromagnetic Fields by Nonlinear
Metamaterials | An analytical theory is developed for parametric interactions in metamaterial
multilayer structures with simultaneous nonlinear electronic and magnetic
responses and with near-zero refractive-index. We demonstrate theoretically
that electromagnetic fields of certain frequencies can be parametrically
shielded by a non... | cond-mat.mtrl-sci | an analytical theory is developed for parametric interactions in metamaterial multilayer structures with simultaneous nonlinear electronic and magnetic responses and with nearzero refractiveindex we demonstrate theoretically that electromagnetic fields of certain frequencies can be parametrically shielded by a nonlinea... | [['an', 'analytical', 'theory', 'is', 'developed', 'for', 'parametric', 'interactions', 'in', 'metamaterial', 'multilayer', 'structures', 'with', 'simultaneous', 'nonlinear', 'electronic', 'and', 'magnetic', 'responses', 'and', 'with', 'nearzero', 'refractiveindex', 'we', 'demonstrate', 'theoretically', 'that', 'electr... | [-0.14907868089850504, 0.24095541105803803, -0.0033020820507469275, 0.0024032500487836924, -0.12960559629712892, -0.1466722215873876, -0.03823793411955727, 0.4535926464343011, -0.23972320774889955, -0.28092888690004447, 0.05350841537254364, -0.2866553882833081, -0.19571831808049195, 0.20635992516246107, 0.0287146231234... |
710.4338 | Stability of atoms and molecules in an ultrarelativistic
Thomas-Fermi-Weizsaecker model | We consider the zero mass limit of a relativistic Thomas-Fermi-Weizsaecker
model of atoms and molecules. We find bounds for the critical nuclear charges
that ensure stability.
| math-ph math.MP math.SP | we consider the zero mass limit of a relativistic thomasfermiweizsaecker model of atoms and molecules we find bounds for the critical nuclear charges that ensure stability | [['we', 'consider', 'the', 'zero', 'mass', 'limit', 'of', 'a', 'relativistic', 'thomasfermiweizsaecker', 'model', 'of', 'atoms', 'and', 'molecules', 'we', 'find', 'bounds', 'for', 'the', 'critical', 'nuclear', 'charges', 'that', 'ensure', 'stability']] | [-0.1303029352426529, 0.1804794943332672, -0.05685054801404476, 0.09770611055195332, 0.08189407460391522, -0.11924775267019867, 0.11336950972676277, 0.2901538357138634, -0.16083223208785058, -0.2599584586918354, 0.046774284802377226, -0.289025512188673, -0.026438426151871683, 0.1175401911046356, 0.029426499772816896, 0... |
710.4339 | Heavy-Quark Masses from the Fermilab Method in Three-Flavor Lattice QCD | We report on heavy quark mass calculations using Fermilab heavy quarks.
Lattice calculations of heavy-strange meson masses are combined with one-loop
(automated) lattice perturbation theory to arrive at the quark mass. Mesons are
constructed from Fermilab heavy quarks and staggered light quarks. We use the
MILC ensem... | hep-lat | we report on heavy quark mass calculations using fermilab heavy quarks lattice calculations of heavystrange meson masses are combined with oneloop automated lattice perturbation theory to arrive at the quark mass mesons are constructed from fermilab heavy quarks and staggered light quarks we use the milc ensembles at t... | [['we', 'report', 'on', 'heavy', 'quark', 'mass', 'calculations', 'using', 'fermilab', 'heavy', 'quarks', 'lattice', 'calculations', 'of', 'heavystrange', 'meson', 'masses', 'are', 'combined', 'with', 'oneloop', 'automated', 'lattice', 'perturbation', 'theory', 'to', 'arrive', 'at', 'the', 'quark', 'mass', 'mesons', 'a... | [-0.026773271477454667, 0.42368626504434975, -0.08344720186689844, 0.12304662270834307, 0.004439461613436798, -0.12112965664596527, 0.1544234543697086, 0.4163063017578868, -0.08130190715604982, -0.2311005185467082, -0.05005585397563439, -0.40353632016808955, 0.13238487407178073, 0.05883971452954915, 0.06982615636056894... |
710.434 | Differential characters as stacks and prequantization | We generalize geometric prequantization of symplectic manifolds to
differentiable stacks. Our approach is atlas-independent and provides a
bijection between isomorphism classes of principal circle bundles (with or
without connections) and second cohomology groups of certain chain complexes.
| math.DG math.RT math.SG | we generalize geometric prequantization of symplectic manifolds to differentiable stacks our approach is atlasindependent and provides a bijection between isomorphism classes of principal circle bundles with or without connections and second cohomology groups of certain chain complexes | [['we', 'generalize', 'geometric', 'prequantization', 'of', 'symplectic', 'manifolds', 'to', 'differentiable', 'stacks', 'our', 'approach', 'is', 'atlasindependent', 'and', 'provides', 'a', 'bijection', 'between', 'isomorphism', 'classes', 'of', 'principal', 'circle', 'bundles', 'with', 'or', 'without', 'connections', ... | [-0.26669265604060555, 0.009431090870445283, -0.07474484310174982, 0.08834752704650681, -0.15831199914423955, -0.1762202965069769, 0.006855454166523284, 0.43676480482746327, -0.3612211142252717, -0.2759426628342933, 0.06602283677137974, -0.2176526681707603, -0.19614929039057138, 0.15964976531944963, -0.2296397171707617... |
710.4341 | Pressure effects in the triangular layered cobaltites NaxCoO2 | We have measured transport properties as a function of temperature and
pressure up to 30GPa in the NaxCoO2 system. For the x=0.5 sample the transition
temperature at 53K increases with pressure, while paradoxically the sample
passes from an insulating to a metallic ground state. A similar transition is
observed in th... | cond-mat.str-el | we have measured transport properties as a function of temperature and pressure up to 30gpa in the naxcoo2 system for the x05 sample the transition temperature at 53k increases with pressure while paradoxically the sample passes from an insulating to a metallic ground state a similar transition is observed in the x031 ... | [['we', 'have', 'measured', 'transport', 'properties', 'as', 'a', 'function', 'of', 'temperature', 'and', 'pressure', 'up', 'to', '30gpa', 'in', 'the', 'naxcoo2', 'system', 'for', 'the', 'x05', 'sample', 'the', 'transition', 'temperature', 'at', '53k', 'increases', 'with', 'pressure', 'while', 'paradoxically', 'the', '... | [-0.0928344040897043, 0.17071265116135778, -0.07550741556735288, -0.035345406275674965, 0.02974678873683193, -0.05755188533415397, 0.1429630370943674, 0.4037493168420735, -0.26751991394641145, -0.32849335149374037, 0.04347722338362863, -0.3813591468303154, -0.05648511023970232, 0.15326812938742695, 0.029891921185134424... |
710.4342 | D=11 massless superparticle covariant quantization, pure spinor BRST
charge and hidden symmetries | We consider the covariant quantization of the D=11 massless superparticle
(M0-brane) in the spinor moving frame or twistor-like Lorentz harmonics
formulation. The action involves the set of 16 constrained 32 component
Majorana spinors, the spinor Lorentz harmonics parametrizing (as homogeneous
coordinates, modulo gau... | hep-th | we consider the covariant quantization of the d11 massless superparticle m0brane in the spinor moving frame or twistorlike lorentz harmonics formulation the action involves the set of 16 constrained 32 component majorana spinors the spinor lorentz harmonics parametrizing as homogeneous coordinates modulo gauge symmetri... | [['we', 'consider', 'the', 'covariant', 'quantization', 'of', 'the', 'd11', 'massless', 'superparticle', 'm0brane', 'in', 'the', 'spinor', 'moving', 'frame', 'or', 'twistorlike', 'lorentz', 'harmonics', 'formulation', 'the', 'action', 'involves', 'the', 'set', 'of', '16', 'constrained', '32', 'component', 'majorana', '... | [-0.18042260718703756, 0.15344619783935706, -0.07085266270754391, 0.07338288659784234, -0.13372161601835386, -0.12617815544554617, 0.005250353729367474, 0.28135288140516795, -0.2248807302838984, -0.2471737517890605, 0.04569105403114804, -0.21014884793310723, -0.14926876402681782, 0.05830540686837716, -0.063597832294382... |
710.4343 | Matrix equations and trilinear commutation relations | In this paper we discuss a general algebraic approach to treating static
equations of matrix models with a mass-like term. In this approach the
equations of motions are considered as consequence of parafermi-like trilinear
commutation relations. In this context we consider several solutions, including
construction of... | hep-th math-ph math.MP | in this paper we discuss a general algebraic approach to treating static equations of matrix models with a masslike term in this approach the equations of motions are considered as consequence of parafermilike trilinear commutation relations in this context we consider several solutions including construction of noncom... | [['in', 'this', 'paper', 'we', 'discuss', 'a', 'general', 'algebraic', 'approach', 'to', 'treating', 'static', 'equations', 'of', 'matrix', 'models', 'with', 'a', 'masslike', 'term', 'in', 'this', 'approach', 'the', 'equations', 'of', 'motions', 'are', 'considered', 'as', 'consequence', 'of', 'parafermilike', 'trilinea... | [-0.17690933898224362, 0.11091918707825243, -0.056680940507378964, 0.10528382059835296, -0.07530216636535313, -0.10262173648724067, -0.015654164272876057, 0.30136247045759645, -0.27436439007786767, -0.2573684227785894, 0.07740553147700016, -0.26812956460552023, -0.21194640975279203, 0.14555772879560078, -0.093835130067... |
710.4344 | Black Hole Bound on the Number of Species and Quantum Gravity at LHC | In theories with a large number N of particle species, black hole physics
imposes an upper bound on the mass of the species equal to M_{Planck}/\sqrt{N}.
This bound suggests a novel solution to the hierarchy problem in which there
are N \approx 10^{32} gravitationally coupled species, for example 10^{32}
copies of th... | hep-th hep-ph | in theories with a large number n of particle species black hole physics imposes an upper bound on the mass of the species equal to m_plancksqrtn this bound suggests a novel solution to the hierarchy problem in which there are n approx 1032 gravitationally coupled species for example 1032 copies of the standard model t... | [['in', 'theories', 'with', 'a', 'large', 'number', 'n', 'of', 'particle', 'species', 'black', 'hole', 'physics', 'imposes', 'an', 'upper', 'bound', 'on', 'the', 'mass', 'of', 'the', 'species', 'equal', 'to', 'm_plancksqrtn', 'this', 'bound', 'suggests', 'a', 'novel', 'solution', 'to', 'the', 'hierarchy', 'problem', 'i... | [-0.12276256132892446, 0.19965878952601776, -0.06302623451025241, 0.1260140697415272, -0.0481856060833428, -0.1569979535079308, 0.036097149959512354, 0.2704269606673907, -0.20016837510081126, -0.3446955514447279, 0.07024667287013908, -0.30361915612054957, -0.05663687514539571, 0.17405408573393424, 0.004980526052986008,... |
710.4345 | A Primer for Black Hole Quantum Physics | The mechanisms which give rise to Hawking radiation are revealed by analyzing
in detail pair production in the presence of horizons. In preparation for the
black hole problem, three preparatory problems are dwelt with at length: pair
production in an external electric field, thermalization of a uniformly
accelerated ... | gr-qc hep-th | the mechanisms which give rise to hawking radiation are revealed by analyzing in detail pair production in the presence of horizons in preparation for the black hole problem three preparatory problems are dwelt with at length pair production in an external electric field thermalization of a uniformly accelerated detect... | [['the', 'mechanisms', 'which', 'give', 'rise', 'to', 'hawking', 'radiation', 'are', 'revealed', 'by', 'analyzing', 'in', 'detail', 'pair', 'production', 'in', 'the', 'presence', 'of', 'horizons', 'in', 'preparation', 'for', 'the', 'black', 'hole', 'problem', 'three', 'preparatory', 'problems', 'are', 'dwelt', 'with', ... | [-0.11603337348542098, 0.15881921880691793, -0.10935791676159387, 0.10521359762781006, -0.04741627515562561, -0.1316203576460166, -0.000781204493660611, 0.2962995388505744, -0.22343186701936515, -0.27671886319753675, 0.08230080538087862, -0.3284851820478675, -0.09175113147832978, 0.20729273179190194, -0.056314196650752... |
710.4346 | Ehrhart polynomials of matroid polytopes and polymatroids | We investigate properties of Ehrhart polynomials for matroid polytopes,
independence matroid polytopes, and polymatroids. In the first half of the
paper we prove that for fixed rank their Ehrhart polynomials are computable in
polynomial time. The proof relies on the geometry of these polytopes as well as
a new refine... | math.CO | we investigate properties of ehrhart polynomials for matroid polytopes independence matroid polytopes and polymatroids in the first half of the paper we prove that for fixed rank their ehrhart polynomials are computable in polynomial time the proof relies on the geometry of these polytopes as well as a new refined anal... | [['we', 'investigate', 'properties', 'of', 'ehrhart', 'polynomials', 'for', 'matroid', 'polytopes', 'independence', 'matroid', 'polytopes', 'and', 'polymatroids', 'in', 'the', 'first', 'half', 'of', 'the', 'paper', 'we', 'prove', 'that', 'for', 'fixed', 'rank', 'their', 'ehrhart', 'polynomials', 'are', 'computable', 'i... | [-0.17259901713953504, 0.004739607099530308, -0.09093804154978243, 0.10622855369543094, -0.11198465603804432, -0.10134433176866624, 0.0458476074401365, 0.3196324917466141, -0.35386224783047343, -0.20283524299495267, 0.1627595402868221, -0.24342568193800573, -0.20579668696493256, 0.15845005950608917, -0.1505906516577788... |
710.4347 | Multiplicative bijections of semigroups of interval-valued continuous
functions | We characterize all compact and Hausdorff spaces $X$ which satisfy that for
every multiplicative bijection $\phi$ on $C(X, I)$, there exist a homeomorphism
$\mu : X \to X$ and a continuous map $p: X \to (0, +\infty)$ such that $$\phi
(f) (x) = f(\mu (x))^{p(x)}$$ for every $f \in C(X,I)$ and $x \in X$. This
allows us... | math.FA math.GN | we characterize all compact and hausdorff spaces x which satisfy that for every multiplicative bijection phi on cx i there exist a homeomorphism mu x to x and a continuous map p x to 0 infty such that phi f x fmu xpx for every f in cxi and x in x this allows us to disprove a conjecture of marovt proc amer math soc bf 1... | [['we', 'characterize', 'all', 'compact', 'and', 'hausdorff', 'spaces', 'x', 'which', 'satisfy', 'that', 'for', 'every', 'multiplicative', 'bijection', 'phi', 'on', 'cx', 'i', 'there', 'exist', 'a', 'homeomorphism', 'mu', 'x', 'to', 'x', 'and', 'a', 'continuous', 'map', 'p', 'x', 'to', '0', 'infty', 'such', 'that', 'ph... | [-0.17789572027594416, 0.07755417438058913, -0.04580594492557494, 0.028330345607150486, -0.03172943495284719, -0.17509911009523121, 0.0918680035031719, 0.3889553545019295, -0.3121881050520423, -0.1619537064357649, 0.022880322080329533, -0.31619700062684747, -0.12817513461731658, 0.20689918790484155, -0.1399779974768834... |
710.4348 | Boundary Entropy Can Increase Under Bulk RG Flow | The boundary entropy log(g) of a critical one-dimensional quantum system (or
two-dimensional conformal field theory) is known to decrease under
renormalization group (RG) flow of the boundary theory. We study instead the
behavior of the boundary entropy as the bulk theory flows between two nearby
critical points. We ... | hep-th cond-mat.stat-mech | the boundary entropy logg of a critical onedimensional quantum system or twodimensional conformal field theory is known to decrease under renormalization group rg flow of the boundary theory we study instead the behavior of the boundary entropy as the bulk theory flows between two nearby critical points we use conforma... | [['the', 'boundary', 'entropy', 'logg', 'of', 'a', 'critical', 'onedimensional', 'quantum', 'system', 'or', 'twodimensional', 'conformal', 'field', 'theory', 'is', 'known', 'to', 'decrease', 'under', 'renormalization', 'group', 'rg', 'flow', 'of', 'the', 'boundary', 'theory', 'we', 'study', 'instead', 'the', 'behavior'... | [-0.16607435649244248, 0.18411621879619947, -0.11534103416904275, 0.06337720998895488, -0.0555190971187715, -0.13705312436546332, 0.03511047336360207, 0.29938727218541317, -0.26779479420344743, -0.2794560705411381, 0.08467520976306073, -0.2994592719894302, -0.16052292097343265, 0.136593171468121, -0.08429185726812907, ... |
710.4349 | Notes on axiomatic Gromov--Witten theory and applications | This an expository article on Givental's axiomatic Gromov--Witten theory and
some of its applications.
| math.AG | this an expository article on giventals axiomatic gromovwitten theory and some of its applications | [['this', 'an', 'expository', 'article', 'on', 'giventals', 'axiomatic', 'gromovwitten', 'theory', 'and', 'some', 'of', 'its', 'applications']] | [-0.16419407642180367, -0.07595753193163546, -0.20482035734624202, 0.1549525430808509, -0.12349854383085455, -0.049906731549916525, 0.014192649454344064, 0.24722432970468486, -0.30223945528268814, -0.17151274305901357, 0.0551894698292017, -0.27425550669431686, -0.35270090507609503, 0.20571632430489575, -0.3772642760138... |
710.435 | Why things fall | In this paper we discuss Internal Relativity, a recent program to address the
problem of quantum gravity. In our approach we change the relationship between
spacetime and matter. Currently we view matter as propagating on spacetime.
Einstein's equations encode how spacetime curves due to the presence of matter
and ho... | gr-qc | in this paper we discuss internal relativity a recent program to address the problem of quantum gravity in our approach we change the relationship between spacetime and matter currently we view matter as propagating on spacetime einsteins equations encode how spacetime curves due to the presence of matter and how space... | [['in', 'this', 'paper', 'we', 'discuss', 'internal', 'relativity', 'a', 'recent', 'program', 'to', 'address', 'the', 'problem', 'of', 'quantum', 'gravity', 'in', 'our', 'approach', 'we', 'change', 'the', 'relationship', 'between', 'spacetime', 'and', 'matter', 'currently', 'we', 'view', 'matter', 'as', 'propagating', ... | [-0.16248973247263562, 0.13823076727430103, -0.16613667672597535, 0.105116285337379, -0.11711880813367392, -0.11727684367379827, -0.005005988324699797, 0.3022638192663642, -0.26479246110243343, -0.327457319949973, 0.04029843043560328, -0.23100380518312777, -0.21439723905019892, 0.15796072831613875, -0.10521388205782516... |
710.4351 | Ricci flow and quantum theory | We show some relations between Ricci flow and quantum theory via Fisher
information and the quantum potential.
| math-ph math.MP | we show some relations between ricci flow and quantum theory via fisher information and the quantum potential | [['we', 'show', 'some', 'relations', 'between', 'ricci', 'flow', 'and', 'quantum', 'theory', 'via', 'fisher', 'information', 'and', 'the', 'quantum', 'potential']] | [-0.13192798397229874, 0.13985673343653188, -0.17832984030246735, 0.10202134455389836, -0.0570524631835082, -0.1878033540047267, -0.00225179927998825, 0.3263619094128337, -0.36728908033931956, -0.2430451223078896, 0.07400705268168274, -0.39244038304861856, -0.32471168479498697, 0.20608186897109537, -0.00287353072096319... |
710.4352 | Measurement based entanglement under conditions of extreme photon loss | The act of measuring optical emissions from two remote qubits can entangle
them. By demanding that a photon from each qubit reaches the detectors, one can
ensure than no photon was lost. But the failure rate then rises quadratically
with loss probability. In [1] this resulted in 30 successes per billion
attempts. We ... | quant-ph | the act of measuring optical emissions from two remote qubits can entangle them by demanding that a photon from each qubit reaches the detectors one can ensure than no photon was lost but the failure rate then rises quadratically with loss probability in 1 this resulted in 30 successes per billion attempts we describe ... | [['the', 'act', 'of', 'measuring', 'optical', 'emissions', 'from', 'two', 'remote', 'qubits', 'can', 'entangle', 'them', 'by', 'demanding', 'that', 'a', 'photon', 'from', 'each', 'qubit', 'reaches', 'the', 'detectors', 'one', 'can', 'ensure', 'than', 'no', 'photon', 'was', 'lost', 'but', 'the', 'failure', 'rate', 'then... | [-0.13773275269311852, 0.18761243901401758, -0.005766884371638298, 0.021448651894927024, -0.01001233702711761, -0.19852049198001623, 0.10882138963788748, 0.4043525533620268, -0.24449358972534538, -0.3488804829195142, 0.0581185006427113, -0.3275807325094938, -0.060696199053898454, 0.19591884249448777, -0.098749852899461... |
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