id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
706.1614 | Non-Cooperative Scheduling of Multiple Bag-of-Task Applications | Multiple applications that execute concurrently on heterogeneous platforms
compete for CPU and network resources. In this paper we analyze the behavior of
$K$ non-cooperative schedulers using the optimal strategy that maximize their
efficiency while fairness is ensured at a system level ignoring applications
characte... | cs.DC cs.GT | multiple applications that execute concurrently on heterogeneous platforms compete for cpu and network resources in this paper we analyze the behavior of k noncooperative schedulers using the optimal strategy that maximize their efficiency while fairness is ensured at a system level ignoring applications characteristic... | [['multiple', 'applications', 'that', 'execute', 'concurrently', 'on', 'heterogeneous', 'platforms', 'compete', 'for', 'cpu', 'and', 'network', 'resources', 'in', 'this', 'paper', 'we', 'analyze', 'the', 'behavior', 'of', 'k', 'noncooperative', 'schedulers', 'using', 'the', 'optimal', 'strategy', 'that', 'maximize', 't... | [-0.17479701778789736, 0.03353961132803766, -0.08168758440156837, 0.0472667878661978, -0.04833334365983056, -0.18777925155058234, 0.11638343730501, 0.38774826613266067, -0.28547835059419097, -0.3141346369050892, 0.09834804348100583, -0.25143526909670916, -0.14830188057104865, 0.17845845844173042, -0.11940966960318325, ... |
706.1615 | A mode elimination technique to improve convergence of iteration methods
for finding solitary waves | We extend the key idea behind the generalized Petviashvili method of Ref.
\cite{gP} by proposing a novel technique based on a similar idea. This
technique systematically eliminates from the iteratively obtained solution a
mode that is "responsible" either for the divergence or the slow convergence of
the iterations. ... | nlin.PS | we extend the key idea behind the generalized petviashvili method of ref citegp by proposing a novel technique based on a similar idea this technique systematically eliminates from the iteratively obtained solution a mode that is responsible either for the divergence or the slow convergence of the iterations we demonst... | [['we', 'extend', 'the', 'key', 'idea', 'behind', 'the', 'generalized', 'petviashvili', 'method', 'of', 'ref', 'citegp', 'by', 'proposing', 'a', 'novel', 'technique', 'based', 'on', 'a', 'similar', 'idea', 'this', 'technique', 'systematically', 'eliminates', 'from', 'the', 'iteratively', 'obtained', 'solution', 'a', 'm... | [-0.05141696082348497, 0.05625359402794359, -0.15056090525741506, 0.11392932403812774, -0.0572445832638659, -0.11926364877189581, 0.062294242147388115, 0.3514298060351712, -0.3015594014372581, -0.2614621774285522, 0.11655437216286062, -0.2161603101537141, -0.20885614568415362, 0.21876745117016327, -0.03899673802945285,... |
706.1616 | Generalized DMPK equation for strongly localized regime - numerical
solution | Generalized Dorokhov-Mello-Pereyra-Kumar (GDMPK) equation [K. A. Muttalib and
J. R. Klauder, Phys. Rev. Lett. {\bf 82}, 4272 (1999)] has been proposed for
the description of the electron transport in strongly localized systems. We
develop an algorithm for the numerical solution of this equation and confirm
that GDMPK... | cond-mat.mes-hall | generalized dorokhovmellopereyrakumar gdmpk equation k a muttalib and j r klauder phys rev lett bf 82 4272 1999 has been proposed for the description of the electron transport in strongly localized systems we develop an algorithm for the numerical solution of this equation and confirm that gdmpk equation correctly desc... | [['generalized', 'dorokhovmellopereyrakumar', 'gdmpk', 'equation', 'k', 'a', 'muttalib', 'and', 'j', 'r', 'klauder', 'phys', 'rev', 'lett', 'bf', '82', '4272', '1999', 'has', 'been', 'proposed', 'for', 'the', 'description', 'of', 'the', 'electron', 'transport', 'in', 'strongly', 'localized', 'systems', 'we', 'develop',... | [-0.13569893065529565, 0.05221708757873987, -0.07062917289634546, -0.023317992797173146, -0.021832737259359823, -0.14918463219267628, 0.016174134384426806, 0.2648863138475766, -0.21253719891214537, -0.28044121346126, 0.019356493530277578, -0.314336963949932, -0.19371240825081865, 0.18953246306627988, -0.042258316340545... |
706.1617 | Relative Strength of Strategy Elimination Procedures | We compare here the relative strength of four widely used procedures on
finite strategic games: iterated elimination of weakly/strictly dominated
strategies by a pure/mixed strategy. A complication is that none of these
procedures is based on a monotonic operator. To deal with this problem we use
'global' versions of... | cs.GT | we compare here the relative strength of four widely used procedures on finite strategic games iterated elimination of weaklystrictly dominated strategies by a puremixed strategy a complication is that none of these procedures is based on a monotonic operator to deal with this problem we use global versions of these op... | [['we', 'compare', 'here', 'the', 'relative', 'strength', 'of', 'four', 'widely', 'used', 'procedures', 'on', 'finite', 'strategic', 'games', 'iterated', 'elimination', 'of', 'weaklystrictly', 'dominated', 'strategies', 'by', 'a', 'puremixed', 'strategy', 'a', 'complication', 'is', 'that', 'none', 'of', 'these', 'proce... | [-0.06825500135595093, 0.054396423948358516, -0.1227746529086512, 0.1085665887530551, -0.059087389134516825, -0.13628411934026802, 0.08809254145515817, 0.4234351517290485, -0.2637900138387875, -0.23170962445057777, 0.14243352122376768, -0.24458842538297176, -0.17900939817939485, 0.18620198531722537, -0.1342783868312835... |
706.1618 | The fluctuation spectra around a Gaussian classical solution of a tensor
model and the general relativity | Tensor models can be interpreted as theory of dynamical fuzzy spaces. In this
paper, I study numerically the fluctuation spectra around a Gaussian classical
solution of a tensor model, which represents a fuzzy flat space in arbitrary
dimensions. It is found that the momentum distribution of the low-lying
low-momentum... | hep-th gr-qc | tensor models can be interpreted as theory of dynamical fuzzy spaces in this paper i study numerically the fluctuation spectra around a gaussian classical solution of a tensor model which represents a fuzzy flat space in arbitrary dimensions it is found that the momentum distribution of the lowlying lowmomentum spectra... | [['tensor', 'models', 'can', 'be', 'interpreted', 'as', 'theory', 'of', 'dynamical', 'fuzzy', 'spaces', 'in', 'this', 'paper', 'i', 'study', 'numerically', 'the', 'fluctuation', 'spectra', 'around', 'a', 'gaussian', 'classical', 'solution', 'of', 'a', 'tensor', 'model', 'which', 'represents', 'a', 'fuzzy', 'flat', 'spa... | [-0.11251292743784662, 0.11983713716969337, -0.12352638485574044, 0.09930426852966631, -0.00386855458969822, -0.11990749572823285, -0.06142832545475979, 0.31559765928120603, -0.23558091906148312, -0.25317059666042835, 0.05172467874801063, -0.2573408445269607, -0.18592515422981049, 0.11934283891886399, -0.03119801576733... |
706.1619 | Alternative linear structures for classical and quantum systems | The possibility of deforming the (associative or Lie) product to obtain
alternative descriptions for a given classical or quantum system has been
considered in many papers. Here we discuss the possibility of obtaining some
novel alternative descriptions by changing the linear structure instead. In
particular we show ... | quant-ph | the possibility of deforming the associative or lie product to obtain alternative descriptions for a given classical or quantum system has been considered in many papers here we discuss the possibility of obtaining some novel alternative descriptions by changing the linear structure instead in particular we show how it... | [['the', 'possibility', 'of', 'deforming', 'the', 'associative', 'or', 'lie', 'product', 'to', 'obtain', 'alternative', 'descriptions', 'for', 'a', 'given', 'classical', 'or', 'quantum', 'system', 'has', 'been', 'considered', 'in', 'many', 'papers', 'here', 'we', 'discuss', 'the', 'possibility', 'of', 'obtaining', 'som... | [-0.12430470320396125, 0.09288800484720477, -0.08647811319679022, 0.07476531201534255, -0.14532192090069349, -0.16888311188250674, 0.021065871240043978, 0.3391648895471831, -0.33462730983606065, -0.24153930435993903, 0.08267441776664576, -0.2126080764387295, -0.16674214779105, 0.20290739013251127, -0.09198060012773944,... |
706.162 | High-quality all-oxide Schottky junctions fabricated on heavily Nb-doped
SrTiO3 substrates | We present a detailed investigation of the electrical properties of epitaxial
La0.7Sr0.3MnO3/SrTi0.98Nb0.02O3 Schottky junctions. A fabrication process that
allows reduction of the junction dimensions to current electronic device size
has been employed. A heavily doped semiconductor has been used as a substrate
in or... | cond-mat.str-el | we present a detailed investigation of the electrical properties of epitaxial la07sr03mno3srti098nb002o3 schottky junctions a fabrication process that allows reduction of the junction dimensions to current electronic device size has been employed a heavily doped semiconductor has been used as a substrate in order to su... | [['we', 'present', 'a', 'detailed', 'investigation', 'of', 'the', 'electrical', 'properties', 'of', 'epitaxial', 'la07sr03mno3srti098nb002o3', 'schottky', 'junctions', 'a', 'fabrication', 'process', 'that', 'allows', 'reduction', 'of', 'the', 'junction', 'dimensions', 'to', 'current', 'electronic', 'device', 'size', 'h... | [-0.18285956667386927, 0.07230198283214122, -0.032869297498837116, -0.02966008891442016, -0.05352870078932028, -0.2063196867587976, 0.07942941516666906, 0.44676946895197034, -0.187631532875821, -0.28044822425581517, -0.03447725892474409, -0.3230303228165212, -0.1443749008467421, 0.2845868724049069, -0.04370349522214382... |
706.1621 | Effective equidistribution of S-integral points on symmetric varieties | Let K be a global field of characteristic not 2. Let Z be a symmetric variety
defined over K and S a finite set of places of K. We obtain counting and
equidistribution results for the S-integral points of Z. Our results are
effective when K is a number field.
| math.NT math.MG | let k be a global field of characteristic not 2 let z be a symmetric variety defined over k and s a finite set of places of k we obtain counting and equidistribution results for the sintegral points of z our results are effective when k is a number field | [['let', 'k', 'be', 'a', 'global', 'field', 'of', 'characteristic', 'not', '2', 'let', 'z', 'be', 'a', 'symmetric', 'variety', 'defined', 'over', 'k', 'and', 's', 'a', 'finite', 'set', 'of', 'places', 'of', 'k', 'we', 'obtain', 'counting', 'and', 'equidistribution', 'results', 'for', 'the', 'sintegral', 'points', 'of',... | [-0.2344003670848906, 0.14447837855666876, -0.1288931253552437, -0.05304484757361934, -0.048506807312369345, -0.15240566182881593, 0.079162317533046, 0.30128452070057393, -0.2542470100522041, -0.2895565143227577, 0.0615304197743535, -0.2549339639022946, -0.03994311839342117, 0.2585452578496188, -0.0029597891494631766, ... |
706.1622 | Out-of-equilibrium tricritical point in a system with long-range
interactions | Systems with long-range interactions display a short-time relaxation towards
Quasi Stationary States (QSSs) whose lifetime increases with system size. With
reference to the Hamiltonian Mean Field (HMF) model, we here show that a
maximum entropy principle, based on Lynden-Bell's pioneering idea of "violent
relaxation"... | cond-mat.stat-mech | systems with longrange interactions display a shorttime relaxation towards quasi stationary states qsss whose lifetime increases with system size with reference to the hamiltonian mean field hmf model we here show that a maximum entropy principle based on lyndenbells pioneering idea of violent relaxation predicts the p... | [['systems', 'with', 'longrange', 'interactions', 'display', 'a', 'shorttime', 'relaxation', 'towards', 'quasi', 'stationary', 'states', 'qsss', 'whose', 'lifetime', 'increases', 'with', 'system', 'size', 'with', 'reference', 'to', 'the', 'hamiltonian', 'mean', 'field', 'hmf', 'model', 'we', 'here', 'show', 'that', 'a'... | [-0.16697615586699696, 0.25479134122123875, -0.10650448201474128, 0.03744160730942844, -0.007326543006464976, -0.16316683690807005, 0.0615436833473606, 0.347424652008767, -0.2526316970011108, -0.2708226229115432, 0.04983103667907075, -0.27889666371389266, -0.08449997956898712, 0.11177750218898878, 0.0861282593574588, 0... |
706.1623 | Angular momentum conservation and torsional oscillations in the Sun and
solar-like stars | The solar torsional oscillations, i.e., the perturbations of the angular
velocity of rotation associated with the eleven-year activity cycle, are a
manifestation of the interaction among the interior magnetic fields, amplified
and modulated by the solar dynamo, and rotation, meridional flow and turbulent
thermal tran... | astro-ph | the solar torsional oscillations ie the perturbations of the angular velocity of rotation associated with the elevenyear activity cycle are a manifestation of the interaction among the interior magnetic fields amplified and modulated by the solar dynamo and rotation meridional flow and turbulent thermal transport there... | [['the', 'solar', 'torsional', 'oscillations', 'ie', 'the', 'perturbations', 'of', 'the', 'angular', 'velocity', 'of', 'rotation', 'associated', 'with', 'the', 'elevenyear', 'activity', 'cycle', 'are', 'a', 'manifestation', 'of', 'the', 'interaction', 'among', 'the', 'interior', 'magnetic', 'fields', 'amplified', 'and'... | [-0.16249487400320153, 0.20080479812737217, -0.07440494321511529, 0.08792216860597217, -0.09478964424887372, -0.028807038274188075, 0.013219975680488372, 0.31994163034664047, -0.2657872813569772, -0.3359017206521164, 0.072491098935115, -0.24493431190269127, -0.11793294534060894, 0.2397757116019831, -0.03325859044871909... |
706.1624 | Some notes concerning the prediction of the amplitude of the two solar
activity cycles | The parameter G, which is determined from the general number of sunspots
groups Ng according to the daily observations G=Sum(1/Ng)^2, is offered. This
parameter is calculated for the days when there is at least one sunspots group.
It characterizes the minimum epoch solar activity. Parameter G mounts to the
maximum du... | astro-ph | the parameter g which is determined from the general number of sunspots groups ng according to the daily observations gsum1ng2 is offered this parameter is calculated for the days when there is at least one sunspots group it characterizes the minimum epoch solar activity parameter g mounts to the maximum during the epo... | [['the', 'parameter', 'g', 'which', 'is', 'determined', 'from', 'the', 'general', 'number', 'of', 'sunspots', 'groups', 'ng', 'according', 'to', 'the', 'daily', 'observations', 'gsum1ng2', 'is', 'offered', 'this', 'parameter', 'is', 'calculated', 'for', 'the', 'days', 'when', 'there', 'is', 'at', 'least', 'one', 'sunsp... | [-0.15461749252676965, 0.21800449586566537, -0.030078007308766246, 0.07475864603184164, -0.09312721464876085, -0.0571089621335268, 0.07798378862440586, 0.3458744054399431, -0.21604435791820287, -0.3996528035402298, 0.12410512228403241, -0.2791783019155264, -0.13385313751548528, 0.1935659731030464, -0.10084614270925522,... |
706.1625 | Small values of Lusternik-Schnirelmann and systolic categories for
manifolds | We prove that manifolds of Lusternik-Schnirelmann category 2 necessarily have
free fundamental group. We thus settle a 1992 conjecture of Gomez-Larranaga and
Gonzalez-Acuna, by generalizing their result in dimension 3, to all higher
dimensions. We examine its ramifications in systolic topology, and provide a
sufficie... | math.AT math.DG | we prove that manifolds of lusternikschnirelmann category 2 necessarily have free fundamental group we thus settle a 1992 conjecture of gomezlarranaga and gonzalezacuna by generalizing their result in dimension 3 to all higher dimensions we examine its ramifications in systolic topology and provide a sufficient conditi... | [['we', 'prove', 'that', 'manifolds', 'of', 'lusternikschnirelmann', 'category', '2', 'necessarily', 'have', 'free', 'fundamental', 'group', 'we', 'thus', 'settle', 'a', '1992', 'conjecture', 'of', 'gomezlarranaga', 'and', 'gonzalezacuna', 'by', 'generalizing', 'their', 'result', 'in', 'dimension', '3', 'to', 'all', 'h... | [-0.16451362696560948, 0.09979853056032549, -0.07605695501816544, 0.09441774137826128, -0.045544796318493105, -0.1780919297174974, 0.04896557843312621, 0.3281658161092888, -0.22626935473897242, -0.2917743155224757, 0.15528514722616157, -0.15527281797999007, -0.1633037128231742, 0.21525552276606588, -0.18974601695822044... |
706.1626 | Near-Infrared Polarimetry of the Eagle Nebula (M16) | We carried out deep and wide (about 8' x 8') JHKs imaging polarimetry in the
southern region of the Eagle Nebula (M16). The polarization intensity map
reveals that two YSOs with near-IR reflection nebulae are located at the tips
of two famous molecular pillars (Pillars 1 and 2) facing toward the exciting
stars of M16... | astro-ph | we carried out deep and wide about 8 x 8 jhks imaging polarimetry in the southern region of the eagle nebula m16 the polarization intensity map reveals that two ysos with nearir reflection nebulae are located at the tips of two famous molecular pillars pillars 1 and 2 facing toward the exciting stars of m16 the centros... | [['we', 'carried', 'out', 'deep', 'and', 'wide', 'about', '8', 'x', '8', 'jhks', 'imaging', 'polarimetry', 'in', 'the', 'southern', 'region', 'of', 'the', 'eagle', 'nebula', 'm16', 'the', 'polarization', 'intensity', 'map', 'reveals', 'that', 'two', 'ysos', 'with', 'nearir', 'reflection', 'nebulae', 'are', 'located', '... | [-0.10276689867861569, 0.10445510050281882, -0.0560850970633328, 0.024712229343131185, -0.07430956067144871, -0.06568257891759276, -0.007988806806504727, 0.4770158930420876, -0.23373959778994322, -0.3069068825989962, 0.06434253150131554, -0.3101022686064243, -0.05921330164000392, 0.18249353079497815, 0.0057646643200423... |
706.1627 | Rectified momentum transport for a kicked Bose-Einstein Condensate | We report the experimental observation of rectified momentum transport for a
Bose-Einstein Condensate kicked at the Talbot time (quantum resonance) by an
optical standing wave. Atoms are initially prepared in a superposition of the 0
and -2*hbar*kl momentum states using an optical pi/2 pulse. By changing the
relative... | quant-ph | we report the experimental observation of rectified momentum transport for a boseeinstein condensate kicked at the talbot time quantum resonance by an optical standing wave atoms are initially prepared in a superposition of the 0 and 2hbarkl momentum states using an optical pi2 pulse by changing the relative phase of t... | [['we', 'report', 'the', 'experimental', 'observation', 'of', 'rectified', 'momentum', 'transport', 'for', 'a', 'boseeinstein', 'condensate', 'kicked', 'at', 'the', 'talbot', 'time', 'quantum', 'resonance', 'by', 'an', 'optical', 'standing', 'wave', 'atoms', 'are', 'initially', 'prepared', 'in', 'a', 'superposition', '... | [-0.2238635997481008, 0.28014942186954855, -0.11186687563682293, 0.0055737212888056, -0.02765509994450684, -0.11318302649732043, 0.023932556388899684, 0.39813489989354844, -0.29127846603713387, -0.2304942098207681, 0.02661126493987423, -0.26798928649698545, -0.07215967040690707, 0.19269456289049874, 0.05742595361818264... |
706.1628 | Thermodynamics of pairing in mesoscopic systems | Using numerical and analytical methods implemented for different models we
conduct a systematic study of thermodynamic properties of pairing correlation
in mesoscopic nuclear systems. Various quantities are calculated and analyzed
using the exact solution of pairing. An in-depth comparison of canonical, grand
canonic... | nucl-th | using numerical and analytical methods implemented for different models we conduct a systematic study of thermodynamic properties of pairing correlation in mesoscopic nuclear systems various quantities are calculated and analyzed using the exact solution of pairing an indepth comparison of canonical grand canonical and... | [['using', 'numerical', 'and', 'analytical', 'methods', 'implemented', 'for', 'different', 'models', 'we', 'conduct', 'a', 'systematic', 'study', 'of', 'thermodynamic', 'properties', 'of', 'pairing', 'correlation', 'in', 'mesoscopic', 'nuclear', 'systems', 'various', 'quantities', 'are', 'calculated', 'and', 'analyzed'... | [-0.1826607200622786, 0.11191829222084275, -0.10375186674766072, 0.10343320268910122, 0.01791058934315015, -0.04364124442742185, 0.04734193447991523, 0.32232346635254966, -0.22441894816721697, -0.25270608913523096, 0.04807481869436687, -0.2817401754179301, -0.14903014230733838, 0.15459426807396057, 0.024922016572397388... |
706.1629 | Emergently Thermalized Islands in the Landscape | In this note, we point out that in the eternal inflation driven by the
metastable vacua of the landscape, it might be possible that some large and
local quantum fluctuations with the null energy condition violation can stride
over the barriers between different vacua and straightly create some islands
with radiation ... | gr-qc | in this note we point out that in the eternal inflation driven by the metastable vacua of the landscape it might be possible that some large and local quantum fluctuations with the null energy condition violation can stride over the barriers between different vacua and straightly create some islands with radiation and ... | [['in', 'this', 'note', 'we', 'point', 'out', 'that', 'in', 'the', 'eternal', 'inflation', 'driven', 'by', 'the', 'metastable', 'vacua', 'of', 'the', 'landscape', 'it', 'might', 'be', 'possible', 'that', 'some', 'large', 'and', 'local', 'quantum', 'fluctuations', 'with', 'the', 'null', 'energy', 'condition', 'violation... | [-0.11361271016054102, 0.2722349163083421, -0.14886105462274218, 0.12833512447912573, -0.034860722037482555, -0.15201486471866432, 0.011607302380930428, 0.3401640963095885, -0.24809668769875726, -0.3029673686865103, 0.0976716610193662, -0.2661090201728947, -0.09727151431962029, 0.1728222902127347, -0.058376842184161136... |
706.163 | An analytic study of the ionization from an ultrathin quantum well in a
weak electrostatic field | We consider the time evolution of a particle bound by an attractive
one-dimensional delta-function potential (at x = 0) when a uniform
electrostatic field (F) is applied. We explore explicit expressions for the
time-dependent wavefunction \psi_F(x,t) and the ionization probability
{\mathcal{P}}(t), respectively, in t... | quant-ph | we consider the time evolution of a particle bound by an attractive onedimensional deltafunction potential at x 0 when a uniform electrostatic field f is applied we explore explicit expressions for the timedependent wavefunction psi_fxt and the ionization probability mathcalpt respectively in the weakfield limit in doi... | [['we', 'consider', 'the', 'time', 'evolution', 'of', 'a', 'particle', 'bound', 'by', 'an', 'attractive', 'onedimensional', 'deltafunction', 'potential', 'at', 'x', '0', 'when', 'a', 'uniform', 'electrostatic', 'field', 'f', 'is', 'applied', 'we', 'explore', 'explicit', 'expressions', 'for', 'the', 'timedependent', 'wa... | [-0.134206530336965, 0.0388064447989595, -0.1202401790952567, 0.11738996031786443, -0.054408772005539, -0.1280938163881415, 0.058419031765440416, 0.3790038535371423, -0.2278375457169424, -0.23210962266653198, 0.05209529294696604, -0.25243879771582656, -0.15966986679745004, 0.17200154363647394, 0.0029635314773447043, 0.... |
706.1631 | Action Principle and Algebraic Approach to Gauge Transformations in
Gauge Theories | The action principle is used to derive, by an entirely algebraic approach,
gauge transformations of the full vacuum-to-vacuum transition amplitude
(generating functional) from the Coulomb gauge to arbitrary covariant gauges
and in turn to the celebrated Fock-Schwinger (FS) gauge for the abelian (QED)
gauge theory wit... | hep-th | the action principle is used to derive by an entirely algebraic approach gauge transformations of the full vacuumtovacuum transition amplitude generating functional from the coulomb gauge to arbitrary covariant gauges and in turn to the celebrated fockschwinger fs gauge for the abelian qed gauge theory without recourse... | [['the', 'action', 'principle', 'is', 'used', 'to', 'derive', 'by', 'an', 'entirely', 'algebraic', 'approach', 'gauge', 'transformations', 'of', 'the', 'full', 'vacuumtovacuum', 'transition', 'amplitude', 'generating', 'functional', 'from', 'the', 'coulomb', 'gauge', 'to', 'arbitrary', 'covariant', 'gauges', 'and', 'in... | [-0.11664227975795613, 0.21627192901407555, -0.13091969823100322, 0.13652171531398577, -0.15989412796562133, -0.1376285729271805, 0.041477410659274974, 0.3576388249133268, -0.202279246571656, -0.2749569110962076, -0.0052556298210022405, -0.21398722371542017, -0.1544498642172624, 0.13188950072609537, -0.0725354970756756... |
706.1632 | Wetting of gradient fields: pathwise estimates | We consider the wetting transition in the framework of an effective interface
model of gradient type, in dimension 2 and higher. We prove pathwise estimates
showing that the interface is localized in the whole thermodynamically-defined
partial wetting regime considered in earlier works. Moreover, we study how the
int... | math.PR math-ph math.MP | we consider the wetting transition in the framework of an effective interface model of gradient type in dimension 2 and higher we prove pathwise estimates showing that the interface is localized in the whole thermodynamicallydefined partial wetting regime considered in earlier works moreover we study how the interface ... | [['we', 'consider', 'the', 'wetting', 'transition', 'in', 'the', 'framework', 'of', 'an', 'effective', 'interface', 'model', 'of', 'gradient', 'type', 'in', 'dimension', '2', 'and', 'higher', 'we', 'prove', 'pathwise', 'estimates', 'showing', 'that', 'the', 'interface', 'is', 'localized', 'in', 'the', 'whole', 'thermod... | [-0.12133391562904884, 0.10484591497081408, -0.09307408468700501, 0.06425944225577665, -0.0198453399422231, -0.14144235888301437, 0.023956985963480688, 0.3611096125930103, -0.25266529483470457, -0.25133587575670496, 0.1036218998991926, -0.25262947687045184, -0.20506163774520408, 0.1099301904766584, -0.04400886656410659... |
706.1633 | Large Attractive Depletion Interactions in Soft Repulsive-Sphere Binary
Mixtures | We consider binary mixtures of soft repulsive spherical particles and
calculate the depletion interaction between two big spheres mediated by the
fluid of small spheres, using different theoretical and simulation methods. The
validity of the theoretical approach, a virial expansion in terms of the
density of the smal... | cond-mat.soft cond-mat.stat-mech | we consider binary mixtures of soft repulsive spherical particles and calculate the depletion interaction between two big spheres mediated by the fluid of small spheres using different theoretical and simulation methods the validity of the theoretical approach a virial expansion in terms of the density of the small sph... | [['we', 'consider', 'binary', 'mixtures', 'of', 'soft', 'repulsive', 'spherical', 'particles', 'and', 'calculate', 'the', 'depletion', 'interaction', 'between', 'two', 'big', 'spheres', 'mediated', 'by', 'the', 'fluid', 'of', 'small', 'spheres', 'using', 'different', 'theoretical', 'and', 'simulation', 'methods', 'the'... | [-0.12869120769253367, 0.18911971955782506, -0.10009691239335618, 0.05560791512043313, -0.005607688434180418, -0.12933599509329977, 0.04149776880500768, 0.34409042177760824, -0.24023379080356042, -0.284846211171068, 0.027965466576145192, -0.29670125599872615, -0.1359781048895799, 0.13554892458497045, 0.0165760264803546... |
706.1634 | Critical Delays and Polynomial Eigenvalue Problems | In this work we present a new method to compute the delays of delay
differential equations (DDEs), such that the DDE has a purely imaginary
eigenvalue. For delay differential equations with multiple delays, the critical
curves or critical surfaces in delay space (that is, the set of delays where
the DDE has a purely ... | math.NA | in this work we present a new method to compute the delays of delay differential equations ddes such that the dde has a purely imaginary eigenvalue for delay differential equations with multiple delays the critical curves or critical surfaces in delay space that is the set of delays where the dde has a purely imaginary... | [['in', 'this', 'work', 'we', 'present', 'a', 'new', 'method', 'to', 'compute', 'the', 'delays', 'of', 'delay', 'differential', 'equations', 'ddes', 'such', 'that', 'the', 'dde', 'has', 'a', 'purely', 'imaginary', 'eigenvalue', 'for', 'delay', 'differential', 'equations', 'with', 'multiple', 'delays', 'the', 'critical'... | [-0.19656549477516566, 0.05350111469526255, -0.07068474245864119, 0.03596071462041352, -0.10681367516084465, -0.1413698579038515, -0.00028210528178660327, 0.31787871494131203, -0.2935688214696034, -0.29316340072546154, 0.11583812754982974, -0.28057435093864497, -0.19674576871329919, 0.21598413344445574, -0.022354053576... |
706.1635 | D-brane States and Disk Amplitudes in OSp Invariant Closed String Field
Theory | We construct solitonic states in the OSp invariant string field theory, which
are BRST invariant in the leading order of regularization parameter $\epsilon$.
We calculate the disk amplitudes using these solitonic states and show that
they describe D-branes and ghost D-branes.
| hep-th | we construct solitonic states in the osp invariant string field theory which are brst invariant in the leading order of regularization parameter epsilon we calculate the disk amplitudes using these solitonic states and show that they describe dbranes and ghost dbranes | [['we', 'construct', 'solitonic', 'states', 'in', 'the', 'osp', 'invariant', 'string', 'field', 'theory', 'which', 'are', 'brst', 'invariant', 'in', 'the', 'leading', 'order', 'of', 'regularization', 'parameter', 'epsilon', 'we', 'calculate', 'the', 'disk', 'amplitudes', 'using', 'these', 'solitonic', 'states', 'and', ... | [-0.2063175877215477, 0.22094453243743173, -0.1349697704994824, 0.20928064365757676, -0.05715434621201783, -0.11187831291974318, -0.01422270745459217, 0.3551490613963546, -0.20385409491818127, -0.2478197725807748, 0.059192718364434634, -0.1931070775452365, -0.18409446095366302, 0.025132832367245745, -0.0841127198825522... |
706.1636 | Background studies and shielding effects for the TPC detector of the
CAST experiment | Sunset solar axions traversing the intense magnetic field of the CERN Axion
Solar Telescope (CAST) experiment may be detected in a Time Projection Chamber
(TPC) detector, as X-rays signals. These signals could be masked, however, by
the inhomogeneous background of materials in the experimental site. A detailed
analys... | astro-ph | sunset solar axions traversing the intense magnetic field of the cern axion solar telescope cast experiment may be detected in a time projection chamber tpc detector as xrays signals these signals could be masked however by the inhomogeneous background of materials in the experimental site a detailed analysis based on ... | [['sunset', 'solar', 'axions', 'traversing', 'the', 'intense', 'magnetic', 'field', 'of', 'the', 'cern', 'axion', 'solar', 'telescope', 'cast', 'experiment', 'may', 'be', 'detected', 'in', 'a', 'time', 'projection', 'chamber', 'tpc', 'detector', 'as', 'xrays', 'signals', 'these', 'signals', 'could', 'be', 'masked', 'ho... | [-0.07461332420167406, 0.17512517730680716, -0.053127994579551495, 0.03670804513581262, -0.037752194379547, -0.08745714371397564, 0.027820656076073647, 0.3670575473358673, -0.17199943243089108, -0.4125587164498536, 0.09590357069886264, -0.3172290731320339, -0.016173259136720304, 0.2105545848772853, 0.002757680404568668... |
706.1637 | t-Wise Independence with Local Dependencies | In this note we prove a large deviation bound on the sum of random variables
with the following dependency structure: there is a dependency graph $G$ with a
bounded chromatic number, in which each vertex represents a random variable.
Variables that are represented by neighboring vertices may be arbitrarily
dependent,... | math.PR math.ST stat.TH | in this note we prove a large deviation bound on the sum of random variables with the following dependency structure there is a dependency graph g with a bounded chromatic number in which each vertex represents a random variable variables that are represented by neighboring vertices may be arbitrarily dependent but col... | [['in', 'this', 'note', 'we', 'prove', 'a', 'large', 'deviation', 'bound', 'on', 'the', 'sum', 'of', 'random', 'variables', 'with', 'the', 'following', 'dependency', 'structure', 'there', 'is', 'a', 'dependency', 'graph', 'g', 'with', 'a', 'bounded', 'chromatic', 'number', 'in', 'which', 'each', 'vertex', 'represents',... | [-0.2042574516199238, 0.21406045651588101, -0.07531572156585753, -0.006783365759474691, -0.11675632644619327, -0.1274962608003989, 0.07561852800427005, 0.36914262422942556, -0.30023252392129507, -0.3108674888499081, 0.06340676277795865, -0.3051067083142698, -0.13496991110150702, 0.10637984891945962, -0.0966811714615687... |
706.1638 | Josephson current in a superconductor -- ferromagnet -- superconductor
junction with in-plane ferromagnetic domains | We study a diffusive superconductor--ferromagnet--superconductor (SFS)
junction with in-plane ferromagnetic domains. Close to the superconducting
transition temperature, we describe the proximity effect in the junction with
the linearized Usadel equations. We find that properties of such a junction
depend on the size... | cond-mat.mes-hall cond-mat.supr-con | we study a diffusive superconductorferromagnetsuperconductor sfs junction with inplane ferromagnetic domains close to the superconducting transition temperature we describe the proximity effect in the junction with the linearized usadel equations we find that properties of such a junction depend on the size of the doma... | [['we', 'study', 'a', 'diffusive', 'superconductorferromagnetsuperconductor', 'sfs', 'junction', 'with', 'inplane', 'ferromagnetic', 'domains', 'close', 'to', 'the', 'superconducting', 'transition', 'temperature', 'we', 'describe', 'the', 'proximity', 'effect', 'in', 'the', 'junction', 'with', 'the', 'linearized', 'usa... | [-0.23545025397995428, 0.12741117400813132, -0.04591952115474151, 0.03032244034362014, -0.031016879078425184, -0.08945358921832676, 0.06071282167074601, 0.3601849849889927, -0.2849213887135722, -0.25014703735544147, 0.029095511232160882, -0.30189264968886403, -0.07641608051991067, 0.16223619892144034, 0.038142084706975... |
706.1639 | The chemical composition of the circumstellar envelopes around yellow
hypergiant stars | The yellow hypergiant stars (YHGs) are extremely luminous and massive objects
whose general properties are poorly known. Only two of this kind of star show
massive circumstellar envelopes, IRC+10420 and AFGL2343. We aim to study the
chemistry of the circumstellar envelopes around these two sources, by
comparison with... | astro-ph | the yellow hypergiant stars yhgs are extremely luminous and massive objects whose general properties are poorly known only two of this kind of star show massive circumstellar envelopes irc10420 and afgl2343 we aim to study the chemistry of the circumstellar envelopes around these two sources by comparison with well kno... | [['the', 'yellow', 'hypergiant', 'stars', 'yhgs', 'are', 'extremely', 'luminous', 'and', 'massive', 'objects', 'whose', 'general', 'properties', 'are', 'poorly', 'known', 'only', 'two', 'of', 'this', 'kind', 'of', 'star', 'show', 'massive', 'circumstellar', 'envelopes', 'irc10420', 'and', 'afgl2343', 'we', 'aim', 'to',... | [-0.025742511221825883, 0.11599175005878727, -0.013899575692103726, 0.0945760531547672, -0.04698019718464287, -0.06965553934348682, 0.023555214987999503, 0.479884949416436, -0.11031445558521603, -0.34161574821838914, 0.05192856665285192, -0.27667492815967776, -0.03368669824302397, 0.14607150443255484, -0.06415511304344... |
706.164 | Independent measurement of the top quark mass and the light- and
bottom-jet energy scales at hadron colliders | A method for the simultaneous determination of the energy scales for b-quark
jets and light jets, the jet energy resolution, and the top quark mass at
hadron colliders is presented. The method exploits the unique kinematics of
events with top-antitop pair production, where one of the top quarks involves a
leptonic an... | hep-ex | a method for the simultaneous determination of the energy scales for bquark jets and light jets the jet energy resolution and the top quark mass at hadron colliders is presented the method exploits the unique kinematics of events with topantitop pair production where one of the top quarks involves a leptonic and one a ... | [['a', 'method', 'for', 'the', 'simultaneous', 'determination', 'of', 'the', 'energy', 'scales', 'for', 'bquark', 'jets', 'and', 'light', 'jets', 'the', 'jet', 'energy', 'resolution', 'and', 'the', 'top', 'quark', 'mass', 'at', 'hadron', 'colliders', 'is', 'presented', 'the', 'method', 'exploits', 'the', 'unique', 'kin... | [-0.058441947077517396, 0.20797112819273025, -0.11514499607728794, 0.13279778776923196, -0.05491297737171408, -0.12849778780364432, 0.022165139963908585, 0.32057012303266674, -0.2169512098422274, -0.27767437952570617, 0.004836410943971714, -0.3147796132019721, 0.10063648773357273, 0.17081244601868092, 0.113950510835275... |
706.1641 | Non-unity gain minimal disturbance measurement | We propose and experimentally demonstrate an optimal non-unity gain Gaussian
scheme for partial measurement of an unknown coherent state that causes minimal
disturbance of the state. The information gain and the state disturbance are
quantified by the noise added to the measurement outcomes and to the output
state, r... | quant-ph | we propose and experimentally demonstrate an optimal nonunity gain gaussian scheme for partial measurement of an unknown coherent state that causes minimal disturbance of the state the information gain and the state disturbance are quantified by the noise added to the measurement outcomes and to the output state respec... | [['we', 'propose', 'and', 'experimentally', 'demonstrate', 'an', 'optimal', 'nonunity', 'gain', 'gaussian', 'scheme', 'for', 'partial', 'measurement', 'of', 'an', 'unknown', 'coherent', 'state', 'that', 'causes', 'minimal', 'disturbance', 'of', 'the', 'state', 'the', 'information', 'gain', 'and', 'the', 'state', 'distu... | [-0.14887502023373686, 0.14095436194336453, -0.07251133506984583, 0.04031552032878002, -0.01481797301398945, -0.1910604612979417, 0.11430701015827556, 0.40148470886162524, -0.323909477106229, -0.2888699762434477, 0.08712378138166275, -0.25550686429432107, -0.16379953773936168, 0.19575989849787825, -0.1113042691001846, ... |
706.1642 | On the growth of components with non fixed excesses | Denote by an $l$-component a connected graph with $l$ edges more than
vertices. We prove that the expected number of creations of $(l+1)$-component,
by means of adding a new edge to an $l$-component in a randomly growing graph
with $n$ vertices, tends to 1 as $l,n$ tends to $\infty$ but with $l =
o(n^{1/4})$. We also... | cs.DM math.CO | denote by an lcomponent a connected graph with l edges more than vertices we prove that the expected number of creations of l1component by means of adding a new edge to an lcomponent in a randomly growing graph with n vertices tends to 1 as ln tends to infty but with l on14 we also show under the same conditions on l a... | [['denote', 'by', 'an', 'lcomponent', 'a', 'connected', 'graph', 'with', 'l', 'edges', 'more', 'than', 'vertices', 'we', 'prove', 'that', 'the', 'expected', 'number', 'of', 'creations', 'of', 'l1component', 'by', 'means', 'of', 'adding', 'a', 'new', 'edge', 'to', 'an', 'lcomponent', 'in', 'a', 'randomly', 'growing', 'g... | [-0.15799410564814492, 0.19929416786833778, -0.007251646381635697, -0.026914215403405998, -0.05892412008371395, -0.15451827201729593, 0.05821967096282886, 0.3417104654016349, -0.2430171945777077, -0.325708577886988, 0.030974298176797442, -0.38439821819655406, -0.10736692260401562, 0.10170209288406067, -0.07263173258755... |
706.1643 | APEX survey of southern high mass star forming regions | A systematic study of a large sample of sources, covering a wide range in
galactocentric distances, masses and luminosities, is a fast and efficient way
of obtaining a good overview of the different stages of high-mass star
formation. With these goals in mind, we have started a survey of 40 color
selected IRAS source... | astro-ph | a systematic study of a large sample of sources covering a wide range in galactocentric distances masses and luminosities is a fast and efficient way of obtaining a good overview of the different stages of highmass star formation with these goals in mind we have started a survey of 40 color selected iras sources south ... | [['a', 'systematic', 'study', 'of', 'a', 'large', 'sample', 'of', 'sources', 'covering', 'a', 'wide', 'range', 'in', 'galactocentric', 'distances', 'masses', 'and', 'luminosities', 'is', 'a', 'fast', 'and', 'efficient', 'way', 'of', 'obtaining', 'a', 'good', 'overview', 'of', 'the', 'different', 'stages', 'of', 'highma... | [-0.09234732896968555, 0.08165961483969573, -0.06944009983974896, 0.0492125225457457, -0.08957447531748186, -0.04737465202646837, 0.0672675013395675, 0.45915952726696313, -0.11118782753271333, -0.3837788711835662, 0.1131816217217992, -0.2782308269564188, -0.028770878754053892, 0.1991714231743153, -0.020849441790304492,... |
706.1644 | Pseudo-Gaussian quantum models | A new family of one-dimensional quantum models is proposed in terms of new
potentials with a Gaussian asymptotic behavior but approaching to the potential
of the harmonic o scillator when $x\to 0$. It is shown that, in the energy
basis of the harmonic oscillator, the matrix elements of the Hamiltonian
operators of th... | math-ph math.MP quant-ph | a new family of onedimensional quantum models is proposed in terms of new potentials with a gaussian asymptotic behavior but approaching to the potential of the harmonic o scillator when xto 0 it is shown that in the energy basis of the harmonic oscillator the matrix elements of the hamiltonian operators of these new m... | [['a', 'new', 'family', 'of', 'onedimensional', 'quantum', 'models', 'is', 'proposed', 'in', 'terms', 'of', 'new', 'potentials', 'with', 'a', 'gaussian', 'asymptotic', 'behavior', 'but', 'approaching', 'to', 'the', 'potential', 'of', 'the', 'harmonic', 'o', 'scillator', 'when', 'xto', '0', 'it', 'is', 'shown', 'that', ... | [-0.09128498783684336, 0.13453313601203262, -0.0817451428854838, 0.022800392676920942, 0.012495882696627329, -0.14464175724424422, 0.0010122847238865991, 0.33248103422423203, -0.28522624683876835, -0.20204021469689906, 0.03223332888058697, -0.28137380493183933, -0.18360322813193003, 0.22451473280477027, -0.029245086324... |
706.1645 | Dynamics of Three Agent Games | We study the dynamics and resulting score distribution of three-agent games
where after each competition a single agent wins and scores a point. A single
competition is described by a triplet of numbers $p$, $t$ and $q$ denoting the
probabilities that the team with the highest, middle or lowest accumulated
score wins... | physics.soc-ph cond-mat.stat-mech | we study the dynamics and resulting score distribution of threeagent games where after each competition a single agent wins and scores a point a single competition is described by a triplet of numbers p t and q denoting the probabilities that the team with the highest middle or lowest accumulated score wins we study th... | [['we', 'study', 'the', 'dynamics', 'and', 'resulting', 'score', 'distribution', 'of', 'threeagent', 'games', 'where', 'after', 'each', 'competition', 'a', 'single', 'agent', 'wins', 'and', 'scores', 'a', 'point', 'a', 'single', 'competition', 'is', 'described', 'by', 'a', 'triplet', 'of', 'numbers', 'p', 't', 'and', '... | [-0.090844481382275, 0.08920235858516418, -0.12104488586941856, 0.07949603337735572, -0.05714449110363638, -0.1789096964901419, 0.10567148428577543, 0.3598300352002246, -0.22837045258033092, -0.3141923180769104, 0.06873234427446605, -0.29885946799332214, -0.1344611968176122, 0.13075132335650055, -0.0363773806589985, -0... |
706.1646 | Limits of ultra-high-precision optical astrometry: Stellar surface
structures | We investigate the astrometric effects of stellar surface structures as a
practical limitation to ultra-high-precision astrometry, e.g. in the context of
exoplanet searches, and to quantify the expected effects in different regions
of the HR-diagram. Stellar surface structures are likely to produce
fluctuations in th... | astro-ph | we investigate the astrometric effects of stellar surface structures as a practical limitation to ultrahighprecision astrometry eg in the context of exoplanet searches and to quantify the expected effects in different regions of the hrdiagram stellar surface structures are likely to produce fluctuations in the integrat... | [['we', 'investigate', 'the', 'astrometric', 'effects', 'of', 'stellar', 'surface', 'structures', 'as', 'a', 'practical', 'limitation', 'to', 'ultrahighprecision', 'astrometry', 'eg', 'in', 'the', 'context', 'of', 'exoplanet', 'searches', 'and', 'to', 'quantify', 'the', 'expected', 'effects', 'in', 'different', 'region... | [-0.094421135335695, 0.13908706508448812, -0.0700439698806149, 0.10409519691159949, -0.12826315144915135, -0.028583874842617662, 0.08303399988263846, 0.3609368846898433, -0.20256611361168325, -0.39051749044656753, 0.11502849631803111, -0.27436727330088617, -0.07393905117083341, 0.23669236955139786, -0.12902398666506634... |
706.1647 | Non-lattice simulation for supersymmetric gauge theories in one
dimension | Lattice simulation of supersymmetric gauge theories is not straightforward.
In some cases the lack of manifest supersymmetry just necessitates cumbersome
fine-tuning, but in the worse cases the chiral and/or Majorana nature of
fermions makes it difficult to even formulate an appropriate lattice theory. We
propose to ... | hep-lat hep-th | lattice simulation of supersymmetric gauge theories is not straightforward in some cases the lack of manifest supersymmetry just necessitates cumbersome finetuning but in the worse cases the chiral andor majorana nature of fermions makes it difficult to even formulate an appropriate lattice theory we propose to circumv... | [['lattice', 'simulation', 'of', 'supersymmetric', 'gauge', 'theories', 'is', 'not', 'straightforward', 'in', 'some', 'cases', 'the', 'lack', 'of', 'manifest', 'supersymmetry', 'just', 'necessitates', 'cumbersome', 'finetuning', 'but', 'in', 'the', 'worse', 'cases', 'the', 'chiral', 'andor', 'majorana', 'nature', 'of',... | [-0.12429188505293016, 0.15984984576310748, -0.033190978323354534, 0.14602980275767072, -0.1073318425210585, -0.2128409406623656, 0.02735131585321046, 0.38462494872510433, -0.1894350947787691, -0.2896506578759535, 0.09907480633027214, -0.2039800361656633, -0.1981328541694797, 0.09141440340088018, -0.09819889910470106, ... |
706.1648 | Persistence of characteristics of an ordered flux line lattice above the
second peak in $Bi_2Sr_2CaCu_2O_{8+ \delta}$ | We report Small Angle Neutron Scattering measurements of the flux lines
lattice (FLL) in $Bi_2Sr_2CaCu_2O_{8+ \delta}$. As previously reported, the
scattered intensity decreases strongly when the magnetic field is increased,
but it remains measurable far above the second peak. The direct observation of
Bragg peaks pr... | cond-mat.supr-con | we report small angle neutron scattering measurements of the flux lines lattice fll in bi_2sr_2cacu_2o_8 delta as previously reported the scattered intensity decreases strongly when the magnetic field is increased but it remains measurable far above the second peak the direct observation of bragg peaks proves that the ... | [['we', 'report', 'small', 'angle', 'neutron', 'scattering', 'measurements', 'of', 'the', 'flux', 'lines', 'lattice', 'fll', 'in', 'bi_2sr_2cacu_2o_8', 'delta', 'as', 'previously', 'reported', 'the', 'scattered', 'intensity', 'decreases', 'strongly', 'when', 'the', 'magnetic', 'field', 'is', 'increased', 'but', 'it', '... | [-0.1696013141446747, 0.22088123940469814, -0.04312415561638772, 0.08822351320530288, -0.07966799094574525, -0.1167538575641811, 0.05635895499261096, 0.42585853188298645, -0.2810886861756444, -0.29985295729711653, 0.09591954514733515, -0.30914469531737265, -0.11972268502460792, 0.16372001900104804, -0.00522214254830032... |
706.1649 | On the Low Energy Spectra of the Nonsupersymmetric Heterotic String
Theories | The ten dimensional string theories as well as eleven dimensional
supergravity are conjectured to arise as limits of a more basic theory,
traditionaly dubbed M--theory. This notion is confined to the ten dimensional
supersymmetric theories. String theory, however, also contains ten dimensional
nonsupersymmetric theor... | hep-th hep-ph | the ten dimensional string theories as well as eleven dimensional supergravity are conjectured to arise as limits of a more basic theory traditionaly dubbed mtheory this notion is confined to the ten dimensional supersymmetric theories string theory however also contains ten dimensional nonsupersymmetric theories that ... | [['the', 'ten', 'dimensional', 'string', 'theories', 'as', 'well', 'as', 'eleven', 'dimensional', 'supergravity', 'are', 'conjectured', 'to', 'arise', 'as', 'limits', 'of', 'a', 'more', 'basic', 'theory', 'traditionaly', 'dubbed', 'mtheory', 'this', 'notion', 'is', 'confined', 'to', 'the', 'ten', 'dimensional', 'supers... | [-0.1080319002660054, 0.16093974838587513, -0.04044165450613946, 0.160424517296419, -0.05169812006241947, -0.18486611326733807, -0.006846772422700995, 0.3106099397781454, -0.16261592343011322, -0.2926299065696819, 0.10048552502647136, -0.2444499952859488, -0.1615817520861365, 0.12551524345723897, -0.10637808731999718, ... |
706.165 | A common limit of super Liouville theory and minimal models | We show that N=1 supersymmetric Liouville theory can be continued to central
charge c=3/2, and that the limiting non-rational superconformal field theory
can also be obtained as a limit of supersymmetric minimal models. This
generalises a result known for the non-supersymmetric case. We present explicit
expressions f... | hep-th | we show that n1 supersymmetric liouville theory can be continued to central charge c32 and that the limiting nonrational superconformal field theory can also be obtained as a limit of supersymmetric minimal models this generalises a result known for the nonsupersymmetric case we present explicit expressions for the thr... | [['we', 'show', 'that', 'n1', 'supersymmetric', 'liouville', 'theory', 'can', 'be', 'continued', 'to', 'central', 'charge', 'c32', 'and', 'that', 'the', 'limiting', 'nonrational', 'superconformal', 'field', 'theory', 'can', 'also', 'be', 'obtained', 'as', 'a', 'limit', 'of', 'supersymmetric', 'minimal', 'models', 'this... | [-0.09904854135468193, 0.11054047587575443, -0.05055025119949645, 0.12846932275148126, -0.03550536343571516, -0.10866635271835082, -0.001331745873316439, 0.2915968648841553, -0.19714388975002076, -0.25111592051769616, 0.09102900144900408, -0.23999669901180773, -0.19774723408205452, 0.18257749278029992, -0.0663423549999... |
706.1651 | On Some Lie Bialgebra Structures on Polynomial Algebras and their
Quantization | We study classical twists of Lie bialgebra structures on the polynomial
current algebra $\mathfrak{g}[u]$, where $\mathfrak{g}$ is a simple complex
finite-dimensional Lie algebra. We focus on the structures induced by the
so-called quasi-trigonometric solutions of the classical Yang-Baxter equation.
It turns out that... | math.QA math-ph math.MP | we study classical twists of lie bialgebra structures on the polynomial current algebra mathfrakgu where mathfrakg is a simple complex finitedimensional lie algebra we focus on the structures induced by the socalled quasitrigonometric solutions of the classical yangbaxter equation it turns out that quasitrigonometric r... | [['we', 'study', 'classical', 'twists', 'of', 'lie', 'bialgebra', 'structures', 'on', 'the', 'polynomial', 'current', 'algebra', 'mathfrakgu', 'where', 'mathfrakg', 'is', 'a', 'simple', 'complex', 'finitedimensional', 'lie', 'algebra', 'we', 'focus', 'on', 'the', 'structures', 'induced', 'by', 'the', 'socalled', 'quasi... | [-0.18029675565619943, 0.03967546238388706, -0.06882152754953631, 0.04692835980270218, -0.20115813625956414, -0.14926840808062303, -0.021613932625260405, 0.29539239310449167, -0.3434842487056089, -0.1728316866592454, 0.09713681439383416, -0.24456210061907768, -0.1724073944052541, 0.1610820144965684, -0.1003259213551158... |
706.1652 | Right and Left Joint System Representation of a Rational Matrix Function
in General Position (System Representation Theory for Dummies) | For a rational matrix function R of one variable in general position, the
matrix functions R(x)/R(y) and R(y)\R(x) of two variables are considered. For
these matrix functions of two variables, representations which are analogous to
the system representations (or realizations) of a rational matrix function of
one vari... | math.CA | for a rational matrix function r of one variable in general position the matrix functions rxry and ryrx of two variables are considered for these matrix functions of two variables representations which are analogous to the system representations or realizations of a rational matrix function of one variable are construc... | [['for', 'a', 'rational', 'matrix', 'function', 'r', 'of', 'one', 'variable', 'in', 'general', 'position', 'the', 'matrix', 'functions', 'rxry', 'and', 'ryrx', 'of', 'two', 'variables', 'are', 'considered', 'for', 'these', 'matrix', 'functions', 'of', 'two', 'variables', 'representations', 'which', 'are', 'analogous', ... | [-0.1319726099881033, 0.09448064061192175, -0.08159417199591795, 0.060397206867734594, -0.05951101593673229, -0.1539182463971277, -0.0143362268495063, 0.36053125659624735, -0.35190692072113355, -0.19525221176445484, 0.13798383400426245, -0.28392220120877026, -0.18604939634678885, 0.13421802771044894, -0.034830747917294... |
706.1653 | Thermodynamic forces, flows, and Onsager coefficients in complex
networks | We present Onsager formalism applied to random networks with arbitrary degree
distribution. Using the well-known methods of non-equilibrium thermodynamics we
identify thermodynamic forces and their conjugated flows induced in networks as
a result of single node degree perturbation. The forces and the flows can be
und... | cond-mat.dis-nn cond-mat.stat-mech | we present onsager formalism applied to random networks with arbitrary degree distribution using the wellknown methods of nonequilibrium thermodynamics we identify thermodynamic forces and their conjugated flows induced in networks as a result of single node degree perturbation the forces and the flows can be understoo... | [['we', 'present', 'onsager', 'formalism', 'applied', 'to', 'random', 'networks', 'with', 'arbitrary', 'degree', 'distribution', 'using', 'the', 'wellknown', 'methods', 'of', 'nonequilibrium', 'thermodynamics', 'we', 'identify', 'thermodynamic', 'forces', 'and', 'their', 'conjugated', 'flows', 'induced', 'in', 'network... | [-0.15080956946289872, 0.12838802966221408, -0.095727308933596, 0.055694590006204484, -0.0521832256831084, -0.16074791141487296, 0.03893662977158951, 0.37406657344562194, -0.32514545762712516, -0.288305505115575, 0.06525815036984214, -0.2895702167224247, -0.21722875983969678, 0.1803440300253835, -0.047238468511247085, ... |
706.1654 | Gravity as an emergent phenomenon: A conceptual description | I describe several broad features of a programme to understand gravity as an
emergent, long wavelength, phenomenon (like elasticity) and discuss one
concrete framework for realizing this paradigm in the backdrop of several
recent results.
| gr-qc astro-ph hep-th | i describe several broad features of a programme to understand gravity as an emergent long wavelength phenomenon like elasticity and discuss one concrete framework for realizing this paradigm in the backdrop of several recent results | [['i', 'describe', 'several', 'broad', 'features', 'of', 'a', 'programme', 'to', 'understand', 'gravity', 'as', 'an', 'emergent', 'long', 'wavelength', 'phenomenon', 'like', 'elasticity', 'and', 'discuss', 'one', 'concrete', 'framework', 'for', 'realizing', 'this', 'paradigm', 'in', 'the', 'backdrop', 'of', 'several', ... | [-0.09853425872113024, 0.07687388435380334, -0.09677518521036421, 0.0856923254040469, -0.0984528717717954, -0.18082974889714803, -0.08035134614578315, 0.3459317986454282, -0.2977082853072456, -0.30087915895107603, 0.12743157873129737, -0.20085906176162618, -0.2236012571624347, 0.2201203486749104, -0.054526411928236485,... |
706.1655 | Pascal's triangle and word bases for blob algebra ideals | We give an elementary proof of isomorphism of the blob (diagram) algebra and
the corresponding extended Temperley-Lieb algebra (defined by presentation).
| math.RT | we give an elementary proof of isomorphism of the blob diagram algebra and the corresponding extended temperleylieb algebra defined by presentation | [['we', 'give', 'an', 'elementary', 'proof', 'of', 'isomorphism', 'of', 'the', 'blob', 'diagram', 'algebra', 'and', 'the', 'corresponding', 'extended', 'temperleylieb', 'algebra', 'defined', 'by', 'presentation']] | [-0.1261012660605567, 0.08084856186663576, -0.11840331687458924, 0.1025219734846836, -0.1758651145999985, -0.1359450640156865, -0.035719916135782286, 0.30373333891232807, -0.37297251927001135, -0.26917916742552606, 0.122119736968584, -0.16082295846371425, -0.11775474436858314, 0.16071758729716143, -0.11406279639119193,... |
706.1656 | Millisecond pulsars around intermediate-mass black holes in globular
clusters | We study the process of dynamical capture of a millisecond pulsar (MSP) by a
single or binary IMBH, simulating various types of single-binary and
binary-binary encounters. It is found that [IMBH,MSP] binaries form over cosmic
time in a cluster, via encounters of wide--orbit binary MSPs off the single
IMBH, and at a l... | astro-ph | we study the process of dynamical capture of a millisecond pulsar msp by a single or binary imbh simulating various types of singlebinary and binarybinary encounters it is found that imbhmsp binaries form over cosmic time in a cluster via encounters of wideorbit binary msps off the single imbh and at a lower pace via i... | [['we', 'study', 'the', 'process', 'of', 'dynamical', 'capture', 'of', 'a', 'millisecond', 'pulsar', 'msp', 'by', 'a', 'single', 'or', 'binary', 'imbh', 'simulating', 'various', 'types', 'of', 'singlebinary', 'and', 'binarybinary', 'encounters', 'it', 'is', 'found', 'that', 'imbhmsp', 'binaries', 'form', 'over', 'cosmi... | [-0.14956976514940834, 0.1651480860354392, -0.0557297966021603, 0.1511013724754946, -0.09864900987425547, -0.05873989975286046, 0.07860639602282997, 0.3497585917987938, -0.15896353717592623, -0.3498376937301752, 0.06152713180866461, -0.3146743317289899, -0.02991782054596115, 0.26354606572931516, 0.006141606982661567, -... |
706.1657 | Dynamical Heterogeneity and Nonlinear Susceptibility in Short-Ranged
Attractive Supercooled Liquids | Recent work has demonstrated the strong qualitative differences between the
dynamics near a glass transition driven by short-ranged repulsion and one
governed by short-ranged attraction. Here, we study in detail the behavior of
non-linear, higher-order correlation functions that measure the growth of
length scales as... | cond-mat.stat-mech | recent work has demonstrated the strong qualitative differences between the dynamics near a glass transition driven by shortranged repulsion and one governed by shortranged attraction here we study in detail the behavior of nonlinear higherorder correlation functions that measure the growth of length scales associated ... | [['recent', 'work', 'has', 'demonstrated', 'the', 'strong', 'qualitative', 'differences', 'between', 'the', 'dynamics', 'near', 'a', 'glass', 'transition', 'driven', 'by', 'shortranged', 'repulsion', 'and', 'one', 'governed', 'by', 'shortranged', 'attraction', 'here', 'we', 'study', 'in', 'detail', 'the', 'behavior', '... | [-0.13343029494325703, 0.17362708980307126, -0.08738197092092238, 0.0989116864825169, -0.00758387572848453, -0.10887472532004512, -0.027930377978079308, 0.34087989006925806, -0.2754755281091023, -0.2522798161058185, 0.03851293444705124, -0.3211824636986981, -0.2492931267568985, 0.14034513144109112, 0.06293769547482952,... |
706.1658 | Limits to the diffuse flux of UHE tau neutrinos at EeV energies from the
Pierre Auger Observatory | With the Pierre Auger Observatory we have the capability of detecting
ultra-high energy neutrinos by searching for very inclined showers with a
significant electromagnetic component. In this work we discuss the
discrimination power of the instrument for earth skimming tau neutrinos with
ultra-high energies. Based on ... | astro-ph | with the pierre auger observatory we have the capability of detecting ultrahigh energy neutrinos by searching for very inclined showers with a significant electromagnetic component in this work we discuss the discrimination power of the instrument for earth skimming tau neutrinos with ultrahigh energies based on the da... | [['with', 'the', 'pierre', 'auger', 'observatory', 'we', 'have', 'the', 'capability', 'of', 'detecting', 'ultrahigh', 'energy', 'neutrinos', 'by', 'searching', 'for', 'very', 'inclined', 'showers', 'with', 'a', 'significant', 'electromagnetic', 'component', 'in', 'this', 'work', 'we', 'discuss', 'the', 'discrimination'... | [-0.09703736327440086, 0.23755660702232306, -0.043472432423436985, 0.14287946103275687, -0.060203610662964806, -0.023317965064737677, 0.016714743149561295, 0.40460893270168186, -0.15093302273906875, -0.4313904201692861, 0.041670321137222556, -0.36216408843039605, -0.014622286191561085, 0.2127067513116028, 0.02973695993... |
706.1659 | Hybrid Quasicrystals, Transport and Localization in Products of Minimal
Sets | We consider convex combinations of finite-valued almost periodic sequences
(mainly substitution sequences) and put them as potentials of one-dimensional
tight-binding models. We prove that these sequences are almost periodic. We
call such combinations {\em hybrid quasicrystals} and these studies are related
to the mi... | math-ph math.MP | we consider convex combinations of finitevalued almost periodic sequences mainly substitution sequences and put them as potentials of onedimensional tightbinding models we prove that these sequences are almost periodic we call such combinations em hybrid quasicrystals and these studies are related to the minimality und... | [['we', 'consider', 'convex', 'combinations', 'of', 'finitevalued', 'almost', 'periodic', 'sequences', 'mainly', 'substitution', 'sequences', 'and', 'put', 'them', 'as', 'potentials', 'of', 'onedimensional', 'tightbinding', 'models', 'we', 'prove', 'that', 'these', 'sequences', 'are', 'almost', 'periodic', 'we', 'call'... | [-0.18518813542629542, 0.136069219706482, -0.03940122615006801, 0.07893231396883493, -0.026183845548841515, -0.11463856337573625, 0.04841830467462147, 0.4273311970142746, -0.36022394711739925, -0.2199519052366285, 0.11647197890928701, -0.31392429017853973, -0.1890398347750306, 0.20509553286185683, -0.06062612772036932,... |
706.166 | Brane Tilings | We review and extend the progress made over the past few years in
understanding the structure of toric quiver gauge theories; those which are
induced on the world-volume of a stack of D3-branes placed at the tip of a
toric Calabi-Yau cone, at an ``orbifold point'' in Kaehler moduli space. These
provide an infinite cl... | hep-th | we review and extend the progress made over the past few years in understanding the structure of toric quiver gauge theories those which are induced on the worldvolume of a stack of d3branes placed at the tip of a toric calabiyau cone at an orbifold point in kaehler moduli space these provide an infinite class of fourd... | [['we', 'review', 'and', 'extend', 'the', 'progress', 'made', 'over', 'the', 'past', 'few', 'years', 'in', 'understanding', 'the', 'structure', 'of', 'toric', 'quiver', 'gauge', 'theories', 'those', 'which', 'are', 'induced', 'on', 'the', 'worldvolume', 'of', 'a', 'stack', 'of', 'd3branes', 'placed', 'at', 'the', 'tip'... | [-0.1551579650938756, 0.12530221640588837, -0.06528483019210399, 0.11032193847319209, -0.09657133633368893, -0.14775259864369505, -0.03161864224024803, 0.3462599678455215, -0.2527288406094732, -0.2512784063485206, 0.11931006219360585, -0.24527275410823915, -0.17069406010406582, 0.11435630407619388, -0.12888505702446165... |
706.1661 | Quantum electrodynamics and experiment demonstrate the non-retarded
nature of electrodynamical force fields | In quantum electrodynamics, the quantitatively most successful theory in the
history of science, intercharge forces obeying the inverse square law are due
to the exchange of space-like virtual photons. The fundamental quantum process
underlying applications as diverse as the gyromagnetic ratio of the electron
and ele... | physics.class-ph | in quantum electrodynamics the quantitatively most successful theory in the history of science intercharge forces obeying the inverse square law are due to the exchange of spacelike virtual photons the fundamental quantum process underlying applications as diverse as the gyromagnetic ratio of the electron and electrica... | [['in', 'quantum', 'electrodynamics', 'the', 'quantitatively', 'most', 'successful', 'theory', 'in', 'the', 'history', 'of', 'science', 'intercharge', 'forces', 'obeying', 'the', 'inverse', 'square', 'law', 'are', 'due', 'to', 'the', 'exchange', 'of', 'spacelike', 'virtual', 'photons', 'the', 'fundamental', 'quantum', ... | [-0.10528864561214665, 0.17607527966257422, -0.09624716962829138, 0.0692632821850612, -0.05225284919260612, -0.12079967731091229, 0.00897485236607822, 0.32355553178187413, -0.2699374050282154, -0.28148212605686507, 0.015939702705739515, -0.30837269202817846, -0.15417333802538394, 0.2238331247457079, 0.01948437457196886... |
706.1662 | Temperature dependence of magnetic anisotropy in bulk and nanoparticles
of Pr_0.5Sr_0.5MnO_3 | Nanoparticles (size 20, 40 and 60 nm) of Pr_0.5Sr_0.5MnO_3 are prepared by
sol-gel technique and their magnetic properties are studied using ferromagnetic
resonance and magnetization measurements. A comparison with the properties of
the bulk material shows that the ferromagnetic transition at 265 K remains
unaffected... | cond-mat.str-el cond-mat.mtrl-sci | nanoparticles size 20 40 and 60 nm of pr_05sr_05mno_3 are prepared by solgel technique and their magnetic properties are studied using ferromagnetic resonance and magnetization measurements a comparison with the properties of the bulk material shows that the ferromagnetic transition at 265 k remains unaffected but the ... | [['nanoparticles', 'size', '20', '40', 'and', '60', 'nm', 'of', 'pr_05sr_05mno_3', 'are', 'prepared', 'by', 'solgel', 'technique', 'and', 'their', 'magnetic', 'properties', 'are', 'studied', 'using', 'ferromagnetic', 'resonance', 'and', 'magnetization', 'measurements', 'a', 'comparison', 'with', 'the', 'properties', 'o... | [-0.11501840408620706, 0.28093914263123687, -0.018036153486951492, -0.03572497566685427, 0.006051776974007141, -0.120904560651641, 0.08069504145532846, 0.43244018457656686, -0.21213186320004074, -0.37893994624704813, 0.04452840873543823, -0.3656738507453092, -0.008203203470424511, 0.17804448007670945, 0.117704844372996... |
706.1663 | Stability of the Einstein static universe in f(R) gravity | We analyze the stability of the Einstein static universe by considering
homogeneous scalar perturbations in the context of f(R) modified theories of
gravity. By considering specific forms of f(R), the stability regions of the
solutions are parameterized by a linear equation of state parameter w=p/rho.
Contrary to cla... | gr-qc astro-ph hep-th | we analyze the stability of the einstein static universe by considering homogeneous scalar perturbations in the context of fr modified theories of gravity by considering specific forms of fr the stability regions of the solutions are parameterized by a linear equation of state parameter wprho contrary to classical gene... | [['we', 'analyze', 'the', 'stability', 'of', 'the', 'einstein', 'static', 'universe', 'by', 'considering', 'homogeneous', 'scalar', 'perturbations', 'in', 'the', 'context', 'of', 'fr', 'modified', 'theories', 'of', 'gravity', 'by', 'considering', 'specific', 'forms', 'of', 'fr', 'the', 'stability', 'regions', 'of', 'th... | [-0.18865818010850086, 0.09842477600193686, -0.1048345751543012, 0.13055750703982388, -0.11124063838376767, -0.1977681196036024, -0.08371243655371169, 0.2563437564815912, -0.18298730167249838, -0.27906974678238233, 0.06890384228382673, -0.20443893461488188, -0.13262335289166205, 0.13904137429263858, -0.0428581980057060... |
706.1664 | A new young stellar cluster embedded in a molecular cloud in the far
outer Galaxy | We report the discovery of a new young stellar cluster and molecular cloud
located in the far outer Galaxy, seen towards IRAS 06361-0142, and we
characterise their properties. Near-infrared images were obtained with
VLT/ISAAC through JHKs filters, millimetre line observations of CO(1-0) were
obtained with SEST, and V... | astro-ph | we report the discovery of a new young stellar cluster and molecular cloud located in the far outer galaxy seen towards iras 063610142 and we characterise their properties nearinfrared images were obtained with vltisaac through jhks filters millimetre line observations of co10 were obtained with sest and vla 6 cm conti... | [['we', 'report', 'the', 'discovery', 'of', 'a', 'new', 'young', 'stellar', 'cluster', 'and', 'molecular', 'cloud', 'located', 'in', 'the', 'far', 'outer', 'galaxy', 'seen', 'towards', 'iras', '063610142', 'and', 'we', 'characterise', 'their', 'properties', 'nearinfrared', 'images', 'were', 'obtained', 'with', 'vltisaa... | [-0.04878871566165359, 0.06979169919786433, -0.04673423217609525, 0.013256328420773629, -0.07336237114073048, -0.08265668857746923, 0.06004850231186156, 0.4916275021409796, -0.16921593580515154, -0.3592356542515899, 0.08032105973501119, -0.30823944871944764, 0.027531956254895174, 0.1450342821633263, -0.0201763702766437... |
706.1665 | Another Proof of Wright's Inequalities | We present a short way of proving the inequalities obtained by Wright in
[Journal of Graph Theory, 4: 393 - 407 (1980)] concerning the number of
connected graphs with $\ell$ edges more than vertices.
| cs.DM math.CO | we present a short way of proving the inequalities obtained by wright in journal of graph theory 4 393 407 1980 concerning the number of connected graphs with ell edges more than vertices | [['we', 'present', 'a', 'short', 'way', 'of', 'proving', 'the', 'inequalities', 'obtained', 'by', 'wright', 'in', 'journal', 'of', 'graph', 'theory', '4', '393', '407', '1980', 'concerning', 'the', 'number', 'of', 'connected', 'graphs', 'with', 'ell', 'edges', 'more', 'than', 'vertices']] | [-0.16559324878846493, 0.09640391478597214, -0.043473915055845726, 0.021322581772410282, -0.0906197459182956, -0.1116056291414707, 0.09493721181625557, 0.3122632229474909, -0.1718627133858249, -0.43446431184808415, 0.05392592958753195, -0.3489509798360593, -0.1471048085103658, 0.1654865675196616, -0.12032309403135018, ... |
706.1666 | x-Evolution of Phenomenological Dipole Cross Sections | Deep inelastic scattering at small x can be described very effectively using
saturation inspired dipole models. We investigate whether such models are
compatible with the numerical solutions of the Balitsky-Kovchegov (BK) equation
which is expected to describe the nonlinear evolution in x of the dipole cross
section.... | hep-ph | deep inelastic scattering at small x can be described very effectively using saturation inspired dipole models we investigate whether such models are compatible with the numerical solutions of the balitskykovchegov bk equation which is expected to describe the nonlinear evolution in x of the dipole cross section we fin... | [['deep', 'inelastic', 'scattering', 'at', 'small', 'x', 'can', 'be', 'described', 'very', 'effectively', 'using', 'saturation', 'inspired', 'dipole', 'models', 'we', 'investigate', 'whether', 'such', 'models', 'are', 'compatible', 'with', 'the', 'numerical', 'solutions', 'of', 'the', 'balitskykovchegov', 'bk', 'equati... | [-0.07668319367862429, 0.10809744364873629, -0.12073511576675104, 0.10211045253490371, -0.019696977812646316, -0.10222451598853852, -0.02492910528066333, 0.34022880827236657, -0.27280757515079745, -0.28909902637730345, 0.049639003675882566, -0.3168322152994347, -0.08391646292022985, 0.18435767379993892, 0.0153276150807... |
706.1667 | On the Moduli Space of non-BPS Attractors for N=2 Symmetric Manifolds | We study the ``flat'' directions of non-BPS extremal black hole attractors
for N=2, d=4 supergravities whose vector multiplets' scalar manifold is endowed
with homogeneous symmetric special Kahler geometry. The non-BPS attractors with
non-vanishing central charge have a moduli space described by real special
geometry... | hep-th | we study the flat directions of nonbps extremal black hole attractors for n2 d4 supergravities whose vector multiplets scalar manifold is endowed with homogeneous symmetric special kahler geometry the nonbps attractors with nonvanishing central charge have a moduli space described by real special geometry and thus rela... | [['we', 'study', 'the', 'flat', 'directions', 'of', 'nonbps', 'extremal', 'black', 'hole', 'attractors', 'for', 'n2', 'd4', 'supergravities', 'whose', 'vector', 'multiplets', 'scalar', 'manifold', 'is', 'endowed', 'with', 'homogeneous', 'symmetric', 'special', 'kahler', 'geometry', 'the', 'nonbps', 'attractors', 'with'... | [-0.20245288411951473, 0.181643249761183, 0.017138012484597263, 0.13611298029546334, -0.08851784969910338, -0.23373774867955474, -0.08111595784023565, 0.2828704449798792, -0.13978138808361304, -0.16938741559598355, 0.13507815755362954, -0.293835078871819, -0.18580362895723954, 0.0828670188584315, -0.09909654759191057, ... |
706.1668 | Controlling Secondary Structures of Bio-Polymers with Hydrogen-Like
Bonding | We present results for a lattice model of bio-polymers where the type of
$\beta$-sheet formation can be controlled by different types of hydrogen bonds
depending on the relative orientation of close segments of the polymer. Tuning
these different interaction strengths leads to low-temperature structures with
differen... | cond-mat.soft cond-mat.stat-mech | we present results for a lattice model of biopolymers where the type of betasheet formation can be controlled by different types of hydrogen bonds depending on the relative orientation of close segments of the polymer tuning these different interaction strengths leads to lowtemperature structures with different types o... | [['we', 'present', 'results', 'for', 'a', 'lattice', 'model', 'of', 'biopolymers', 'where', 'the', 'type', 'of', 'betasheet', 'formation', 'can', 'be', 'controlled', 'by', 'different', 'types', 'of', 'hydrogen', 'bonds', 'depending', 'on', 'the', 'relative', 'orientation', 'of', 'close', 'segments', 'of', 'the', 'polym... | [-0.15317824934064955, 0.18164391992855575, -0.039377643690480815, -0.02747618968374785, 0.005451481747017665, -0.094098754299732, 0.07992695768019063, 0.40653539405434164, -0.2736059347433703, -0.3383607225516787, 0.041609386623196014, -0.22523891425074696, -0.14654592934439514, 0.09809600851534829, 0.0698898437904653... |
706.1669 | The Elongated Structure of the Hercules dSph from Deep LBT Imaging | We present a deep, wide-field photometric survey of the newly-discovered
Hercules dwarf spheroidal galaxy, based on data from the Large Binocular
Telescope. Images in B, V and r were obtained with the Large Binocular Camera
covering a 23' times 23' field of view to a magnitude of ~25.5 (5 sigma). This
permitted the c... | astro-ph | we present a deep widefield photometric survey of the newlydiscovered hercules dwarf spheroidal galaxy based on data from the large binocular telescope images in b v and r were obtained with the large binocular camera covering a 23 times 23 field of view to a magnitude of 255 5 sigma this permitted the construction of ... | [['we', 'present', 'a', 'deep', 'widefield', 'photometric', 'survey', 'of', 'the', 'newlydiscovered', 'hercules', 'dwarf', 'spheroidal', 'galaxy', 'based', 'on', 'data', 'from', 'the', 'large', 'binocular', 'telescope', 'images', 'in', 'b', 'v', 'and', 'r', 'were', 'obtained', 'with', 'the', 'large', 'binocular', 'came... | [-0.11628012008968854, 0.04202651681327632, -0.135214553667478, 0.07003237948379387, -0.16798577070041754, -0.0713643119268274, 0.07902204921753095, 0.3905751367846688, -0.1760550238534931, -0.3940133885019919, 0.01764355991470658, -0.28441164316097783, -0.0913647647849847, 0.20598307122722023, -0.07854394407579574, -0... |
706.167 | Strong dipolar effects in a quantum ferrofluid | We report on the realization of a Chromium Bose-Einstein condensate (BEC)
with strong dipolar interaction. By using a Feshbach resonance, we reduce the
usual isotropic contact interaction, such that the anisotropic magnetic
dipole-dipole interaction between 52Cr atoms becomes comparable in strength.
This induces a ch... | cond-mat.other | we report on the realization of a chromium boseeinstein condensate bec with strong dipolar interaction by using a feshbach resonance we reduce the usual isotropic contact interaction such that the anisotropic magnetic dipoledipole interaction between 52cr atoms becomes comparable in strength this induces a change of th... | [['we', 'report', 'on', 'the', 'realization', 'of', 'a', 'chromium', 'boseeinstein', 'condensate', 'bec', 'with', 'strong', 'dipolar', 'interaction', 'by', 'using', 'a', 'feshbach', 'resonance', 'we', 'reduce', 'the', 'usual', 'isotropic', 'contact', 'interaction', 'such', 'that', 'the', 'anisotropic', 'magnetic', 'dip... | [-0.17810275021518907, 0.2063600033218267, -0.05447788070887327, 0.06355549990125424, -0.02696278605920573, -0.10443638977030235, -0.029223420510816417, 0.3231158343595312, -0.2465765761550177, -0.28568862676338264, -0.015543214990457549, -0.2481914531072658, -0.10529797077073123, 0.17891019325576385, 0.102228148561676... |
706.1671 | Symplectic Structure of the Real Ginibre Ensemble | We give a simple derivation of all $n$-point densities for the eigenvalues of
the real Ginibre ensemble with even dimension $N$ as quaternion determinants. A
very simple symplectic kernel governs both, the real and complex correlations.
1-and-2-point correlations are discussed in more detail. Scaling forms for
large ... | cond-mat.stat-mech | we give a simple derivation of all npoint densities for the eigenvalues of the real ginibre ensemble with even dimension n as quaternion determinants a very simple symplectic kernel governs both the real and complex correlations 1and2point correlations are discussed in more detail scaling forms for large dimension n ar... | [['we', 'give', 'a', 'simple', 'derivation', 'of', 'all', 'npoint', 'densities', 'for', 'the', 'eigenvalues', 'of', 'the', 'real', 'ginibre', 'ensemble', 'with', 'even', 'dimension', 'n', 'as', 'quaternion', 'determinants', 'a', 'very', 'simple', 'symplectic', 'kernel', 'governs', 'both', 'the', 'real', 'and', 'complex... | [-0.17326571381418035, 0.1451752762310207, -0.03754061179235577, 0.1613150321505964, -0.003102653780952096, -0.1354187353514135, -0.08223640572046861, 0.35264968547970055, -0.17200498349964619, -0.218937571272254, 0.057369987068232146, -0.301417334433645, -0.23953739655204118, 0.19278951022773982, 0.03502363312989473, ... |
706.1672 | Resonant phenomena in extended chaotic systems subject to external
noise: the Lorenz'96 model case | We investigate the effects of a time-correlated noise on an extended chaotic
system. The chosen model is the Lorenz'96, a kind of "toy" model used for
climate studies. Through the analysis of the system's time evolution and its
time and space correlations, we have obtained numerical evidence for two
stochastic resona... | nlin.CD cond-mat.stat-mech physics.ao-ph | we investigate the effects of a timecorrelated noise on an extended chaotic system the chosen model is the lorenz96 a kind of toy model used for climate studies through the analysis of the systems time evolution and its time and space correlations we have obtained numerical evidence for two stochastic resonancelike beh... | [['we', 'investigate', 'the', 'effects', 'of', 'a', 'timecorrelated', 'noise', 'on', 'an', 'extended', 'chaotic', 'system', 'the', 'chosen', 'model', 'is', 'the', 'lorenz96', 'a', 'kind', 'of', 'toy', 'model', 'used', 'for', 'climate', 'studies', 'through', 'the', 'analysis', 'of', 'the', 'systems', 'time', 'evolution'... | [-0.15587236383216124, 0.09213106600795089, -0.08300221817802951, 0.1408241934243102, -0.01583126321365343, -0.11390083546045228, 0.040118214334839974, 0.35415460113610064, -0.28007036823535636, -0.2778065241699185, 0.13528579578378072, -0.27140061906321306, -0.21402030355714818, 0.2126474898595746, -0.0240876678351278... |
706.1673 | Representations and classification of traveling wave solutions to
Sinh-G{\"o}rdon equation | Two concepts named atom solution and combinatory solution are defined. The
classification of all single traveling wave atom solutions to Sinh-G{\"o}rdon
equation is obtained, and qualitative properties of solutions are discussed. In
particular, we point out that some qualitative properties derived intuitively
from dy... | nlin.SI nlin.PS | two concepts named atom solution and combinatory solution are defined the classification of all single traveling wave atom solutions to sinhgordon equation is obtained and qualitative properties of solutions are discussed in particular we point out that some qualitative properties derived intuitively from dynamic syste... | [['two', 'concepts', 'named', 'atom', 'solution', 'and', 'combinatory', 'solution', 'are', 'defined', 'the', 'classification', 'of', 'all', 'single', 'traveling', 'wave', 'atom', 'solutions', 'to', 'sinhgordon', 'equation', 'is', 'obtained', 'and', 'qualitative', 'properties', 'of', 'solutions', 'are', 'discussed', 'in... | [-0.10725030521705245, 0.006932465826701425, -0.06986644420396076, 0.06400443741847667, -0.09278530943510907, -0.15453780664319403, 0.019317466859820852, 0.3417511525134859, -0.27906763398355355, -0.27822409779503104, 0.06425621277087609, -0.3442319124790557, -0.19965081165931867, 0.22370459047392052, -0.06551035388969... |
706.1674 | Fluctuations of the Casimir-Polder force between an atom and a
conducting wall | We consider the quantum fluctuations of the Casimir-Polder force between a
neutral atom and a perfectly conducting wall in the ground state of the system.
In order to obtain the atom-wall force fluctuation we first define an operator
directly associated to the force experienced by the atom considered as a
polarizable... | quant-ph | we consider the quantum fluctuations of the casimirpolder force between a neutral atom and a perfectly conducting wall in the ground state of the system in order to obtain the atomwall force fluctuation we first define an operator directly associated to the force experienced by the atom considered as a polarizable body... | [['we', 'consider', 'the', 'quantum', 'fluctuations', 'of', 'the', 'casimirpolder', 'force', 'between', 'a', 'neutral', 'atom', 'and', 'a', 'perfectly', 'conducting', 'wall', 'in', 'the', 'ground', 'state', 'of', 'the', 'system', 'in', 'order', 'to', 'obtain', 'the', 'atomwall', 'force', 'fluctuation', 'we', 'first', '... | [-0.16615425606902975, 0.18363072060422453, -0.12523618429326094, 0.06394748263007316, -0.010878697152321155, -0.06755918260448827, 0.033846635462787864, 0.343145927772499, -0.27156386189879134, -0.26405301317572594, 0.002259998194550952, -0.31596046974882486, -0.10121524207150707, 0.1608924795443622, 0.002766440772952... |
706.1675 | On Phases of Generic Toric Singularities | We systematically study the phases of generic toric singularities, using
methods initiated in hep-th/0612046. These correspond to Gauged Linear Sigma
Models with arbitrary charges. We show that complete information about generic
$U(1)^r$ GLSMs can be obtained by studying the GLSM Lagrangian, appropriately
modified in... | hep-th | we systematically study the phases of generic toric singularities using methods initiated in hepth0612046 these correspond to gauged linear sigma models with arbitrary charges we show that complete information about generic u1r glsms can be obtained by studying the glsm lagrangian appropriately modified in the differen... | [['we', 'systematically', 'study', 'the', 'phases', 'of', 'generic', 'toric', 'singularities', 'using', 'methods', 'initiated', 'in', 'hepth0612046', 'these', 'correspond', 'to', 'gauged', 'linear', 'sigma', 'models', 'with', 'arbitrary', 'charges', 'we', 'show', 'that', 'complete', 'information', 'about', 'generic', '... | [-0.10313699948243224, 0.13321610772265838, -0.10944352860634143, 0.1410085931330776, -0.0365732513081569, -0.1570294048780432, -0.021343290427914607, 0.3469965524684924, -0.23048779771018488, -0.28443427750697503, 0.10716278923388857, -0.23462890016917998, -0.19081991175906016, 0.11582812628207298, -0.0830314609437034... |
706.1676 | Discovery of the strongly eccentric, short-period binary nature of the
B-type system HD 313926 by the MOST satellite | The MOST photometric space mission discovered an eclipsing binary among its
guide stars in June 2006 which combines a relatively large eccentricity e =
0.20 with an orbital period of only 2.27 days. HD 313926 appears to consist of
two early-type stars of spectral type B3 - B7. It has a largest eccentricity
among know... | astro-ph | the most photometric space mission discovered an eclipsing binary among its guide stars in june 2006 which combines a relatively large eccentricity e 020 with an orbital period of only 227 days hd 313926 appears to consist of two earlytype stars of spectral type b3 b7 it has a largest eccentricity among known earlytype... | [['the', 'most', 'photometric', 'space', 'mission', 'discovered', 'an', 'eclipsing', 'binary', 'among', 'its', 'guide', 'stars', 'in', 'june', '2006', 'which', 'combines', 'a', 'relatively', 'large', 'eccentricity', 'e', '020', 'with', 'an', 'orbital', 'period', 'of', 'only', '227', 'days', 'hd', '313926', 'appears', '... | [-0.14893496463702496, 0.147788703748398, -0.08931740576743472, 0.04624354281600527, -0.15372530083951294, -0.15496023750284268, 0.07385217299570843, 0.38892264797219206, -0.15850128862788254, -0.3567889251042994, 0.0691229014868886, -0.2902183093915204, -0.059527053155613185, 0.25701526130288416, -0.13555727402052406,... |
706.1677 | Pure point diffraction implies zero entropy for Delone sets with uniform
cluster frequencies | Delone sets of finite local complexity in Euclidean space are investigated.
We show that such a set has patch counting and topological entropy 0 if it has
uniform cluster frequencies and is pure point diffractive. We also note that
the patch counting entropy is 0 whenever the repetitivity function satisfies a
certain... | math.DS math.CO | delone sets of finite local complexity in euclidean space are investigated we show that such a set has patch counting and topological entropy 0 if it has uniform cluster frequencies and is pure point diffractive we also note that the patch counting entropy is 0 whenever the repetitivity function satisfies a certain gro... | [['delone', 'sets', 'of', 'finite', 'local', 'complexity', 'in', 'euclidean', 'space', 'are', 'investigated', 'we', 'show', 'that', 'such', 'a', 'set', 'has', 'patch', 'counting', 'and', 'topological', 'entropy', '0', 'if', 'it', 'has', 'uniform', 'cluster', 'frequencies', 'and', 'is', 'pure', 'point', 'diffractive', '... | [-0.13148948704582397, 0.16187190474549965, -0.1257996491191012, 0.09119255087528101, -0.05580944464438491, -0.10269552588255869, 0.044344908704429316, 0.3671814423718455, -0.2997233733638293, -0.15793015907143448, 0.09611775745698078, -0.31905132019892335, -0.14888042273620763, 0.14329444391101046, -0.0915886675852730... |
706.1678 | Nonequilibrium Steady States of Matrix Product Form: A Solver's Guide | We consider the general problem of determining the steady state of stochastic
nonequilibrium systems such as those that have been used to model (among other
things) biological transport and traffic flow. We begin with a broad overview
of this class of driven diffusive systems - which includes exclusion processes
- fo... | cond-mat.stat-mech | we consider the general problem of determining the steady state of stochastic nonequilibrium systems such as those that have been used to model among other things biological transport and traffic flow we begin with a broad overview of this class of driven diffusive systems which includes exclusion processes focusing on... | [['we', 'consider', 'the', 'general', 'problem', 'of', 'determining', 'the', 'steady', 'state', 'of', 'stochastic', 'nonequilibrium', 'systems', 'such', 'as', 'those', 'that', 'have', 'been', 'used', 'to', 'model', 'among', 'other', 'things', 'biological', 'transport', 'and', 'traffic', 'flow', 'we', 'begin', 'with', '... | [-0.08911386649236705, 0.12882426778767442, -0.08519249245303102, 0.09009529423028563, -0.06276196128651869, -0.13511988259667512, 0.038493407659675224, 0.3454671295378173, -0.27710030845707595, -0.29260691664513605, 0.10783315648550702, -0.2498857264861114, -0.16622192857644089, 0.20715288076685778, -0.028571907311014... |
706.1679 | Ground state solutions for the nonlinear Schrodinger-Maxwell equations
with a singular potential | We prove the existence of ground state solutions for the nonlinear
Schrodinger-Maxwell equations with a singular potential.
| math.AP math-ph math.MP | we prove the existence of ground state solutions for the nonlinear schrodingermaxwell equations with a singular potential | [['we', 'prove', 'the', 'existence', 'of', 'ground', 'state', 'solutions', 'for', 'the', 'nonlinear', 'schrodingermaxwell', 'equations', 'with', 'a', 'singular', 'potential']] | [-0.2279610420741579, 0.024755383266464752, -0.08527857152854695, 0.024838918614584732, -0.06206448858275133, -0.1309093369225807, -0.03077420504654155, 0.19870262121891274, -0.274150632760104, -0.15472138092360077, 0.16666859911535592, -0.35404570838984323, -0.14827706095050364, 0.12766615839620285, 0.0415340054451542... |
706.168 | On fundamental groups related to the Hirzebruch surface F_1 | Given a projective surface and a generic projection to the plane, the braid
monodromy factorization (and thus, the braid monodromy type) of the complement
of its branch curve is one of the most important topological invariants, stable
on deformations. From this factorization, one can compute the fundamental group
of ... | math.AG | given a projective surface and a generic projection to the plane the braid monodromy factorization and thus the braid monodromy type of the complement of its branch curve is one of the most important topological invariants stable on deformations from this factorization one can compute the fundamental group of the compl... | [['given', 'a', 'projective', 'surface', 'and', 'a', 'generic', 'projection', 'to', 'the', 'plane', 'the', 'braid', 'monodromy', 'factorization', 'and', 'thus', 'the', 'braid', 'monodromy', 'type', 'of', 'the', 'complement', 'of', 'its', 'branch', 'curve', 'is', 'one', 'of', 'the', 'most', 'important', 'topological', '... | [-0.18802421316504478, 0.06807622759127602, -0.1610036724479869, 0.0556806405644036, -0.10230631865561009, -0.12279669200587603, 0.010435616721709569, 0.31636173523341615, -0.3141494458955195, -0.22464468187342088, 0.15122393952915444, -0.2579090218861691, -0.18135830803722558, 0.22862779665479643, -0.12011171033761153... |
706.1681 | Very large spontaneous electric polarization in BiFeO3 single crystals
at room temperature and its evolution under cycling fields | Electric polarization loops are measured at room temperature on highly pure
BiFeO3 single crystals synthesized by a flux growth method. Because the
crystals have a high electrical resistivity, the resulting low leakage currents
allow us to measure a large spontaneous polarization reaching 100
microC.cm^{-2}, a value ... | cond-mat.mtrl-sci | electric polarization loops are measured at room temperature on highly pure bifeo3 single crystals synthesized by a flux growth method because the crystals have a high electrical resistivity the resulting low leakage currents allow us to measure a large spontaneous polarization reaching 100 microccm2 a value never repo... | [['electric', 'polarization', 'loops', 'are', 'measured', 'at', 'room', 'temperature', 'on', 'highly', 'pure', 'bifeo3', 'single', 'crystals', 'synthesized', 'by', 'a', 'flux', 'growth', 'method', 'because', 'the', 'crystals', 'have', 'a', 'high', 'electrical', 'resistivity', 'the', 'resulting', 'low', 'leakage', 'curr... | [-0.13485802854100862, 0.24122027532061718, -0.032299799788743255, -0.05014553138675789, -0.037592589088405175, -0.10806386816004912, 0.10953201964342346, 0.39528103192026415, -0.27171915538609026, -0.3306723268718148, 0.08616566765277336, -0.29756936386227606, -0.010253133466467262, 0.21329435476412376, 0.008118468628... |
706.1682 | Asteroseismology of alpha Cen A. Evidence of rotational splitting | Asteroseismology provides a unique tool for studying stellar interiors.
Recently p modes have been detected on the bright solar-like star alpha Cen A
thanks to high-precision radial-velocity measurements. However a better
characterisation of these p modes is clearly needed to constrain theoretical
models. We observed... | astro-ph | asteroseismology provides a unique tool for studying stellar interiors recently p modes have been detected on the bright solarlike star alpha cen a thanks to highprecision radialvelocity measurements however a better characterisation of these p modes is clearly needed to constrain theoretical models we observed alpha c... | [['asteroseismology', 'provides', 'a', 'unique', 'tool', 'for', 'studying', 'stellar', 'interiors', 'recently', 'p', 'modes', 'have', 'been', 'detected', 'on', 'the', 'bright', 'solarlike', 'star', 'alpha', 'cen', 'a', 'thanks', 'to', 'highprecision', 'radialvelocity', 'measurements', 'however', 'a', 'better', 'charact... | [-0.13065321950961162, 0.1449101048627307, -0.08557772416031302, 0.05116696933533369, -0.12321781359801973, -0.08293317140444265, 0.07726089697905199, 0.37526552738750923, -0.1855271956756582, -0.3565550531712499, 0.009833699227414453, -0.26744831255337426, -0.04868515182083639, 0.23957161823089354, -0.0226161585715, 0... |
706.1683 | Simple Combined Model for Nonlinear Excitations in DNA | We propose a new simple model for DNA denaturation bases on the pendulum
model of Englander\cite{A1} and the microscopic model of Peyrard {\it et
al.},\cite{A3} so called "combined model". The main parameters of our model
are: the coupling constant $k$ along each strand, the mean stretching $y^\ast$
of the hydrogen b... | physics.bio-ph physics.atm-clus | we propose a new simple model for dna denaturation bases on the pendulum model of englandercitea1 and the microscopic model of peyrard it et alcitea3 so called combined model the main parameters of our model are the coupling constant k along each strand the mean stretching yast of the hydrogen bonds the ratio of the da... | [['we', 'propose', 'a', 'new', 'simple', 'model', 'for', 'dna', 'denaturation', 'bases', 'on', 'the', 'pendulum', 'model', 'of', 'englandercitea1', 'and', 'the', 'microscopic', 'model', 'of', 'peyrard', 'it', 'et', 'alcitea3', 'so', 'called', 'combined', 'model', 'the', 'main', 'parameters', 'of', 'our', 'model', 'are'... | [-0.15867951224538854, 0.1633895701901584, -0.02163732842753459, -0.0172655202181933, -0.04602327001684336, -0.17237955289076745, 0.08143635521422035, 0.3787955801127498, -0.27874171449658797, -0.2600752333198319, -0.005422594388778869, -0.27040653712279406, -0.12283858193622268, 0.17130667321652787, 0.0182626243853538... |
706.1684 | The Total Number of Giant Planets in Debris Disks with Central Clearings | Infrared spectra from the Spitzer Space Telescope (SSC) of many debris disks
are well fit with a single black body temperature which suggest clearings
within the disk. We assume that inside the clearing orbital instability due to
planets removes dust generating planetesimal belts and dust generated by the
outer disk ... | astro-ph | infrared spectra from the spitzer space telescope ssc of many debris disks are well fit with a single black body temperature which suggest clearings within the disk we assume that inside the clearing orbital instability due to planets removes dust generating planetesimal belts and dust generated by the outer disk that ... | [['infrared', 'spectra', 'from', 'the', 'spitzer', 'space', 'telescope', 'ssc', 'of', 'many', 'debris', 'disks', 'are', 'well', 'fit', 'with', 'a', 'single', 'black', 'body', 'temperature', 'which', 'suggest', 'clearings', 'within', 'the', 'disk', 'we', 'assume', 'that', 'inside', 'the', 'clearing', 'orbital', 'instabi... | [-0.11375659385273738, 0.16429634497174622, -0.05111259938356407, 0.08467259516746321, -0.07258391988394346, -0.021925915010332902, 0.023819864212356982, 0.34259900733447096, -0.1760314684559373, -0.3627137141426074, 0.09799930854685644, -0.28663699634118067, -0.04836329983416053, 0.15942368894429046, -0.09409942803285... |
706.1685 | Theory on Plasmon Modes of the Cell Membranes | Considering the plasmon oscillation of each layer of the cell membranes as a
quasi-particle, we introduce a simple model for the membrane collective charge
excitations, take into account the surface effective potential of the
plasmon-plasmon interaction between two layers. By using the useful Bogoliubov
transformatio... | physics.bio-ph physics.gen-ph | considering the plasmon oscillation of each layer of the cell membranes as a quasiparticle we introduce a simple model for the membrane collective charge excitations take into account the surface effective potential of the plasmonplasmon interaction between two layers by using the useful bogoliubov transformation metho... | [['considering', 'the', 'plasmon', 'oscillation', 'of', 'each', 'layer', 'of', 'the', 'cell', 'membranes', 'as', 'a', 'quasiparticle', 'we', 'introduce', 'a', 'simple', 'model', 'for', 'the', 'membrane', 'collective', 'charge', 'excitations', 'take', 'into', 'account', 'the', 'surface', 'effective', 'potential', 'of', ... | [-0.14882081846610226, 0.1715363240800798, -0.06492460739595451, 0.02649802956114598, -0.015065606897589803, -0.11784372324038339, 0.07970164430424057, 0.3571891297168773, -0.2288367123310936, -0.27622286338444757, -0.025942252999728268, -0.27945000398636466, -0.16264032940754944, 0.2035514284326727, 0.0417376774759299... |
706.1686 | A classification of CO spaces which are continuous images of compact
ordered spaces | A compact Hausdorff space X is called a CO space, if every closed subset of X
is homeomorphic to an open subset of X. Every successor ordinal with its order
topology is a CO space. We find an explicit characterization of the class K of
CO spaces which are a continuous image of a Dedkind complete totally ordered
set. ... | math.GN | a compact hausdorff space x is called a co space if every closed subset of x is homeomorphic to an open subset of x every successor ordinal with its order topology is a co space we find an explicit characterization of the class k of co spaces which are a continuous image of a dedkind complete totally ordered set the to... | [['a', 'compact', 'hausdorff', 'space', 'x', 'is', 'called', 'a', 'co', 'space', 'if', 'every', 'closed', 'subset', 'of', 'x', 'is', 'homeomorphic', 'to', 'an', 'open', 'subset', 'of', 'x', 'every', 'successor', 'ordinal', 'with', 'its', 'order', 'topology', 'is', 'a', 'co', 'space', 'we', 'find', 'an', 'explicit', 'ch... | [-0.18241180681190858, 0.15516563065145642, -0.05502153613685271, 0.03803425198457548, -0.10581938732107442, -0.11379006814475603, 0.06352754620703187, 0.3769466905693311, -0.32060739386269427, -0.15445225628635545, 0.1050937105113215, -0.3150080178174975, -0.06330184631716959, 0.141283918899946, -0.041494247265248085,... |
706.1687 | Effects of Inelastic Neutrino-Nucleus Scattering on Supernova Dynamics
and Radiated Neutrino Spectra | Based on the shell model for Gamow-Teller and the Random Phase Approximation
for forbidden transitions, we have calculated reaction rates for inelastic
neutrino-nucleus scattering (INNS) under supernova (SN) conditions, assuming a
matter composition given by Nuclear Statistical Equilibrium. The rates have
been incorp... | astro-ph hep-ex nucl-ex nucl-th | based on the shell model for gamowteller and the random phase approximation for forbidden transitions we have calculated reaction rates for inelastic neutrinonucleus scattering inns under supernova sn conditions assuming a matter composition given by nuclear statistical equilibrium the rates have been incorporated into... | [['based', 'on', 'the', 'shell', 'model', 'for', 'gamowteller', 'and', 'the', 'random', 'phase', 'approximation', 'for', 'forbidden', 'transitions', 'we', 'have', 'calculated', 'reaction', 'rates', 'for', 'inelastic', 'neutrinonucleus', 'scattering', 'inns', 'under', 'supernova', 'sn', 'conditions', 'assuming', 'a', 'm... | [-0.03740917385504064, 0.21190763837485402, -0.03088699065982062, 0.18654662479309114, -0.01869941726801227, -0.08392635020168705, 0.06456483644864487, 0.40172812304700967, -0.1848472127759898, -0.2919726394875734, 0.009025696698464107, -0.32062641691192295, 0.0016674169089162239, 0.2170995953859313, 0.0920387753069883... |
706.1688 | Continuation of connecting orbits in 3D-ODEs: (I) Point-to-cycle
connections | We propose new methods for the numerical continuation of point-to-cycle
connecting orbits in 3-dimensional autonomous ODE's using projection boundary
conditions. In our approach, the projection boundary conditions near the cycle
are formulated using an eigenfunction of the associated adjoint variational
equation, avo... | math.DS math.NA | we propose new methods for the numerical continuation of pointtocycle connecting orbits in 3dimensional autonomous odes using projection boundary conditions in our approach the projection boundary conditions near the cycle are formulated using an eigenfunction of the associated adjoint variational equation avoiding cos... | [['we', 'propose', 'new', 'methods', 'for', 'the', 'numerical', 'continuation', 'of', 'pointtocycle', 'connecting', 'orbits', 'in', '3dimensional', 'autonomous', 'odes', 'using', 'projection', 'boundary', 'conditions', 'in', 'our', 'approach', 'the', 'projection', 'boundary', 'conditions', 'near', 'the', 'cycle', 'are'... | [-0.14629287170246244, 0.02250384164116163, -0.07320020336900716, 0.05923564617886491, -0.08520620945719597, -0.1553534290348382, -0.053861546613599945, 0.3586477185559014, -0.27963976153051073, -0.2409096639279438, 0.171927047814445, -0.24419879022094867, -0.1569475215981188, 0.24860195177404776, -0.05759871963249601,... |
706.1689 | Wigner crystallization in a single and bilayer graphene | We study the possibility of Wigner crystallization in both single- and and
bi-layer graphene using a real space tight binding model. In addition to
verifying our earlier prediction for single layer graphene, we predict that the
bilayer graphene can undergo a Wigner crystal transition at low enough carrier
density thu... | cond-mat.str-el cond-mat.mes-hall | we study the possibility of wigner crystallization in both single and and bilayer graphene using a real space tight binding model in addition to verifying our earlier prediction for single layer graphene we predict that the bilayer graphene can undergo a wigner crystal transition at low enough carrier density thus offe... | [['we', 'study', 'the', 'possibility', 'of', 'wigner', 'crystallization', 'in', 'both', 'single', 'and', 'and', 'bilayer', 'graphene', 'using', 'a', 'real', 'space', 'tight', 'binding', 'model', 'in', 'addition', 'to', 'verifying', 'our', 'earlier', 'prediction', 'for', 'single', 'layer', 'graphene', 'we', 'predict', '... | [-0.14715787151499707, 0.2157038681811708, -0.05271398278008051, -0.006802181937896153, -0.014372112145921325, -0.15801201327429976, 0.14393840953707696, 0.427440884884666, -0.2677910825018497, -0.27800714380162606, -0.06029478973051643, -0.2805838933762382, -0.18142420525854344, 0.10721296048175324, 0.0652952903662534... |
706.169 | Direct observation of the strange b baryon Xi_b^{-} | We report the first direct observation of the strange b baryon Xi_b^{-}. We
reconstruct the decay Xi_b^{-} to J/psi Xi^{-}, with J/psi to dimuons and
Xi^{-} to Lambda pion, in ppbar collisions at sqrt(s) = 1.96 TeV. Using 1.3
fb^{-1} of data collected by the D0 detector, we observe 15.2 +/- 4.4(stat.)+
1.9/-0.4(syst.... | hep-ex | we report the first direct observation of the strange b baryon xi_b we reconstruct the decay xi_b to jpsi xi with jpsi to dimuons and xi to lambda pion in ppbar collisions at sqrts 196 tev using 13 fb1 of data collected by the d0 detector we observe 152 44stat 1904syst xi_b candidates at a mass of 5774 0011stat 0015 sy... | [['we', 'report', 'the', 'first', 'direct', 'observation', 'of', 'the', 'strange', 'b', 'baryon', 'xi_b', 'we', 'reconstruct', 'the', 'decay', 'xi_b', 'to', 'jpsi', 'xi', 'with', 'jpsi', 'to', 'dimuons', 'and', 'xi', 'to', 'lambda', 'pion', 'in', 'ppbar', 'collisions', 'at', 'sqrts', '196', 'tev', 'using', '13', 'fb1',... | [-0.07031800487425689, 0.21565256587357498, -0.09988281805086516, 0.12514213438479083, -0.015922023476484942, -0.09707930210667352, 0.08469421522207923, 0.29342142905236457, -0.19199457015915244, -0.30182969346231614, -0.079525465110326, -0.4604140131131691, 0.1572631649837336, 0.08986525127764645, 0.07129057946925361,... |
706.1691 | A Stochastic Measure for Eternal Inflation | We use the stochastic approach to investigate the measure for slow roll
eternal inflation. The probability for the universe of a given Hubble radius
can be calculated in this framework. In a solvable model, it is shown that the
probability for the universe to evolve from a state with a smaller Hubble
radius to that o... | hep-th astro-ph gr-qc | we use the stochastic approach to investigate the measure for slow roll eternal inflation the probability for the universe of a given hubble radius can be calculated in this framework in a solvable model it is shown that the probability for the universe to evolve from a state with a smaller hubble radius to that of a l... | [['we', 'use', 'the', 'stochastic', 'approach', 'to', 'investigate', 'the', 'measure', 'for', 'slow', 'roll', 'eternal', 'inflation', 'the', 'probability', 'for', 'the', 'universe', 'of', 'a', 'given', 'hubble', 'radius', 'can', 'be', 'calculated', 'in', 'this', 'framework', 'in', 'a', 'solvable', 'model', 'it', 'is', ... | [-0.0867927787688901, 0.186098180576944, -0.1265290375942221, 0.11493607098796368, -0.07218194370999789, -0.12314452581519547, 0.004883111481411526, 0.29519055586066456, -0.2649983013084588, -0.2550918133033869, 0.0653972030559089, -0.22302654570935723, -0.062284099887340114, 0.20283853572282867, -0.06090698676864402, ... |
706.1692 | A Methodology for Efficient Space-Time Adapter Design Space Exploration:
A Case Study of an Ultra Wide Band Interleaver | This paper presents a solution to efficiently explore the design space of
communication adapters. In most digital signal processing (DSP) applications,
the overall architecture of the system is significantly affected by
communication architecture, so the designers need specifically optimized
adapters. By explicitly m... | cs.AR | this paper presents a solution to efficiently explore the design space of communication adapters in most digital signal processing dsp applications the overall architecture of the system is significantly affected by communication architecture so the designers need specifically optimized adapters by explicitly modeling ... | [['this', 'paper', 'presents', 'a', 'solution', 'to', 'efficiently', 'explore', 'the', 'design', 'space', 'of', 'communication', 'adapters', 'in', 'most', 'digital', 'signal', 'processing', 'dsp', 'applications', 'the', 'overall', 'architecture', 'of', 'the', 'system', 'is', 'significantly', 'affected', 'by', 'communic... | [-0.19632874479199328, -0.013485428139286274, -0.06479284800286216, 0.012839766662204412, -0.14844963891333257, -0.21056295368759856, 0.059479666193303596, 0.4227107432254446, -0.2953611311883234, -0.38575267820520615, 0.0856060742502805, -0.20017360514257013, -0.2190185861730176, 0.16659374500064528, -0.12307966904283... |
706.1693 | Unsymmetrical and symmetrical one-range addition theorems for Slater
type orbitals and Coulomb-Yukawa like correlated interaction potentials of
integer and noninteger indices | Using one-center expansion relations for the Slater type orbitals (STOs) of
noninteger principal quantum numbers in terms of integer n STOs derived in this
study with the help of - exponential type orbitals (-ETOs, the general formulas
are established for the unsymmetrical and symmetrical one-range addition
theorems ... | physics.chem-ph | using onecenter expansion relations for the slater type orbitals stos of noninteger principal quantum numbers in terms of integer n stos derived in this study with the help of exponential type orbitals etos the general formulas are established for the unsymmetrical and symmetrical onerange addition theorems of stos and... | [['using', 'onecenter', 'expansion', 'relations', 'for', 'the', 'slater', 'type', 'orbitals', 'stos', 'of', 'noninteger', 'principal', 'quantum', 'numbers', 'in', 'terms', 'of', 'integer', 'n', 'stos', 'derived', 'in', 'this', 'study', 'with', 'the', 'help', 'of', 'exponential', 'type', 'orbitals', 'etos', 'the', 'gene... | [-0.14157323452777096, 0.13004514595404976, -0.0024378397635051183, 0.10570473234790066, 0.04136399428936697, -0.17163679512395036, 0.024959914927326497, 0.3051075457462243, -0.21396571908678327, -0.25386203335864205, 0.02495126817153678, -0.28405694063930287, -0.18867166361416735, 0.20703430773989698, 0.03727241982996... |
706.1694 | Ricci Flow of Biaxial Bianchi IX Metrics | We use the Ricci flow with surgery to study four-dimensional SU(2) x
U(1)-symmetric metrics on a manifold with fixed boundary given by a squashed
3-sphere. Depending on the initial metric we show that the flow converges to
either the Taub-Bolt or the Taub-NUT metric, the latter case potentially
requiring surgery at s... | hep-th | we use the ricci flow with surgery to study fourdimensional su2 x u1symmetric metrics on a manifold with fixed boundary given by a squashed 3sphere depending on the initial metric we show that the flow converges to either the taubbolt or the taubnut metric the latter case potentially requiring surgery at some point in ... | [['we', 'use', 'the', 'ricci', 'flow', 'with', 'surgery', 'to', 'study', 'fourdimensional', 'su2', 'x', 'u1symmetric', 'metrics', 'on', 'a', 'manifold', 'with', 'fixed', 'boundary', 'given', 'by', 'a', 'squashed', '3sphere', 'depending', 'on', 'the', 'initial', 'metric', 'we', 'show', 'that', 'the', 'flow', 'converges'... | [-0.1716158176977735, 0.082678294855663, -0.13234071046223536, 0.03645383854506209, -0.1285757631090853, -0.16536286532714525, -0.009371181928059634, 0.3434030024006086, -0.2035184070796651, -0.24861840114873998, 0.1261547612368732, -0.28200388443673385, -0.1743217571008512, 0.13551939586451386, -0.13584101930096307, 0... |
706.1695 | Long-time convergence of an Adaptive Biasing Force method | We propose a proof of convergence of an adaptive method used in molecular
dynamics to compute free energy profiles. Mathematically, it amounts to
studying the long-time behavior of a stochastic process which satisfies a
non-linear stochastic differential equation, where the drift depends on
conditional expectations o... | math.AP cond-mat.stat-mech physics.comp-ph | we propose a proof of convergence of an adaptive method used in molecular dynamics to compute free energy profiles mathematically it amounts to studying the longtime behavior of a stochastic process which satisfies a nonlinear stochastic differential equation where the drift depends on conditional expectations of some ... | [['we', 'propose', 'a', 'proof', 'of', 'convergence', 'of', 'an', 'adaptive', 'method', 'used', 'in', 'molecular', 'dynamics', 'to', 'compute', 'free', 'energy', 'profiles', 'mathematically', 'it', 'amounts', 'to', 'studying', 'the', 'longtime', 'behavior', 'of', 'a', 'stochastic', 'process', 'which', 'satisfies', 'a',... | [-0.09195409187426169, 0.03710528591205181, -0.17625906874263098, 0.11186288227540828, -0.055785843991630134, -0.1026759251863474, 0.033352896386373135, 0.3103114126272322, -0.3414757966418706, -0.22231148354827412, 0.08635920394648103, -0.245700635814241, -0.14115427147656207, 0.1817276869227903, -0.07794185608093228,... |
706.1696 | Minimal Walking Technicolor: Set Up for Collider Physics | Different theoretical and phenomenological aspects of the Minimal and
Nonminimal Walking Technicolor theories have recently been studied. The goal
here is to make the models ready for collider phenomenology. We do this by
constructing the low energy effective theory containing scalars, pseudoscalars,
vector mesons an... | hep-ph | different theoretical and phenomenological aspects of the minimal and nonminimal walking technicolor theories have recently been studied the goal here is to make the models ready for collider phenomenology we do this by constructing the low energy effective theory containing scalars pseudoscalars vector mesons and othe... | [['different', 'theoretical', 'and', 'phenomenological', 'aspects', 'of', 'the', 'minimal', 'and', 'nonminimal', 'walking', 'technicolor', 'theories', 'have', 'recently', 'been', 'studied', 'the', 'goal', 'here', 'is', 'to', 'make', 'the', 'models', 'ready', 'for', 'collider', 'phenomenology', 'we', 'do', 'this', 'by',... | [-0.06969190114314723, 0.21430771096321918, -0.1284617471105508, 0.1544391468675766, -0.12452096604016226, -0.19673028734498932, 0.009778013317640322, 0.34281466093243046, -0.2024313846777659, -0.30745701886275234, 0.0439773453741937, -0.26801301744896644, -0.15253610766547568, 0.10728702725592644, 0.011025987839435829... |
706.1697 | Equations of motion approach to the spin-1/2 Ising model on the Bethe
lattice | We exactly solve the ferromagnetic spin-1/2 Ising model on the Bethe lattice
in the presence of an external magnetic field by means of the equations of
motion method within the Green's function formalism. In particular, such an
approach is applied to an isomorphic model of localized Fermi particles
interacting via an... | cond-mat.stat-mech cond-mat.str-el | we exactly solve the ferromagnetic spin12 ising model on the bethe lattice in the presence of an external magnetic field by means of the equations of motion method within the greens function formalism in particular such an approach is applied to an isomorphic model of localized fermi particles interacting via an inters... | [['we', 'exactly', 'solve', 'the', 'ferromagnetic', 'spin12', 'ising', 'model', 'on', 'the', 'bethe', 'lattice', 'in', 'the', 'presence', 'of', 'an', 'external', 'magnetic', 'field', 'by', 'means', 'of', 'the', 'equations', 'of', 'motion', 'method', 'within', 'the', 'greens', 'function', 'formalism', 'in', 'particular'... | [-0.1376081890569207, 0.12750824437723743, -0.05848532630031118, 0.05537400236273298, -0.04836402919840153, -0.10058755126518716, 0.014737651441672831, 0.3491974904393877, -0.2590864990262016, -0.26914347387416615, 0.008554084862774338, -0.30746198287920207, -0.11859904565023728, 0.16294535891088935, 0.0639075650033747... |
706.1698 | The Explicit Chaotic Representation of the powers of increments of Levy
Processes | An explicit formula for the chaotic representation of the powers of
increments, (X_{t+t_0}-X_{t_0})^n, of a Levy process is presented. There are
two different chaos expansions of a square integrable functional of a Levy
process: one with respect to the compensated Poisson random measure and the
other with respect to ... | math.PR math.ST stat.TH | an explicit formula for the chaotic representation of the powers of increments x_tt_0x_t_0n of a levy process is presented there are two different chaos expansions of a square integrable functional of a levy process one with respect to the compensated poisson random measure and the other with respect to the orthogonal ... | [['an', 'explicit', 'formula', 'for', 'the', 'chaotic', 'representation', 'of', 'the', 'powers', 'of', 'increments', 'x_tt_0x_t_0n', 'of', 'a', 'levy', 'process', 'is', 'presented', 'there', 'are', 'two', 'different', 'chaos', 'expansions', 'of', 'a', 'square', 'integrable', 'functional', 'of', 'a', 'levy', 'process', ... | [-0.139292450728161, 0.12247916899359552, -0.11208430303349382, 0.06970643481498492, -0.05686291348455208, -0.0725507760952626, 0.014576632120380444, 0.35364208154025534, -0.28258776973400795, -0.20352442315668753, 0.1306780456277054, -0.2610382560551876, -0.16248609983317908, 0.2151448412221812, -0.06497560929551366, ... |
706.1699 | OPERA first events from the CNGS neutrino beam | The aim of the OPERA experiment is to search for the appearance of the tau
neutrino in the quasi pure muon neutrino beam produced at CERN (CNGS). The
detector, installed in the Gran Sasso underground laboratory 730 km away from
CERN, consists of a lead/emulsion target complemented with electronic
detectors. A report ... | hep-ex | the aim of the opera experiment is to search for the appearance of the tau neutrino in the quasi pure muon neutrino beam produced at cern cngs the detector installed in the gran sasso underground laboratory 730 km away from cern consists of a leademulsion target complemented with electronic detectors a report is given ... | [['the', 'aim', 'of', 'the', 'opera', 'experiment', 'is', 'to', 'search', 'for', 'the', 'appearance', 'of', 'the', 'tau', 'neutrino', 'in', 'the', 'quasi', 'pure', 'muon', 'neutrino', 'beam', 'produced', 'at', 'cern', 'cngs', 'the', 'detector', 'installed', 'in', 'the', 'gran', 'sasso', 'underground', 'laboratory', '73... | [-0.06988947227282423, 0.21427488525588276, -0.09067912572061072, 0.06524441534535251, -0.035358833332716576, -0.12340057992153394, 0.020061417207331726, 0.2770412073234542, -0.13705032625281527, -0.34082936765757244, 0.08649138307434992, -0.3950557839322153, 0.059339193646914104, 0.22719710937071538, 0.060750132610260... |
706.17 | Information Criteria and Arithmetic Codings : An Illustration on Raw
Images | In this paper we give a short theoretical description of the general
predictive adaptive arithmetic coding technique. The links between this
technique and the works of J. Rissanen in the 80's, in particular the BIC
information criterion used in parametrical model selection problems, are
established. We also design lo... | cs.IT math.IT | in this paper we give a short theoretical description of the general predictive adaptive arithmetic coding technique the links between this technique and the works of j rissanen in the 80s in particular the bic information criterion used in parametrical model selection problems are established we also design lossless a... | [['in', 'this', 'paper', 'we', 'give', 'a', 'short', 'theoretical', 'description', 'of', 'the', 'general', 'predictive', 'adaptive', 'arithmetic', 'coding', 'technique', 'the', 'links', 'between', 'this', 'technique', 'and', 'the', 'works', 'of', 'j', 'rissanen', 'in', 'the', '80s', 'in', 'particular', 'the', 'bic', 'i... | [-0.07559527802399137, -0.01077954556280993, -0.16220883092626562, 0.10183720858226543, -0.07028310636425732, -0.2075896873171638, 0.08070786233456857, 0.4284884111929527, -0.2705503184459841, -0.27975729754535666, 0.10614736470279881, -0.21577658380617873, -0.2166578109822118, 0.23356480695615509, -0.16568285281914222... |
706.1701 | Constraints, MMSNP and expander relational structures | We give a poly-time construction for a combinatorial classic known as Sparse
Incomparability Lemma, studied by Erdos, Lovasz, Nesetril, Rodl and others: We
show that every Constraint Satisfaction Problem is poly-time equivalent to its
restriction to structures with large girth. This implies that the complexity
classe... | math.CO | we give a polytime construction for a combinatorial classic known as sparse incomparability lemma studied by erdos lovasz nesetril rodl and others we show that every constraint satisfaction problem is polytime equivalent to its restriction to structures with large girth this implies that the complexity classes csp and ... | [['we', 'give', 'a', 'polytime', 'construction', 'for', 'a', 'combinatorial', 'classic', 'known', 'as', 'sparse', 'incomparability', 'lemma', 'studied', 'by', 'erdos', 'lovasz', 'nesetril', 'rodl', 'and', 'others', 'we', 'show', 'that', 'every', 'constraint', 'satisfaction', 'problem', 'is', 'polytime', 'equivalent', '... | [-0.1306035109071268, 0.04500977082384957, -0.04388697816886836, 0.1602613790335858, -0.15139945615794406, -0.17478136748282447, 0.07255164959286857, 0.3227885699727469, -0.36566211175587443, -0.29843059425345725, 0.09278906402178108, -0.2049071629298851, -0.17824409452991352, 0.15044680509923233, -0.18802588833495976,... |
706.1702 | Theory of the Pseudospin Resonance in Semiconductor Bilayers | The pseudospin degree of freedom in a semiconductor bilayer gives rise to a
collective mode analogous to the ferromagnetic resonance mode of a ferromagnet.
We present a theory of the dependence of the energy and the damping of this
mode on layer separation $d$. Based on these results, we discuss the
possibility of re... | cond-mat.mes-hall cond-mat.str-el | the pseudospin degree of freedom in a semiconductor bilayer gives rise to a collective mode analogous to the ferromagnetic resonance mode of a ferromagnet we present a theory of the dependence of the energy and the damping of this mode on layer separation d based on these results we discuss the possibility of realizing... | [['the', 'pseudospin', 'degree', 'of', 'freedom', 'in', 'a', 'semiconductor', 'bilayer', 'gives', 'rise', 'to', 'a', 'collective', 'mode', 'analogous', 'to', 'the', 'ferromagnetic', 'resonance', 'mode', 'of', 'a', 'ferromagnet', 'we', 'present', 'a', 'theory', 'of', 'the', 'dependence', 'of', 'the', 'energy', 'and', 't... | [-0.23548444536321894, 0.18041854835886123, -0.07065065695647278, -0.022907290874643188, -0.0590610572554428, -0.129189175505448, 0.09219604732813956, 0.32788998405609665, -0.2346388369895004, -0.2534308555246941, -0.008784569421550259, -0.27370988890721365, -0.15256794538862747, 0.18724603653917538, 0.0364703617765214... |
706.1703 | Correlation between galactic HI and the Cosmic Microwave Background | We revisit the issue of a correlation between the atomic hydrogen gas in our
local Galaxy and the Cosmic Microwave Background (CMB), a detection of which
has been claimed in some literature. We cross-correlate the 21-cm emission of
Galactic atomic hydrogen as traced by the Leiden/Argentine/Bonn Galactic HI
survey wit... | astro-ph | we revisit the issue of a correlation between the atomic hydrogen gas in our local galaxy and the cosmic microwave background cmb a detection of which has been claimed in some literature we crosscorrelate the 21cm emission of galactic atomic hydrogen as traced by the leidenargentinebonn galactic hi survey with the 3yea... | [['we', 'revisit', 'the', 'issue', 'of', 'a', 'correlation', 'between', 'the', 'atomic', 'hydrogen', 'gas', 'in', 'our', 'local', 'galaxy', 'and', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'a', 'detection', 'of', 'which', 'has', 'been', 'claimed', 'in', 'some', 'literature', 'we', 'crosscorrelate', 'the', '21c... | [-0.0804815074281158, 0.05931793398355158, -0.02411618470572508, 0.08050517265040141, -0.06359116553973693, 0.002682397374883294, -0.005690307774318335, 0.3970756471061554, -0.1992035563617276, -0.3137082463751237, 0.005934049760421308, -0.37980273896111894, -0.011552106147297682, 0.19829560523160183, 0.104710547480350... |
706.1704 | Forbidden lists (NP and CSP for combinatorialists) | We present a definition of the class NP in combinatorial context as the set
of languages of structures defined by finitely many forbidden lifted
substructures. We apply this to special syntactically defined subclasses and
show how they correspond to naturally defined (and intensively studied)
combinatorial problems. ... | math.CO | we present a definition of the class np in combinatorial context as the set of languages of structures defined by finitely many forbidden lifted substructures we apply this to special syntactically defined subclasses and show how they correspond to naturally defined and intensively studied combinatorial problems we sho... | [['we', 'present', 'a', 'definition', 'of', 'the', 'class', 'np', 'in', 'combinatorial', 'context', 'as', 'the', 'set', 'of', 'languages', 'of', 'structures', 'defined', 'by', 'finitely', 'many', 'forbidden', 'lifted', 'substructures', 'we', 'apply', 'this', 'to', 'special', 'syntactically', 'defined', 'subclasses', 'a... | [-0.10920824176382, 0.036563983452089915, -0.028307433405037347, 0.12988405460416058, -0.13276491055219639, -0.11925367769081055, 0.05603513319037733, 0.34926634156372305, -0.3869759837597063, -0.34385443077142525, 0.08374175765623558, -0.19772187277591385, -0.16497443349865393, 0.18762865739049223, -0.1382852768993035... |
706.1705 | Investigations of Ra$^+$ properties to test possibilities of new optical
frequency standards | The present work tests the suitability of the narrow transitions $7s \
^2S_{1/2} \to 6d ^2D_{3/2}$ and $7s ^2S_{1/2} \to 6d ^2D_{5/2}$ in Ra$^+$ for
optical frequency standard studies. Our calculations of the lifetimes of the
metastable $6d$ states using the relativistic coupled-cluster theory suggest
that they are s... | physics.atom-ph physics.optics | the present work tests the suitability of the narrow transitions 7s 2s_12 to 6d 2d_32 and 7s 2s_12 to 6d 2d_52 in ra for optical frequency standard studies our calculations of the lifetimes of the metastable 6d states using the relativistic coupledcluster theory suggest that they are sufficiently long for ra to be cons... | [['the', 'present', 'work', 'tests', 'the', 'suitability', 'of', 'the', 'narrow', 'transitions', '7s', '2s_12', 'to', '6d', '2d_32', 'and', '7s', '2s_12', 'to', '6d', '2d_52', 'in', 'ra', 'for', 'optical', 'frequency', 'standard', 'studies', 'our', 'calculations', 'of', 'the', 'lifetimes', 'of', 'the', 'metastable', '6... | [-0.09388336938024423, 0.18109728731686683, 0.03474868562316051, 0.0350880867081705, 0.07398854140406368, -0.09696134213550851, 0.07793335261321145, 0.3750856166127427, -0.13552163763442773, -0.2715654362249991, -0.007268897339369802, -0.25523771332769557, -0.059121256501510226, 0.1132263837826449, 0.08142218512921841,... |
706.1706 | Spatiotemporal structure of Lyapunov vectors in chaotic coupled-map
lattices | The spatiotemporal dynamics of Lyapunov vectors (LVs) in spatially extended
chaotic systems is studied by means of coupled-map lattices. We determine
intrinsic length scales and spatiotemporal correlations of LVs corresponding to
the leading unstable directions by translating the problem to the language of
scale-inva... | nlin.CD cond-mat.stat-mech | the spatiotemporal dynamics of lyapunov vectors lvs in spatially extended chaotic systems is studied by means of coupledmap lattices we determine intrinsic length scales and spatiotemporal correlations of lvs corresponding to the leading unstable directions by translating the problem to the language of scaleinvariant g... | [['the', 'spatiotemporal', 'dynamics', 'of', 'lyapunov', 'vectors', 'lvs', 'in', 'spatially', 'extended', 'chaotic', 'systems', 'is', 'studied', 'by', 'means', 'of', 'coupledmap', 'lattices', 'we', 'determine', 'intrinsic', 'length', 'scales', 'and', 'spatiotemporal', 'correlations', 'of', 'lvs', 'corresponding', 'to',... | [-0.17602552047972886, 0.1276143151403898, -0.11555135278396454, 0.12584608670337782, 0.005928086735509044, -0.13561419077735742, -0.026595124573099847, 0.3473216929018164, -0.3196545112421553, -0.23221654543087034, 0.08023726008033526, -0.24702072636607816, -0.2049153507413233, 0.18310377154814297, -0.0229348024243817... |
706.1707 | The centrality dependence of elliptic flow at LHC | We present predictions for the centrality dependence of elliptic flow at
mid-rapidity in Pb-Pb collisions at the LHC.
| nucl-th | we present predictions for the centrality dependence of elliptic flow at midrapidity in pbpb collisions at the lhc | [['we', 'present', 'predictions', 'for', 'the', 'centrality', 'dependence', 'of', 'elliptic', 'flow', 'at', 'midrapidity', 'in', 'pbpb', 'collisions', 'at', 'the', 'lhc']] | [-0.06543201197766596, 0.20820141050757635, -0.326465938705951, 0.09694693113366763, 0.06478058733046055, -0.12084203441109923, -0.2504005104743151, 0.3408501785662439, -0.20339292743139797, -0.24847142512185705, -0.15132962819835585, -0.5054083249221245, 0.23572069926497838, 0.1434815920268496, 0.10337106645521191, 0.... |
706.1708 | Effective Actions of IIB Matrix Model on S^3 | S^3 is a simple principle bundle which is locally S^2 \times S^1. It has been
shown that such a space can be constructed in terms of matrix models. It has
been also shown that such a space can be realized by a generalized
compactification procedure in the S^1 direction. We investigate the effective
action of supersym... | hep-th | s3 is a simple principle bundle which is locally s2 times s1 it has been shown that such a space can be constructed in terms of matrix models it has been also shown that such a space can be realized by a generalized compactification procedure in the s1 direction we investigate the effective action of supersymmetric gau... | [['s3', 'is', 'a', 'simple', 'principle', 'bundle', 'which', 'is', 'locally', 's2', 'times', 's1', 'it', 'has', 'been', 'shown', 'that', 'such', 'a', 'space', 'can', 'be', 'constructed', 'in', 'terms', 'of', 'matrix', 'models', 'it', 'has', 'been', 'also', 'shown', 'that', 'such', 'a', 'space', 'can', 'be', 'realized',... | [-0.11084510314665262, 0.1999522857737939, -0.10108719188654401, 0.12837327355568126, -0.06946532422033938, -0.15305545683097566, -0.034873435345911225, 0.40059911359993505, -0.20999400286515518, -0.2470312794673742, 0.13353314083381096, -0.2700024511153534, -0.179819007548438, 0.1632613662505706, -0.07595695174810752,... |
706.1709 | The Higher Order Schwarzian Derivative: Its Applications for Chaotic
Behavior and New Invariant Sufficient Condition of Chaos | The Schwarzian derivative of a function f(x) which is defined in the interval
(a, b) having higher order derivatives is given by
Sf(x)=(f''(x)/f'(x))'-1/2(f''(x)/f'(x))^2 . A sufficient condition for a
function to behave chaotically is that its Schwarzian derivative is negative.
In this paper, we try to find a suffic... | nlin.CD | the schwarzian derivative of a function fx which is defined in the interval a b having higher order derivatives is given by sfxfxfx12fxfx2 a sufficient condition for a function to behave chaotically is that its schwarzian derivative is negative in this paper we try to find a sufficient condition for a nonlinear dynamic... | [['the', 'schwarzian', 'derivative', 'of', 'a', 'function', 'fx', 'which', 'is', 'defined', 'in', 'the', 'interval', 'a', 'b', 'having', 'higher', 'order', 'derivatives', 'is', 'given', 'by', 'sfxfxfx12fxfx2', 'a', 'sufficient', 'condition', 'for', 'a', 'function', 'to', 'behave', 'chaotically', 'is', 'that', 'its', 's... | [-0.18298852732454343, 0.07571671996581326, -0.08614811442716037, 0.06517107031313042, -0.0959585549669567, -0.10288165276438964, -0.043075385172703554, 0.29115805745361345, -0.3007539716997632, -0.23912113653643738, 0.13083863240683935, -0.274560179837324, -0.21177608310984122, 0.12799507508143074, -0.0322718167980571... |
706.171 | New method for atmospheric calibration at the Pierre Auger Observatory
using FRAM, a robotic astronomical telescope | FRAM - F/(Ph)otometric Robotic Atmospheric Monitor is the latest addition to
the atmospheric monitoring instruments of the Pierre Auger Observatory. An
optical telescope equipped with CCD camera and photometer, it automatically
observes a set of selected standard stars and a calibrated terrestrial source.
Primarily, ... | astro-ph | fram fphotometric robotic atmospheric monitor is the latest addition to the atmospheric monitoring instruments of the pierre auger observatory an optical telescope equipped with ccd camera and photometer it automatically observes a set of selected standard stars and a calibrated terrestrial source primarily the wavelen... | [['fram', 'fphotometric', 'robotic', 'atmospheric', 'monitor', 'is', 'the', 'latest', 'addition', 'to', 'the', 'atmospheric', 'monitoring', 'instruments', 'of', 'the', 'pierre', 'auger', 'observatory', 'an', 'optical', 'telescope', 'equipped', 'with', 'ccd', 'camera', 'and', 'photometer', 'it', 'automatically', 'observ... | [-0.11320841472299226, 0.12302830296919363, -0.07462527929492031, 0.05684992120667171, -0.1083949957026449, -0.10847448053629657, 0.015033032722973091, 0.43887105940190035, -0.2132139588640261, -0.37202484482915793, 0.13111575572458878, -0.2887120327038641, -0.07312492063615174, 0.3102531049491228, -0.05353008813494651... |
706.1711 | Ergodicity of the extended anisotropic 1D Heisenberg model: response at
low temperatures | We present the results of exact diagonalization calculations of the isolated
and isothermal on-site static susceptibilities in the anisotropic extended
Heisenberg model on a linear chain with periodic boundary conditions. Based on
the ergodicity considerations we conclude that the isothermal susceptibility
will diver... | cond-mat.str-el cond-mat.soft | we present the results of exact diagonalization calculations of the isolated and isothermal onsite static susceptibilities in the anisotropic extended heisenberg model on a linear chain with periodic boundary conditions based on the ergodicity considerations we conclude that the isothermal susceptibility will diverge a... | [['we', 'present', 'the', 'results', 'of', 'exact', 'diagonalization', 'calculations', 'of', 'the', 'isolated', 'and', 'isothermal', 'onsite', 'static', 'susceptibilities', 'in', 'the', 'anisotropic', 'extended', 'heisenberg', 'model', 'on', 'a', 'linear', 'chain', 'with', 'periodic', 'boundary', 'conditions', 'based',... | [-0.20679480938071554, 0.16338329901213222, -0.0897424661582618, 0.05698542212220756, -0.012253348853185096, -0.12872927097575457, 0.07501307083999342, 0.3607030137244499, -0.21027812322206568, -0.20217768297615377, 0.13979587832000107, -0.31254521463856555, -0.10917577752490726, 0.15798176755197346, 0.0797387382551801... |
706.1712 | Test Functions Space in Noncommutative Quantum Field Theory | It is proven that the $\star$-product of field operators implies that the
space of test functions in the Wightman approach to noncommutative quantum
field theory is one of the Gel'fand-Shilov spaces $S^{\beta}$ with $\beta <
1/2$. This class of test functions smears the noncommutative Wightman
functions, which are in... | hep-th | it is proven that the starproduct of field operators implies that the space of test functions in the wightman approach to noncommutative quantum field theory is one of the gelfandshilov spaces sbeta with beta 12 this class of test functions smears the noncommutative wightman functions which are in this case generalized... | [['it', 'is', 'proven', 'that', 'the', 'starproduct', 'of', 'field', 'operators', 'implies', 'that', 'the', 'space', 'of', 'test', 'functions', 'in', 'the', 'wightman', 'approach', 'to', 'noncommutative', 'quantum', 'field', 'theory', 'is', 'one', 'of', 'the', 'gelfandshilov', 'spaces', 'sbeta', 'with', 'beta', '12', '... | [-0.08768619982292876, 0.11184638835838996, -0.13641062781680374, 0.16524549635505537, -0.036869934576679954, -0.08897964307107031, -0.0431324472578126, 0.31634194422513245, -0.2186124248779379, -0.21645717285573482, 0.048290650820854354, -0.20856164279393852, -0.1769020759500563, 0.21324530785204843, -0.06112712085523... |
706.1713 | Dynamics of the giant planets of the solar system in the gaseous
proto-planetary disk and relationship to the current orbital architecture | We study the orbital evolution of the 4 giant planets of our solar system in
a gas disk. Our investigation extends the previous works by Masset and
Snellgrove (2001) and Morbidelli and Crida (2007, MC07), which focussed on the
dynamics of the Jupiter-Saturn system. The only systems that we found to reach
a steady sta... | astro-ph | we study the orbital evolution of the 4 giant planets of our solar system in a gas disk our investigation extends the previous works by masset and snellgrove 2001 and morbidelli and crida 2007 mc07 which focussed on the dynamics of the jupitersaturn system the only systems that we found to reach a steady state are thos... | [['we', 'study', 'the', 'orbital', 'evolution', 'of', 'the', '4', 'giant', 'planets', 'of', 'our', 'solar', 'system', 'in', 'a', 'gas', 'disk', 'our', 'investigation', 'extends', 'the', 'previous', 'works', 'by', 'masset', 'and', 'snellgrove', '2001', 'and', 'morbidelli', 'and', 'crida', '2007', 'mc07', 'which', 'focus... | [-0.1559595914185169, 0.13644522868818482, -0.05670079605468593, 0.03433890262599157, -0.010503329490238304, -0.05682288234595073, 0.042421388099730714, 0.3403959787153293, -0.1965333688303253, -0.33008069250030514, 0.10858395889325857, -0.2663771678883758, -0.11022005995360071, 0.20621890992813632, -0.0469018358082622... |
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