id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.4635 | Color superconductivity in dense quark matter | Matter at high density and low temperature is expected to be a color
superconductor, which is a degenerate Fermi gas of quarks with a condensate of
Cooper pairs near the Fermi surface that induces color Meissner effects. At the
highest densities, where the QCD coupling is weak, rigorous calculations are
possible, and... | hep-ph astro-ph cond-mat.supr-con nucl-th | matter at high density and low temperature is expected to be a color superconductor which is a degenerate fermi gas of quarks with a condensate of cooper pairs near the fermi surface that induces color meissner effects at the highest densities where the qcd coupling is weak rigorous calculations are possible and the gr... | [['matter', 'at', 'high', 'density', 'and', 'low', 'temperature', 'is', 'expected', 'to', 'be', 'a', 'color', 'superconductor', 'which', 'is', 'a', 'degenerate', 'fermi', 'gas', 'of', 'quarks', 'with', 'a', 'condensate', 'of', 'cooper', 'pairs', 'near', 'the', 'fermi', 'surface', 'that', 'induces', 'color', 'meissner',... | [-0.15633965281457854, 0.30064794436793296, -0.133136860750637, 0.10572205876982396, -0.06834615398085965, -0.11212425169952471, 0.0942682950595533, 0.35235952342935334, -0.2032646216992717, -0.28858899217280937, 0.04192705697717209, -0.2866883117186398, -0.04652315513337909, 0.09881413331919017, 0.0027647486903929503,... |
709.4636 | Gauge-invariant coherent states for Loop Quantum Gravity II: Non-abelian
gauge groups | This is the second paper concerning gauge-invariant coherent states for Loop
Quantum Gravity. Here, we deal with the gauge group SU(2), this being a
significant complication compared to the abelian U(1) case encountered in the
previous article. We study gauge-invariant coherent states on certain special
graphs by ana... | gr-qc | this is the second paper concerning gaugeinvariant coherent states for loop quantum gravity here we deal with the gauge group su2 this being a significant complication compared to the abelian u1 case encountered in the previous article we study gaugeinvariant coherent states on certain special graphs by analytical and ... | [['this', 'is', 'the', 'second', 'paper', 'concerning', 'gaugeinvariant', 'coherent', 'states', 'for', 'loop', 'quantum', 'gravity', 'here', 'we', 'deal', 'with', 'the', 'gauge', 'group', 'su2', 'this', 'being', 'a', 'significant', 'complication', 'compared', 'to', 'the', 'abelian', 'u1', 'case', 'encountered', 'in', '... | [-0.18156869583013388, 0.18687841439791322, -0.0790496202900027, 0.1009576874656871, -0.05600874880881254, -0.08240972308568277, 0.017637976256822695, 0.3810419284233476, -0.19753170177593068, -0.24586431662378422, 0.08569956530907617, -0.28303879623940625, -0.1532780208143453, 0.13257342642488873, -0.08147001251779591... |
709.4637 | SU(4)_C X SU(2)_L X SU(2)_R Models With C-parity | We construct supersymmetric SU(4)_C X SU(2)_L X SU(2)_R models with
spontaneously broken left-right symmetry (C-parity). The minimal supersymmetric
standard model (MSSM) can be recovered at low scales by exploiting the missing
partner mechanism. The field content is compatible with realistic fermion
masses and mixing... | hep-ph | we construct supersymmetric su4_c x su2_l x su2_r models with spontaneously broken leftright symmetry cparity the minimal supersymmetric standard model mssm can be recovered at low scales by exploiting the missing partner mechanism the field content is compatible with realistic fermion masses and mixings proton lifetim... | [['we', 'construct', 'supersymmetric', 'su4_c', 'x', 'su2_l', 'x', 'su2_r', 'models', 'with', 'spontaneously', 'broken', 'leftright', 'symmetry', 'cparity', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'can', 'be', 'recovered', 'at', 'low', 'scales', 'by', 'exploiting', 'the', 'missing', 'partner', ... | [-0.11196974322887226, 0.30942800721996244, 0.006356567593424448, 0.20802485261707002, -0.12522406499400468, -0.23392092477228116, 0.005673697451129556, 0.368116152500512, -0.21098056899028875, -0.3310089403738467, 0.07089747113475044, -0.2416548936965964, 0.029565613578944022, 0.048897136274414756, -0.0056100050209178... |
709.4638 | Multiparticle SUSY simulations at LHC & ILC: Off-Shell effects,
interferences and radiative corrections | The interesting but difficult phenomenology of supersymmetric models at the
LHC and ILC demands a corresponding complexity and maturity from simulation
tools. This includes multi-particle final states, reducible and irreducible
backgrounds, spin correlations, real emission of photons and gluons, virtual
corrections e... | hep-ph | the interesting but difficult phenomenology of supersymmetric models at the lhc and ilc demands a corresponding complexity and maturity from simulation tools this includes multiparticle final states reducible and irreducible backgrounds spin correlations real emission of photons and gluons virtual corrections etc most ... | [['the', 'interesting', 'but', 'difficult', 'phenomenology', 'of', 'supersymmetric', 'models', 'at', 'the', 'lhc', 'and', 'ilc', 'demands', 'a', 'corresponding', 'complexity', 'and', 'maturity', 'from', 'simulation', 'tools', 'this', 'includes', 'multiparticle', 'final', 'states', 'reducible', 'and', 'irreducible', 'ba... | [-0.06913859767207343, 0.17428762963437106, -0.05398813351648786, 0.16883377431492722, -0.005865963460463617, -0.1399996773901558, -0.03285645963328462, 0.3558786246770372, -0.18511956471613505, -0.27883843880974585, 0.07260489686103981, -0.34349393944204265, -0.05960490980318615, 0.20218707156914567, 0.031488368605514... |
709.4639 | Hadronic loop contributions to $J/\psi$ and $\psi^\prime$ radiative
decays into $\gamma\eta_c$ or $\gamma\eta_c^\prime$ | Intermediate hadronic meson loop contributions to $J/\psi$, $\psi^\prime \to
\gamma\eta_c$ ($\gamma\eta_c^\prime$) are studied apart from the dominant M1
transitions in an effective Lagrangian approach. Due to the property of the
unique antisymmetric tensor coupling in $V\to VP$, the hadronic loop
transitions provide... | hep-ph | intermediate hadronic meson loop contributions to jpsi psiprime to gammaeta_c gammaeta_cprime are studied apart from the dominant m1 transitions in an effective lagrangian approach due to the property of the unique antisymmetric tensor coupling in vto vp the hadronic loop transitions provide explicit corrections to the... | [['intermediate', 'hadronic', 'meson', 'loop', 'contributions', 'to', 'jpsi', 'psiprime', 'to', 'gammaeta_c', 'gammaeta_cprime', 'are', 'studied', 'apart', 'from', 'the', 'dominant', 'm1', 'transitions', 'in', 'an', 'effective', 'lagrangian', 'approach', 'due', 'to', 'the', 'property', 'of', 'the', 'unique', 'antisymme... | [-0.09770928755058862, 0.2529572564100991, -0.08390369219705462, 0.13801418364469317, -0.033463022055193074, -0.13978690573768246, 0.08233184349900555, 0.28471922535848404, -0.19275575440731788, -0.21105837444109576, -0.05007251804373005, -0.3283818798450132, -0.07695970076712824, 0.08252036490122833, 0.108625765579442... |
709.464 | Two populations are better than one: Short gamma-ray bursts from SGR
giant flares and NS-NS mergers | With a peak luminosity of ~10^47 erg/s, the December 27th 2004 giant flare
from SGR1806-20 would have been visible by BATSE (the Burst and Transient
Source Experiment) out to ~50 Mpc. It is thus plausible that some fraction of
the short duration Gamma-Ray Bursts (sGRBs) in the BATSE catalogue were due to
extragalacti... | astro-ph | with a peak luminosity of 1047 ergs the december 27th 2004 giant flare from sgr180620 would have been visible by batse the burst and transient source experiment out to 50 mpc it is thus plausible that some fraction of the short duration gammaray bursts sgrbs in the batse catalogue were due to extragalactic magnetar gia... | [['with', 'a', 'peak', 'luminosity', 'of', '1047', 'ergs', 'the', 'december', '27th', '2004', 'giant', 'flare', 'from', 'sgr180620', 'would', 'have', 'been', 'visible', 'by', 'batse', 'the', 'burst', 'and', 'transient', 'source', 'experiment', 'out', 'to', '50', 'mpc', 'it', 'is', 'thus', 'plausible', 'that', 'some', '... | [-0.04411058046715769, 0.13083619880245206, -0.04059291093296885, 0.24493992996780706, -0.15253055379006558, -0.0462112251068596, 0.0753388158742025, 0.46355360597546136, -0.06805923894139129, -0.39220104585118837, 0.0026287284334816875, -0.3495551749550363, 0.02285541024473991, 0.2653710668934857, -0.02889685892330256... |
709.4641 | Adiabaticity and spectral splits in collective neutrino transformations | Neutrinos streaming off a supernova core transform collectively by
neutrino-neutrino interactions, leading to "spectral splits" where an energy
E_split divides the transformed spectrum sharply into parts of almost pure but
different flavors. We present a detailed description of the spectral split
phenomenon which is ... | hep-ph | neutrinos streaming off a supernova core transform collectively by neutrinoneutrino interactions leading to spectral splits where an energy e_split divides the transformed spectrum sharply into parts of almost pure but different flavors we present a detailed description of the spectral split phenomenon which is concept... | [['neutrinos', 'streaming', 'off', 'a', 'supernova', 'core', 'transform', 'collectively', 'by', 'neutrinoneutrino', 'interactions', 'leading', 'to', 'spectral', 'splits', 'where', 'an', 'energy', 'e_split', 'divides', 'the', 'transformed', 'spectrum', 'sharply', 'into', 'parts', 'of', 'almost', 'pure', 'but', 'differen... | [-0.13548274552769504, 0.17437864313429072, -0.13413333034014885, 0.13638328222063803, -0.061146943257652395, -0.10961130677317163, 0.05236442408965232, 0.33934150014840464, -0.2638067052315722, -0.25945769193518253, 0.034127243956238146, -0.23547206482430563, -0.09314701268769346, 0.14666230886248616, -0.0064148457600... |
709.4642 | Multipartite entanglement in four-qubit cluster-class states | Based on quantitative complementarity relations (QCRs), we analyze the
multipartite correlations in four-qubit cluster-class states. It is proven
analytically that the average multipartite correlation $E_{ms}$ is entanglement
monotone. Moreover, it is also shown that the mixed three-tangle is a
correlation measure co... | quant-ph | based on quantitative complementarity relations qcrs we analyze the multipartite correlations in fourqubit clusterclass states it is proven analytically that the average multipartite correlation e_ms is entanglement monotone moreover it is also shown that the mixed threetangle is a correlation measure compatible with t... | [['based', 'on', 'quantitative', 'complementarity', 'relations', 'qcrs', 'we', 'analyze', 'the', 'multipartite', 'correlations', 'in', 'fourqubit', 'clusterclass', 'states', 'it', 'is', 'proven', 'analytically', 'that', 'the', 'average', 'multipartite', 'correlation', 'e_ms', 'is', 'entanglement', 'monotone', 'moreover... | [-0.1466543727007735, 0.13865500976048087, -0.14280810230074154, 0.15399684269062203, 0.050926973132173654, -0.16482870819290046, 0.017882059766924467, 0.3401271220890508, -0.22041790819038515, -0.22067434703796238, 0.06917363094955521, -0.31157395594409143, -0.16182315558789, 0.1684306203050242, -0.02140105135090973, ... |
709.4643 | Periodic solutions of periodically perturbed planar autonomous systems:
A topological approach | Aim of this paper is to investigate the existence of periodic solutions of a
nonlinear planar autonomous system having a limit cycle x_0 of least period
T_0>0 when it is perturbed by a small parameter, T_1-periodic, perturbation. In
the case when T_0/T_1 is a rational number l/k, with l, k prime numbers, we
provide c... | math.CA | aim of this paper is to investigate the existence of periodic solutions of a nonlinear planar autonomous system having a limit cycle x_0 of least period t_00 when it is perturbed by a small parameter t_1periodic perturbation in the case when t_0t_1 is a rational number lk with l k prime numbers we provide conditions to... | [['aim', 'of', 'this', 'paper', 'is', 'to', 'investigate', 'the', 'existence', 'of', 'periodic', 'solutions', 'of', 'a', 'nonlinear', 'planar', 'autonomous', 'system', 'having', 'a', 'limit', 'cycle', 'x_0', 'of', 'least', 'period', 't_00', 'when', 'it', 'is', 'perturbed', 'by', 'a', 'small', 'parameter', 't_1periodic'... | [-0.2524586604285171, 0.11960328007450355, -0.0864132276384641, 0.01793480647067903, -0.012286499629895024, -0.1461136216599963, 0.021145222474210308, 0.30432586048711213, -0.26871281750006787, -0.21814664160764918, 0.14978812540424927, -0.2733172887923899, -0.1436747204564783, 0.1840877201013415, -0.05638153328473945,... |
709.4644 | Conditional preparation of states containing a definite number of
photons | A technique for conditionally creating single- or multimode photon-number
states is analyzed using Bayesian theory. We consider the heralded N-photon
states created from the photons produced by an unseeded optical parametric
amplifier when the heralding detector is the time-multiplexed
photon-number-resolving detecto... | quant-ph | a technique for conditionally creating single or multimode photonnumber states is analyzed using bayesian theory we consider the heralded nphoton states created from the photons produced by an unseeded optical parametric amplifier when the heralding detector is the timemultiplexed photonnumberresolving detector recentl... | [['a', 'technique', 'for', 'conditionally', 'creating', 'single', 'or', 'multimode', 'photonnumber', 'states', 'is', 'analyzed', 'using', 'bayesian', 'theory', 'we', 'consider', 'the', 'heralded', 'nphoton', 'states', 'created', 'from', 'the', 'photons', 'produced', 'by', 'an', 'unseeded', 'optical', 'parametric', 'amp... | [-0.05011672604697964, 0.1889870478241824, -0.07262864770385825, -0.035605805206058314, 0.019344657399574097, -0.2019153051213949, 0.06971436195884768, 0.4416185437500459, -0.12452522187846378, -0.351356094904262, -0.047853447751196335, -0.295406101036419, -0.1105433980622374, 0.2582607251632669, -0.12815307393597747, ... |
709.4645 | Contracting Endomorphisms and Gorenstein Modules | We characterize Gorenstein modules over those local rings that admit a finite
contracting endomorphism.
| math.AC | we characterize gorenstein modules over those local rings that admit a finite contracting endomorphism | [['we', 'characterize', 'gorenstein', 'modules', 'over', 'those', 'local', 'rings', 'that', 'admit', 'a', 'finite', 'contracting', 'endomorphism']] | [-0.2650433659686574, 0.023036189709923098, -0.15514388786894934, 0.07260987162590027, -0.05614613635199411, -0.25586404129197554, -0.22667651922841156, 0.4325816205569676, -0.4568989393966539, 0.0025841197265045984, 0.11068997715067651, -0.22709943833095686, -0.09478714689612389, 0.13876490048798068, -0.20264110295102... |
709.4646 | Positve Entropy Geodesic Flows on Nilmanifolds | Let T be the nilpotent group of 4 x 4 real upper triangular matrices. In this
note we show that the Euler equations of certain left-invariant riemannian
metrics on T have a horseshoe. We also show, with the aid of a numerical
computation of a Melnikov-type integral, that the Euler equations of the
sub-riemannian Carn... | math.DS math.DG | let t be the nilpotent group of 4 x 4 real upper triangular matrices in this note we show that the euler equations of certain leftinvariant riemannian metrics on t have a horseshoe we also show with the aid of a numerical computation of a melnikovtype integral that the euler equations of the subriemannian carnot metric... | [['let', 't', 'be', 'the', 'nilpotent', 'group', 'of', '4', 'x', '4', 'real', 'upper', 'triangular', 'matrices', 'in', 'this', 'note', 'we', 'show', 'that', 'the', 'euler', 'equations', 'of', 'certain', 'leftinvariant', 'riemannian', 'metrics', 'on', 't', 'have', 'a', 'horseshoe', 'we', 'also', 'show', 'with', 'the', '... | [-0.21265059462602948, 0.09771765962232166, -0.12680056098033674, 0.019815811185981146, -0.1079772414173931, -0.13800679775886238, -0.037714968842919916, 0.31435365496436135, -0.22741020806133747, -0.24140779364388437, 0.09602339364791987, -0.27597929621115325, -0.18565323611255735, 0.2454660184565, -0.1075729623025836... |
709.4647 | Electrostatics in Periodic Boundary Conditions and Real-space
Corrections | We address periodic-image errors arising from the use of periodic boundary
conditions to describe systems that do not exhibit full three-dimensional
periodicity. The difference between the periodic potential, as
straightforwardly obtained from a Fourier transform, and the potential
satisfying any other boundary condi... | cond-mat.other | we address periodicimage errors arising from the use of periodic boundary conditions to describe systems that do not exhibit full threedimensional periodicity the difference between the periodic potential as straightforwardly obtained from a fourier transform and the potential satisfying any other boundary conditions c... | [['we', 'address', 'periodicimage', 'errors', 'arising', 'from', 'the', 'use', 'of', 'periodic', 'boundary', 'conditions', 'to', 'describe', 'systems', 'that', 'do', 'not', 'exhibit', 'full', 'threedimensional', 'periodicity', 'the', 'difference', 'between', 'the', 'periodic', 'potential', 'as', 'straightforwardly', 'o... | [-0.11937712939645818, 0.08096601333616288, -0.12015942123252898, 0.06743896815869785, -0.038210190845549934, -0.12920228259948394, 0.03552198199705109, 0.3973180179708396, -0.291567706086897, -0.2736637899722188, 0.12048800967103387, -0.21572170713894862, -0.14617662399972756, 0.23652608326261138, -0.04949452857383423... |
709.4648 | Spectral properties of the non-hermitian Wilson-Dirac operator in the
Schroedinger functional | We report on some preparatory investigations for the simulation of the QCD
Schroedinger functional with a non-hermitian polynomial hybrid Monte Carlo
algorithm. The complex spectrum of the non-hermitean free operator with SF
boundary condititons is computed semianalytically. Then it is shown how one can
obtain releva... | hep-lat | we report on some preparatory investigations for the simulation of the qcd schroedinger functional with a nonhermitian polynomial hybrid monte carlo algorithm the complex spectrum of the nonhermitean free operator with sf boundary condititons is computed semianalytically then it is shown how one can obtain relevant inf... | [['we', 'report', 'on', 'some', 'preparatory', 'investigations', 'for', 'the', 'simulation', 'of', 'the', 'qcd', 'schroedinger', 'functional', 'with', 'a', 'nonhermitian', 'polynomial', 'hybrid', 'monte', 'carlo', 'algorithm', 'the', 'complex', 'spectrum', 'of', 'the', 'nonhermitean', 'free', 'operator', 'with', 'sf', ... | [-0.1263383140243162, 0.11146472446066705, -0.11106028763350805, 0.0584807463003656, -0.0597631840312199, -0.09780075618874508, 0.0028937741157573625, 0.3793548836523818, -0.2565976446746169, -0.22835486211713302, 0.14329727928191927, -0.26513411952937777, -0.1709190148457482, 0.1869716328895978, -0.005091258211413751,... |
709.4649 | Factorizations of one dimensional classical systems | A class of one dimensional classical systems is characterized from an
algebraic point of view. The Hamiltonians of these systems are factorized in
terms of two functions that together with the Hamiltonian itself close a
Poisson algebra. These two functions lead directly to two time-dependent
integrals of motion from ... | physics.class-ph physics.gen-ph | a class of one dimensional classical systems is characterized from an algebraic point of view the hamiltonians of these systems are factorized in terms of two functions that together with the hamiltonian itself close a poisson algebra these two functions lead directly to two timedependent integrals of motion from which... | [['a', 'class', 'of', 'one', 'dimensional', 'classical', 'systems', 'is', 'characterized', 'from', 'an', 'algebraic', 'point', 'of', 'view', 'the', 'hamiltonians', 'of', 'these', 'systems', 'are', 'factorized', 'in', 'terms', 'of', 'two', 'functions', 'that', 'together', 'with', 'the', 'hamiltonian', 'itself', 'close',... | [-0.16786447787072156, 0.11580036950122244, -0.08809701610054518, 0.06709261913941167, -0.015605597052018385, -0.12938631933836922, -0.033476480465332, 0.30404101125895977, -0.3446904093631216, -0.22951895154609875, 0.08912139200146084, -0.25805918148064333, -0.1726721176827276, 0.2625956882319942, -0.02164360475600571... |
709.465 | CP Violation and Neutrino Masses and Mixings from Quark Mass Hierarchies | We study the connection between quark and lepton mass matrices in a
supersymmetric SO(10) GUT model in six dimensions, compactified on an orbifold.
The physical quarks and leptons are mixtures of brane and bulk states. This
leads to a characteristic pattern of mass matrices and high-energy CP violating
phases. The hi... | hep-ph | we study the connection between quark and lepton mass matrices in a supersymmetric so10 gut model in six dimensions compactified on an orbifold the physical quarks and leptons are mixtures of brane and bulk states this leads to a characteristic pattern of mass matrices and highenergy cp violating phases the hierarchy o... | [['we', 'study', 'the', 'connection', 'between', 'quark', 'and', 'lepton', 'mass', 'matrices', 'in', 'a', 'supersymmetric', 'so10', 'gut', 'model', 'in', 'six', 'dimensions', 'compactified', 'on', 'an', 'orbifold', 'the', 'physical', 'quarks', 'and', 'leptons', 'are', 'mixtures', 'of', 'brane', 'and', 'bulk', 'states',... | [-0.12632582007029738, 0.40293489081097783, 0.06426507085561753, 0.19506237786263228, -0.055516286240890625, -0.1710480759672534, 0.1080682016344956, 0.26511354066718085, -0.1885463688065871, -0.326018858997402, 0.041265476662486505, -0.3015399271264099, 0.011821820748557981, 0.0738290608412801, 0.02690277433452698, 0.... |
709.4651 | Comment on "Is There a "Most Perfect Fluid" Consistent with Quantum
Field Theory?" | This is a comment on hep-th/0702136
| hep-th hep-ph nucl-th | this is a comment on hepth0702136 | [['this', 'is', 'a', 'comment', 'on', 'hepth0702136']] | [-0.21415500938892365, 0.10114628821611404, -0.15367542495951056, 0.049587417393922806, -0.15845250450074672, -0.013680655416101218, 0.11685236990451812, 0.32352621108293533, -0.022586753964424132, -0.1547233171761036, 0.23054298907518386, -0.296547194570303, -0.22051888555288315, 0.21063961684703827, -0.19979685302823... |
709.4652 | Asymmetry of rotational catalysis of single membrane-bound F0F1-ATP
synthase | Erroneous submission in violation of copyright removed by arXiv admin.
| physics.bio-ph | erroneous submission in violation of copyright removed by arxiv admin | [['erroneous', 'submission', 'in', 'violation', 'of', 'copyright', 'removed', 'by', 'arxiv', 'admin']] | [-0.22172706332057715, 0.0338669303804636, -0.022779538901522754, -0.03168745934963226, -0.14088220447301864, -0.2398522425442934, 0.24546607797965408, 0.1183283731341362, -0.17965693990699946, -0.4359526693820953, 0.10541128780459985, -0.35726712383329867, 0.01606849010568112, -0.11570813357830048, -0.4147948315367102... |
709.4653 | On superstatistical multiplicative-noise processes | In this manuscript we analyse the long-term probability density function of
non-stationary dynamical processes which are enclosed inward the Feller class
of processes with time varying exponents for multiplicative noise. The update
in the value of the exponent occurs in the same conditions presented by Beck
and Cohen... | cond-mat.stat-mech | in this manuscript we analyse the longterm probability density function of nonstationary dynamical processes which are enclosed inward the feller class of processes with time varying exponents for multiplicative noise the update in the value of the exponent occurs in the same conditions presented by beck and cohen for ... | [['in', 'this', 'manuscript', 'we', 'analyse', 'the', 'longterm', 'probability', 'density', 'function', 'of', 'nonstationary', 'dynamical', 'processes', 'which', 'are', 'enclosed', 'inward', 'the', 'feller', 'class', 'of', 'processes', 'with', 'time', 'varying', 'exponents', 'for', 'multiplicative', 'noise', 'the', 'up... | [-0.11683278955834013, 0.15184129837533117, -0.10546869201861112, 0.09691763358210331, -0.01966994855320081, -0.10180357874135001, 0.06229756932548234, 0.3241008688764594, -0.27790530816927345, -0.26095434898694214, 0.06950355070466044, -0.19975090402007942, -0.1680798767475595, 0.17667152341717565, -0.0761111260614764... |
709.4654 | Deuteron Momentum Distribution in KD2HPO4 | The momentum distribution in KD2PO4(DKDP) has been measured using neutron
Compton scattering above and below the weakly first order
paraelectric-ferroelectric phase transition(T=229K). There is very litte
difference between the two distributions, and no sign of the coherence over two
locations for the proton observed... | cond-mat.other | the momentum distribution in kd2po4dkdp has been measured using neutron compton scattering above and below the weakly first order paraelectricferroelectric phase transitiont229k there is very litte difference between the two distributions and no sign of the coherence over two locations for the proton observed in the pa... | [['the', 'momentum', 'distribution', 'in', 'kd2po4dkdp', 'has', 'been', 'measured', 'using', 'neutron', 'compton', 'scattering', 'above', 'and', 'below', 'the', 'weakly', 'first', 'order', 'paraelectricferroelectric', 'phase', 'transitiont229k', 'there', 'is', 'very', 'litte', 'difference', 'between', 'the', 'two', 'di... | [-0.13036665663219474, 0.2489654216754796, -0.08582809749400597, 0.09083255842741547, 0.005138348137702921, -0.08248291198507449, 0.0313090068832088, 0.4193308799174325, -0.22958526933758422, -0.2853219151288143, 0.04387535223414206, -0.3119158568503014, -0.07754536035896183, 0.21213024791835905, 0.04940606785535708, 0... |
709.4655 | Mining for trees in a graph is NP-complete | Mining for trees in a graph is shown to be NP-complete.
| cs.DB cs.AI | mining for trees in a graph is shown to be npcomplete | [['mining', 'for', 'trees', 'in', 'a', 'graph', 'is', 'shown', 'to', 'be', 'npcomplete']] | [-0.06916450674179941, 0.08360263332724571, -0.1197733421894637, 0.15704152128786186, -0.2402517804029313, -0.14285020407458598, 0.04356053403832696, 0.48915747756307776, -0.3885436769236218, -0.27788879282095214, 0.1650533358121968, -0.26892368211834267, -0.20302105695009232, 0.20160152356732974, -0.188268527303907, 0... |
709.4656 | Nonextensive statistical mechanics and central limit theorems I -
Convolution of independent random variables and q-product | In this article we review the standard versions of the Central and of the
Levy-Gnedenko Limit Theorems, and illustrate their application to the
convolution of independent random variables associated with the distribution
known as q-Gaussian. This distribution emerges upon extremisation of the
nonadditive entropy, bas... | cond-mat.soft | in this article we review the standard versions of the central and of the levygnedenko limit theorems and illustrate their application to the convolution of independent random variables associated with the distribution known as qgaussian this distribution emerges upon extremisation of the nonadditive entropy basis of n... | [['in', 'this', 'article', 'we', 'review', 'the', 'standard', 'versions', 'of', 'the', 'central', 'and', 'of', 'the', 'levygnedenko', 'limit', 'theorems', 'and', 'illustrate', 'their', 'application', 'to', 'the', 'convolution', 'of', 'independent', 'random', 'variables', 'associated', 'with', 'the', 'distribution', 'kn... | [-0.06275384363953054, 0.14211015743726382, -0.1425473864012345, 0.08303893350890072, 0.01150091377851682, -0.1073498283020728, 0.05125253828766763, 0.2751952992237317, -0.27111072514236456, -0.23885636730498172, 0.08219213713323925, -0.2848886357226629, -0.12425357461679817, 0.16275537141780483, -0.0904119028653041, 0... |
709.4657 | Power-law Behavior of High Energy String Scatterings in Compact Spaces | We calculate high energy massive scattering amplitudes of closed bosonic
string compactified on the torus. We obtain infinite linear relations among
high energy scattering amplitudes. For some kinematic regimes, we discover that
some linear relations break down and, simultaneously, the amplitudes enhance to
power-law... | hep-th | we calculate high energy massive scattering amplitudes of closed bosonic string compactified on the torus we obtain infinite linear relations among high energy scattering amplitudes for some kinematic regimes we discover that some linear relations break down and simultaneously the amplitudes enhance to powerlaw behavio... | [['we', 'calculate', 'high', 'energy', 'massive', 'scattering', 'amplitudes', 'of', 'closed', 'bosonic', 'string', 'compactified', 'on', 'the', 'torus', 'we', 'obtain', 'infinite', 'linear', 'relations', 'among', 'high', 'energy', 'scattering', 'amplitudes', 'for', 'some', 'kinematic', 'regimes', 'we', 'discover', 'tha... | [-0.17347254256031128, 0.21526511871453488, -0.13036390315421453, 0.19699825728994164, -0.109771878143415, -0.16074728297841068, 0.034472177783497655, 0.33821867161543306, -0.2228636472401294, -0.26041148137301207, 0.03281169344972104, -0.2799808357729379, -0.12807539353297667, 0.13858930296217553, -0.01095867582192324... |
709.4658 | Structure Factor of the 3D Random Field XY Model | We have performed Monte Carlo studies of the 3D random field XY model on $L
\times L \times L$ simple cubic lattices, with random field strengths of $h_r$
= 1 and 2. We present results for the angle-averaged magnetic structure factor,
$S (k)$ at $L = 64$. Our results appear to indicate a phase transition into a
ferro... | cond-mat.dis-nn cond-mat.stat-mech | we have performed monte carlo studies of the 3d random field xy model on l times l times l simple cubic lattices with random field strengths of h_r 1 and 2 we present results for the angleaveraged magnetic structure factor s k at l 64 our results appear to indicate a phase transition into a ferromagnetic state this is ... | [['we', 'have', 'performed', 'monte', 'carlo', 'studies', 'of', 'the', '3d', 'random', 'field', 'xy', 'model', 'on', 'l', 'times', 'l', 'times', 'l', 'simple', 'cubic', 'lattices', 'with', 'random', 'field', 'strengths', 'of', 'h_r', '1', 'and', '2', 'we', 'present', 'results', 'for', 'the', 'angleaveraged', 'magnetic'... | [-0.18915272135795516, 0.20544408581918105, -0.05420402198267931, 0.012929111217751844, -0.04552383101227778, -0.16985909731804646, 0.08068465668739835, 0.4100073925642805, -0.21844368235377426, -0.2682283697014844, 0.0739127331180498, -0.28639967972412705, -0.08710846847812222, 0.1362734638942956, 0.08369373623281717,... |
709.4659 | Stellar Populations Found in the Central kpc of Four Luminous Compact
Blue Galaxies at Intermediate Redshift | We investigate the star formation history of the central regions of four
Luminous Compact Blue Galaxies (LCBGs). LCBGs are blue (B-V<0.6), compact
(MU_B<21.5 mag arcsec^-2) galaxies with absolute magnitudes M_B brighter than
-17.5. The LCBGs analyzed here are located at 0.436<z<0.525. They are among the
most luminous... | astro-ph | we investigate the star formation history of the central regions of four luminous compact blue galaxies lcbgs lcbgs are blue bv06 compact mu_b215 mag arcsec2 galaxies with absolute magnitudes m_b brighter than 175 the lcbgs analyzed here are located at 0436z0525 they are among the most luminous m_b 205 blue bv 04 and h... | [['we', 'investigate', 'the', 'star', 'formation', 'history', 'of', 'the', 'central', 'regions', 'of', 'four', 'luminous', 'compact', 'blue', 'galaxies', 'lcbgs', 'lcbgs', 'are', 'blue', 'bv06', 'compact', 'mu_b215', 'mag', 'arcsec2', 'galaxies', 'with', 'absolute', 'magnitudes', 'm_b', 'brighter', 'than', '175', 'the'... | [-0.03159996839707803, 0.1155779732948473, -0.11827633248166684, 0.1450172212120013, -0.09471762489924933, -0.042756699183936306, 0.030542355220741495, 0.49456091061483864, -0.06706971595615195, -0.3694370605215181, 0.040936165612003916, -0.3029335151936968, -0.026745362468375573, 0.18686909886404252, -0.07546048513399... |
709.466 | Operating molecular transistors as heat pumps | We study heat transport in transistor-like devices composed of two reservoirs
and a gate electrode, with a ballistic electronic one-dimensional system
connected between the two reservoirs and interacting with a laser field. We
derive in a simple way an equation for the heat flux in terms of the
Floquet-Green operator... | cond-mat.mes-hall | we study heat transport in transistorlike devices composed of two reservoirs and a gate electrode with a ballistic electronic onedimensional system connected between the two reservoirs and interacting with a laser field we derive in a simple way an equation for the heat flux in terms of the floquetgreen operator of the... | [['we', 'study', 'heat', 'transport', 'in', 'transistorlike', 'devices', 'composed', 'of', 'two', 'reservoirs', 'and', 'a', 'gate', 'electrode', 'with', 'a', 'ballistic', 'electronic', 'onedimensional', 'system', 'connected', 'between', 'the', 'two', 'reservoirs', 'and', 'interacting', 'with', 'a', 'laser', 'field', 'w... | [-0.19718151493774105, 0.13935176278185585, -0.054518232494592665, -0.01752351609369119, 0.015803278736226882, -0.15553290344929943, 0.0678357572760433, 0.3789993625813319, -0.2642441492042659, -0.27684271580850084, 0.06314708605350461, -0.2909630964044482, -0.12211265369551257, 0.2568027166669102, -0.00184729786124080... |
709.4661 | Nonextensive statistical mechanics and central limit theorems II -
Convolution of q-independent random variables | In this article we review recent generalisations of the central limit theorem
for the sum of specially correlated (or q-independent) variables, focusing on q
greater or equal than 1. Specifically, this kind of correlation turns the
probability density function known as q-Gaussian, which emerges upon
maximisation of t... | cond-mat.stat-mech | in this article we review recent generalisations of the central limit theorem for the sum of specially correlated or qindependent variables focusing on q greater or equal than 1 specifically this kind of correlation turns the probability density function known as qgaussian which emerges upon maximisation of the entropy... | [['in', 'this', 'article', 'we', 'review', 'recent', 'generalisations', 'of', 'the', 'central', 'limit', 'theorem', 'for', 'the', 'sum', 'of', 'specially', 'correlated', 'or', 'qindependent', 'variables', 'focusing', 'on', 'q', 'greater', 'or', 'equal', 'than', '1', 'specifically', 'this', 'kind', 'of', 'correlation', ... | [-0.10246988828293979, 0.13921701850370027, -0.11826866541377967, 0.11837556807222427, -0.011050999359213165, -0.10292516584013356, 0.052710469341036514, 0.28670355464419117, -0.25441205774768605, -0.2439461655822015, 0.1075222455592666, -0.258190042224669, -0.14325468558308785, 0.1572975680419404, -0.05060519758626469... |
709.4662 | Spectroscopy of new c,b-mesons | Masses of the lowest multiplets of c,b-mesons in S- and P-wave states with
quantum numbers JPC: 0-+, 1--, 0++, 1+-, 1++, 2++ are obtained with the help of
dispersion N/D method of heavy quark effective theory. The results are in a
good agreement with experimental data. Radiative decay widths for some states
mentioned... | hep-ph | masses of the lowest multiplets of cbmesons in s and pwave states with quantum numbers jpc 0 1 0 1 1 2 are obtained with the help of dispersion nd method of heavy quark effective theory the results are in a good agreement with experimental data radiative decay widths for some states mentioned above were calculated | [['masses', 'of', 'the', 'lowest', 'multiplets', 'of', 'cbmesons', 'in', 's', 'and', 'pwave', 'states', 'with', 'quantum', 'numbers', 'jpc', '0', '1', '0', '1', '1', '2', 'are', 'obtained', 'with', 'the', 'help', 'of', 'dispersion', 'nd', 'method', 'of', 'heavy', 'quark', 'effective', 'theory', 'the', 'results', 'are',... | [-0.09227432623844255, 0.2649031830866906, 0.007352007011120969, 0.12420059276575392, 0.04927551234987649, -0.19884900101037187, 0.0493232994784855, 0.35664936707101086, -0.16472850269214673, -0.335835550962524, -0.005352836347777735, -0.3841604803096164, 0.02240066047419201, 0.14603625653650273, 0.09746697998859666, 0... |
709.4663 | Electron coherence at low temperatures: The role of magnetic impurities | We review recent experimental progress on the saturation problem in metallic
quantum wires. In particular, we address the influence of magnetic impurities
on the electron phase coherence time. We also present new measurements of the
phase coherence time in ultra-clean gold and silver wires and analyse the
saturation ... | cond-mat.mes-hall | we review recent experimental progress on the saturation problem in metallic quantum wires in particular we address the influence of magnetic impurities on the electron phase coherence time we also present new measurements of the phase coherence time in ultraclean gold and silver wires and analyse the saturation of tau... | [['we', 'review', 'recent', 'experimental', 'progress', 'on', 'the', 'saturation', 'problem', 'in', 'metallic', 'quantum', 'wires', 'in', 'particular', 'we', 'address', 'the', 'influence', 'of', 'magnetic', 'impurities', 'on', 'the', 'electron', 'phase', 'coherence', 'time', 'we', 'also', 'present', 'new', 'measurement... | [-0.1213936524776121, 0.2231534938277897, -0.007678948202601043, 0.044980442612081444, 0.031541964387200694, -0.11416810275285795, 0.0913977721575848, 0.402953967464567, -0.21917380361507335, -0.33640891759185704, 0.03780840336275037, -0.3344014531341932, -0.0480257764218315, 0.15822019900685996, -0.009594626539456908,... |
709.4664 | An asymptotic-numerical approach for examining global solutions to an
ordinary differential equation | Purely numerical methods do not always provide an accurate way to find all
the global solutions to nonlinear ODE on infinite intervals. For example,
finite-difference methods fail to capture the asymptotic behavior of solutions,
which might be critical for ensuring global existence. We first show, by way of
a detaile... | math.CA | purely numerical methods do not always provide an accurate way to find all the global solutions to nonlinear ode on infinite intervals for example finitedifference methods fail to capture the asymptotic behavior of solutions which might be critical for ensuring global existence we first show by way of a detailed exampl... | [['purely', 'numerical', 'methods', 'do', 'not', 'always', 'provide', 'an', 'accurate', 'way', 'to', 'find', 'all', 'the', 'global', 'solutions', 'to', 'nonlinear', 'ode', 'on', 'infinite', 'intervals', 'for', 'example', 'finitedifference', 'methods', 'fail', 'to', 'capture', 'the', 'asymptotic', 'behavior', 'of', 'sol... | [-0.08760564851444982, -0.058749788741853576, -0.19436372793519618, 0.12732047827064646, -0.13558985615033925, -0.1370047348042585, 0.0538641090610439, 0.3594297505339089, -0.25085035266988365, -0.3020717307406756, 0.13127755091439203, -0.2580613449945585, -0.18172850333077392, 0.24120987221459406, -0.02033565350875412... |
709.4665 | New Dual Conformally Invariant Off-Shell Integrals | Evidence has recently emerged for a hidden symmetry of scattering amplitudes
in N=4 super Yang-Mills theory called dual conformal symmetry. At weak coupling
the presence of this symmetry has been observed through five loops, while at
strong coupling the symmetry has been shown to have a natural interpretation in
term... | hep-th | evidence has recently emerged for a hidden symmetry of scattering amplitudes in n4 super yangmills theory called dual conformal symmetry at weak coupling the presence of this symmetry has been observed through five loops while at strong coupling the symmetry has been shown to have a natural interpretation in terms of a... | [['evidence', 'has', 'recently', 'emerged', 'for', 'a', 'hidden', 'symmetry', 'of', 'scattering', 'amplitudes', 'in', 'n4', 'super', 'yangmills', 'theory', 'called', 'dual', 'conformal', 'symmetry', 'at', 'weak', 'coupling', 'the', 'presence', 'of', 'this', 'symmetry', 'has', 'been', 'observed', 'through', 'five', 'loo... | [-0.16924995600160772, 0.16837241213207924, -0.0801116390534306, 0.12025324545390102, -0.1128433624492778, -0.0934358820649645, -0.02584951073031432, 0.38894577510654926, -0.14180859839243273, -0.24473447204437307, 0.07236641762097196, -0.2875629753445185, -0.2249690412633842, 0.083949977910066, 0.006234102266570253, 0... |
709.4666 | Low Temperature Shear Modulus Changes in Solid 4-He and Connection to
Supersolidity | Superfluidity, liquid flow without friction, is familiar in helium. The first
evidence for "supersolidity", its analogue in quantum solids, came from recent
torsional oscillator (TO) measurements involving 4-He. At temperatures below
200 mK, TO frequencies increased, suggesting that some of the solid decoupled
from t... | cond-mat.other | superfluidity liquid flow without friction is familiar in helium the first evidence for supersolidity its analogue in quantum solids came from recent torsional oscillator to measurements involving 4he at temperatures below 200 mk to frequencies increased suggesting that some of the solid decoupled from the oscillator t... | [['superfluidity', 'liquid', 'flow', 'without', 'friction', 'is', 'familiar', 'in', 'helium', 'the', 'first', 'evidence', 'for', 'supersolidity', 'its', 'analogue', 'in', 'quantum', 'solids', 'came', 'from', 'recent', 'torsional', 'oscillator', 'to', 'measurements', 'involving', '4he', 'at', 'temperatures', 'below', '2... | [-0.1141629194228343, 0.2922870575035315, -0.07490559269259077, 0.02138826880874821, -0.02034510294122257, -0.13469634054522234, 0.06748275918336889, 0.3768683715936039, -0.26605566418932186, -0.3041268426256821, 0.05747199770627523, -0.31957769847940654, -0.094280540482546, 0.18059064266170657, -0.007840030672251369, ... |
709.4667 | The Distance and Age of the SNR Kes 73 and AXP 1E 1841-045 | We provide a new distance estimate to the supernova remnant (SNR) Kes 73 and
its associated anomalous X-ray pulsar (AXP) 1E 1841-045. 21 cm HI images and HI
absorption/ emission spectra from new VLA observations, and 13CO emission
spectra of Kes 73 and two adjacent compact HII regions (G27.276+0.148 and
G27.491+0.189... | astro-ph | we provide a new distance estimate to the supernova remnant snr kes 73 and its associated anomalous xray pulsar axp 1e 1841045 21 cm hi images and hi absorption emission spectra from new vla observations and 13co emission spectra of kes 73 and two adjacent compact hii regions g272760148 and g274910189 are analyzed the ... | [['we', 'provide', 'a', 'new', 'distance', 'estimate', 'to', 'the', 'supernova', 'remnant', 'snr', 'kes', '73', 'and', 'its', 'associated', 'anomalous', 'xray', 'pulsar', 'axp', '1e', '1841045', '21', 'cm', 'hi', 'images', 'and', 'hi', 'absorption', 'emission', 'spectra', 'from', 'new', 'vla', 'observations', 'and', '1... | [-0.07953579504824776, 0.024558234420174827, -0.00522460206785304, 0.0935523648557059, -0.11307980255398123, -0.10086264279247685, 0.10956475308306894, 0.4736232050261236, -0.15585116095303056, -0.34107260712805915, 0.03369416590446337, -0.339159096939798, 0.02698760671026875, 0.18397315385885896, 0.02249428970405563, ... |
709.4668 | Consequences of the Gross/Zagier formulae: Stability of average
L-values, subconvexity, and non-vanishing mod p | In this paper we investigate some consequences of the Gross/Zagier types of
formulae which were introduced by Gross and Zagier, and were then generalized
in various directions by Hatcher, Zhang, Kudla and several other people.
Working in the classical context of central values of L-series of holomorphic
forms of prim... | math.NT | in this paper we investigate some consequences of the grosszagier types of formulae which were introduced by gross and zagier and were then generalized in various directions by hatcher zhang kudla and several other people working in the classical context of central values of lseries of holomorphic forms of prime level ... | [['in', 'this', 'paper', 'we', 'investigate', 'some', 'consequences', 'of', 'the', 'grosszagier', 'types', 'of', 'formulae', 'which', 'were', 'introduced', 'by', 'gross', 'and', 'zagier', 'and', 'were', 'then', 'generalized', 'in', 'various', 'directions', 'by', 'hatcher', 'zhang', 'kudla', 'and', 'several', 'other', '... | [-0.16952547005804203, 0.049782170042018604, -0.0849913765097507, 0.08536790993508543, -0.0976986041484035, -0.10695812097863755, 0.04658574781219571, 0.25255929669104166, -0.259290477992079, -0.3136682636583241, 0.0980728265217932, -0.2270335453305672, -0.17434099535936506, 0.2581449665877724, -0.13752971792802493, 0.... |
709.4669 | The Extended Edit Distance Metric | Similarity search is an important problem in information retrieval. This
similarity is based on a distance. Symbolic representation of time series has
attracted many researchers recently, since it reduces the dimensionality of
these high dimensional data objects. We propose a new distance metric that is
applied to sy... | cs.IR | similarity search is an important problem in information retrieval this similarity is based on a distance symbolic representation of time series has attracted many researchers recently since it reduces the dimensionality of these high dimensional data objects we propose a new distance metric that is applied to symbolic... | [['similarity', 'search', 'is', 'an', 'important', 'problem', 'in', 'information', 'retrieval', 'this', 'similarity', 'is', 'based', 'on', 'a', 'distance', 'symbolic', 'representation', 'of', 'time', 'series', 'has', 'attracted', 'many', 'researchers', 'recently', 'since', 'it', 'reduces', 'the', 'dimensionality', 'of'... | [-0.0942168514757009, 0.010291547251746237, -0.1285096076683382, 0.10389156791177484, -0.14144914954759474, -0.11435006588718362, 0.03172577264603604, 0.4440832605187813, -0.3039844946705558, -0.30453249715854613, 0.11925599417581191, -0.3072952546514152, -0.17345088877286133, 0.23189127701334655, -0.1341747825211856, ... |
709.467 | Search for Lorentz and CPT Violation Effects in Muon Spin Precession | The spin precession frequency of muons stored in the $(g-2)$ storage ring has
been analyzed for evidence of Lorentz and CPT violation. Two Lorentz and CPT
violation signatures were searched for: a nonzero $\Delta\omega_{a}$
(=$\omega_{a}^{\mu^{+}}-\omega_{a}^{\mu^{-}}$); and a sidereal variation of
$\omega_{a}^{\mu^{... | hep-ex hep-ph | the spin precession frequency of muons stored in the g2 storage ring has been analyzed for evidence of lorentz and cpt violation two lorentz and cpt violation signatures were searched for a nonzero deltaomega_a omega_amuomega_amu and a sidereal variation of omega_amupm no significant effect is found and the following l... | [['the', 'spin', 'precession', 'frequency', 'of', 'muons', 'stored', 'in', 'the', 'g2', 'storage', 'ring', 'has', 'been', 'analyzed', 'for', 'evidence', 'of', 'lorentz', 'and', 'cpt', 'violation', 'two', 'lorentz', 'and', 'cpt', 'violation', 'signatures', 'were', 'searched', 'for', 'a', 'nonzero', 'deltaomega_a', 'omeg... | [-0.17832030884254677, 0.26144746541517017, 0.06129936291548757, 0.13735783520516837, 0.0008394812222248243, -0.11608093798758438, 0.07965073298754884, 0.32911750678846863, -0.0902370208138485, -0.41203927215372704, 0.08803200492215699, -0.32508846558630466, 0.12883310426992398, 0.2348620189399815, 0.061307817694650574... |
709.4671 | Secrecy Capacity Region of a Multi-Antenna Gaussian Broadcast Channel
with Confidential Messages | In wireless data networks, communication is particularly susceptible to
eavesdropping due to its broadcast nature. Security and privacy systems have
become critical for wireless providers and enterprise networks. This paper
considers the problem of secret communication over the Gaussian broadcast
channel, where a mul... | cs.IT math.IT | in wireless data networks communication is particularly susceptible to eavesdropping due to its broadcast nature security and privacy systems have become critical for wireless providers and enterprise networks this paper considers the problem of secret communication over the gaussian broadcast channel where a multiante... | [['in', 'wireless', 'data', 'networks', 'communication', 'is', 'particularly', 'susceptible', 'to', 'eavesdropping', 'due', 'to', 'its', 'broadcast', 'nature', 'security', 'and', 'privacy', 'systems', 'have', 'become', 'critical', 'for', 'wireless', 'providers', 'and', 'enterprise', 'networks', 'this', 'paper', 'consid... | [-0.3010635115995498, -0.017889646837608835, -0.015337868059569664, 0.03822811515501958, -0.05803441174728217, -0.3689175245515202, 0.1872791274231043, 0.3512336285521755, -0.29672143993488814, -0.20662347178927248, 0.12394565873579412, -0.28680612594625876, -0.12908073905908035, 0.12498675504999267, -0.192931621963563... |
709.4672 | Einstein, Sciascia, Majorana, Amaldi, e il Rapporto tra Intellettuali e
Potere (Einstein, Sciascia, Majorana, Amaldi, and the Relationship of
Intellectuals with the Power) | In Europe (e.g., in Italy), and in the States, the opinion is widely
spreading that the negative consequences of modern progress are the fault of
"Science". A lively debate on this topic took place among the famous writer
Leonardo Sciascia and Italian physicists like Edoardo Amaldi and Emilio Segre',
when Sciascia wr... | physics.gen-ph physics.hist-ph physics.pop-ph | in europe eg in italy and in the states the opinion is widely spreading that the negative consequences of modern progress are the fault of science a lively debate on this topic took place among the famous writer leonardo sciascia and italian physicists like edoardo amaldi and emilio segre when sciascia wrote his known ... | [['in', 'europe', 'eg', 'in', 'italy', 'and', 'in', 'the', 'states', 'the', 'opinion', 'is', 'widely', 'spreading', 'that', 'the', 'negative', 'consequences', 'of', 'modern', 'progress', 'are', 'the', 'fault', 'of', 'science', 'a', 'lively', 'debate', 'on', 'this', 'topic', 'took', 'place', 'among', 'the', 'famous', 'w... | [-0.06613242086534614, 0.0882255683934063, -0.09215938381340961, 0.08370476160912817, -0.17173077367249678, -0.1338883477340763, 0.06489373946819935, 0.2916724275749981, -0.20679992388900384, -0.345066943018923, 0.10111627991753983, -0.3022481441086821, -0.16790759534694988, 0.17889296262794893, -0.152175314997404, -0.... |
709.4673 | D-branes, obstructed curves, and minimal model superpotentials | In this short note we apply methods of Aspinwall-Katz to compute
superpotentials of D-branes wrapped on more general obstructed rational curves
in Calabi-Yau threefolds. We find an a priori unexpected match between
superpotentials from certain such curves and the superpotentials of
Landau-Ginzburg models correspondin... | hep-th math.AG | in this short note we apply methods of aspinwallkatz to compute superpotentials of dbranes wrapped on more general obstructed rational curves in calabiyau threefolds we find an a priori unexpected match between superpotentials from certain such curves and the superpotentials of landauginzburg models corresponding to mi... | [['in', 'this', 'short', 'note', 'we', 'apply', 'methods', 'of', 'aspinwallkatz', 'to', 'compute', 'superpotentials', 'of', 'dbranes', 'wrapped', 'on', 'more', 'general', 'obstructed', 'rational', 'curves', 'in', 'calabiyau', 'threefolds', 'we', 'find', 'an', 'a', 'priori', 'unexpected', 'match', 'between', 'superpoten... | [-0.14195389434968567, 0.013092634896051806, -0.12037085617244568, 0.21465789128611187, -0.07772151424306566, -0.21446747981700237, -0.0005631797628112785, 0.3718365204581262, -0.2125820509036598, -0.2777541077432587, 0.03397013404426853, -0.24982501216151792, -0.23972353383736766, 0.1920701236990483, -0.26310845659843... |
709.4674 | Possible way out of the Hawking paradox: Erasing the information at the
horizon | We show that small deviations from spherical symmetry, described by means of
exact solutions to Einstein equations, provide a mechanism to "bleach" the
information about the collapsing body as it falls through the aparent horizon,
thereby resolving the information loss paradox. The resulting picture and its
implicati... | gr-qc astro-ph hep-th | we show that small deviations from spherical symmetry described by means of exact solutions to einstein equations provide a mechanism to bleach the information about the collapsing body as it falls through the aparent horizon thereby resolving the information loss paradox the resulting picture and its implication relat... | [['we', 'show', 'that', 'small', 'deviations', 'from', 'spherical', 'symmetry', 'described', 'by', 'means', 'of', 'exact', 'solutions', 'to', 'einstein', 'equations', 'provide', 'a', 'mechanism', 'to', 'bleach', 'the', 'information', 'about', 'the', 'collapsing', 'body', 'as', 'it', 'falls', 'through', 'the', 'aparent'... | [-0.12721896185167517, 0.06896942791330521, -0.11239074335479346, 0.12430029325225375, -0.10558353388895754, -0.09531326556089716, 0.05787582100811796, 0.2595859276222401, -0.2864560965662364, -0.3005543731641574, 0.12012138794611407, -0.28357007685804464, -0.11889585101457893, 0.16810295416317025, -0.05502532675316496... |
709.4675 | Measurement of the ac Stark shift with a guided matter-wave
interferometer | We demonstrate the effectiveness of a guided-wave Bose-Einstein condensate
interferometer for practical measurements. Taking advantage of the large arm
separations obtainable in our interferometer, the energy levels of the 87Rb
atoms in one arm of the interferometer are shifted by a calibrated laser beam.
The resulti... | physics.atom-ph | we demonstrate the effectiveness of a guidedwave boseeinstein condensate interferometer for practical measurements taking advantage of the large arm separations obtainable in our interferometer the energy levels of the 87rb atoms in one arm of the interferometer are shifted by a calibrated laser beam the resulting phas... | [['we', 'demonstrate', 'the', 'effectiveness', 'of', 'a', 'guidedwave', 'boseeinstein', 'condensate', 'interferometer', 'for', 'practical', 'measurements', 'taking', 'advantage', 'of', 'the', 'large', 'arm', 'separations', 'obtainable', 'in', 'our', 'interferometer', 'the', 'energy', 'levels', 'of', 'the', '87rb', 'ato... | [-0.14822738617874198, 0.16956559489861117, -0.07398390943719144, 0.03676574361075095, 0.01947185776575848, -0.1003429933787427, 0.057357515975901927, 0.4081961337338995, -0.21112428553385176, -0.2852759178279451, 0.00978934678305113, -0.29699273365635975, -0.042557924602146226, 0.2297345957054791, 0.02196144787767143,... |
709.4676 | Binomial Coefficients and the Distribution of the Primes | Let omega(n) be the number of distinct prime factors dividing n and m > n
natural numbers. We calculate a formula showing which prime numbers in which
intervals divide a given binomial coefficient. From this formula we get an
identity omega(binom(nk)(mk))=sum_i (pi(k/b(i))- pi(k/a(i))) + O(sqrt(k)).
Erdoes mentioned ... | math.NT | let omegan be the number of distinct prime factors dividing n and m n natural numbers we calculate a formula showing which prime numbers in which intervals divide a given binomial coefficient from this formula we get an identity omegabinomnkmksum_i pikbi pikai osqrtk erdoes mentioned that omegabinomnkmk log nnmm nmnm k... | [['let', 'omegan', 'be', 'the', 'number', 'of', 'distinct', 'prime', 'factors', 'dividing', 'n', 'and', 'm', 'n', 'natural', 'numbers', 'we', 'calculate', 'a', 'formula', 'showing', 'which', 'prime', 'numbers', 'in', 'which', 'intervals', 'divide', 'a', 'given', 'binomial', 'coefficient', 'from', 'this', 'formula', 'we... | [-0.2030740507889068, 0.11189472814402998, -0.08562869922225845, 0.07947805825615538, -0.05342150216215644, -0.1894647350063783, 0.08634938192607343, 0.23405345326996055, -0.2927932044780203, -0.3562596120882308, -0.00225980794619255, -0.3156015098351857, -0.11638185429525957, 0.20544704816025822, -0.05964878482487181,... |
709.4677 | A continuation principle for a class of periodically perturbed
autonomous systems | In this paper we evaluate the topological index of periodic solutions otained
via the Malkin-Loud bifurcation result. Incidentally, we do not assume that the
perturbation is differentiale.
| math.CA | in this paper we evaluate the topological index of periodic solutions otained via the malkinloud bifurcation result incidentally we do not assume that the perturbation is differentiale | [['in', 'this', 'paper', 'we', 'evaluate', 'the', 'topological', 'index', 'of', 'periodic', 'solutions', 'otained', 'via', 'the', 'malkinloud', 'bifurcation', 'result', 'incidentally', 'we', 'do', 'not', 'assume', 'that', 'the', 'perturbation', 'is', 'differentiale']] | [-0.21135865807533263, 0.08205991841852665, -0.12975177586078643, 0.06439993873238564, -0.09293005134910345, -0.06512268081307411, 0.061023034579120575, 0.3511021650582552, -0.2521196736395359, -0.19650233149528504, 0.142649469464086, -0.26098460257053374, -0.29794233053922653, 0.12158828173298389, -0.13165425278246404... |
709.4678 | The Dirichlet Markov Ensemble | We equip the polytope of $n\times n$ Markov matrices with the normalized
trace of the Lebesgue measure of $\mathbb{R}^{n^2}$. This probability space
provides random Markov matrices, with i.i.d. rows following the Dirichlet
distribution of mean $(1/n,...,1/n)$. We show that if $\bM$ is such a random
matrix, then the e... | math.PR math.SP | we equip the polytope of ntimes n markov matrices with the normalized trace of the lebesgue measure of mathbbrn2 this probability space provides random markov matrices with iid rows following the dirichlet distribution of mean 1n1n we show that if bm is such a random matrix then the empirical distribution built from th... | [['we', 'equip', 'the', 'polytope', 'of', 'ntimes', 'n', 'markov', 'matrices', 'with', 'the', 'normalized', 'trace', 'of', 'the', 'lebesgue', 'measure', 'of', 'mathbbrn2', 'this', 'probability', 'space', 'provides', 'random', 'markov', 'matrices', 'with', 'iid', 'rows', 'following', 'the', 'dirichlet', 'distribution', ... | [-0.09085675551770972, 0.13632637990298324, -0.09091181431252222, 0.06243050787060593, -0.033407398444922784, -0.0908195296374078, 0.05712612739835794, 0.37764431001045384, -0.290696051516212, -0.1990246976707847, 0.0954775216568333, -0.31370897555652144, -0.1624191184844956, 0.09056055560851327, -0.06748754875018047, ... |
709.4679 | Periodic bifurcation from families of periodic solutions for semilinear
differential equations with Lipschitzian perturbations in Banach spaces | Let A:D(A)\to E be an infinitesimal generator either of an analytic compact
semigroup or of a contractive C_0-semigroup of linear operators acting in a
Banach space E. In this paper we give both necessary and sufficient conditions
for bifurcation of $T$-periodic solutions for the equation x'=Ax+f(t,x)+e
g(t,x,e) from... | math.CA | let adato e be an infinitesimal generator either of an analytic compact semigroup or of a contractive c_0semigroup of linear operators acting in a banach space e in this paper we give both necessary and sufficient conditions for bifurcation of tperiodic solutions for the equation xaxftxe gtxe from a kparameterized fami... | [['let', 'adato', 'e', 'be', 'an', 'infinitesimal', 'generator', 'either', 'of', 'an', 'analytic', 'compact', 'semigroup', 'or', 'of', 'a', 'contractive', 'c_0semigroup', 'of', 'linear', 'operators', 'acting', 'in', 'a', 'banach', 'space', 'e', 'in', 'this', 'paper', 'we', 'give', 'both', 'necessary', 'and', 'sufficien... | [-0.18479923686941108, 0.04984978148907734, -0.11423166291324452, 0.05415263609123999, -0.11108854195913224, -0.09873519121949387, 0.0237880445026785, 0.2824931377469282, -0.3039774152230683, -0.18749518091866096, 0.13127990818783125, -0.2488027970813881, -0.17764205656135532, 0.18908613335579724, -0.09879165809086668,... |
709.468 | Parameter Tuning of Three-Flavor Dynamical Anisotropic Clover Action | In this work, we perform parameter tuning with dynamical anisotropic clover
lattices using the Schr\"odinger functional and stout-smearing in the fermion
field. We find that $\xi_R/\xi_0$ is relatively close to 1 in our parameter
search, which allows us to fix $\xi_0$ in our runs. We proposed to determine
the gauge a... | hep-lat | in this work we perform parameter tuning with dynamical anisotropic clover lattices using the schrodinger functional and stoutsmearing in the fermion field we find that xi_rxi_0 is relatively close to 1 in our parameter search which allows us to fix xi_0 in our runs we proposed to determine the gauge and fermion anisot... | [['in', 'this', 'work', 'we', 'perform', 'parameter', 'tuning', 'with', 'dynamical', 'anisotropic', 'clover', 'lattices', 'using', 'the', 'schrodinger', 'functional', 'and', 'stoutsmearing', 'in', 'the', 'fermion', 'field', 'we', 'find', 'that', 'xi_rxi_0', 'is', 'relatively', 'close', 'to', '1', 'in', 'our', 'paramete... | [-0.09929167331418319, 0.20724752245940894, -0.10073033934372051, 0.08706476959338952, -0.08725906507477652, -0.15605132402003544, 0.05156188282819691, 0.4255478901040053, -0.16536995959598746, -0.2966602146320881, 0.025252354421618037, -0.2611278918046541, -0.12730965103571104, 0.15664845084223164, 0.00720114656941634... |
709.4681 | Regularity theory for fully nonlinear integro-differential equations | We consider nonlinear integro-differential equations, like the ones that
arise from stochastic control problems with purely jump L\`evy processes. We
obtain a nonlocal version of the ABP estimate, Harnack inequality, and interior
$C^{1,\alpha}$ regularity for general fully nonlinear integro-differential
equations. Ou... | math.AP | we consider nonlinear integrodifferential equations like the ones that arise from stochastic control problems with purely jump levy processes we obtain a nonlocal version of the abp estimate harnack inequality and interior c1alpha regularity for general fully nonlinear integrodifferential equations our estimates remain... | [['we', 'consider', 'nonlinear', 'integrodifferential', 'equations', 'like', 'the', 'ones', 'that', 'arise', 'from', 'stochastic', 'control', 'problems', 'with', 'purely', 'jump', 'levy', 'processes', 'we', 'obtain', 'a', 'nonlocal', 'version', 'of', 'the', 'abp', 'estimate', 'harnack', 'inequality', 'and', 'interior',... | [-0.08212180349842778, 0.05281039542917695, -0.096687649389995, 0.12877810447742896, -0.14763698013765472, -0.18106396745092102, -0.08699744822889832, 0.26049133951642683, -0.38596883301756213, -0.22871774962238436, 0.17521646617512618, -0.32094901641165574, -0.1498718623180009, 0.2068719652215285, -0.09263766947801091... |
709.4682 | Gravitational waves | These lectures are envisioned to be an introductory, basic course in
gravitational-wave physics.
| gr-qc | these lectures are envisioned to be an introductory basic course in gravitationalwave physics | [['these', 'lectures', 'are', 'envisioned', 'to', 'be', 'an', 'introductory', 'basic', 'course', 'in', 'gravitationalwave', 'physics']] | [-0.00406950583251623, 0.26383944454965574, -0.09834490702129327, 0.17608374672440383, -0.22449624108580443, -0.13472733410218588, -0.2257940031301517, 0.2861782988676658, -0.24975027717076814, -0.4276725889111941, 0.17790695311179242, -0.25387026484196, -0.1875358851483235, 0.30040208544009006, -0.1353956819153749, -0... |
710.0001 | Moduli Stabilization in Stringy ISS Models | We present a stringy realization of the ISS metastable SUSY breaking model
with moduli stabilization. The mass moduli of the ISS model is stabilized by
gauging of a U(1) symmetry and its D-term potential. The SUSY is broken both by
F-terms and D-terms. It is possible to obtain de-Sitter vacua with a
vanishingly small... | hep-th hep-ph | we present a stringy realization of the iss metastable susy breaking model with moduli stabilization the mass moduli of the iss model is stabilized by gauging of a u1 symmetry and its dterm potential the susy is broken both by fterms and dterms it is possible to obtain desitter vacua with a vanishingly small cosmologic... | [['we', 'present', 'a', 'stringy', 'realization', 'of', 'the', 'iss', 'metastable', 'susy', 'breaking', 'model', 'with', 'moduli', 'stabilization', 'the', 'mass', 'moduli', 'of', 'the', 'iss', 'model', 'is', 'stabilized', 'by', 'gauging', 'of', 'a', 'u1', 'symmetry', 'and', 'its', 'dterm', 'potential', 'the', 'susy', '... | [-0.2049548505317597, 0.2912248668192963, -0.040211920914728014, 0.11931668671165845, -0.11412325710989535, -0.19557022915354796, 0.016537566924290287, 0.30681951208010555, -0.22049042286853943, -0.29648701323284987, 0.1642217078719229, -0.1606779188390762, -0.10293693092489054, 0.04682187767817624, -0.0814888678077194... |
710.0002 | The Spectral Shape of the Gamma-ray Background from Blazars | The spectral shape of the unresolved emission from different classes of
gamma-ray emitters can be used to disentangle the contributions from these
populations to the extragalactic gamma-ray background (EGRB). We present a
calculation of the unabsorbed spectral shape of the unresolved blazar
contribution to the EGRB s... | astro-ph | the spectral shape of the unresolved emission from different classes of gammaray emitters can be used to disentangle the contributions from these populations to the extragalactic gammaray background egrb we present a calculation of the unabsorbed spectral shape of the unresolved blazar contribution to the egrb starting... | [['the', 'spectral', 'shape', 'of', 'the', 'unresolved', 'emission', 'from', 'different', 'classes', 'of', 'gammaray', 'emitters', 'can', 'be', 'used', 'to', 'disentangle', 'the', 'contributions', 'from', 'these', 'populations', 'to', 'the', 'extragalactic', 'gammaray', 'background', 'egrb', 'we', 'present', 'a', 'calc... | [-0.014281105961279046, 0.1354000625041328, -0.08887070192535615, 0.20172338144928506, -0.09171089534816655, -0.10016507686265393, 0.042675385831908316, 0.4238694760311453, -0.23482867170347219, -0.3919191897166362, 0.03588994603647508, -0.29637546016028815, 0.0011328089538324682, 0.21308992563661217, -0.04522312835939... |
710.0003 | Elemental Abundances of Blue Compact Dwarfs from mid-IR Spectroscopy
with Spitzer | We present a study of elemental abundances in a sample of thirteen Blue
Compact Dwarf (BCD) galaxies, using the $\sim$10--37$\mu$m high resolution
spectra obtained with Spitzer/IRS. We derive the abundances of neon and sulfur
for our sample using the infrared fine-structure lines probing regions which
may be obscured... | astro-ph | we present a study of elemental abundances in a sample of thirteen blue compact dwarf bcd galaxies using the sim1037mum high resolution spectra obtained with spitzerirs we derive the abundances of neon and sulfur for our sample using the infrared finestructure lines probing regions which may be obscured by dust in the ... | [['we', 'present', 'a', 'study', 'of', 'elemental', 'abundances', 'in', 'a', 'sample', 'of', 'thirteen', 'blue', 'compact', 'dwarf', 'bcd', 'galaxies', 'using', 'the', 'sim1037mum', 'high', 'resolution', 'spectra', 'obtained', 'with', 'spitzerirs', 'we', 'derive', 'the', 'abundances', 'of', 'neon', 'and', 'sulfur', 'fo... | [0.031728056123295025, 0.09551507487555431, -0.029318269540975144, 0.05668280454357944, 0.03390770497029288, -0.05643605361338596, 0.09011660578214067, 0.5096800891976607, -0.11190465614281334, -0.34289450338280525, 0.0023607550419006518, -0.33847463370317166, -0.006020994526089022, 0.17561323366642587, -0.052807049602... |
710.0004 | Synchronization problems for unidirectional feedback coupled nonlinear
systems | In this paper we consider three different synchronization problems consisting
in designing a nonlinear feedback unidirectional coupling term for two
(possibly chaotic) dynamical systems in order to drive the trajectories of one
of them, the slave system, to a reference trajectory or to a prescribed
neighborhood of th... | math.CA | in this paper we consider three different synchronization problems consisting in designing a nonlinear feedback unidirectional coupling term for two possibly chaotic dynamical systems in order to drive the trajectories of one of them the slave system to a reference trajectory or to a prescribed neighborhood of the refe... | [['in', 'this', 'paper', 'we', 'consider', 'three', 'different', 'synchronization', 'problems', 'consisting', 'in', 'designing', 'a', 'nonlinear', 'feedback', 'unidirectional', 'coupling', 'term', 'for', 'two', 'possibly', 'chaotic', 'dynamical', 'systems', 'in', 'order', 'to', 'drive', 'the', 'trajectories', 'of', 'on... | [-0.20034502629058423, 0.10521492126711904, -0.08897873035565944, 0.023227383490078725, -0.0311331732760696, -0.15729735015626975, 0.019025951397285613, 0.3078484245625562, -0.31909546258269683, -0.26992566630618986, 0.12716775630895577, -0.25764350934078456, -0.1690141496885039, 0.21953093786944344, -0.055002618115395... |
710.0005 | A refined analysis of the remarkable Bp star HR 6000 | UVES spectra of the very young (~10^7 years) peculiar B-type star HR 6000
were analyzed in the near-UV and visual spectral regions (3050-9460 A) with the
aim to extend to other spectral ranges the study made previously in the UV
using IUE spectra. Stellar parameters Teff=12850K, logg=4.10, and xi=0km/s, as
determined... | astro-ph | uves spectra of the very young 107 years peculiar btype star hr 6000 were analyzed in the nearuv and visual spectral regions 30509460 a with the aim to extend to other spectral ranges the study made previously in the uv using iue spectra stellar parameters teff12850k logg410 and xi0kms as determined from h_beta h_gamma... | [['uves', 'spectra', 'of', 'the', 'very', 'young', '107', 'years', 'peculiar', 'btype', 'star', 'hr', '6000', 'were', 'analyzed', 'in', 'the', 'nearuv', 'and', 'visual', 'spectral', 'regions', '30509460', 'a', 'with', 'the', 'aim', 'to', 'extend', 'to', 'other', 'spectral', 'ranges', 'the', 'study', 'made', 'previously... | [-0.004218239574631872, 0.09580821408225777, 0.042510421035235356, 0.055721382209939246, -0.005294917876821465, -0.1874442501958631, 0.06566220578755938, 0.43917907816266005, -0.1861489725741098, -0.36688553932962303, 0.0023979880762023016, -0.33089936221337046, 0.01535116876429081, 0.10767220491126002, -0.019123751625... |
710.0006 | Poincare index and periodic solutions of perturbed autonomous systems | The basic tool of classical results by Malkin and Melnikov on bifurcation of
periodic solutions from nondegenerate cycles of autonomous systems with
periodic perturbations is an implicit function theorem. In this paper the
Poincare index is used to avoid the requirement of nondegeneracity for the
unperturbed cycles a... | math.CA | the basic tool of classical results by malkin and melnikov on bifurcation of periodic solutions from nondegenerate cycles of autonomous systems with periodic perturbations is an implicit function theorem in this paper the poincare index is used to avoid the requirement of nondegeneracity for the unperturbed cycles and ... | [['the', 'basic', 'tool', 'of', 'classical', 'results', 'by', 'malkin', 'and', 'melnikov', 'on', 'bifurcation', 'of', 'periodic', 'solutions', 'from', 'nondegenerate', 'cycles', 'of', 'autonomous', 'systems', 'with', 'periodic', 'perturbations', 'is', 'an', 'implicit', 'function', 'theorem', 'in', 'this', 'paper', 'the... | [-0.21401802696666475, 0.037196763651297524, -0.11964547507843729, 0.04659658082626697, -0.04468185776623629, -0.11699050298686754, 0.023167255995558352, 0.26388549097513747, -0.29059108899180164, -0.2680272361168922, 0.15835443240101055, -0.2410801399846451, -0.20616686375716986, 0.23774754754820113, -0.11222143734852... |
710.0007 | Surface Brightness Profiles of Composite Images of Compact Galaxies at
z~4-6 in the HUDF | The Hubble Ultra Deep Field (HUDF) contains a significant number of B, V and
i'-band dropout objects, many of which were recently confirmed to be young
star-forming galaxies at z~4-6. These galaxies are too faint individually to
accurately measure their radial surface brightness profiles. Their average
light profiles... | astro-ph | the hubble ultra deep field hudf contains a significant number of b v and iband dropout objects many of which were recently confirmed to be young starforming galaxies at z46 these galaxies are too faint individually to accurately measure their radial surface brightness profiles their average light profiles are potentia... | [['the', 'hubble', 'ultra', 'deep', 'field', 'hudf', 'contains', 'a', 'significant', 'number', 'of', 'b', 'v', 'and', 'iband', 'dropout', 'objects', 'many', 'of', 'which', 'were', 'recently', 'confirmed', 'to', 'be', 'young', 'starforming', 'galaxies', 'at', 'z46', 'these', 'galaxies', 'are', 'too', 'faint', 'individua... | [-0.02904013023412674, 0.06513778717440989, -0.10105119412865265, 0.1104557415965246, -0.07298694510847845, -0.07656596848743182, 0.02426985968636943, 0.5167662204877506, -0.13773002974881693, -0.39711460093606327, 0.05557726218078109, -0.30161458630403826, -0.04149940983314019, 0.21801755747959572, -0.0717353897614822... |
710.0008 | Dissociative electron attachment to the H2O molecule. I. Complex-valued
potential-energy surfaces for the 2B1, 2A1, and 2B2 metastable states of the
water anion | We present the results of calculations defining global, three-dimensional
representations of the complex-valued potential-energy surfaces of the doublet
B1, doublet A1, and doublet B2 metastable states of the water anion that
underlie the physical process of dissociative electron attachment to water. The
real part of... | physics.chem-ph | we present the results of calculations defining global threedimensional representations of the complexvalued potentialenergy surfaces of the doublet b1 doublet a1 and doublet b2 metastable states of the water anion that underlie the physical process of dissociative electron attachment to water the real part of the reso... | [['we', 'present', 'the', 'results', 'of', 'calculations', 'defining', 'global', 'threedimensional', 'representations', 'of', 'the', 'complexvalued', 'potentialenergy', 'surfaces', 'of', 'the', 'doublet', 'b1', 'doublet', 'a1', 'and', 'doublet', 'b2', 'metastable', 'states', 'of', 'the', 'water', 'anion', 'that', 'unde... | [-0.08151712302761756, 0.09403238383543899, -0.056958357059805516, 0.055276051971527164, -0.005137892037951689, -0.09731847305427031, 0.027245793235320732, 0.36151179040802256, -0.1829984419972455, -0.25579004959628765, 0.0013722384284860153, -0.2773828089451618, -0.10693404606456379, 0.12212499461753173, 0.01346910647... |
710.0009 | Bio-linguistic transition and Baldwin effect in an evolutionary
naming-game model | We examine an evolutionary naming-game model where communicating agents are
equipped with an evolutionarily selected learning ability. Such a coupling of
biological and linguistic ingredients results in an abrupt transition: upon a
small change of a model control parameter a poorly communicating group of
linguistical... | cs.CL cond-mat.stat-mech cs.AI physics.soc-ph q-bio.PE | we examine an evolutionary naminggame model where communicating agents are equipped with an evolutionarily selected learning ability such a coupling of biological and linguistic ingredients results in an abrupt transition upon a small change of a model control parameter a poorly communicating group of linguistically un... | [['we', 'examine', 'an', 'evolutionary', 'naminggame', 'model', 'where', 'communicating', 'agents', 'are', 'equipped', 'with', 'an', 'evolutionarily', 'selected', 'learning', 'ability', 'such', 'a', 'coupling', 'of', 'biological', 'and', 'linguistic', 'ingredients', 'results', 'in', 'an', 'abrupt', 'transition', 'upon'... | [-0.10270081643414285, 0.18683986646491185, -0.09038235506575022, 0.04548417225596495, -0.15802203522762284, -0.1923076258573149, 0.09891069742318775, 0.4260010311912213, -0.28973937762369, -0.2994735445328323, 0.026248883178258048, -0.25754292200519036, -0.19388858569020936, 0.1058138757944107, -0.11636154885470334, -... |
710.001 | On algebraic time-derivative estimation and deadbeat state
reconstruction | This note places into perspective the so-called algebraic time-derivative
estimation method recently introduced by Fliess and co-authors with standard
results from linear state-space theory for control systems. In particular, it
is shown that the algebraic method can in a sense be seen as a special case of
deadbeat s... | math.OC | this note places into perspective the socalled algebraic timederivative estimation method recently introduced by fliess and coauthors with standard results from linear statespace theory for control systems in particular it is shown that the algebraic method can in a sense be seen as a special case of deadbeat state est... | [['this', 'note', 'places', 'into', 'perspective', 'the', 'socalled', 'algebraic', 'timederivative', 'estimation', 'method', 'recently', 'introduced', 'by', 'fliess', 'and', 'coauthors', 'with', 'standard', 'results', 'from', 'linear', 'statespace', 'theory', 'for', 'control', 'systems', 'in', 'particular', 'it', 'is',... | [-0.08396878665100026, 0.018148676768513554, -0.11486277994463, 0.03336943931861828, -0.06394164358912888, -0.1578673076168713, 0.0010741478112384173, 0.2691807273017653, -0.29178106948985894, -0.2687648388683417, 0.14282015112023486, -0.20042135280367554, -0.2387431207728588, 0.24272683247039883, -0.14662849069651912,... |
710.0011 | Negative Refraction Requires Strong Inhomogeneity | The paper establishes explicit lower bounds for the lattice cell size of
periodic structures (metamaterials and photonic crystals) capable of supporting
backward waves and producing negative refraction. At optical frequencies, this
result implies strong inhomogeneity, in the sense that the cell size cannot be
negligi... | physics.optics | the paper establishes explicit lower bounds for the lattice cell size of periodic structures metamaterials and photonic crystals capable of supporting backward waves and producing negative refraction at optical frequencies this result implies strong inhomogeneity in the sense that the cell size cannot be negligible rel... | [['the', 'paper', 'establishes', 'explicit', 'lower', 'bounds', 'for', 'the', 'lattice', 'cell', 'size', 'of', 'periodic', 'structures', 'metamaterials', 'and', 'photonic', 'crystals', 'capable', 'of', 'supporting', 'backward', 'waves', 'and', 'producing', 'negative', 'refraction', 'at', 'optical', 'frequencies', 'this... | [-0.19222634566778488, 0.23341253240677443, -0.00589225823059678, 0.022591425518674605, -0.08938017854128372, -0.11747844979505648, 0.07196815061933276, 0.4146553941748359, -0.2416883419013836, -0.24378832297568973, 0.04750871482855556, -0.20870826587250288, -0.12482107728719712, 0.23501978519965303, -0.038548015870831... |
710.0012 | The Segal-Bargmann transform for compact quotients of symmetric spaces
of the complex type | Let G/K be a Riemannian symmetric space of the complex type, meaning that G
is complex semisimple and K is a compact real form. Now let {\Gamma} be a
discrete subgroup of G that acts freely and cocompactly on G/K. We consider the
Segal--Bargmann transform, defined in terms of the heat equation, on the
compact quotien... | math-ph math.MP math.RT | let gk be a riemannian symmetric space of the complex type meaning that g is complex semisimple and k is a compact real form now let gamma be a discrete subgroup of g that acts freely and cocompactly on gk we consider the segalbargmann transform defined in terms of the heat equation on the compact quotient gammagk we o... | [['let', 'gk', 'be', 'a', 'riemannian', 'symmetric', 'space', 'of', 'the', 'complex', 'type', 'meaning', 'that', 'g', 'is', 'complex', 'semisimple', 'and', 'k', 'is', 'a', 'compact', 'real', 'form', 'now', 'let', 'gamma', 'be', 'a', 'discrete', 'subgroup', 'of', 'g', 'that', 'acts', 'freely', 'and', 'cocompactly', 'on'... | [-0.13829236858577656, 0.09378389916698432, -0.09107626703078464, 0.05878746807298986, -0.1820590338606577, -0.12572705240572912, 0.01415182685901774, 0.395254240513353, -0.2661921174060238, -0.2038184610211243, 0.13505047004594925, -0.2419407567151396, -0.1553788761809563, 0.2658652994758055, -0.09650956276916184, -0.... |
710.0013 | Lagrangian Relaxation for MAP Estimation in Graphical Models | We develop a general framework for MAP estimation in discrete and Gaussian
graphical models using Lagrangian relaxation techniques. The key idea is to
reformulate an intractable estimation problem as one defined on a more
tractable graph, but subject to additional constraints. Relaxing these
constraints gives a tract... | cs.AI | we develop a general framework for map estimation in discrete and gaussian graphical models using lagrangian relaxation techniques the key idea is to reformulate an intractable estimation problem as one defined on a more tractable graph but subject to additional constraints relaxing these constraints gives a tractable ... | [['we', 'develop', 'a', 'general', 'framework', 'for', 'map', 'estimation', 'in', 'discrete', 'and', 'gaussian', 'graphical', 'models', 'using', 'lagrangian', 'relaxation', 'techniques', 'the', 'key', 'idea', 'is', 'to', 'reformulate', 'an', 'intractable', 'estimation', 'problem', 'as', 'one', 'defined', 'on', 'a', 'mo... | [-0.10104700773067926, 0.02844553371674302, -0.08396373060531914, 0.09963198572049053, -0.1310562861275885, -0.1742466032214531, 0.08083660597325551, 0.3578742225430137, -0.34767904759752094, -0.31424090429849993, 0.13970490241500147, -0.2107018659728656, -0.18152287045393328, 0.17172142488501727, -0.09509580602459268,... |
710.0014 | Using evolutionary algorithms to extract field theory mass spectra | The spectrum of masses from a lattice QCD simulation may be found by fitting
exponential functions to correlators of operators possessing the quantum
numbers of the particles of interest. The ability of evolutionary algorithms to
find globally optimized solutions containing a variable number of states across
multiple... | hep-lat | the spectrum of masses from a lattice qcd simulation may be found by fitting exponential functions to correlators of operators possessing the quantum numbers of the particles of interest the ability of evolutionary algorithms to find globally optimized solutions containing a variable number of states across multiple da... | [['the', 'spectrum', 'of', 'masses', 'from', 'a', 'lattice', 'qcd', 'simulation', 'may', 'be', 'found', 'by', 'fitting', 'exponential', 'functions', 'to', 'correlators', 'of', 'operators', 'possessing', 'the', 'quantum', 'numbers', 'of', 'the', 'particles', 'of', 'interest', 'the', 'ability', 'of', 'evolutionary', 'alg... | [-0.13040316433069252, 0.10103213713164368, -0.13039917383520377, 0.06527601344795483, -0.03884274820752796, -0.10984501218245853, 0.06401525744946585, 0.33933391670386, -0.2590680993531668, -0.33101851595861337, 0.09494424583242526, -0.27942382180619807, -0.07634342373127029, 0.20470732939799155, 0.01759028969894326, ... |
710.0015 | Using Chemistry to Unveil the Kinematics of Starless Cores: Complex
Radial Motions in Barnard 68 | We present observations of 13CO, C18O, HCO+, H13CO+, DCO+ and N2H+ line
emission towards the Barnard 68 starless core. The line profiles are
interpreted using a chemical network coupled with a radiative transfer code in
order to reconstruct the radial velocity profile of the core. Our observations
and modeling indica... | astro-ph | we present observations of 13co c18o hco h13co dco and n2h line emission towards the barnard 68 starless core the line profiles are interpreted using a chemical network coupled with a radiative transfer code in order to reconstruct the radial velocity profile of the core our observations and modeling indicate the prese... | [['we', 'present', 'observations', 'of', '13co', 'c18o', 'hco', 'h13co', 'dco', 'and', 'n2h', 'line', 'emission', 'towards', 'the', 'barnard', '68', 'starless', 'core', 'the', 'line', 'profiles', 'are', 'interpreted', 'using', 'a', 'chemical', 'network', 'coupled', 'with', 'a', 'radiative', 'transfer', 'code', 'in', 'o... | [-0.06284554245493074, 0.08242128563927502, -0.045035839630804195, 0.030401025280011745, -0.06893604175429645, -0.03669276275474021, 0.015462875382710748, 0.4233491478082687, -0.20677698972656972, -0.3352917072905858, 0.06954245431821676, -0.21376520161806628, -0.015223753154571132, 0.12606413253238352, 0.0425685850402... |
710.0016 | Fluid turbulence and eddy viscosity in relativistic heavy-ion collisions | The eddy viscosity for a turbulent compressible fluid with a relativistic
equation of state is derived. Compressibility allows for sound modes, but the
eddy viscosity in the shear mode is found to be the same as for incompressible
fluids. For two space dimensions (which is the relevant case for the dynamics
of relati... | nucl-th hep-ph nucl-ex physics.flu-dyn | the eddy viscosity for a turbulent compressible fluid with a relativistic equation of state is derived compressibility allows for sound modes but the eddy viscosity in the shear mode is found to be the same as for incompressible fluids for two space dimensions which is the relevant case for the dynamics of relativistic... | [['the', 'eddy', 'viscosity', 'for', 'a', 'turbulent', 'compressible', 'fluid', 'with', 'a', 'relativistic', 'equation', 'of', 'state', 'is', 'derived', 'compressibility', 'allows', 'for', 'sound', 'modes', 'but', 'the', 'eddy', 'viscosity', 'in', 'the', 'shear', 'mode', 'is', 'found', 'to', 'be', 'the', 'same', 'as', ... | [-0.15906424262364835, 0.2527056498354987, -0.13982707527711202, 0.06092611447246255, -0.07529277818179445, -0.10407618630775496, -0.11440015224445807, 0.22142956994081797, -0.2929676868021488, -0.2368759169586395, 0.0732472218597602, -0.2646120536020087, 0.006096750948774187, 0.206201401294062, 0.04606262459909837, 0.... |
710.0017 | Improvement of the pion spectrum with HYP-smeared staggered fermions | We extend our previous study of taste-symmetry breaking using HYP-smeared
staggered fermions in two ways. First, we improve the statistics of a
comparison of unimproved and HYP-smeared staggered fermions on quenched
lattices with $a\approx 0.1 $fm. This allows us to obtain a signal for all pion
tastes, rather than ju... | hep-lat | we extend our previous study of tastesymmetry breaking using hypsmeared staggered fermions in two ways first we improve the statistics of a comparison of unimproved and hypsmeared staggered fermions on quenched lattices with aapprox 01 fm this allows us to obtain a signal for all pion tastes rather than just a subset a... | [['we', 'extend', 'our', 'previous', 'study', 'of', 'tastesymmetry', 'breaking', 'using', 'hypsmeared', 'staggered', 'fermions', 'in', 'two', 'ways', 'first', 'we', 'improve', 'the', 'statistics', 'of', 'a', 'comparison', 'of', 'unimproved', 'and', 'hypsmeared', 'staggered', 'fermions', 'on', 'quenched', 'lattices', 'w... | [-0.05725670466962896, 0.2785011998026586, -0.0884898155049772, 0.0910630452209992, -0.08637477555999258, -0.11227292530085953, 0.165519038327878, 0.40996113948554536, -0.14374087769614502, -0.28620342514286823, 0.02516085983704409, -0.308238113764912, -0.047116557739247555, 0.07569147091068816, 0.021394992953349578, 0... |
710.0018 | Comment on "Critique of the foundations of time-dependent density
functional theory" [Phys. Rev.A. 75, 022513 (2007)] | A recent paper (Phys. Rev A. 75, 022513 (2007), arXiv:cond-mat/0602020)
challenges exact time-dependent density functional theory (TDDFT) on several
grounds. We explain why these criticisms are either irrelevant or incorrect,
and that TDDFT is both formally exact and predictive.
| cond-mat.other | a recent paper phys rev a 75 022513 2007 arxivcondmat0602020 challenges exact timedependent density functional theory tddft on several grounds we explain why these criticisms are either irrelevant or incorrect and that tddft is both formally exact and predictive | [['a', 'recent', 'paper', 'phys', 'rev', 'a', '75', '022513', '2007', 'arxivcondmat0602020', 'challenges', 'exact', 'timedependent', 'density', 'functional', 'theory', 'tddft', 'on', 'several', 'grounds', 'we', 'explain', 'why', 'these', 'criticisms', 'are', 'either', 'irrelevant', 'or', 'incorrect', 'and', 'that', 'td... | [-0.04258684410811647, 0.0030620929687038847, -0.09743231485940908, 0.10619188124914408, -0.08867300434136077, -0.1663205492261209, 0.10950740102041316, 0.3619055696763098, -0.113335157671061, -0.3234438700111289, 0.02448630214272079, -0.34865761283589036, -0.27758323752296793, 0.11557432175246313, -0.16380273028105302... |
710.0019 | The Glue Content of the Pion | We perform a quenched computation of the glue momentum fraction in the pion.
Different discretizations of the gluonic energy-momentum tensor are studied on
the lattice for that purpose. We discuss some implications based on the
momentum sum rule. Finally we point out promising applications of the
techniques developed... | hep-lat | we perform a quenched computation of the glue momentum fraction in the pion different discretizations of the gluonic energymomentum tensor are studied on the lattice for that purpose we discuss some implications based on the momentum sum rule finally we point out promising applications of the techniques developed here | [['we', 'perform', 'a', 'quenched', 'computation', 'of', 'the', 'glue', 'momentum', 'fraction', 'in', 'the', 'pion', 'different', 'discretizations', 'of', 'the', 'gluonic', 'energymomentum', 'tensor', 'are', 'studied', 'on', 'the', 'lattice', 'for', 'that', 'purpose', 'we', 'discuss', 'some', 'implications', 'based', '... | [-0.12883775510198, 0.1553300323572998, -0.11757819780281611, 0.09366980925254638, -0.06763748351332484, -0.034583518652207386, 0.08240881284736858, 0.406320544225829, -0.1896173495571224, -0.16958445778154596, 0.0723311986788461, -0.24210117405698617, -0.13437536085138516, 0.16217388444561132, 0.05490711832725519, 0.0... |
710.002 | A Probability Model for Lifetime of Wireless Sensor Networks | Considering a wireless sensor network whose nodes are distributed randomly
over a given area, a probability model for the network lifetime is provided.
Using this model and assuming that packet generation follows a Poisson
distribution, an analytical expression for the complementary cumulative density
function (ccdf)... | cs.NI | considering a wireless sensor network whose nodes are distributed randomly over a given area a probability model for the network lifetime is provided using this model and assuming that packet generation follows a poisson distribution an analytical expression for the complementary cumulative density function ccdf of the... | [['considering', 'a', 'wireless', 'sensor', 'network', 'whose', 'nodes', 'are', 'distributed', 'randomly', 'over', 'a', 'given', 'area', 'a', 'probability', 'model', 'for', 'the', 'network', 'lifetime', 'is', 'provided', 'using', 'this', 'model', 'and', 'assuming', 'that', 'packet', 'generation', 'follows', 'a', 'poiss... | [-0.1557838253130386, 0.09105233423522602, -0.051503182886840984, 0.023344297567544144, -0.0008489478592916081, -0.16236412533584776, 0.03126547779376981, 0.3955272399729842, -0.27523891122352023, -0.302291257164648, 0.08396973947270049, -0.2703227043320011, -0.16784727220753362, 0.20895176999975876, -0.068601829446076... |
710.0021 | New families of cryptographic systems | A symmetric encryption method based on properties of quasicrystals is
proposed. The advantages of the cipher are strict aperiodicity and everywhere
discontinuous property as well as the speed of computation, simplicity of
implementation and a straightforward possibility of extending the method to
encryption of higher... | cs.CR math.GM | a symmetric encryption method based on properties of quasicrystals is proposed the advantages of the cipher are strict aperiodicity and everywhere discontinuous property as well as the speed of computation simplicity of implementation and a straightforward possibility of extending the method to encryption of higher dim... | [['a', 'symmetric', 'encryption', 'method', 'based', 'on', 'properties', 'of', 'quasicrystals', 'is', 'proposed', 'the', 'advantages', 'of', 'the', 'cipher', 'are', 'strict', 'aperiodicity', 'and', 'everywhere', 'discontinuous', 'property', 'as', 'well', 'as', 'the', 'speed', 'of', 'computation', 'simplicity', 'of', 'i... | [-0.12213474290168032, -0.009731182313345849, -0.11562097875123963, 0.011129314865064906, -0.10928673764809649, -0.16775533558919709, 0.046946587873266096, 0.35770541025286023, -0.28321994254563715, -0.22898234308083007, 0.1786296460777521, -0.20395856481441793, -0.14608660734635084, 0.2411601489330543, -0.093801374615... |
710.0022 | Astronomical constraints on some long-range models of modified gravity | In this paper we use the corrections to the usual Newton-Einstein secular
precessions of the perihelia of the inner planets of the Solar System,
phenomenologically estimated as solve-for parameters by the Russian astronomer
E.V. Pitjeva by fitting almost one century of data with the EPM2004
ephemerides, in order to c... | gr-qc astro-ph hep-ph physics.space-ph | in this paper we use the corrections to the usual newtoneinstein secular precessions of the perihelia of the inner planets of the solar system phenomenologically estimated as solvefor parameters by the russian astronomer ev pitjeva by fitting almost one century of data with the epm2004 ephemerides in order to constrain... | [['in', 'this', 'paper', 'we', 'use', 'the', 'corrections', 'to', 'the', 'usual', 'newtoneinstein', 'secular', 'precessions', 'of', 'the', 'perihelia', 'of', 'the', 'inner', 'planets', 'of', 'the', 'solar', 'system', 'phenomenologically', 'estimated', 'as', 'solvefor', 'parameters', 'by', 'the', 'russian', 'astronomer'... | [-0.0918828851378075, 0.1120480765243779, -0.06615783143895217, 0.12390164901814268, -0.08130413659258198, -0.12838771228477686, 0.04196070245589762, 0.30166470976759685, -0.21856146633895185, -0.35922381898942796, 0.09569499419934564, -0.27775514532388934, -0.08901741625634484, 0.21106527883467044, -0.0590247961617864... |
710.0023 | Pairing with Unconventional Symmetry around BCS-BEC Crossover: Fermionic
Atoms in 2D Optical Lattices to Correlated Electron Systems | We study superfluid properties of fermions on a 2D lattice using a
finite-range pairing interaction derivable from an extended Hubbard model. We
obtain signatures of unconventional pair-symmetry states, $d_{x^2-y^2}$ and
extended-s ($s^*$), in the BCS-BEC crossover region. The fermion momentum
distribution function, ... | cond-mat.supr-con cond-mat.other | we study superfluid properties of fermions on a 2d lattice using a finiterange pairing interaction derivable from an extended hubbard model we obtain signatures of unconventional pairsymmetry states d_x2y2 and extendeds s in the bcsbec crossover region the fermion momentum distribution function v_k2 the ratio of the bo... | [['we', 'study', 'superfluid', 'properties', 'of', 'fermions', 'on', 'a', '2d', 'lattice', 'using', 'a', 'finiterange', 'pairing', 'interaction', 'derivable', 'from', 'an', 'extended', 'hubbard', 'model', 'we', 'obtain', 'signatures', 'of', 'unconventional', 'pairsymmetry', 'states', 'd_x2y2', 'and', 'extendeds', 's', ... | [-0.16348257507898553, 0.21036291189672632, -0.11849119265936815, 0.08902367995551197, -0.03951564680169066, -0.15793505468736252, 0.07745215061661456, 0.37081302836617475, -0.2420046497336639, -0.19601958481374607, -0.03003537903604929, -0.33854293718092865, -0.1300816154307736, 0.1497564415136973, 0.08920291174761451... |
710.0024 | Optimized Broad-Histogram Ensembles for the Simulation of Quantum
Systems | The efficiency of statistical sampling in broad-histogram Monte Carlo
simulations can be considerably improved by optimizing the simulated extended
ensemble for fastest equilibration. Here we describe how a recently developed
feedback algorithm can be generalized to find optimized sampling distributions
for the simul... | cond-mat.stat-mech | the efficiency of statistical sampling in broadhistogram monte carlo simulations can be considerably improved by optimizing the simulated extended ensemble for fastest equilibration here we describe how a recently developed feedback algorithm can be generalized to find optimized sampling distributions for the simulatio... | [['the', 'efficiency', 'of', 'statistical', 'sampling', 'in', 'broadhistogram', 'monte', 'carlo', 'simulations', 'can', 'be', 'considerably', 'improved', 'by', 'optimizing', 'the', 'simulated', 'extended', 'ensemble', 'for', 'fastest', 'equilibration', 'here', 'we', 'describe', 'how', 'a', 'recently', 'developed', 'fee... | [-0.08011695159160916, 0.13863806918989746, -0.1198298030615072, 0.06947804759992697, -0.007913358523236477, -0.09558991432491251, 0.06431232195224285, 0.4028546097414458, -0.30175756274119897, -0.29344951115148005, 0.11979489128947642, -0.22923613811487004, -0.14301626477732926, 0.16175131906536133, 0.0065855997897870... |
710.0025 | Search for Ultra-High Energy Photons with the Pierre Auger Observatory | Data taken at the Pierre Auger Observatory are used to search for air showers
initiated by ultra-high energy (UHE) photons. Results of searches are reported
from hybrid observations where events are measured with both fluorescence and
array detectors. Additionally, a more stringent test of the photon fluxes
predicted... | astro-ph | data taken at the pierre auger observatory are used to search for air showers initiated by ultrahigh energy uhe photons results of searches are reported from hybrid observations where events are measured with both fluorescence and array detectors additionally a more stringent test of the photon fluxes predicted with en... | [['data', 'taken', 'at', 'the', 'pierre', 'auger', 'observatory', 'are', 'used', 'to', 'search', 'for', 'air', 'showers', 'initiated', 'by', 'ultrahigh', 'energy', 'uhe', 'photons', 'results', 'of', 'searches', 'are', 'reported', 'from', 'hybrid', 'observations', 'where', 'events', 'are', 'measured', 'with', 'both', 'f... | [-0.05794621013827028, 0.2617000699299725, -0.01261729981912219, 0.13222203233685897, -0.004384671898045834, -0.06972540554631015, 0.011984596022175274, 0.41180468158985395, -0.11306967045706899, -0.4758368511346803, 0.04474925000787429, -0.4262806215471979, 0.024319446335236233, 0.28803675296797376, 0.1070690994569356... |
710.0026 | Irrational Stable Commutator Length in Finitely Presented Groups | We give examples of finitely presented groups containing elements with
irrational (in fact, transcendental) stable commutator length, thus answering
in the negative a question of M. Gromov. Our examples come from 1-dimensional
dynamics, and are related to the generalized Thompson groups studied by M.
Stein, I. Liouss... | math.GT math.DS | we give examples of finitely presented groups containing elements with irrational in fact transcendental stable commutator length thus answering in the negative a question of m gromov our examples come from 1dimensional dynamics and are related to the generalized thompson groups studied by m stein i liousse and others | [['we', 'give', 'examples', 'of', 'finitely', 'presented', 'groups', 'containing', 'elements', 'with', 'irrational', 'in', 'fact', 'transcendental', 'stable', 'commutator', 'length', 'thus', 'answering', 'in', 'the', 'negative', 'a', 'question', 'of', 'm', 'gromov', 'our', 'examples', 'come', 'from', '1dimensional', 'd... | [-0.12467775129092236, 0.17002390246489085, -0.03483989636879414, 0.10686648265497449, -0.08817372161138337, -0.17677440281840973, 0.04614245344419032, 0.3529128592150907, -0.3210993737836058, -0.25985682644629077, 0.05633104228278777, -0.30994869347584125, -0.1625527891640862, 0.25918450294799794, -0.15570409659994766... |
710.0027 | Ramsey numbers of sparse hypergraphs | We give a short proof that any k-uniform hypergraph H on n vertices with
bounded degree \Delta has Ramsey number at most c(\Delta, k)n, for an
appropriate constant c(\Delta, k). This result was recently proved by several
authors, but those proofs are all based on applications of the hypergraph
regularity method. Here... | math.CO | we give a short proof that any kuniform hypergraph h on n vertices with bounded degree delta has ramsey number at most cdelta kn for an appropriate constant cdelta k this result was recently proved by several authors but those proofs are all based on applications of the hypergraph regularity method here we give a much ... | [['we', 'give', 'a', 'short', 'proof', 'that', 'any', 'kuniform', 'hypergraph', 'h', 'on', 'n', 'vertices', 'with', 'bounded', 'degree', 'delta', 'has', 'ramsey', 'number', 'at', 'most', 'cdelta', 'kn', 'for', 'an', 'appropriate', 'constant', 'cdelta', 'k', 'this', 'result', 'was', 'recently', 'proved', 'by', 'several'... | [-0.12206730693095487, 0.11383656715646931, -0.08649876610662952, 0.011109857234236954, -0.0997487341914818, -0.1970678962234103, 0.08018691501427887, 0.3330139101266205, -0.20650563619550574, -0.33495412264077823, 0.059298745692567024, -0.2864838942151214, -0.132458268297227, 0.2220603048174683, -0.08783543716424948, ... |
710.0028 | Constraints on Unparticles from Low Energy Neutrino-Electron Scattering | We place limits on scalar and vector unparticle couplings to electrons and
neutrinos using data from reactor neutrino experiments originally designed to
search for neutrino magnetic moment. Upper bounds on Standard Model
lepton-scalar unparticle and lepton-vector unparticle couplings $\lambda_0$,
and $\lambda_1$ are ... | hep-ph | we place limits on scalar and vector unparticle couplings to electrons and neutrinos using data from reactor neutrino experiments originally designed to search for neutrino magnetic moment upper bounds on standard model leptonscalar unparticle and leptonvector unparticle couplings lambda_0 and lambda_1 are given for va... | [['we', 'place', 'limits', 'on', 'scalar', 'and', 'vector', 'unparticle', 'couplings', 'to', 'electrons', 'and', 'neutrinos', 'using', 'data', 'from', 'reactor', 'neutrino', 'experiments', 'originally', 'designed', 'to', 'search', 'for', 'neutrino', 'magnetic', 'moment', 'upper', 'bounds', 'on', 'standard', 'model', 'l... | [-0.08450165396894921, 0.2669540554877709, 0.0227998703294857, 0.19409866019744765, -0.06041491126683964, -0.16760089771864428, 0.03734907459901561, 0.2829287347383797, -0.19409095523032274, -0.35876245695081627, 0.048160175733606925, -0.3360345713201572, -0.016897637181153353, 0.23313840158199045, 0.1198366898365996, ... |
710.0029 | Candidate Rotating Toroids around High-Mass (Proto)Stars | Using the OVRO, Nobeyama, and IRAM mm-arrays, we searched for
``disk''-outflow systems in three high-mass (proto)star forming regions:
G16.59-0.05, G23.01-0.41, and G28.87+0.07. These were selected from a sample of
NH3 cores associated with OH and H2O maser emission and with no or very faint
continuum emission. Our i... | astro-ph | using the ovro nobeyama and iram mmarrays we searched for diskoutflow systems in three highmass protostar forming regions g1659005 g2301041 and g2887007 these were selected from a sample of nh3 cores associated with oh and h2o maser emission and with no or very faint continuum emission our imaging of molecular line inc... | [['using', 'the', 'ovro', 'nobeyama', 'and', 'iram', 'mmarrays', 'we', 'searched', 'for', 'diskoutflow', 'systems', 'in', 'three', 'highmass', 'protostar', 'forming', 'regions', 'g1659005', 'g2301041', 'and', 'g2887007', 'these', 'were', 'selected', 'from', 'a', 'sample', 'of', 'nh3', 'cores', 'associated', 'with', 'oh... | [-0.08742981309497869, 0.10480138608141668, -0.0014854360484577375, 0.04371531384418583, -0.06756914681078054, -0.08107609505814373, 0.012814832744619394, 0.4734621854244612, -0.1743546250736031, -0.3197338336746368, 0.09420616956148707, -0.2540160539541558, -0.0038495803013903454, 0.14780453716492944, 0.03522950715061... |
710.003 | Topological Mott Insulators | We consider extended Hubbard models with repulsive interactions on a
Honeycomb lattice and the transitions from the semi-metal phase at half-filling
to Mott insulating phases. In particular, due to the frustrating nature of the
second-neighbor repulsive interactions, topological Mott phases displaying the
quantum Hal... | cond-mat.mes-hall cond-mat.str-el | we consider extended hubbard models with repulsive interactions on a honeycomb lattice and the transitions from the semimetal phase at halffilling to mott insulating phases in particular due to the frustrating nature of the secondneighbor repulsive interactions topological mott phases displaying the quantum hall and th... | [['we', 'consider', 'extended', 'hubbard', 'models', 'with', 'repulsive', 'interactions', 'on', 'a', 'honeycomb', 'lattice', 'and', 'the', 'transitions', 'from', 'the', 'semimetal', 'phase', 'at', 'halffilling', 'to', 'mott', 'insulating', 'phases', 'in', 'particular', 'due', 'to', 'the', 'frustrating', 'nature', 'of',... | [-0.2207109869729417, 0.3125375768286176, -0.06214459374192908, 0.08615761920615721, -0.0037938804453006014, -0.24200475049534967, 0.12539318956745168, 0.35749930413051817, -0.25052831240464, -0.2008602101316986, -0.005303448790073162, -0.36546816511933383, -0.18087652158768228, 0.03097613520609836, 0.10643387302358558... |
710.0031 | Study of $B_{c}^{-}$ ${\to}$ $J/{\psi}{\pi}^{-}$, ${\eta}_{c}{\pi}^{-}$
Decays with QCD Factorization | The $B_{c}$ ${\to}$ $J/{\psi}{\pi}$, ${\eta}_{c}{\pi}$ decays are studied in
the scheme of the QCD factorization approach. The branching ratios are
calculated with the asymptotic distribution amplitude of the pion. The charm
quark mass effect is considered. We find that the mass effect on the branching
ratios is smal... | hep-ph | the b_c to jpsipi eta_cpi decays are studied in the scheme of the qcd factorization approach the branching ratios are calculated with the asymptotic distribution amplitude of the pion the charm quark mass effect is considered we find that the mass effect on the branching ratios is small | [['the', 'b_c', 'to', 'jpsipi', 'eta_cpi', 'decays', 'are', 'studied', 'in', 'the', 'scheme', 'of', 'the', 'qcd', 'factorization', 'approach', 'the', 'branching', 'ratios', 'are', 'calculated', 'with', 'the', 'asymptotic', 'distribution', 'amplitude', 'of', 'the', 'pion', 'the', 'charm', 'quark', 'mass', 'effect', 'is'... | [-0.12437497932357171, 0.26440537579280016, -0.10795984929427505, 0.15348803202990288, -0.0015090100932866335, -0.04382512328447774, 0.0725998411483791, 0.332166551767538, -0.14793604382187672, -0.18989248833774278, -0.021488818963310525, -0.2989113808143884, 0.011610516346991062, 0.10969004702443878, 0.089305180124938... |
710.0032 | Extended TQFT's and Quantum Gravity | This paper gives a definition of an extended topological quantum field theory
(TQFT) as a weak 2-functor Z: nCob_2 -> 2Vect, by analogy with the description
of a TQFT as a functor Z: nCob -> Vect. We also show how to obtain such a
theory from any finite group G. This theory is related to a topological gauge
theory, t... | math.QA math.CT | this paper gives a definition of an extended topological quantum field theory tqft as a weak 2functor z ncob_2 2vect by analogy with the description of a tqft as a functor z ncob vect we also show how to obtain such a theory from any finite group g this theory is related to a topological gauge theory the dijkgraafwitte... | [['this', 'paper', 'gives', 'a', 'definition', 'of', 'an', 'extended', 'topological', 'quantum', 'field', 'theory', 'tqft', 'as', 'a', 'weak', '2functor', 'z', 'ncob_2', '2vect', 'by', 'analogy', 'with', 'the', 'description', 'of', 'a', 'tqft', 'as', 'a', 'functor', 'z', 'ncob', 'vect', 'we', 'also', 'show', 'how', 'to... | [-0.13513718943773623, 0.11926409427413669, -0.12498210347725086, 0.12109617159017418, -0.10853686839731104, -0.12495239007746778, 0.002121227549811653, 0.3736318600135874, -0.31487342620635006, -0.24747967882919683, 0.05727364284399687, -0.2141100586484089, -0.20910652334536295, 0.171062472163247, -0.16935847943974097... |
710.0033 | Particle Tracking with a Thin Pixel Telescope | We report results on a tracking performance study performed using a beam
telescope made of 50 micron-thick CMOS pixel sensors on the 1.5 GeV electron
beam at the LBNL ALS.
| physics.ins-det | we report results on a tracking performance study performed using a beam telescope made of 50 micronthick cmos pixel sensors on the 15 gev electron beam at the lbnl als | [['we', 'report', 'results', 'on', 'a', 'tracking', 'performance', 'study', 'performed', 'using', 'a', 'beam', 'telescope', 'made', 'of', '50', 'micronthick', 'cmos', 'pixel', 'sensors', 'on', 'the', '15', 'gev', 'electron', 'beam', 'at', 'the', 'lbnl', 'als']] | [-0.0735459161301454, 0.09991254699416459, -0.025276716969286402, -0.05784999846170346, 0.05257749965724846, -0.16833068799848358, 0.06364722764119506, 0.4978215917944908, -0.0862480773900946, -0.4005792647600174, 0.08087913556955754, -0.3608486708253622, 0.03778644353151321, 0.2968274037353694, -0.05248898764451345, 0... |
710.0034 | Developments in finite Phan theory | This is a final report on finite Phan theory, a project that has been
concerned with a revision and generalisation of Phan's presentation results of
twisted Chevalley groups over finite fields with simply laced diagrams by
unitary subgroups of rank one and two. Finite Phan theory has been initiated on
request by Rich... | math.GR math.HO | this is a final report on finite phan theory a project that has been concerned with a revision and generalisation of phans presentation results of twisted chevalley groups over finite fields with simply laced diagrams by unitary subgroups of rank one and two finite phan theory has been initiated on request by richard l... | [['this', 'is', 'a', 'final', 'report', 'on', 'finite', 'phan', 'theory', 'a', 'project', 'that', 'has', 'been', 'concerned', 'with', 'a', 'revision', 'and', 'generalisation', 'of', 'phans', 'presentation', 'results', 'of', 'twisted', 'chevalley', 'groups', 'over', 'finite', 'fields', 'with', 'simply', 'laced', 'diagra... | [-0.12432090422584557, 0.1342601843873485, -0.11533252227211922, 0.004654428095255099, -0.1346663315255772, -0.09801485964661123, 0.07573623547632195, 0.36327906469748894, -0.19767582307661502, -0.24956890951159974, 0.1296998615684906, -0.24894083829098185, -0.10708543923306345, 0.18822596084431442, -0.1781349606733297... |
710.0035 | On a two variable class of Bernstein-Szego measures | The one variable Bernstein-Szego theory for orthogonal polynomials on the
real line is extended to a class of two variable measures. The polynomials
orthonormal in the total degree ordering and the lexicographical ordering are
constructed and their recurrence coefficients discussed.
| math.CA | the one variable bernsteinszego theory for orthogonal polynomials on the real line is extended to a class of two variable measures the polynomials orthonormal in the total degree ordering and the lexicographical ordering are constructed and their recurrence coefficients discussed | [['the', 'one', 'variable', 'bernsteinszego', 'theory', 'for', 'orthogonal', 'polynomials', 'on', 'the', 'real', 'line', 'is', 'extended', 'to', 'a', 'class', 'of', 'two', 'variable', 'measures', 'the', 'polynomials', 'orthonormal', 'in', 'the', 'total', 'degree', 'ordering', 'and', 'the', 'lexicographical', 'ordering'... | [-0.21849402751540764, 0.13522668567020446, -0.023383116582408547, 0.07902706609165762, -0.11152950194664299, -0.1135730994050391, 0.02719288753287401, 0.3846991420723498, -0.30807245476171374, -0.19129510892089457, 0.11992797470011282, -0.2919341573258862, -0.1262100285384804, 0.1365385077893734, 0.024287637695670126,... |
710.0036 | Time-Loop Formalism for Irreversible Quantum Problems: Steady State
Transport in Junctions with Asymmetric Dynamics | Non-unitary quantum mechanics has been used in the past to study
irreversibility, dissipation and decay in a variety of physical systems. In
this letter, we propose a general scheme to deal with systems governed by
non-Hermitian Hamiltonians. We argue that the Schwinger-Keldysh formalism gives
a natural description f... | cond-mat.mes-hall hep-th physics.atom-ph quant-ph | nonunitary quantum mechanics has been used in the past to study irreversibility dissipation and decay in a variety of physical systems in this letter we propose a general scheme to deal with systems governed by nonhermitian hamiltonians we argue that the schwingerkeldysh formalism gives a natural description for those ... | [['nonunitary', 'quantum', 'mechanics', 'has', 'been', 'used', 'in', 'the', 'past', 'to', 'study', 'irreversibility', 'dissipation', 'and', 'decay', 'in', 'a', 'variety', 'of', 'physical', 'systems', 'in', 'this', 'letter', 'we', 'propose', 'a', 'general', 'scheme', 'to', 'deal', 'with', 'systems', 'governed', 'by', 'n... | [-0.15476539837254677, 0.13099104321026972, -0.11843437129864469, 0.06998891460243613, -0.03429485954111442, -0.18396835276507773, -0.018974682749831117, 0.30550576860550793, -0.2683348196616862, -0.26902739104116336, -0.01632980966969626, -0.22054943162947893, -0.23922075883019717, 0.20912445948633832, -0.092460451880... |
710.0037 | Notes on a paper of Tyagi and Holm: A new integral representation for
the Riemann Zeta function | It is shown that a new series representation of Riemann s Zeta function
obtained by Tyagi and Holm leads to an interesting new recursion for Bernoulli
numbers of even index as well as new representations of, and infinite series
involving, Zeta functions of special (integer) argument.
| math.CA math.CV | it is shown that a new series representation of riemann s zeta function obtained by tyagi and holm leads to an interesting new recursion for bernoulli numbers of even index as well as new representations of and infinite series involving zeta functions of special integer argument | [['it', 'is', 'shown', 'that', 'a', 'new', 'series', 'representation', 'of', 'riemann', 's', 'zeta', 'function', 'obtained', 'by', 'tyagi', 'and', 'holm', 'leads', 'to', 'an', 'interesting', 'new', 'recursion', 'for', 'bernoulli', 'numbers', 'of', 'even', 'index', 'as', 'well', 'as', 'new', 'representations', 'of', 'an... | [-0.16696818512813796, 0.09267820255184273, -0.12824460641359506, 0.12224886065561567, -0.12869314144810903, -0.18149151777565156, 0.040557957550450024, 0.2697052654364835, -0.32267077250973036, -0.28230323245667893, 0.09389131427135157, -0.20721630728297422, -0.2408101254183313, 0.2832242630563838, -0.0405450729734223... |
710.0038 | Characterization of the matrix whose norm is determined by its action on
decreasing sequences:The exceptional cases | Let $A=(a_{j,k})_{j,k \ge 1}$ be a non-negative matrix. In this paper, we
characterize those $A$ for which $\|A\|_{\ell_p,\ell_q}$ are determined by
their actions on non-negative decreasing sequences, where one of $p$ and $q$ is
1 or $\infty$. The conditions forcing on $A$ are sufficient and they are also
necessary f... | math.FA math.CA | let aa_jk_jk ge 1 be a nonnegative matrix in this paper we characterize those a for which a_ell_pell_q are determined by their actions on nonnegative decreasing sequences where one of p and q is 1 or infty the conditions forcing on a are sufficient and they are also necessary for nonnegative finite matrices | [['let', 'aa_jk_jk', 'ge', '1', 'be', 'a', 'nonnegative', 'matrix', 'in', 'this', 'paper', 'we', 'characterize', 'those', 'a', 'for', 'which', 'a_ell_pell_q', 'are', 'determined', 'by', 'their', 'actions', 'on', 'nonnegative', 'decreasing', 'sequences', 'where', 'one', 'of', 'p', 'and', 'q', 'is', '1', 'or', 'infty', '... | [-0.12977835152517347, 0.2223209896325773, -0.03558773649673836, 0.045090775389005154, -0.0133952125039536, -0.21050596228052004, -0.02506910006323939, 0.38505060159984755, -0.28566017856492715, -0.20847656922049673, 0.1978033404117085, -0.30793746045845394, -0.13705284173563853, 0.1371694942160199, -0.0828284522628083... |
710.0039 | Search for the Invisible Decay of $\jpsi$ in
$\psi(2S)\to\pi+\pi^-J/\psi$ | Using 14.0 million $\psi(2S) events collected with the BES-II detector, a
search for the decay of the $\jpsi$ to an invisible final state in $\psipto$ is
performed. The $\jpsi$ peak in the distribution of mass recoiling against the
$\pi^+\pi^-$ is used to tag $\psi$ invisible decay. No signal is found, and an
upper l... | hep-ex | using 140 million psi2s events collected with the besii detector a search for the decay of the jpsi to an invisible final state in psipto is performed the jpsi peak in the distribution of mass recoiling against the pipi is used to tag psi invisible decay no signal is found and an upper limit at the 90 confidence level ... | [['using', '140', 'million', 'psi2s', 'events', 'collected', 'with', 'the', 'besii', 'detector', 'a', 'search', 'for', 'the', 'decay', 'of', 'the', 'jpsi', 'to', 'an', 'invisible', 'final', 'state', 'in', 'psipto', 'is', 'performed', 'the', 'jpsi', 'peak', 'in', 'the', 'distribution', 'of', 'mass', 'recoiling', 'agains... | [-0.06551146433677202, 0.19464331179879532, -0.11731882690578516, 0.13393687617815572, -0.020260761307989372, -0.08373916192256191, 0.06875512504053337, 0.274848695533971, -0.1743530110904464, -0.3037826046577574, 0.016651386809017923, -0.4209246238992538, 0.11376752845230109, 0.15790111912747867, 0.08208778587365408, ... |
710.004 | K* production in Heavy Ion Collisions at RHIC | Study of resonances with their short life-times provides useful tools to
probe the properties of hot and dense matter produced in relativistic heavy ion
collisions. The high density and/or high temperature of the medium can modify
resonance properties such as mass and width. Therefore, measurement of these
properties... | nucl-ex | study of resonances with their short lifetimes provides useful tools to probe the properties of hot and dense matter produced in relativistic heavy ion collisions the high density andor high temperature of the medium can modify resonance properties such as mass and width therefore measurement of these properties can re... | [['study', 'of', 'resonances', 'with', 'their', 'short', 'lifetimes', 'provides', 'useful', 'tools', 'to', 'probe', 'the', 'properties', 'of', 'hot', 'and', 'dense', 'matter', 'produced', 'in', 'relativistic', 'heavy', 'ion', 'collisions', 'the', 'high', 'density', 'andor', 'high', 'temperature', 'of', 'the', 'medium',... | [-0.06516125453036335, 0.26659251713532617, -0.17247022946266402, 0.10378479034019013, 0.02033557107488653, -0.10087479883804917, -0.06722639696531449, 0.37619734637326363, -0.21379470244529797, -0.3570203089127035, -0.04642312050264357, -0.3788324860065724, 0.13584169445587604, 0.15860565604507978, 0.0959453691488527,... |
710.0041 | Low-Temperature Phase Boundary of dilute Lattice Spin Glasses | The thermal-to-percolative crossover exponent \phi, well-known for
ferromagnetic systems, is studied extensively for Edwards-Anderson spin
glasses. The scaling of defect energies are determined at the bond percolation
threshold p_c, using an improved algorithm. Simulations extend to system sizes
above N=10^8 in dimen... | cond-mat.dis-nn cond-mat.mtrl-sci | the thermaltopercolative crossover exponent phi wellknown for ferromagnetic systems is studied extensively for edwardsanderson spin glasses the scaling of defect energies are determined at the bond percolation threshold p_c using an improved algorithm simulations extend to system sizes above n108 in dimensions d27 the ... | [['the', 'thermaltopercolative', 'crossover', 'exponent', 'phi', 'wellknown', 'for', 'ferromagnetic', 'systems', 'is', 'studied', 'extensively', 'for', 'edwardsanderson', 'spin', 'glasses', 'the', 'scaling', 'of', 'defect', 'energies', 'are', 'determined', 'at', 'the', 'bond', 'percolation', 'threshold', 'p_c', 'using'... | [-0.07632268780194547, 0.21104598251163817, -0.08513319353046625, 0.0658678988845128, 0.02480251070101867, -0.16574522950888976, 0.06053380281259508, 0.32076645972126205, -0.2347823682403111, -0.24901908283000407, 0.061616236908847224, -0.31412984618674156, -0.13261301944680187, 0.19479787485755007, 0.06595506948297439... |
710.0042 | Shear Thickening and Scaling of the Elastic Modulus in a Fractal
Colloidal System with Attractive Interactions | Dilute oil dispersions of fractal carbon black particles with attractive Van
der Waals interactions display continuous shear thickening followed by shear
thinning at high shear rates. The shear thickening transition occurs at
$\dot\gamma_{c}\approx 10^{2}-10^{3}s^{-1}$ and is driven by hydrodynamic
breakup of cluster... | cond-mat.soft | dilute oil dispersions of fractal carbon black particles with attractive van der waals interactions display continuous shear thickening followed by shear thinning at high shear rates the shear thickening transition occurs at dotgamma_capprox 102103s1 and is driven by hydrodynamic breakup of clusters preshearing dispers... | [['dilute', 'oil', 'dispersions', 'of', 'fractal', 'carbon', 'black', 'particles', 'with', 'attractive', 'van', 'der', 'waals', 'interactions', 'display', 'continuous', 'shear', 'thickening', 'followed', 'by', 'shear', 'thinning', 'at', 'high', 'shear', 'rates', 'the', 'shear', 'thickening', 'transition', 'occurs', 'at... | [-0.11482184433817179, 0.2673684323056676, -0.11628636701538324, 0.00283915497865742, 0.02658302944699495, -0.11719050353671286, 0.009365751627490095, 0.3355877311236557, -0.3173344217397369, -0.2414750809575185, -0.01040141833223531, -0.30340880286162614, -0.10198693842380896, 0.17929045744400857, 0.041032858635666886... |
710.0043 | Graph rigidity, Cyclic Belief Propagation and Point Pattern Matching | A recent paper \cite{CaeCaeSchBar06} proposed a provably optimal, polynomial
time method for performing near-isometric point pattern matching by means of
exact probabilistic inference in a chordal graphical model. Their fundamental
result is that the chordal graph in question is shown to be globally rigid,
implying t... | cs.CV | a recent paper citecaecaeschbar06 proposed a provably optimal polynomial time method for performing nearisometric point pattern matching by means of exact probabilistic inference in a chordal graphical model their fundamental result is that the chordal graph in question is shown to be globally rigid implying that exact... | [['a', 'recent', 'paper', 'citecaecaeschbar06', 'proposed', 'a', 'provably', 'optimal', 'polynomial', 'time', 'method', 'for', 'performing', 'nearisometric', 'point', 'pattern', 'matching', 'by', 'means', 'of', 'exact', 'probabilistic', 'inference', 'in', 'a', 'chordal', 'graphical', 'model', 'their', 'fundamental', 'r... | [-0.10213008710921521, 0.031110643374957267, -0.11208814833019125, 0.06507012873434609, -0.11260840145773009, -0.15488903634250165, 0.061037037335336206, 0.4144734644380055, -0.2902848422625347, -0.28763030056449534, 0.11109881349777999, -0.2149307144255114, -0.20441539541475082, 0.1767973733600229, -0.1185576747931344... |
710.0044 | A modular absolute bound condition for primitive association schemes | The well-known absolute bound condition for a primitive symmetric association
scheme (X,S) gives an upper bound for |X| in terms of |S| and the minimal
non-principal multiplicity of the scheme. In this paper we prove another upper
bounds for |X| for an arbitrary primitive scheme (X,S). They do not depend on
|S| but d... | math.CO math.RT | the wellknown absolute bound condition for a primitive symmetric association scheme xs gives an upper bound for x in terms of s and the minimal nonprincipal multiplicity of the scheme in this paper we prove another upper bounds for x for an arbitrary primitive scheme xs they do not depend on s but depend on some invari... | [['the', 'wellknown', 'absolute', 'bound', 'condition', 'for', 'a', 'primitive', 'symmetric', 'association', 'scheme', 'xs', 'gives', 'an', 'upper', 'bound', 'for', 'x', 'in', 'terms', 'of', 's', 'and', 'the', 'minimal', 'nonprincipal', 'multiplicity', 'of', 'the', 'scheme', 'in', 'this', 'paper', 'we', 'prove', 'anoth... | [-0.22133976548642226, 0.10959298909886593, -0.09825291291950908, 0.050738685675067445, -0.08794524171708586, -0.17705561517265767, 0.10401572940443732, 0.3033911120465459, -0.2860769085739165, -0.250612875625287, 0.07925076390080767, -0.24142590226375893, -0.07468287022592984, 0.23114046498922605, -0.09098164614749281... |
710.0045 | Quantum Entangled Dark Solitons Formed by Ultracold Atoms in Optical
Lattices | Inspired by experiments on Bose-Einstein condensates in optical lattices, we
study the quantum evolution of dark soliton initial conditions in the context
of the Bose-Hubbard Hamiltonian. An extensive set of quantum measures is
utilized in our analysis, including von Neumann and generalized quantum
entropies, quantum... | cond-mat.mes-hall nlin.PS quant-ph | inspired by experiments on boseeinstein condensates in optical lattices we study the quantum evolution of dark soliton initial conditions in the context of the bosehubbard hamiltonian an extensive set of quantum measures is utilized in our analysis including von neumann and generalized quantum entropies quantum depleti... | [['inspired', 'by', 'experiments', 'on', 'boseeinstein', 'condensates', 'in', 'optical', 'lattices', 'we', 'study', 'the', 'quantum', 'evolution', 'of', 'dark', 'soliton', 'initial', 'conditions', 'in', 'the', 'context', 'of', 'the', 'bosehubbard', 'hamiltonian', 'an', 'extensive', 'set', 'of', 'quantum', 'measures', '... | [-0.12999159620460315, 0.17026928487397638, -0.13387158630204568, 0.11171909818814625, 0.017964526300424152, -0.11625950646193065, -0.019076614334612853, 0.3693734811998174, -0.23008018444243042, -0.21781408235661148, 0.015316757591940539, -0.31756646646013886, -0.14297216532022222, 0.18348710506088725, 0.0173197203056... |
710.0046 | The basis digraphs of p-schemes | It is proved that association schemes with bipartite basis graphs are exactly
2-schemes. This result follows from a characterization of p-schemes for an
arbitrary prime p in terms of basis digraphs.
| math.CO | it is proved that association schemes with bipartite basis graphs are exactly 2schemes this result follows from a characterization of pschemes for an arbitrary prime p in terms of basis digraphs | [['it', 'is', 'proved', 'that', 'association', 'schemes', 'with', 'bipartite', 'basis', 'graphs', 'are', 'exactly', '2schemes', 'this', 'result', 'follows', 'from', 'a', 'characterization', 'of', 'pschemes', 'for', 'an', 'arbitrary', 'prime', 'p', 'in', 'terms', 'of', 'basis', 'digraphs']] | [-0.18127329827596744, 0.1013836452625886, -0.10235226849714915, 0.04803158398717642, -0.033118645350138344, -0.16895363708026706, 0.002719687670469284, 0.36054342209051055, -0.25901539375384647, -0.2646430065855384, 0.059830570248110844, -0.23685377451280754, -0.14201825812148552, 0.21063032746315002, -0.0884876911838... |
710.0047 | Addendum: Triton and hypertriton binding energies calculated from SU_6
quark-model baryon-baryon interactions | Previously we calculated the binding energies of the triton and hypertriton,
using an SU_6 quark-model interaction derived from a resonating-group method of
two baryon clusters. In contrast to the previous calculations employing the
energy-dependent interaction kernel, we present new results using a
renormalized inte... | nucl-th | previously we calculated the binding energies of the triton and hypertriton using an su_6 quarkmodel interaction derived from a resonatinggroup method of two baryon clusters in contrast to the previous calculations employing the energydependent interaction kernel we present new results using a renormalized interaction ... | [['previously', 'we', 'calculated', 'the', 'binding', 'energies', 'of', 'the', 'triton', 'and', 'hypertriton', 'using', 'an', 'su_6', 'quarkmodel', 'interaction', 'derived', 'from', 'a', 'resonatinggroup', 'method', 'of', 'two', 'baryon', 'clusters', 'in', 'contrast', 'to', 'the', 'previous', 'calculations', 'employing... | [-0.0524840654974634, 0.1881545378245805, -0.08996800064447928, 0.13840967427134854, -0.010512254858357746, -0.10583870547548445, 0.04279727917587892, 0.35886715203523634, -0.18620594948191535, -0.33787290791726926, -0.04819051880939779, -0.3434347786009312, -0.0019188920110040767, 0.17189517865931106, 0.09174462642351... |
710.0048 | Modeling Diffusive Dynamics in Adaptive Resolution Simulation of Liquid
Water | We present a dual-resolution molecular dynamics (MD) simulation of liquid
water employing a recently introduced Adaptive Resolution Scheme (AdResS). The
spatially adaptive molecular resolution procedure allows for changing from a
coarse-grained to an all-atom representation and vice-versa on-the-fly. In
order to find... | cond-mat.soft cond-mat.stat-mech | we present a dualresolution molecular dynamics md simulation of liquid water employing a recently introduced adaptive resolution scheme adress the spatially adaptive molecular resolution procedure allows for changing from a coarsegrained to an allatom representation and viceversa onthefly in order to find the most appr... | [['we', 'present', 'a', 'dualresolution', 'molecular', 'dynamics', 'md', 'simulation', 'of', 'liquid', 'water', 'employing', 'a', 'recently', 'introduced', 'adaptive', 'resolution', 'scheme', 'adress', 'the', 'spatially', 'adaptive', 'molecular', 'resolution', 'procedure', 'allows', 'for', 'changing', 'from', 'a', 'coa... | [-0.08797054594254185, 0.1002660950783295, -0.1240853823111232, 0.02379752974074077, 0.0006612851477131762, -0.11899644437422655, 0.010329962416616236, 0.38197152054515376, -0.2730042143508085, -0.31585522037930785, 0.02511943865583503, -0.19010029971802303, -0.15899519843113577, 0.09096563837234059, -0.007805737212364... |
710.0049 | On equivariant mirror symmetry for local P^2 | We solve the problem of equivariant mirror symmetry for O(-3)->P^2 for the
(three) cases of one independent equivariant parameter. This gives a
decomposition of mirror symmetry for local P^2 into that of three subspaces,
each of which may be considered independently. Finally, we give a new
interpretation of mirror sy... | math.AG hep-th | we solve the problem of equivariant mirror symmetry for o3p2 for the three cases of one independent equivariant parameter this gives a decomposition of mirror symmetry for local p2 into that of three subspaces each of which may be considered independently finally we give a new interpretation of mirror symmetry for oko2... | [['we', 'solve', 'the', 'problem', 'of', 'equivariant', 'mirror', 'symmetry', 'for', 'o3p2', 'for', 'the', 'three', 'cases', 'of', 'one', 'independent', 'equivariant', 'parameter', 'this', 'gives', 'a', 'decomposition', 'of', 'mirror', 'symmetry', 'for', 'local', 'p2', 'into', 'that', 'of', 'three', 'subspaces', 'each'... | [-0.15562227273359894, 0.09366652121767402, -0.13131719276309015, 0.05542356661288068, -0.08413516368716956, -0.2016281651891768, 0.0033966107107698917, 0.3123510617017746, -0.29587639139033856, -0.2621963689848781, 0.13764183644205333, -0.17242447167634964, -0.10939492642879486, 0.18393301900476217, -0.085503891208209... |
710.005 | Combinatorial Stokes formulas via minimal resolutions | We describe an explicit chain map from the standard resolution to the minimal
resolution for the finite cyclic group Z_k of order k. We then demonstrate how
such a chain map induces a "Z_k-combinatorial Stokes theorem", which in turn
implies "Dold's theorem" that there is no equivariant map from an n-connected
to an ... | math.CO math.AT | we describe an explicit chain map from the standard resolution to the minimal resolution for the finite cyclic group z_k of order k we then demonstrate how such a chain map induces a z_kcombinatorial stokes theorem which in turn implies dolds theorem that there is no equivariant map from an nconnected to an ndimensiona... | [['we', 'describe', 'an', 'explicit', 'chain', 'map', 'from', 'the', 'standard', 'resolution', 'to', 'the', 'minimal', 'resolution', 'for', 'the', 'finite', 'cyclic', 'group', 'z_k', 'of', 'order', 'k', 'we', 'then', 'demonstrate', 'how', 'such', 'a', 'chain', 'map', 'induces', 'a', 'z_kcombinatorial', 'stokes', 'theor... | [-0.10268194687448377, 0.04019241720969399, -0.12802037772931288, 0.07690875561494412, -0.10430638350803277, -0.15664933324823604, 0.04945334854760561, 0.3258982386383838, -0.35233916843346125, -0.2515720225176132, 0.11493497175979428, -0.21967506373566092, -0.1815945651896041, 0.21094052065156324, -0.17957296208398224... |
710.0051 | Doubly heavy baryon production at polarized photon collider | We study the inclusive production of doubly heavy baryon $\Xi_{cc}$ at
polarized photon collider. Our results show that proper choice of the initial
beam polarizations may increase the production rate of $\Xi_{cc}$ approximately
10%.
| hep-ph | we study the inclusive production of doubly heavy baryon xi_cc at polarized photon collider our results show that proper choice of the initial beam polarizations may increase the production rate of xi_cc approximately 10 | [['we', 'study', 'the', 'inclusive', 'production', 'of', 'doubly', 'heavy', 'baryon', 'xi_cc', 'at', 'polarized', 'photon', 'collider', 'our', 'results', 'show', 'that', 'proper', 'choice', 'of', 'the', 'initial', 'beam', 'polarizations', 'may', 'increase', 'the', 'production', 'rate', 'of', 'xi_cc', 'approximately', '... | [-0.10213239249424078, 0.2850193223943386, -0.04769193349570474, 0.10543105449965771, -0.0027798615012537033, -0.09257007609395419, 0.07989699700299431, 0.32588383862200904, -0.18492782981518438, -0.23755844309926033, -0.06270086613264592, -0.3946060052908519, 0.15160007205079584, 0.14916495869264884, 0.118927429813672... |
710.0052 | Influence of a small perturbation on Poincare-Andronov operators with
not well defined topological degree | Let $P_e\in C^0(R^n,R^n)$ be the Poincare-Andronov operator over period $T>0$
of the $T$-periodically perturbed autonomous system $x'=f(x)+e g(t,x,e),$ where
$e>0$ is small. Assuming that for $e=0$ this system has a $T$-periodic limit
cycle $x_0$ we evaluate the topological degree $d(I-P_e,U)$ of $I-P_e$ on an
open b... | math.CA | let p_ein c0rnrn be the poincareandronov operator over period t0 of the tperiodically perturbed autonomous system xfxe gtxe where e0 is small assuming that for e0 this system has a tperiodic limit cycle x_0 we evaluate the topological degree dip_eu of ip_e on an open bounded set u whose boundary contains x_00t and does... | [['let', 'p_ein', 'c0rnrn', 'be', 'the', 'poincareandronov', 'operator', 'over', 'period', 't0', 'of', 'the', 'tperiodically', 'perturbed', 'autonomous', 'system', 'xfxe', 'gtxe', 'where', 'e0', 'is', 'small', 'assuming', 'that', 'for', 'e0', 'this', 'system', 'has', 'a', 'tperiodic', 'limit', 'cycle', 'x_0', 'we', 'ev... | [-0.23790711333119385, 0.10340862585675299, -0.08363455810021979, -0.029470047265341557, -0.047287620771844105, -0.1371042102969646, 0.05559784538313948, 0.29028743207622487, -0.27590241929230924, -0.205258433866474, 0.10996605592388094, -0.31766025270838794, -0.12634885777627025, 0.17306043687570202, -0.09701756898498... |
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