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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710.0253 | Crystal graphs for general linear Lie superalgebras and quasi-symmetric
functions | We give a new representation theoretic interpretation of the ring of
quasi-symmetric functions. This is obtained by showing that the super analogue
of the Gessel's fundamental quasi-symmetric function can be realized as the
character of an irreducible crystal for the Lie superalgebra $\frak{gl}_{n|n}$
associated to i... | math.RT math.QA | we give a new representation theoretic interpretation of the ring of quasisymmetric functions this is obtained by showing that the super analogue of the gessels fundamental quasisymmetric function can be realized as the character of an irreducible crystal for the lie superalgebra frakgl_nn associated to its nonstandard... | [['we', 'give', 'a', 'new', 'representation', 'theoretic', 'interpretation', 'of', 'the', 'ring', 'of', 'quasisymmetric', 'functions', 'this', 'is', 'obtained', 'by', 'showing', 'that', 'the', 'super', 'analogue', 'of', 'the', 'gessels', 'fundamental', 'quasisymmetric', 'function', 'can', 'be', 'realized', 'as', 'the',... | [-0.1602784429663135, 0.09787092975945116, -0.11301905778236687, 0.06782479801297407, -0.15677505565862007, -0.08082743685500805, -0.020458768724518663, 0.3493811272577766, -0.3621509333195932, -0.16561010523754008, 0.08641318078426753, -0.19154658365775556, -0.19952142389272065, 0.24809900136417984, -0.081296508898958... |
710.0254 | Generalized plasma-like permittivity and thermal Casimir force between
real metals | The physical reasons why the Drude dielectric function is not compatible with
the Lifshitz formula, as opposed to the generalized plasma-like permittivity,
are presented. Essentially, the problem is connected with the finite size of
metal plates. It is shown that the Lifshitz theory combined with the
generalized plas... | quant-ph cond-mat.stat-mech physics.optics | the physical reasons why the drude dielectric function is not compatible with the lifshitz formula as opposed to the generalized plasmalike permittivity are presented essentially the problem is connected with the finite size of metal plates it is shown that the lifshitz theory combined with the generalized plasmalike p... | [['the', 'physical', 'reasons', 'why', 'the', 'drude', 'dielectric', 'function', 'is', 'not', 'compatible', 'with', 'the', 'lifshitz', 'formula', 'as', 'opposed', 'to', 'the', 'generalized', 'plasmalike', 'permittivity', 'are', 'presented', 'essentially', 'the', 'problem', 'is', 'connected', 'with', 'the', 'finite', 's... | [-0.08963711504922965, 0.16759313363581896, -0.07853335665109065, 0.03369106650531579, -0.14305522454042846, -0.20117453740050012, -0.018530873575050812, 0.3853292528611536, -0.21343138258760938, -0.2008217659134131, 0.010605434663235568, -0.3107991418801248, -0.2061164921436172, 0.15762616884827507, -0.054838564515543... |
710.0255 | Searches for Leptoquark Production at D0 | Recent searches for leptoquark production in proton-antiproton collisions at
sqrt(s)=1.96TeV are presented using data samples with integrated luminosities
up to 1fb^(-1) recorded with the D0 detector.
| hep-ex | recent searches for leptoquark production in protonantiproton collisions at sqrts196tev are presented using data samples with integrated luminosities up to 1fb1 recorded with the d0 detector | [['recent', 'searches', 'for', 'leptoquark', 'production', 'in', 'protonantiproton', 'collisions', 'at', 'sqrts196tev', 'are', 'presented', 'using', 'data', 'samples', 'with', 'integrated', 'luminosities', 'up', 'to', '1fb1', 'recorded', 'with', 'the', 'd0', 'detector']] | [0.051816522439297005, 0.20748057990120009, -0.0576427941246388, 0.08692103194502684, 0.02073929637957078, -0.13575410993339923, -0.07940942736772391, 0.39840637505627596, -0.10264036962046073, -0.4163944859487506, -0.0044762081189009435, -0.5817013060530791, 0.23916290163134152, 0.17966109002904537, 0.1393624441877294... |
710.0256 | Charmonium spectrum including higher spin and exotic states | We study the charmonium spectrum including higher spin and exotic states. We
use the Sheikholeslami-Wilson (clover) action for $N_f=2$ sea quarks as well as
for the charm valence quark. In order to access excited states we apply a
variational method with a basis of highly optimized operators.
| hep-lat | we study the charmonium spectrum including higher spin and exotic states we use the sheikholeslamiwilson clover action for n_f2 sea quarks as well as for the charm valence quark in order to access excited states we apply a variational method with a basis of highly optimized operators | [['we', 'study', 'the', 'charmonium', 'spectrum', 'including', 'higher', 'spin', 'and', 'exotic', 'states', 'we', 'use', 'the', 'sheikholeslamiwilson', 'clover', 'action', 'for', 'n_f2', 'sea', 'quarks', 'as', 'well', 'as', 'for', 'the', 'charm', 'valence', 'quark', 'in', 'order', 'to', 'access', 'excited', 'states', '... | [-0.04107781971230152, 0.29932033246819006, -0.09980278795565221, 0.15810095849744182, -0.00801529093804036, -0.10287259604306297, 0.12793853863122615, 0.38650970113404254, -0.11920233053016535, -0.22810205727062643, 0.03500067981386042, -0.3287175805208848, -0.047390021581916096, 0.09933980661345289, 0.059295197869551... |
710.0257 | Gas Density and the Volume Schmidt Law for Spiral Galaxies | The thickness of the equilibrium isothermal gaseous layers and their volume
densities \rho_{gas}(R) in the disc midplane are calculated for 7 spiral
galaxies (including our Galaxy) in the frame of self-consistent axisymmetric
model. Local velocity dispersions of stellar discs were assumed to be close to
marginal valu... | astro-ph | the thickness of the equilibrium isothermal gaseous layers and their volume densities rho_gasr in the disc midplane are calculated for 7 spiral galaxies including our galaxy in the frame of selfconsistent axisymmetric model local velocity dispersions of stellar discs were assumed to be close to marginal values necessar... | [['the', 'thickness', 'of', 'the', 'equilibrium', 'isothermal', 'gaseous', 'layers', 'and', 'their', 'volume', 'densities', 'rho_gasr', 'in', 'the', 'disc', 'midplane', 'are', 'calculated', 'for', '7', 'spiral', 'galaxies', 'including', 'our', 'galaxy', 'in', 'the', 'frame', 'of', 'selfconsistent', 'axisymmetric', 'mod... | [-0.08007301472687339, 0.11596977192731131, -0.0606765639477609, 0.0800929816625891, 0.008781875758653595, -0.060228469495528514, 0.02318811364072774, 0.3951846043623629, -0.16784951399036108, -0.32849510830960105, 0.06119355081491882, -0.2620883105367067, 0.010389548251848846, 0.16227120645676874, -0.00427643114900482... |
710.0258 | Next to leading order gravitational wave emission and dynamical
evolution of compact binary systems with spin | Compact binary systems with spinning components are considered. Finite size
effects due to rotational deformation are taken into account. The dynamical
evolution and next to leading order gravitational wave forms are calculated,
taking into account the orbital motion up to the first post-Newtonian
approximation.
| gr-qc | compact binary systems with spinning components are considered finite size effects due to rotational deformation are taken into account the dynamical evolution and next to leading order gravitational wave forms are calculated taking into account the orbital motion up to the first postnewtonian approximation | [['compact', 'binary', 'systems', 'with', 'spinning', 'components', 'are', 'considered', 'finite', 'size', 'effects', 'due', 'to', 'rotational', 'deformation', 'are', 'taken', 'into', 'account', 'the', 'dynamical', 'evolution', 'and', 'next', 'to', 'leading', 'order', 'gravitational', 'wave', 'forms', 'are', 'calculate... | [-0.17817103981294416, 0.17258975887671113, -0.08669228231619028, 0.07080729809505018, -0.10408574164929715, -0.03422287347017449, -0.073479227213697, 0.33574457944963465, -0.25227557647634635, -0.2743043504147367, 0.06667673411059448, -0.23303836821155113, -0.04742103228768842, 0.1577515798536214, 0.06442936146843502,... |
710.0259 | On-line recognition of supernova neutrino bursts in the LVD detector | In this paper we show the capabilities of the Large Volume Detector (INFN
Gran Sasso National Laboratory) to identify a neutrino burst associated to a
supernova explosion, in the absence of an "external trigger", e.g., an optical
observation. We describe how the detector trigger and event selection have been
optimize... | astro-ph hep-ph | in this paper we show the capabilities of the large volume detector infn gran sasso national laboratory to identify a neutrino burst associated to a supernova explosion in the absence of an external trigger eg an optical observation we describe how the detector trigger and event selection have been optimized for this p... | [['in', 'this', 'paper', 'we', 'show', 'the', 'capabilities', 'of', 'the', 'large', 'volume', 'detector', 'infn', 'gran', 'sasso', 'national', 'laboratory', 'to', 'identify', 'a', 'neutrino', 'burst', 'associated', 'to', 'a', 'supernova', 'explosion', 'in', 'the', 'absence', 'of', 'an', 'external', 'trigger', 'eg', 'an... | [-0.06747694122929905, 0.09854114497774877, -0.044449302914747316, 0.12451427468223238, -0.05391943214331255, -0.09868760102666742, 0.013316546427356728, 0.39884899357377096, -0.19594232945941215, -0.3264500996054605, 0.09813237457324989, -0.3105940180180898, -0.07388716230038987, 0.21375527893203897, -0.03765230933420... |
710.026 | Higher order group cohomology and the Eichler-Shimura map | Higher order group cohomology is defined and first properties are given.
Using modular symbols, an Eichler-Shimura homomorphism is constructed mapping
spaces of higher order cusp forms to higher order cohomology groups.
| math.NT | higher order group cohomology is defined and first properties are given using modular symbols an eichlershimura homomorphism is constructed mapping spaces of higher order cusp forms to higher order cohomology groups | [['higher', 'order', 'group', 'cohomology', 'is', 'defined', 'and', 'first', 'properties', 'are', 'given', 'using', 'modular', 'symbols', 'an', 'eichlershimura', 'homomorphism', 'is', 'constructed', 'mapping', 'spaces', 'of', 'higher', 'order', 'cusp', 'forms', 'to', 'higher', 'order', 'cohomology', 'groups']] | [-0.2601651917061498, 0.0539973810237209, -0.08653230688744976, 0.11424889157886707, -0.1827293437334799, -0.05910777420766892, -0.09550541423020824, 0.34355749706587485, -0.3536100839414904, -0.27461014585869925, 0.13219657696543202, -0.25878369673005036, -0.1869506670853063, 0.17400046161586238, -0.1179726609900113, ... |
710.0261 | Chain models on Hecke algebra for corner type representations | We consider the integrable open chain models formulated in terms of
generators of the Hecke algebra. The spectrum of the Hamiltonians for the open
Hecke chains of finite size with free boundary conditions is deduced for
special (corner type) irreducible representations of the Hecke algebra.
| math.QA math.RT | we consider the integrable open chain models formulated in terms of generators of the hecke algebra the spectrum of the hamiltonians for the open hecke chains of finite size with free boundary conditions is deduced for special corner type irreducible representations of the hecke algebra | [['we', 'consider', 'the', 'integrable', 'open', 'chain', 'models', 'formulated', 'in', 'terms', 'of', 'generators', 'of', 'the', 'hecke', 'algebra', 'the', 'spectrum', 'of', 'the', 'hamiltonians', 'for', 'the', 'open', 'hecke', 'chains', 'of', 'finite', 'size', 'with', 'free', 'boundary', 'conditions', 'is', 'deduced'... | [-0.19967203508648607, 0.1182633012222747, -0.016419179954876503, 0.062119503621943295, -0.0760920611054947, -0.18615449691812197, -0.07703075826995903, 0.2992611501779821, -0.3573285277518961, -0.16436127279367713, 0.1610846864240658, -0.23768710627013612, -0.052576721873548296, 0.19463500123884941, -0.104308634603189... |
710.0262 | Incomplete Lineage Sorting: Consistent Phylogeny Estimation From
Multiple Loci | We introduce a simple algorithm for reconstructing phylogenies from multiple
gene trees in the presence of incomplete lineage sorting, that is, when the
topology of the gene trees may differ from that of the species tree. We show
that our technique is statistically consistent under standard stochastic
assumptions, th... | q-bio.PE cs.CE cs.DS math.PR math.ST stat.TH | we introduce a simple algorithm for reconstructing phylogenies from multiple gene trees in the presence of incomplete lineage sorting that is when the topology of the gene trees may differ from that of the species tree we show that our technique is statistically consistent under standard stochastic assumptions that is ... | [['we', 'introduce', 'a', 'simple', 'algorithm', 'for', 'reconstructing', 'phylogenies', 'from', 'multiple', 'gene', 'trees', 'in', 'the', 'presence', 'of', 'incomplete', 'lineage', 'sorting', 'that', 'is', 'when', 'the', 'topology', 'of', 'the', 'gene', 'trees', 'may', 'differ', 'from', 'that', 'of', 'the', 'species',... | [-0.09703652323888881, 0.13824392478646977, -0.07924074340345603, 0.14280129284930548, -0.0601424362909581, -0.13136901218843247, 0.10772914474031754, 0.4021565324493817, -0.3072390408388206, -0.25935033194670853, 0.06518760833589893, -0.24690453372895718, -0.23911666365872536, 0.19885760061442853, -0.13119886265402395... |
710.0263 | Enhancement of equilibrium fraction by heterogeneous nucleation in a
"phase separated" half-doped manganite | Glass-like arrest of kinetics has been observed across many magnetic
first-order transitions. By traversing the two control variable H-T space,
tunable coexisting fractions of arrested and equilibrium phases have been
observed. We report here a fortuitous situation in a half-doped manganite
sample, where these featur... | cond-mat.str-el cond-mat.stat-mech | glasslike arrest of kinetics has been observed across many magnetic firstorder transitions by traversing the two control variable ht space tunable coexisting fractions of arrested and equilibrium phases have been observed we report here a fortuitous situation in a halfdoped manganite sample where these features occur b... | [['glasslike', 'arrest', 'of', 'kinetics', 'has', 'been', 'observed', 'across', 'many', 'magnetic', 'firstorder', 'transitions', 'by', 'traversing', 'the', 'two', 'control', 'variable', 'ht', 'space', 'tunable', 'coexisting', 'fractions', 'of', 'arrested', 'and', 'equilibrium', 'phases', 'have', 'been', 'observed', 'we... | [-0.15623496741070844, 0.30853965070540296, -0.0460311239225233, -0.040330419576121976, -0.013692598900344875, -0.1546588018872612, 0.12304845497674625, 0.3932916625503681, -0.2535084309920515, -0.32926027716819156, 0.06843890873691279, -0.25233964281655924, -0.0908464833748402, 0.15027532357837736, 0.05295946994873205... |
710.0264 | Baryon currents in the C-broken phase of QCD | In a space with some sufficiently small compact dimension (with non-trivial
cycles) and with periodic boundary conditions for the fermions, the charge
conjugation (C), spatial parity (P), time reversal (T) and CPT symmetries are
spontaneously broken in QCD. We have investigated what are the physical
consequences of t... | hep-lat | in a space with some sufficiently small compact dimension with nontrivial cycles and with periodic boundary conditions for the fermions the charge conjugation c spatial parity p time reversal t and cpt symmetries are spontaneously broken in qcd we have investigated what are the physical consequences of the breaking of ... | [['in', 'a', 'space', 'with', 'some', 'sufficiently', 'small', 'compact', 'dimension', 'with', 'nontrivial', 'cycles', 'and', 'with', 'periodic', 'boundary', 'conditions', 'for', 'the', 'fermions', 'the', 'charge', 'conjugation', 'c', 'spatial', 'parity', 'p', 'time', 'reversal', 't', 'and', 'cpt', 'symmetries', 'are',... | [-0.21054232155183855, 0.2974730954039842, -0.06473319546494168, 0.076421660669439, -0.08347299580054823, -0.13320906719309278, 0.007274293311638758, 0.3847413016017526, -0.261825855076313, -0.2404114725010004, 0.10337813498044852, -0.2312307240325026, -0.09272726430208422, 0.08054812506306916, 0.008359829720575362, 0.... |
710.0265 | Two permanents in the universal enveloping algebras of the symplectic
Lie algebras | This paper presents new generators for the center of the universal enveloping
algebra of the symplectic Lie algebra. These generators are expressed in terms
of the column-permanent, and it is easy to calculate their eigenvalues on
irreducible representations. We can regard these generators as the counterpart
of centr... | math.RT | this paper presents new generators for the center of the universal enveloping algebra of the symplectic lie algebra these generators are expressed in terms of the columnpermanent and it is easy to calculate their eigenvalues on irreducible representations we can regard these generators as the counterpart of central ele... | [['this', 'paper', 'presents', 'new', 'generators', 'for', 'the', 'center', 'of', 'the', 'universal', 'enveloping', 'algebra', 'of', 'the', 'symplectic', 'lie', 'algebra', 'these', 'generators', 'are', 'expressed', 'in', 'terms', 'of', 'the', 'columnpermanent', 'and', 'it', 'is', 'easy', 'to', 'calculate', 'their', 'ei... | [-0.18676085941578177, 0.046470835426589474, -0.03845363643697717, 0.015240803759132343, -0.1429867492300797, -0.04716984981165628, -0.06546856531614056, 0.32761104470542207, -0.35993911677294155, -0.20551719129170207, 0.16487159419788935, -0.21237939414144916, -0.14869408747604626, 0.19354098226705735, -0.143725658502... |
710.0266 | Graph model of the Heisenberg-Weyl algebra | We consider an algebraic formulation of Quantum Theory and develop a
combinatorial model of the Heisenberg-Weyl algebra structure. It is shown that
by lifting this structure to the richer algebra of graph operator calculus, we
gain a simple interpretation involving, for example, the natural composition of
graphs. Thi... | quant-ph math-ph math.CO math.MP | we consider an algebraic formulation of quantum theory and develop a combinatorial model of the heisenbergweyl algebra structure it is shown that by lifting this structure to the richer algebra of graph operator calculus we gain a simple interpretation involving for example the natural composition of graphs this provid... | [['we', 'consider', 'an', 'algebraic', 'formulation', 'of', 'quantum', 'theory', 'and', 'develop', 'a', 'combinatorial', 'model', 'of', 'the', 'heisenbergweyl', 'algebra', 'structure', 'it', 'is', 'shown', 'that', 'by', 'lifting', 'this', 'structure', 'to', 'the', 'richer', 'algebra', 'of', 'graph', 'operator', 'calcul... | [-0.10312479370253974, 0.05224015869378132, -0.19644419279631595, 0.11975436103300677, -0.19752527831096045, -0.11592382649090928, 0.04063257404839174, 0.3166814669442009, -0.37109628616189455, -0.2719825300794672, 0.05269726966573319, -0.19024456882665694, -0.26460260766702637, 0.17390834419122359, -0.0916084726013138... |
710.0267 | Uniqueness of real closure * of Baer regular rings | It was pointed out in my last paper that there are rings whose real closure *
are not unique. In [4] we also discussed some example of rings by which there
is a unique real closure * (mainly the real closed rings). Now we want to
determine more classes of rings by which real closure * is unique. The main
results invo... | math.AC math.AG | it was pointed out in my last paper that there are rings whose real closure are not unique in 4 we also discussed some example of rings by which there is a unique real closure mainly the real closed rings now we want to determine more classes of rings by which real closure is unique the main results involve characteris... | [['it', 'was', 'pointed', 'out', 'in', 'my', 'last', 'paper', 'that', 'there', 'are', 'rings', 'whose', 'real', 'closure', 'are', 'not', 'unique', 'in', '4', 'we', 'also', 'discussed', 'some', 'example', 'of', 'rings', 'by', 'which', 'there', 'is', 'a', 'unique', 'real', 'closure', 'mainly', 'the', 'real', 'closed', 'r... | [-0.1641356841106407, 0.026747349877884363, -0.07692080030475205, 0.06440979733919286, -0.09489368196819128, -0.11309531320461898, -0.06742569530520937, 0.3852543194997844, -0.3079233715022967, -0.21069633008200464, 0.16577895581428856, -0.2535471670496149, -0.16905587562927749, 0.2477996551973094, -0.07604215404291342... |
710.0268 | Schur type functions associated with polynomial sequences of binomial
type | We introduce a class of Schur type functions associated with polynomial
sequences of binomial type. This can be regarded as a generalization of the
ordinary Schur functions and the factorial Schur functions. This generalization
satisfies some interesting expansion formulas, in which there is a curious
duality. Moreov... | math.RT math.CO | we introduce a class of schur type functions associated with polynomial sequences of binomial type this can be regarded as a generalization of the ordinary schur functions and the factorial schur functions this generalization satisfies some interesting expansion formulas in which there is a curious duality moreover thi... | [['we', 'introduce', 'a', 'class', 'of', 'schur', 'type', 'functions', 'associated', 'with', 'polynomial', 'sequences', 'of', 'binomial', 'type', 'this', 'can', 'be', 'regarded', 'as', 'a', 'generalization', 'of', 'the', 'ordinary', 'schur', 'functions', 'and', 'the', 'factorial', 'schur', 'functions', 'this', 'general... | [-0.11672893021669653, 0.04282017635543727, -0.07618122910045916, 0.12651945714929347, -0.15285425860848692, -0.16379794407273746, -0.032552131205900676, 0.2829854177511556, -0.36302420067497426, -0.15136137535511, 0.11211379415342687, -0.19712991831410262, -0.2378297969440205, 0.2254958718808161, -0.14368018196768795,... |
710.0269 | Einstein universes stabilized | The hypothesis that gravitational self-binding energy may be the source for
the vacuum energy term of cosmology is studied in a Newtonian Ansatz. For
spherical spaces the attractive force of gravitation and the negative pressure
of the vacuum energy term form a self stabilizing system under very reasonable
restrictio... | gr-qc | the hypothesis that gravitational selfbinding energy may be the source for the vacuum energy term of cosmology is studied in a newtonian ansatz for spherical spaces the attractive force of gravitation and the negative pressure of the vacuum energy term form a self stabilizing system under very reasonable restrictions f... | [['the', 'hypothesis', 'that', 'gravitational', 'selfbinding', 'energy', 'may', 'be', 'the', 'source', 'for', 'the', 'vacuum', 'energy', 'term', 'of', 'cosmology', 'is', 'studied', 'in', 'a', 'newtonian', 'ansatz', 'for', 'spherical', 'spaces', 'the', 'attractive', 'force', 'of', 'gravitation', 'and', 'the', 'negative'... | [-0.1827502976730466, 0.1609219303354621, -0.1261325904354453, 0.128836848171195, -0.1216686344332993, -0.1566754778509494, -0.03146418442949653, 0.32670240189880134, -0.2423128150869161, -0.2913884716667235, 0.05273195682675578, -0.22358387247659267, -0.07230448539601639, 0.19506720347097142, 0.01170092668326106, 0.00... |
710.027 | An Analytical Study of a Structured Overlay in the presence of Dynamic
Membership | In this paper we present an analytical study of dynamic membership (aka
churn) in structured peer-to-peer networks. We use a fluid model approach to
describe steady-state or transient phenomena, and apply it to the Chord system.
For any rate of churn and stabilization rates, and any system size, we
accurately account... | cs.NI cond-mat.stat-mech cs.DC | in this paper we present an analytical study of dynamic membership aka churn in structured peertopeer networks we use a fluid model approach to describe steadystate or transient phenomena and apply it to the chord system for any rate of churn and stabilization rates and any system size we accurately account for the fun... | [['in', 'this', 'paper', 'we', 'present', 'an', 'analytical', 'study', 'of', 'dynamic', 'membership', 'aka', 'churn', 'in', 'structured', 'peertopeer', 'networks', 'we', 'use', 'a', 'fluid', 'model', 'approach', 'to', 'describe', 'steadystate', 'or', 'transient', 'phenomena', 'and', 'apply', 'it', 'to', 'the', 'chord',... | [-0.12841973489633313, 0.017680401888921754, -0.06262455634013922, 0.07870296545335333, -0.06275483536775465, -0.13888015399850837, 0.1045506493628232, 0.4019173887377191, -0.2615316068578977, -0.3070878124330193, 0.1236085485442783, -0.25949978830068615, -0.18955666255809506, 0.17624843823033626, -0.07655227315370683,... |
710.0271 | Hyperbolic Conservation Laws and Hydrodynamic Limit for Particle Systems | We study the following class of scalar hyperbolic conservation laws with
discontinuous fluxes: \partial_t\rho+\partial_xF(x,\rho)=0. The main feature of
such a conservation law is the discontinuity of the flux function in the space
variable x. Kruzkov's approach for the L1-contraction does not apply since it
requires... | math.AP math-ph math.MP | we study the following class of scalar hyperbolic conservation laws with discontinuous fluxes partial_trhopartial_xfxrho0 the main feature of such a conservation law is the discontinuity of the flux function in the space variable x kruzkovs approach for the l1contraction does not apply since it requires the lipschitz c... | [['we', 'study', 'the', 'following', 'class', 'of', 'scalar', 'hyperbolic', 'conservation', 'laws', 'with', 'discontinuous', 'fluxes', 'partial_trhopartial_xfxrho0', 'the', 'main', 'feature', 'of', 'such', 'a', 'conservation', 'law', 'is', 'the', 'discontinuity', 'of', 'the', 'flux', 'function', 'in', 'the', 'space', '... | [-0.11966963606515582, 0.0683107059826945, -0.10392692294821947, 0.06573705200571567, -0.06745694298200557, -0.1159626512200846, 0.031727672585950877, 0.25858808406995787, -0.29041792774240627, -0.2639587482928271, 0.10365514845429838, -0.2780876151243557, -0.11417452235613405, 0.17910326778583413, -0.08263119480464437... |
710.0272 | The ANTARES neutrino telescope: a status report | ANTARES is a large volume neutrino telescope currently under construction off
La Seyne-sur-mer, France, at 2475m depth. Neutrino telescopes aim at detecting
neutrinos as a new probe for a sky study at energies greater than 1 TeV. The
detection principle relies on the observation, using photomultipliers, of the
Cheren... | astro-ph | antares is a large volume neutrino telescope currently under construction off la seynesurmer france at 2475m depth neutrino telescopes aim at detecting neutrinos as a new probe for a sky study at energies greater than 1 tev the detection principle relies on the observation using photomultipliers of the cherenkov light ... | [['antares', 'is', 'a', 'large', 'volume', 'neutrino', 'telescope', 'currently', 'under', 'construction', 'off', 'la', 'seynesurmer', 'france', 'at', '2475m', 'depth', 'neutrino', 'telescopes', 'aim', 'at', 'detecting', 'neutrinos', 'as', 'a', 'new', 'probe', 'for', 'a', 'sky', 'study', 'at', 'energies', 'greater', 'th... | [-0.06635313701790657, 0.2062924522774172, -0.025539913909377935, 0.08798571531040207, -0.04799491715623088, -0.11963767765429298, 0.023985774037484305, 0.3529052787112543, -0.16888866452949056, -0.36920580637068995, 0.11627583504242105, -0.36514975026205004, -0.009282125516357013, 0.23104346218148628, 0.01507350132682... |
710.0273 | Deflection of ultra slow light under gravity | Recent experiments on ultra slow light in strongly dispersive media by
several research groups reporting slowing down of the optical pulses down to
speeds of a few metres per second encourage us to examine the intriguing
possibility of detecting a deflection or fall of the ultra slow light under
Earth's gravity, i.e.... | physics.optics physics.atom-ph | recent experiments on ultra slow light in strongly dispersive media by several research groups reporting slowing down of the optical pulses down to speeds of a few metres per second encourage us to examine the intriguing possibility of detecting a deflection or fall of the ultra slow light under earths gravity ie on th... | [['recent', 'experiments', 'on', 'ultra', 'slow', 'light', 'in', 'strongly', 'dispersive', 'media', 'by', 'several', 'research', 'groups', 'reporting', 'slowing', 'down', 'of', 'the', 'optical', 'pulses', 'down', 'to', 'speeds', 'of', 'a', 'few', 'metres', 'per', 'second', 'encourage', 'us', 'to', 'examine', 'the', 'in... | [-0.17472674837759272, 0.24088041102520286, -0.07138638663613661, 0.021859417657304387, -0.08369249894961038, -0.12798909666757521, 0.04598915851780806, 0.377747377444228, -0.23275936322117394, -0.3230302441579459, 0.07483632041681135, -0.28250416381051763, -0.07966539939992469, 0.23762333155609666, -0.0193054338107520... |
710.0274 | About calculation of traces of Dirac $\gamma$-matrices contracted with
massless vectors in Minkowski space | A new method for calculation of traces of Dirac $\gamma$-matrices contracted
with massless vectors in Minkowski space is discussed
| hep-ph | a new method for calculation of traces of dirac gammamatrices contracted with massless vectors in minkowski space is discussed | [['a', 'new', 'method', 'for', 'calculation', 'of', 'traces', 'of', 'dirac', 'gammamatrices', 'contracted', 'with', 'massless', 'vectors', 'in', 'minkowski', 'space', 'is', 'discussed']] | [-0.15423218111850714, 0.19980197390051266, -0.04969446655166777, 0.05327932207575558, -0.07892008410080482, -0.11216885719362549, -0.01675011825404669, 0.3304621498835714, -0.1510353664818563, -0.20016589368644513, 0.0036727029425827297, -0.30636007446599633, -0.15565576423939906, 0.18583572175549834, 0.01132458575854... |
710.0275 | Quantum Zeno Effect in Cavity QED: Experimental Proposal with Non Ideal
Cavities and Detectors | We propose an experiment with two coupled microwave cavities and a
"tunneling" photon observed by the passage of Rydberg atoms. We model the
coupled cavities as in Ref. \cite{art1} and include dissipative effects as well
as limited detection efficiency. We also consider realistic finite atom-field
interaction times a... | quant-ph | we propose an experiment with two coupled microwave cavities and a tunneling photon observed by the passage of rydberg atoms we model the coupled cavities as in ref citeart1 and include dissipative effects as well as limited detection efficiency we also consider realistic finite atomfield interaction times and provide ... | [['we', 'propose', 'an', 'experiment', 'with', 'two', 'coupled', 'microwave', 'cavities', 'and', 'a', 'tunneling', 'photon', 'observed', 'by', 'the', 'passage', 'of', 'rydberg', 'atoms', 'we', 'model', 'the', 'coupled', 'cavities', 'as', 'in', 'ref', 'citeart1', 'and', 'include', 'dissipative', 'effects', 'as', 'well',... | [-0.1227456964493458, 0.20382175669593508, 0.008601460747326477, 0.057516464179593926, -0.0013116392472027978, -0.18026870392451558, 0.027913384829188072, 0.40348046794062176, -0.1921589782143224, -0.3179575191056238, 0.02016088883304096, -0.2986982862311828, -0.11393050184544129, 0.23178194240148214, 0.043159504368005... |
710.0276 | Molecular dynamics study of contact mechanics: contact area and
interfacial separation from small to full contact | We report a molecular dynamics study of the contact between a rigid solid
with a randomly rough surface and an elastic block with a flat surface. We
study the contact area and the interfacial separation from small contact (low
load) to full contact (high load). For small load the contact area varies
linearly with the... | cond-mat.soft | we report a molecular dynamics study of the contact between a rigid solid with a randomly rough surface and an elastic block with a flat surface we study the contact area and the interfacial separation from small contact low load to full contact high load for small load the contact area varies linearly with the load an... | [['we', 'report', 'a', 'molecular', 'dynamics', 'study', 'of', 'the', 'contact', 'between', 'a', 'rigid', 'solid', 'with', 'a', 'randomly', 'rough', 'surface', 'and', 'an', 'elastic', 'block', 'with', 'a', 'flat', 'surface', 'we', 'study', 'the', 'contact', 'area', 'and', 'the', 'interfacial', 'separation', 'from', 'sm... | [-0.1945671435445547, 0.16491049237968886, -0.059374723944347355, -0.01442407215363346, -0.03599208920495585, -0.21780439428209017, 0.09018486249066579, 0.3680672849528491, -0.27887883433140814, -0.32589208090115185, 0.07569476677260051, -0.2732214668843274, -0.12574976375520538, 0.18234992316574788, -0.099635241102078... |
710.0277 | Quantum Gowdy $T^3$ Model: Schrodinger Representation with Unitary
Dynamics | The linearly polarized Gowdy $T^3$ model is paradigmatic for studying
technical and conceptual issues in the quest for a quantum theory of gravity
since, after a suitable and almost complete gauge fixing, it becomes an exactly
soluble midisuperspace model. Recently, a new quantization of the model,
possessing desired... | gr-qc | the linearly polarized gowdy t3 model is paradigmatic for studying technical and conceptual issues in the quest for a quantum theory of gravity since after a suitable and almost complete gauge fixing it becomes an exactly soluble midisuperspace model recently a new quantization of the model possessing desired features ... | [['the', 'linearly', 'polarized', 'gowdy', 't3', 'model', 'is', 'paradigmatic', 'for', 'studying', 'technical', 'and', 'conceptual', 'issues', 'in', 'the', 'quest', 'for', 'a', 'quantum', 'theory', 'of', 'gravity', 'since', 'after', 'a', 'suitable', 'and', 'almost', 'complete', 'gauge', 'fixing', 'it', 'becomes', 'an',... | [-0.09996690382582268, 0.13761282595992919, -0.1268844516016543, 0.06725166321349596, -0.05913971996467028, -0.17806227740698627, 0.002373312529276258, 0.3413507371276085, -0.2711693559174559, -0.26764530744736215, 0.10126387738315056, -0.25008463813657206, -0.15271420985061143, 0.16278274830464007, -0.0323870894357761... |
710.0278 | Demonstrating anyonic fractional statistics with a six-qubit quantum
simulator | Anyons are exotic quasiparticles living in two dimensions that do not fit
into the usual categories of fermions and bosons, but obey a new form of
fractional statistics. Following a recent proposal [Phys. Rev. Lett. 98, 150404
(2007)], we present an experimental demonstration of the fractional statistics
of anyons in... | quant-ph cond-mat.stat-mech | anyons are exotic quasiparticles living in two dimensions that do not fit into the usual categories of fermions and bosons but obey a new form of fractional statistics following a recent proposal phys rev lett 98 150404 2007 we present an experimental demonstration of the fractional statistics of anyons in the kitaev s... | [['anyons', 'are', 'exotic', 'quasiparticles', 'living', 'in', 'two', 'dimensions', 'that', 'do', 'not', 'fit', 'into', 'the', 'usual', 'categories', 'of', 'fermions', 'and', 'bosons', 'but', 'obey', 'a', 'new', 'form', 'of', 'fractional', 'statistics', 'following', 'a', 'recent', 'proposal', 'phys', 'rev', 'lett', '98... | [-0.1440138321942524, 0.2835298379567748, -0.0705086946097278, 0.02648466207592555, -0.05092538476225224, -0.19651870082577202, 0.0841487813950726, 0.33612824049316814, -0.16649092509419666, -0.30593931575571626, -0.018118001799610955, -0.2646551452627456, -0.13773825452117636, 0.16185113079195657, -0.05546302585610868... |
710.0279 | Zariski $k$-plets via dessins d'enfants | We construct exponentially large collections of pairwise distinct
equisingular deformation families of irreducible plane curves sharing the same
sets of singularities. The fundamental groups of all curves constructed are
abelian.
| math.AG | we construct exponentially large collections of pairwise distinct equisingular deformation families of irreducible plane curves sharing the same sets of singularities the fundamental groups of all curves constructed are abelian | [['we', 'construct', 'exponentially', 'large', 'collections', 'of', 'pairwise', 'distinct', 'equisingular', 'deformation', 'families', 'of', 'irreducible', 'plane', 'curves', 'sharing', 'the', 'same', 'sets', 'of', 'singularities', 'the', 'fundamental', 'groups', 'of', 'all', 'curves', 'constructed', 'are', 'abelian']] | [-0.3157703979561726, 0.1503094371408224, -0.09291399829089642, 0.1351730345127483, -0.06610949745712182, -0.12474291706457734, -0.036360760281483336, 0.34014760653177895, -0.3235798445840677, -0.19421292281088728, 0.046179859604065614, -0.3252640829732021, -0.11081831576302648, 0.2285922236740589, -0.11301832897588611... |
710.028 | New Cardiovascular Indices Based on a Nonlinear Spectral Analysis of
Arterial Blood Pressure Waveforms | A new method for analyzing arterial blood pressure is presented in this
report. The technique is based on the scattering transform and consists in
solving the spectral problem associated to a one-dimensional Schr\"odinger
operator with a potential depending linearly upon the pressure. This potential
is then expressed... | math-ph math.MP | a new method for analyzing arterial blood pressure is presented in this report the technique is based on the scattering transform and consists in solving the spectral problem associated to a onedimensional schrodinger operator with a potential depending linearly upon the pressure this potential is then expressed with t... | [['a', 'new', 'method', 'for', 'analyzing', 'arterial', 'blood', 'pressure', 'is', 'presented', 'in', 'this', 'report', 'the', 'technique', 'is', 'based', 'on', 'the', 'scattering', 'transform', 'and', 'consists', 'in', 'solving', 'the', 'spectral', 'problem', 'associated', 'to', 'a', 'onedimensional', 'schrodinger', '... | [-0.078062764734624, 0.09993310821282983, -0.1275921563555035, 0.0438485181589748, -0.09226972364500577, -0.13246528697742915, -0.02237763129134714, 0.3555528048848722, -0.26847760351317607, -0.25073549748781176, 0.11244323568638596, -0.2712624872751831, -0.1937883842891465, 0.22327107272755092, -0.04767042559005914, 0... |
710.0281 | How to reveal the mysteries of the most obscured high-energy sources of
our Galaxy, discovered by INTEGRAL? | A new type of high-energy binary systems has been revealed by the INTEGRAL
satellite. These sources are in the course of being unveiled by means of
multi-wavelength optical, near- and mid-infrared observations. Among these
sources, two distinct classes are appearing: the first one is constituted of
intrinsically obsc... | astro-ph | a new type of highenergy binary systems has been revealed by the integral satellite these sources are in the course of being unveiled by means of multiwavelength optical near and midinfrared observations among these sources two distinct classes are appearing the first one is constituted of intrinsically obscured highen... | [['a', 'new', 'type', 'of', 'highenergy', 'binary', 'systems', 'has', 'been', 'revealed', 'by', 'the', 'integral', 'satellite', 'these', 'sources', 'are', 'in', 'the', 'course', 'of', 'being', 'unveiled', 'by', 'means', 'of', 'multiwavelength', 'optical', 'near', 'and', 'midinfrared', 'observations', 'among', 'these', ... | [-0.11396312249013975, 0.13397678260046703, -0.04857934540173469, 0.06407403871596146, -0.0989664952413967, -0.09462310465124364, 0.04369482362929445, 0.4371505967771205, -0.20247294667553015, -0.2994685561275289, 0.15189076989996605, -0.3383730739211807, -0.11559529843596884, 0.2536016329818477, -0.03038263890820627, ... |
710.0282 | Constraints on the three-fluid model of curvaton decay | A three fluid system describing the decay of the curvaton is studied by
numerical and analytical means. We place constraints on the allowed interaction
strengths between the fluids and initial curvaton density by requiring that the
curvaton decays before nucleosynthesis while nucleosynthesis, radiation-matter
equalit... | astro-ph | a three fluid system describing the decay of the curvaton is studied by numerical and analytical means we place constraints on the allowed interaction strengths between the fluids and initial curvaton density by requiring that the curvaton decays before nucleosynthesis while nucleosynthesis radiationmatter equality and... | [['a', 'three', 'fluid', 'system', 'describing', 'the', 'decay', 'of', 'the', 'curvaton', 'is', 'studied', 'by', 'numerical', 'and', 'analytical', 'means', 'we', 'place', 'constraints', 'on', 'the', 'allowed', 'interaction', 'strengths', 'between', 'the', 'fluids', 'and', 'initial', 'curvaton', 'density', 'by', 'requir... | [-0.16842244924671293, 0.21078338868640087, -0.09479729119489935, 0.106226056671046, -0.0501960142015445, -0.15887007705384382, -0.007693024644524687, 0.3059704995739998, -0.24707312577024654, -0.3147354132875248, 0.07348046833907979, -0.22501804133256276, -0.06004945675118102, 0.15005738779867964, 0.04203987123651637,... |
710.0283 | Heegner divisors, $L$-functions and harmonic weak Maass forms | Recent works, mostly related to Ramanujan's mock theta functions, make use of
the fact that harmonic weak Maass forms can be combinatorial generating
functions. Generalizing works of Waldspurger, Kohnen and Zagier, we prove that
such forms also serve as "generating functions" for central values and
derivatives of qua... | math.NT math.AG | recent works mostly related to ramanujans mock theta functions make use of the fact that harmonic weak maass forms can be combinatorial generating functions generalizing works of waldspurger kohnen and zagier we prove that such forms also serve as generating functions for central values and derivatives of quadratic twi... | [['recent', 'works', 'mostly', 'related', 'to', 'ramanujans', 'mock', 'theta', 'functions', 'make', 'use', 'of', 'the', 'fact', 'that', 'harmonic', 'weak', 'maass', 'forms', 'can', 'be', 'combinatorial', 'generating', 'functions', 'generalizing', 'works', 'of', 'waldspurger', 'kohnen', 'and', 'zagier', 'we', 'prove', '... | [-0.2193208366146554, 0.028987855152429447, -0.14239408624479952, 0.11227675648507379, -0.1615702098397457, -0.0911537312457095, -0.00935896403034744, 0.2684527999357037, -0.31024538667305657, -0.22291015921079593, 0.06832033261231592, -0.2574346043060675, -0.23191782368104094, 0.29598378735877895, -0.10369916397916235... |
710.0284 | A Low-temperature 1H NMR Study of H2O and D2O Associated Competitively
with Immunoglobulin G in Solution | An approach has been proposed to characterize the competitive association of
D2O and to study the heterogeneity of hydration water adsorbed by the protein,
immunoglobulin G, using methodology for determining of non-freezing water in
mixed H2O-D2O protein solutions by low-temperature 1H NMR technique. Direct
data on t... | physics.gen-ph physics.bio-ph | an approach has been proposed to characterize the competitive association of d2o and to study the heterogeneity of hydration water adsorbed by the protein immunoglobulin g using methodology for determining of nonfreezing water in mixed h2od2o protein solutions by lowtemperature 1h nmr technique direct data on the numbe... | [['an', 'approach', 'has', 'been', 'proposed', 'to', 'characterize', 'the', 'competitive', 'association', 'of', 'd2o', 'and', 'to', 'study', 'the', 'heterogeneity', 'of', 'hydration', 'water', 'adsorbed', 'by', 'the', 'protein', 'immunoglobulin', 'g', 'using', 'methodology', 'for', 'determining', 'of', 'nonfreezing', '... | [-0.05046309975189436, 0.1517328769644273, -0.031154070983812877, 0.01631474224361146, 0.03684507278506021, -0.13479143113882583, 0.08477495175750724, 0.38252965728663335, -0.23769621784905576, -0.3160601690245472, 0.01995700161613429, -0.2813796040892696, -0.09210147451280147, 0.14411821497521202, 0.007075152027711367... |
710.0285 | Quantum-limited metrology with product states | We study the performance of initial product states of n-body systems in
generalized quantum metrology protocols that involve estimating an unknown
coupling constant in a nonlinear k-body (k << n) Hamiltonian. We obtain the
theoretical lower bound on the uncertainty in the estimate of the parameter.
For arbitrary init... | quant-ph cond-mat.other | we study the performance of initial product states of nbody systems in generalized quantum metrology protocols that involve estimating an unknown coupling constant in a nonlinear kbody k n hamiltonian we obtain the theoretical lower bound on the uncertainty in the estimate of the parameter for arbitrary initial states ... | [['we', 'study', 'the', 'performance', 'of', 'initial', 'product', 'states', 'of', 'nbody', 'systems', 'in', 'generalized', 'quantum', 'metrology', 'protocols', 'that', 'involve', 'estimating', 'an', 'unknown', 'coupling', 'constant', 'in', 'a', 'nonlinear', 'kbody', 'k', 'n', 'hamiltonian', 'we', 'obtain', 'the', 'the... | [-0.1751298023574054, 0.19423600849782816, -0.09597306037942568, 0.07770389275780569, 0.01323511899759372, -0.15354620745405556, 0.05059909676977744, 0.32386088761190573, -0.23388491615653037, -0.2890713203698397, 0.06076416537708913, -0.2356073467619717, -0.1267243927596913, 0.19905914474637634, -0.0008904583596934875... |
710.0286 | Random Field Potts model with dipolar-like interactions: hysteresis,
avalanches and microstructure | A model for the study of hysteresis and avalanches in a first-order phase
transition from a single variant phase to a multivariant phase is presented.
The model is based on a modification of the Random Field Potts model with
metastable dynamics by adding a dipolar interaction term truncated at nearest
neighbors. We f... | cond-mat.stat-mech | a model for the study of hysteresis and avalanches in a firstorder phase transition from a single variant phase to a multivariant phase is presented the model is based on a modification of the random field potts model with metastable dynamics by adding a dipolar interaction term truncated at nearest neighbors we focus ... | [['a', 'model', 'for', 'the', 'study', 'of', 'hysteresis', 'and', 'avalanches', 'in', 'a', 'firstorder', 'phase', 'transition', 'from', 'a', 'single', 'variant', 'phase', 'to', 'a', 'multivariant', 'phase', 'is', 'presented', 'the', 'model', 'is', 'based', 'on', 'a', 'modification', 'of', 'the', 'random', 'field', 'pot... | [-0.11266963025959938, 0.15680251717297494, -0.0765811815533949, 0.04148404586695782, -0.039383949057293546, -0.12597934495441723, 0.08035420156691385, 0.3681814814715282, -0.2304861754502939, -0.26087226952169684, 0.08209921667804483, -0.29229256041024043, -0.20144607331873715, 0.12518491186673983, 0.03022208510884556... |
710.0287 | A geometric framework for the subfield problem of generic polynomials
via Tschirnhausen transformation | Let $k$ be an arbitrary field. We study a general method to solve the
subfield problem of generic polynomials for the symmetric groups over $k$ via
Tschirnhausen transformation. Based on the general result in the former part,
we give an explicit solution to the field isomorphism problem and the subfield
problem of cu... | math.NT math.AG | let k be an arbitrary field we study a general method to solve the subfield problem of generic polynomials for the symmetric groups over k via tschirnhausen transformation based on the general result in the former part we give an explicit solution to the field isomorphism problem and the subfield problem of cubic gener... | [['let', 'k', 'be', 'an', 'arbitrary', 'field', 'we', 'study', 'a', 'general', 'method', 'to', 'solve', 'the', 'subfield', 'problem', 'of', 'generic', 'polynomials', 'for', 'the', 'symmetric', 'groups', 'over', 'k', 'via', 'tschirnhausen', 'transformation', 'based', 'on', 'the', 'general', 'result', 'in', 'the', 'forme... | [-0.1842615819952794, 0.008798347981179464, -0.057615237923240976, -0.02593686715332105, -0.1108160711775877, -0.1310917490688888, -0.004340793153173045, 0.33069365978927207, -0.34869616542403636, -0.23485145830598317, 0.09444231022682384, -0.21513918893240197, -0.16858990269247442, 0.24776008869766405, -0.026402484797... |
710.0288 | Possible implications of the channeling effect in NaI(Tl) crystals | The channeling effect of low energy ions along the crystallographic axes and
planes of NaI(Tl) crystals is discussed in the framework of corollary
investigations on WIMP Dark Matter candidates. In fact, the modeling of this
existing effect implies a more complex evaluation of the luminosity yield for
low energy recoi... | astro-ph | the channeling effect of low energy ions along the crystallographic axes and planes of naitl crystals is discussed in the framework of corollary investigations on wimp dark matter candidates in fact the modeling of this existing effect implies a more complex evaluation of the luminosity yield for low energy recoiling n... | [['the', 'channeling', 'effect', 'of', 'low', 'energy', 'ions', 'along', 'the', 'crystallographic', 'axes', 'and', 'planes', 'of', 'naitl', 'crystals', 'is', 'discussed', 'in', 'the', 'framework', 'of', 'corollary', 'investigations', 'on', 'wimp', 'dark', 'matter', 'candidates', 'in', 'fact', 'the', 'modeling', 'of', '... | [-0.10490052146725619, 0.15860008904841585, -0.03464864491498176, 0.09631123577415103, -0.061902710754739146, -0.11646093047079696, 0.005472961103241943, 0.3919877643946191, -0.18090148626918523, -0.3172224323776826, 0.015123408394341002, -0.30816349347817223, -0.0508643435511056, 0.20260062097558673, -0.00292705362793... |
710.0289 | The Form of the Effective Interaction in Harmonic-Oscillator-Based
Effective Theory | I explore the form of the effective interaction in harmonic-oscillator-based
effective theory (HOBET) in next-to-next-to-next-to-leading order (N3LO). As
the included space in a HOBET (as in the shell model) is defined by the
oscillator energy, both long-distance (low-momentum) and short-distance
(high-momentum) degr... | nucl-th | i explore the form of the effective interaction in harmonicoscillatorbased effective theory hobet in nexttonexttonexttoleading order n3lo as the included space in a hobet as in the shell model is defined by the oscillator energy both longdistance lowmomentum and shortdistance highmomentum degrees of freedom reside in t... | [['i', 'explore', 'the', 'form', 'of', 'the', 'effective', 'interaction', 'in', 'harmonicoscillatorbased', 'effective', 'theory', 'hobet', 'in', 'nexttonexttonexttoleading', 'order', 'n3lo', 'as', 'the', 'included', 'space', 'in', 'a', 'hobet', 'as', 'in', 'the', 'shell', 'model', 'is', 'defined', 'by', 'the', 'oscilla... | [-0.1429000674372329, 0.16432807387911563, -0.10116161720670237, 0.1046833209812493, -0.018481964116676176, -0.08364585414969813, 0.017536331688681843, 0.3303857785014605, -0.23388220247050578, -0.3138734525330647, 0.015210574239697025, -0.2900559123478491, -0.07763678729348943, 0.15351709885351628, 0.05070273734798485... |
710.029 | Experimental demonstration of a quantum protocol for Byzantine agreement
and liar detection | We introduce a new quantum protocol for solving detectable Byzantine
agreement (also called detectable broadcast) between three parties, and also
for solving the detectable liar detection problem. The protocol is suggested by
the properties of a four-qubit entangled state, and the classical part of the
protocol is si... | quant-ph | we introduce a new quantum protocol for solving detectable byzantine agreement also called detectable broadcast between three parties and also for solving the detectable liar detection problem the protocol is suggested by the properties of a fourqubit entangled state and the classical part of the protocol is simpler th... | [['we', 'introduce', 'a', 'new', 'quantum', 'protocol', 'for', 'solving', 'detectable', 'byzantine', 'agreement', 'also', 'called', 'detectable', 'broadcast', 'between', 'three', 'parties', 'and', 'also', 'for', 'solving', 'the', 'detectable', 'liar', 'detection', 'problem', 'the', 'protocol', 'is', 'suggested', 'by', ... | [-0.19304188485539547, 0.10973548194394397, -0.06441952293795167, 0.035285053848796946, -0.009628675962713633, -0.26603063936768606, 0.08886530153650904, 0.35761381237005646, -0.21135228716373217, -0.3026295687551751, 0.052367896074429154, -0.2632338563262513, -0.14203474072344374, 0.23298369145557057, -0.0449779873050... |
710.0291 | On Outage Behavior of Wideband Slow-Fading Channels | This paper investigates point-to-point information transmission over a
wideband slow-fading channel, modeled as an (asymptotically) large number of
independent identically distributed parallel channels, with the random channel
fading realizations remaining constant over the entire coding block. On the one
hand, in th... | cs.IT math.IT | this paper investigates pointtopoint information transmission over a wideband slowfading channel modeled as an asymptotically large number of independent identically distributed parallel channels with the random channel fading realizations remaining constant over the entire coding block on the one hand in the wideband ... | [['this', 'paper', 'investigates', 'pointtopoint', 'information', 'transmission', 'over', 'a', 'wideband', 'slowfading', 'channel', 'modeled', 'as', 'an', 'asymptotically', 'large', 'number', 'of', 'independent', 'identically', 'distributed', 'parallel', 'channels', 'with', 'the', 'random', 'channel', 'fading', 'realiz... | [-0.26934372387447597, 0.09408597205255817, 0.006157955876946197, 0.0010206967034498177, -0.023918681701061206, -0.2852578881330851, 0.15263096406321847, 0.3858004912581442, -0.26033666830951885, -0.25603759751423644, 0.10263460154097927, -0.25657888617903246, -0.09961712395767076, 0.14559782510307634, -0.0941547110780... |
710.0292 | Obscured sources and Supergiant Fast X-ray Transients: new classes of
high mass X-ray binaries | A new type of high-energy binary systems has been revealed by the INTEGRAL
satellite. These sources are in the course of being unveiled by means of
multi-wavelength optical, near- and mid-infrared observations. Among these
sources, two distinct classes are appearing: the first one is constituted of
intrinsically obsc... | astro-ph | a new type of highenergy binary systems has been revealed by the integral satellite these sources are in the course of being unveiled by means of multiwavelength optical near and midinfrared observations among these sources two distinct classes are appearing the first one is constituted of intrinsically obscured highen... | [['a', 'new', 'type', 'of', 'highenergy', 'binary', 'systems', 'has', 'been', 'revealed', 'by', 'the', 'integral', 'satellite', 'these', 'sources', 'are', 'in', 'the', 'course', 'of', 'being', 'unveiled', 'by', 'means', 'of', 'multiwavelength', 'optical', 'near', 'and', 'midinfrared', 'observations', 'among', 'these', ... | [-0.11489992865183371, 0.12674080072836558, -0.04652148705389036, 0.0676960562975605, -0.09597247027673982, -0.07970624300323322, 0.055228624066574056, 0.42946179685327157, -0.19351614590383356, -0.3113218531767595, 0.14848550852522596, -0.3407306209809973, -0.10011440835906271, 0.2502315743927988, -0.02999865958749146... |
710.0293 | Continuum limit of self-driven particles with orientation interaction | We consider the discrete Couzin-Vicsek algorithm (CVA), which describes the
interactions of individuals among animal societies such as fish schools. In
this article, we propose a kinetic (mean-field) version of the CVA model and
provide its formal macroscopic limit. The final macroscopic model involves a
conservation... | math-ph math.MP | we consider the discrete couzinvicsek algorithm cva which describes the interactions of individuals among animal societies such as fish schools in this article we propose a kinetic meanfield version of the cva model and provide its formal macroscopic limit the final macroscopic model involves a conservation equation fo... | [['we', 'consider', 'the', 'discrete', 'couzinvicsek', 'algorithm', 'cva', 'which', 'describes', 'the', 'interactions', 'of', 'individuals', 'among', 'animal', 'societies', 'such', 'as', 'fish', 'schools', 'in', 'this', 'article', 'we', 'propose', 'a', 'kinetic', 'meanfield', 'version', 'of', 'the', 'cva', 'model', 'an... | [-0.13234058095749174, 0.12176054222980158, -0.15968682660441322, 0.0976041495509634, -0.0811315791474085, -0.11150407287281718, 0.023888549728193476, 0.26289578598369373, -0.24236134067177773, -0.259974100449112, 0.03838847044808267, -0.2678119050014471, -0.151908844416396, 0.12397945146442632, -0.07357707189584381, 0... |
710.0294 | Thin and dressed Polyakov loops from spectral sums of lattice
differential operators | We represent thin and dressed Polyakov loops as spectral sums of eigenvalues
of differential operators on the lattice. For that purpose we calculate
complete sets of eigenvalues of the staggered Dirac and the covariant Laplace
operator for several temporal boundary conditions. The spectra from different
boundary cond... | hep-lat | we represent thin and dressed polyakov loops as spectral sums of eigenvalues of differential operators on the lattice for that purpose we calculate complete sets of eigenvalues of the staggered dirac and the covariant laplace operator for several temporal boundary conditions the spectra from different boundary conditio... | [['we', 'represent', 'thin', 'and', 'dressed', 'polyakov', 'loops', 'as', 'spectral', 'sums', 'of', 'eigenvalues', 'of', 'differential', 'operators', 'on', 'the', 'lattice', 'for', 'that', 'purpose', 'we', 'calculate', 'complete', 'sets', 'of', 'eigenvalues', 'of', 'the', 'staggered', 'dirac', 'and', 'the', 'covariant'... | [-0.1540326033438365, 0.19807536741269818, -0.05876518047627914, 0.10174651347459798, -0.04335292023382183, -0.06605839302359395, 0.04626209935150951, 0.4267237648726946, -0.1963077646186463, -0.23238789747435465, 0.08374448205170457, -0.31455338104482156, -0.10248495500074722, 0.1356614246285599, -0.013430818101862469... |
710.0295 | Equation of motion of an interstellar Bussard ramjet with radiation and
mass losses | An interstellar Bussard ramjet is a spaceship using the protons of the
interstellar medium in a fusion engine to produce thrust. In recent papers, it
was shown that the relativistic equation of motion of an ideal ramjet and of a
ramjet with radiation loss are analytical. When a mass loss appears, the limit
speed of t... | physics.class-ph physics.space-ph | an interstellar bussard ramjet is a spaceship using the protons of the interstellar medium in a fusion engine to produce thrust in recent papers it was shown that the relativistic equation of motion of an ideal ramjet and of a ramjet with radiation loss are analytical when a mass loss appears the limit speed of the ram... | [['an', 'interstellar', 'bussard', 'ramjet', 'is', 'a', 'spaceship', 'using', 'the', 'protons', 'of', 'the', 'interstellar', 'medium', 'in', 'a', 'fusion', 'engine', 'to', 'produce', 'thrust', 'in', 'recent', 'papers', 'it', 'was', 'shown', 'that', 'the', 'relativistic', 'equation', 'of', 'motion', 'of', 'an', 'ideal',... | [-0.12398286362489065, 0.1412193318046775, -0.09454426820060083, 0.008297236028010958, -0.02949007381685078, -0.03166257969375389, -0.00812242014023165, 0.38287782374148566, -0.2600831356210013, -0.2691499544928471, 0.05247116996324621, -0.24862205759466935, -0.028695499799990407, 0.21721093201388916, -0.06636439034870... |
710.0296 | On the unipotent support of character sheaves | Let $G$ be a connected reductive group over $F_q$, where $q$ is large enough
and the center of $G$ is connected. We are concerned with Lusztig's theory of
{\em character sheaves}, a geometric version of the classical character theory
of the finite group $G(F_q)$. We show that under a certain technical condition,
the ... | math.RT | let g be a connected reductive group over f_q where q is large enough and the center of g is connected we are concerned with lusztigs theory of em character sheaves a geometric version of the classical character theory of the finite group gf_q we show that under a certain technical condition the restriction of a charac... | [['let', 'g', 'be', 'a', 'connected', 'reductive', 'group', 'over', 'f_q', 'where', 'q', 'is', 'large', 'enough', 'and', 'the', 'center', 'of', 'g', 'is', 'connected', 'we', 'are', 'concerned', 'with', 'lusztigs', 'theory', 'of', 'em', 'character', 'sheaves', 'a', 'geometric', 'version', 'of', 'the', 'classical', 'char... | [-0.25572947107139044, 0.10512853707070463, -0.15039163717068732, 0.0027794533350970598, -0.13389172862749546, -0.12385734044015408, -0.004147153852973134, 0.3113831601291895, -0.3570147021114826, -0.16465132068493404, 0.0843136657832656, -0.2099831318925135, -0.14841103743994608, 0.20993982072686776, -0.15469598209019... |
710.0297 | GL(2,R) geometry of ODE's | We study five dimensional geometries associated with the 5-dimensional
irreducible representation of GL(2,R). These are special Weyl geometries in
signature (3,2) having the structure group reduced from CO(3,2) to GL(2,R). The
reduction is obtained by means of a conformal class of totally symmetric
3-tensors. Among a... | math.DG | we study five dimensional geometries associated with the 5dimensional irreducible representation of gl2r these are special weyl geometries in signature 32 having the structure group reduced from co32 to gl2r the reduction is obtained by means of a conformal class of totally symmetric 3tensors among all gl2r geometries ... | [['we', 'study', 'five', 'dimensional', 'geometries', 'associated', 'with', 'the', '5dimensional', 'irreducible', 'representation', 'of', 'gl2r', 'these', 'are', 'special', 'weyl', 'geometries', 'in', 'signature', '32', 'having', 'the', 'structure', 'group', 'reduced', 'from', 'co32', 'to', 'gl2r', 'the', 'reduction', ... | [-0.21446390431133888, 0.06993334355837483, -0.05072925924121038, 0.03292173795078112, -0.09936556749592494, -0.14564334327840936, -0.09247442671836799, 0.35393265772448934, -0.2576244776542096, -0.20936677708978887, 0.13351306035689522, -0.2555533094807407, -0.18993274225124523, 0.17113098924291198, -0.055619715779776... |
710.0298 | Monitoring of Transient Black Hole Candidates observed in the INTEGRAL
survey | The INTEGRAL/IBIS survey was performed collecting all the GPS and GCDE data
together with all the available public data . The second catalogue, published
in 2006 by Bird et al., is dominated by detection of 113 X-ray binaries, with
38 being high-mass and 67 low-mass. In most systems the compact object is a
neutron st... | astro-ph | the integralibis survey was performed collecting all the gps and gcde data together with all the available public data the second catalogue published in 2006 by bird et al is dominated by detection of 113 xray binaries with 38 being highmass and 67 lowmass in most systems the compact object is a neutron star but the sa... | [['the', 'integralibis', 'survey', 'was', 'performed', 'collecting', 'all', 'the', 'gps', 'and', 'gcde', 'data', 'together', 'with', 'all', 'the', 'available', 'public', 'data', 'the', 'second', 'catalogue', 'published', 'in', '2006', 'by', 'bird', 'et', 'al', 'is', 'dominated', 'by', 'detection', 'of', '113', 'xray', ... | [-0.0902813552852927, 0.07399773083411024, -0.047592448602829664, 0.09570718922519258, -0.11485672742128372, -0.09965384068218844, 0.10182337900291064, 0.4020626042851262, -0.10718811565588805, -0.42232040259876247, 0.1734289876665802, -0.39870624666634413, -0.04889167466160235, 0.23073709311355498, -0.0545154609717428... |
710.0299 | Nonabelian solutions in a Melvin magnetic universe | We show the existence of D=4 nonabelian solutions approaching asymptotically
a dilatonic Melvin spacetime background. An exact solution generalizing the
Chamseddine-Volkov soliton for a nonzero external U(1) magnetic field is also
reported.
| hep-th | we show the existence of d4 nonabelian solutions approaching asymptotically a dilatonic melvin spacetime background an exact solution generalizing the chamseddinevolkov soliton for a nonzero external u1 magnetic field is also reported | [['we', 'show', 'the', 'existence', 'of', 'd4', 'nonabelian', 'solutions', 'approaching', 'asymptotically', 'a', 'dilatonic', 'melvin', 'spacetime', 'background', 'an', 'exact', 'solution', 'generalizing', 'the', 'chamseddinevolkov', 'soliton', 'for', 'a', 'nonzero', 'external', 'u1', 'magnetic', 'field', 'is', 'also',... | [-0.28969250186797113, 0.16885079750312387, -0.03051959392764876, 0.10824921617900292, -0.1278314628908711, -0.1845515874785281, -0.06151609768670413, 0.279026547086335, -0.07341985290329303, -0.21968205243108735, 0.07231033677535673, -0.29821433030789896, -0.1506123219526583, 0.1161906423587953, -0.00887576106094545, ... |
710.03 | The contribution of very massive high-redshift SWIRE galaxies to the
stellar mass function | (Abridged) We selected high-z massive galaxies at 5.8 microns, in the SWIRE
ELAIS-S1 field (1 sq. deg.). Galaxies with the 1.6 microns stellar peak
redshifted into the IRAC bands (z~1-3, called ``IR-peakers'') were identified.
Stellar masses were derived by means of spectro-photometric fitting and used to
compute the... | astro-ph | abridged we selected highz massive galaxies at 58 microns in the swire elaiss1 field 1 sq deg galaxies with the 16 microns stellar peak redshifted into the irac bands z13 called irpeakers were identified stellar masses were derived by means of spectrophotometric fitting and used to compute the stellar mass function mf ... | [['abridged', 'we', 'selected', 'highz', 'massive', 'galaxies', 'at', '58', 'microns', 'in', 'the', 'swire', 'elaiss1', 'field', '1', 'sq', 'deg', 'galaxies', 'with', 'the', '16', 'microns', 'stellar', 'peak', 'redshifted', 'into', 'the', 'irac', 'bands', 'z13', 'called', 'irpeakers', 'were', 'identified', 'stellar', '... | [-0.004745019591280247, 0.09576162618842163, -0.05129339881688682, 0.13158618410343637, -0.07495661320644695, -0.02984855606476878, 0.06282915927237917, 0.44655311359783967, -0.058436733439735516, -0.4117192820105478, 0.02054795681389138, -0.293556093653119, 0.04113980348391751, 0.17796072865049375, -0.0057315994176086... |
710.0301 | Spacetime: Arena or Reality? | For small values of the mass (in relation to the angular momentum and
electric charge), the Kerr-Newman (KN) solution of Einstein equation reduces to
a naked singularity of circular shape. By considering the Hawking and Ellis
extended interpretation of the KN spacetime, as well as Wheeler's idea of
"charge without ch... | gr-qc hep-th | for small values of the mass in relation to the angular momentum and electric charge the kerrnewman kn solution of einstein equation reduces to a naked singularity of circular shape by considering the hawking and ellis extended interpretation of the kn spacetime as well as wheelers idea of charge without charge the non... | [['for', 'small', 'values', 'of', 'the', 'mass', 'in', 'relation', 'to', 'the', 'angular', 'momentum', 'and', 'electric', 'charge', 'the', 'kerrnewman', 'kn', 'solution', 'of', 'einstein', 'equation', 'reduces', 'to', 'a', 'naked', 'singularity', 'of', 'circular', 'shape', 'by', 'considering', 'the', 'hawking', 'and', ... | [-0.14989443089839793, 0.13013741263798137, -0.10929317228000263, 0.09412644425634857, -0.07893990108863913, -0.12936219712384314, -0.012069800717876755, 0.27961753812625256, -0.2267425288881758, -0.31693923113224426, 0.0559080848378203, -0.26413173686793384, -0.0962520345589883, 0.1721090591820828, -0.0144121665172546... |
710.0302 | A Protocol For Cooling and Controlling Composite Systems by Local
Interactions | We discuss an explicit protocol which allows one to externally cool and
control a composite system by operating on a small subset of it. The scheme
permits to transfer arbitrary and unknown quantum states from a memory on the
network ("upload access") as well as the inverse ("download access"). In
particular it yield... | quant-ph | we discuss an explicit protocol which allows one to externally cool and control a composite system by operating on a small subset of it the scheme permits to transfer arbitrary and unknown quantum states from a memory on the network upload access as well as the inverse download access in particular it yields a method f... | [['we', 'discuss', 'an', 'explicit', 'protocol', 'which', 'allows', 'one', 'to', 'externally', 'cool', 'and', 'control', 'a', 'composite', 'system', 'by', 'operating', 'on', 'a', 'small', 'subset', 'of', 'it', 'the', 'scheme', 'permits', 'to', 'transfer', 'arbitrary', 'and', 'unknown', 'quantum', 'states', 'from', 'a',... | [-0.13064234631562258, 0.08027740345179632, -0.06951247068453517, 0.037104078963146374, -0.05991544945449647, -0.20583257508479944, 0.14061819692931565, 0.37945826951477485, -0.2885140078931542, -0.32835428176795023, 0.13131679245468103, -0.21555014394674551, -0.09438378227306372, 0.25288212411421335, -0.04939675902537... |
710.0303 | Polyelectrolyte-Compression Forces between Spherical DNA Brushes | Optical tweezers are employed to measure the forces of interaction within a
single pair of DNA-grafted colloids in dependence of the molecular weight of
the DNA-chains, and the concentration and valence of the surrounding ionic
medium. The resulting forces are short-range and set in as the
surface-to-surface distance... | cond-mat.soft | optical tweezers are employed to measure the forces of interaction within a single pair of dnagrafted colloids in dependence of the molecular weight of the dnachains and the concentration and valence of the surrounding ionic medium the resulting forces are shortrange and set in as the surfacetosurface distance between ... | [['optical', 'tweezers', 'are', 'employed', 'to', 'measure', 'the', 'forces', 'of', 'interaction', 'within', 'a', 'single', 'pair', 'of', 'dnagrafted', 'colloids', 'in', 'dependence', 'of', 'the', 'molecular', 'weight', 'of', 'the', 'dnachains', 'and', 'the', 'concentration', 'and', 'valence', 'of', 'the', 'surrounding... | [-0.11302493927125339, 0.16141669418142046, -0.08398606079650582, -0.0014886946933123694, 0.024792888276879827, -0.0698638304527248, 0.05658901004140736, 0.385313009062121, -0.25368460816561533, -0.31430728369992056, 0.007455510149900151, -0.32003470099661296, -0.06968657665395288, 0.17171573655940192, 0.05341569118962... |
710.0304 | Effects of temperature and surface step on the incipient plasticity in
strained aluminium studied by atomistic simulations | Atomistic simulations using an EAM potential are carried out to investigate
the first stages of plasticity in aluminum slabs, in particular the effect of
both temperature and step geometry on the nucleation of dislocations from
surface steps. Temperature is shown to significantly reduce the elastic limit,
and to acti... | cond-mat.other | atomistic simulations using an eam potential are carried out to investigate the first stages of plasticity in aluminum slabs in particular the effect of both temperature and step geometry on the nucleation of dislocations from surface steps temperature is shown to significantly reduce the elastic limit and to activate ... | [['atomistic', 'simulations', 'using', 'an', 'eam', 'potential', 'are', 'carried', 'out', 'to', 'investigate', 'the', 'first', 'stages', 'of', 'plasticity', 'in', 'aluminum', 'slabs', 'in', 'particular', 'the', 'effect', 'of', 'both', 'temperature', 'and', 'step', 'geometry', 'on', 'the', 'nucleation', 'of', 'dislocati... | [-0.11342200047124319, 0.1475258004231617, -0.07748458627611399, -0.020487763161499854, -0.01596170885464813, -0.059180777101435614, 0.07046184555002594, 0.41922842173636715, -0.2506204106715284, -0.25699243135750294, 0.047187149137128855, -0.25941613324788176, -0.15591274032551983, 0.11198877697645486, 0.0258619630977... |
710.0305 | Homology and K--Theory Methods for Classes of Branes Wrapping Nontrivial
Cycles | We apply some methods of homology and K-theory to special classes of branes
wrapping homologically nontrivial cycles. We treat the classification of
four-geometries in terms of compact stabilizers (by analogy with Thurston's
classification of three-geometries) and derive the K-amenability of Lie groups
associated wit... | hep-th | we apply some methods of homology and ktheory to special classes of branes wrapping homologically nontrivial cycles we treat the classification of fourgeometries in terms of compact stabilizers by analogy with thurstons classification of threegeometries and derive the kamenability of lie groups associated with locally ... | [['we', 'apply', 'some', 'methods', 'of', 'homology', 'and', 'ktheory', 'to', 'special', 'classes', 'of', 'branes', 'wrapping', 'homologically', 'nontrivial', 'cycles', 'we', 'treat', 'the', 'classification', 'of', 'fourgeometries', 'in', 'terms', 'of', 'compact', 'stabilizers', 'by', 'analogy', 'with', 'thurstons', 'c... | [-0.2078045703431902, 0.055643745557597234, 0.006231313911340539, 0.08236567266858257, -0.06470075858727334, -0.20015512503053445, -0.02431483217237872, 0.385587254701744, -0.21364150130345175, -0.20544534864362388, 0.10929055771853272, -0.27769594491941724, -0.12897335076408964, 0.19495701476643307, -0.195675603553859... |
710.0306 | Unitary Isobar Model - MAID2007 | The unitary isobar model MAID2007 has been developed to analyze the world
data of pion photo- and electroproduction. The model contains both a common
background and several resonance terms. The background is unitarized according
to the K-matrix prescription, and the 13 four-star resonances with masses below
2 GeV are... | nucl-th hep-ph | the unitary isobar model maid2007 has been developed to analyze the world data of pion photo and electroproduction the model contains both a common background and several resonance terms the background is unitarized according to the kmatrix prescription and the 13 fourstar resonances with masses below 2 gev are describ... | [['the', 'unitary', 'isobar', 'model', 'maid2007', 'has', 'been', 'developed', 'to', 'analyze', 'the', 'world', 'data', 'of', 'pion', 'photo', 'and', 'electroproduction', 'the', 'model', 'contains', 'both', 'a', 'common', 'background', 'and', 'several', 'resonance', 'terms', 'the', 'background', 'is', 'unitarized', 'ac... | [-0.031268682901729614, 0.1545270891841098, -0.10589779478211242, 0.1660460562449701, -0.054804757792645924, -0.10275851809777893, -0.008058662763617646, 0.37397014593275696, -0.13389345175192618, -0.29584110171037115, 0.022327677771010294, -0.33921355429965144, -0.02613964383412027, 0.1394528271496081, 0.0566728776231... |
710.0307 | Reconstruction of Rayleigh-Lamb dispersion spectrum based on noise
obtained from an air-jet forcing | The time-domain cross-correlation of incoherent and random noise recorded by
a series of passive sensors contains the impulse response of the medium between
these sensors. By using noise generated by a can of compressed air sprayed on
the surface of a plexiglass plate, we are able to reconstruct not only the time
of ... | physics.class-ph physics.gen-ph | the timedomain crosscorrelation of incoherent and random noise recorded by a series of passive sensors contains the impulse response of the medium between these sensors by using noise generated by a can of compressed air sprayed on the surface of a plexiglass plate we are able to reconstruct not only the time of flight... | [['the', 'timedomain', 'crosscorrelation', 'of', 'incoherent', 'and', 'random', 'noise', 'recorded', 'by', 'a', 'series', 'of', 'passive', 'sensors', 'contains', 'the', 'impulse', 'response', 'of', 'the', 'medium', 'between', 'these', 'sensors', 'by', 'using', 'noise', 'generated', 'by', 'a', 'can', 'of', 'compressed',... | [-0.15928846033856126, 0.1359138585778495, -0.07730437285765956, -0.015801803515524012, -0.04367418049871191, -0.060257306462458145, 0.050113920371955126, 0.38608162528743933, -0.2714893377395164, -0.2638230924939682, 0.11881786879696853, -0.29204570920224865, -0.13636821951546702, 0.2121438123605342, -0.02256856000757... |
710.0308 | Electron Beam Dynamics in 4GLS | Studies of the electron beam dynamics for the 4GLS design are presented. 4GLS
will provide three different electron bunch trains to a variety of user
synchrotron sources. The 1 kHz XUV-FEL and 100 mA High Average Current branches
share a common 540 MeV linac, whilst the 13 MHz IR-FEL must be
well-synchronised to them... | physics.acc-ph | studies of the electron beam dynamics for the 4gls design are presented 4gls will provide three different electron bunch trains to a variety of user synchrotron sources the 1 khz xuvfel and 100 ma high average current branches share a common 540 mev linac whilst the 13 mhz irfel must be wellsynchronised to them an over... | [['studies', 'of', 'the', 'electron', 'beam', 'dynamics', 'for', 'the', '4gls', 'design', 'are', 'presented', '4gls', 'will', 'provide', 'three', 'different', 'electron', 'bunch', 'trains', 'to', 'a', 'variety', 'of', 'user', 'synchrotron', 'sources', 'the', '1', 'khz', 'xuvfel', 'and', '100', 'ma', 'high', 'average', ... | [-0.12681428007781506, 0.18394800724296753, -0.027180531377800635, 0.06375536457764813, -0.05409389639486714, -0.1516111700174709, -0.011861832274330988, 0.4287907441974514, -0.20441750701801437, -0.334649172756407, 0.08145464255552118, -0.28134931094116633, 0.04676984677401682, 0.257026738466488, -0.01431871280591521,... |
710.0309 | Structural, electronic and optical properties of tetrahedral
$Si_xGe_{47-x}:H_{60}$ nanocrystals: A Density Functional study | The structural, cohesive, electronic and optical properties of mixed SiGe:H
quantum dots are studied by Density Functional Theory (DFT) calculations on a
representative ensemble of medium size nanoparticles of the form
$Si_xGe_{47-x}:H_{60}$. The calculations have been performed in the framework
of the hybrid non-loc... | cond-mat.mtrl-sci | the structural cohesive electronic and optical properties of mixed sigeh quantum dots are studied by density functional theory dft calculations on a representative ensemble of medium size nanoparticles of the form si_xge_47xh_60 the calculations have been performed in the framework of the hybrid nonlocal exchangecorrel... | [['the', 'structural', 'cohesive', 'electronic', 'and', 'optical', 'properties', 'of', 'mixed', 'sigeh', 'quantum', 'dots', 'are', 'studied', 'by', 'density', 'functional', 'theory', 'dft', 'calculations', 'on', 'a', 'representative', 'ensemble', 'of', 'medium', 'size', 'nanoparticles', 'of', 'the', 'form', 'si_xge_47x... | [-0.06151462101021453, 0.12980799233294366, -0.06060921478578273, 0.01811634766174179, 0.02173514842220089, -0.10973837435902918, 0.07250913356170606, 0.427189456353731, -0.21341211996589074, -0.329921103257905, 0.039426637388190584, -0.3130921823136947, -0.13595138575251708, 0.1520402712309185, 0.046096255493295546, 0... |
710.031 | Shell model description of the 14C dating beta decay with
Brown-Rho-scaled NN interactions | We present shell model calculations for the beta-decay of the 14C ground
state to the 14N ground state, treating the states of the A=14 multiplet as two
0p holes in an 16O core. We employ low-momentum nucleon-nucleon (NN)
interactions derived from the realistic Bonn-B potential and find that the
Gamow-Teller matrix e... | nucl-th | we present shell model calculations for the betadecay of the 14c ground state to the 14n ground state treating the states of the a14 multiplet as two 0p holes in an 16o core we employ lowmomentum nucleonnucleon nn interactions derived from the realistic bonnb potential and find that the gamowteller matrix element is to... | [['we', 'present', 'shell', 'model', 'calculations', 'for', 'the', 'betadecay', 'of', 'the', '14c', 'ground', 'state', 'to', 'the', '14n', 'ground', 'state', 'treating', 'the', 'states', 'of', 'the', 'a14', 'multiplet', 'as', 'two', '0p', 'holes', 'in', 'an', '16o', 'core', 'we', 'employ', 'lowmomentum', 'nucleonnucleo... | [-0.05911760665196225, 0.1988705539914186, -0.0744861652046141, 0.11532923747777511, 0.050422824541092814, -0.07435984481686264, 0.03888660908984791, 0.353867625397511, -0.2070363865170936, -0.2718227689813358, -0.015293032485865672, -0.3240666961563485, -0.06190637053739756, 0.09306169087347343, 0.09954303595468514, 0... |
710.0311 | The Shapes of Galaxy Groups | We derive probability density functions for the projected axial ratios of the
real and mock 2PIGG galaxy groups, and use this data to investigate the
intrinsic three dimensional shape of the dark matter ellipsoids that they
trace. As well as analysing the raw data for groups of varying multiplicities,
a convolution c... | astro-ph | we derive probability density functions for the projected axial ratios of the real and mock 2pigg galaxy groups and use this data to investigate the intrinsic three dimensional shape of the dark matter ellipsoids that they trace as well as analysing the raw data for groups of varying multiplicities a convolution correc... | [['we', 'derive', 'probability', 'density', 'functions', 'for', 'the', 'projected', 'axial', 'ratios', 'of', 'the', 'real', 'and', 'mock', '2pigg', 'galaxy', 'groups', 'and', 'use', 'this', 'data', 'to', 'investigate', 'the', 'intrinsic', 'three', 'dimensional', 'shape', 'of', 'the', 'dark', 'matter', 'ellipsoids', 'th... | [-0.046567913159179464, 0.0552402139523999, -0.13568624590850992, 0.13049428112997322, -0.04210420031941466, -0.07595833241471757, 0.005382166886234392, 0.40533406741610944, -0.18580137508135655, -0.35037810620788024, 0.07331785981035174, -0.29617454977089447, -0.0608672888303116, 0.18883297144760672, -0.00370736819745... |
710.0312 | A relativistic model for neutrino pion production from nuclei in the
resonance region | We present a relativistic model for electroweak pion production from nuclei,
focusing on the $\Delta$ and the second resonance region. Bound states are
derived in the Hartree approximation to the $\sigma-\omega$ Walecka model.
Final-state interactions of the outgoing pion and nucleon are described in a
factorized way... | nucl-th | we present a relativistic model for electroweak pion production from nuclei focusing on the delta and the second resonance region bound states are derived in the hartree approximation to the sigmaomega walecka model finalstate interactions of the outgoing pion and nucleon are described in a factorized way by means of a... | [['we', 'present', 'a', 'relativistic', 'model', 'for', 'electroweak', 'pion', 'production', 'from', 'nuclei', 'focusing', 'on', 'the', 'delta', 'and', 'the', 'second', 'resonance', 'region', 'bound', 'states', 'are', 'derived', 'in', 'the', 'hartree', 'approximation', 'to', 'the', 'sigmaomega', 'walecka', 'model', 'fi... | [-0.0825405086875738, 0.23046660436938207, -0.1206552226197285, 0.18354841853181522, -0.013880114033818246, -0.09766258895397187, 0.05227275045899053, 0.33895034093409776, -0.1705599400897821, -0.24240988050897916, -0.10978175311970215, -0.3153533420248035, -0.001850944384932518, 0.12425969417206943, 0.1507295164337847... |
710.0313 | Gravitational Stability and Bulk Cosmology | We present a discussion of the effects induced by bulk viscosity either on
the very early Universe stability and on the dynamics associated to the extreme
gravitational collapse of a gas cloud. In both cases the viscosity coefficient
is related to the energy density $\rho$ via a power-law of the form
$\zeta=\zeta_0 \... | gr-qc astro-ph | we present a discussion of the effects induced by bulk viscosity either on the very early universe stability and on the dynamics associated to the extreme gravitational collapse of a gas cloud in both cases the viscosity coefficient is related to the energy density rho via a powerlaw of the form zetazeta_0 rhos where z... | [['we', 'present', 'a', 'discussion', 'of', 'the', 'effects', 'induced', 'by', 'bulk', 'viscosity', 'either', 'on', 'the', 'very', 'early', 'universe', 'stability', 'and', 'on', 'the', 'dynamics', 'associated', 'to', 'the', 'extreme', 'gravitational', 'collapse', 'of', 'a', 'gas', 'cloud', 'in', 'both', 'cases', 'the',... | [-0.14433104435983113, 0.1352787795087788, -0.11419665631036514, 0.06341508568291465, -0.02981823652330786, -0.06415401167515665, 0.004325902635231614, 0.2903400150109082, -0.25013583783619103, -0.23988609280716627, 0.09180770289106295, -0.2587364572919905, -0.11084827082604169, 0.14112509915194824, 0.00961548192705959... |
710.0314 | Charm Meson Spectroscopy at Babar and CLEO-C | In this mini-review we report on the most recent progress in charm meson
spectroscopy. We discuss the precision measurements performed by the BaBar and
CLEO-c experiments in the non strange charm meson part and we present the newly
discovered strange charmed meson excited states.
| hep-ex | in this minireview we report on the most recent progress in charm meson spectroscopy we discuss the precision measurements performed by the babar and cleoc experiments in the non strange charm meson part and we present the newly discovered strange charmed meson excited states | [['in', 'this', 'minireview', 'we', 'report', 'on', 'the', 'most', 'recent', 'progress', 'in', 'charm', 'meson', 'spectroscopy', 'we', 'discuss', 'the', 'precision', 'measurements', 'performed', 'by', 'the', 'babar', 'and', 'cleoc', 'experiments', 'in', 'the', 'non', 'strange', 'charm', 'meson', 'part', 'and', 'we', 'p... | [-0.06925497629510408, 0.26671658286464994, -0.1172519843305715, 0.10006253809445877, -0.06579073797911406, -0.07030454612421719, 0.16963364972881126, 0.2988717067478733, -0.12347131661954336, -0.17628789233938072, -0.04436825733070939, -0.45971413191661914, -0.01238091764124957, 0.11182633361948485, 0.0914920085025104... |
710.0315 | Conservation laws and scattering for de Sitter classical particles | Starting from an intrinsic geometric characterization of de Sitter timelike
and lightlike geodesics we give a new description of the conserved quantities
associated with classical free particles on the de Sitter manifold. These
quantities allow for a natural discussion of classical pointlike scattering and
decay proc... | hep-th | starting from an intrinsic geometric characterization of de sitter timelike and lightlike geodesics we give a new description of the conserved quantities associated with classical free particles on the de sitter manifold these quantities allow for a natural discussion of classical pointlike scattering and decay process... | [['starting', 'from', 'an', 'intrinsic', 'geometric', 'characterization', 'of', 'de', 'sitter', 'timelike', 'and', 'lightlike', 'geodesics', 'we', 'give', 'a', 'new', 'description', 'of', 'the', 'conserved', 'quantities', 'associated', 'with', 'classical', 'free', 'particles', 'on', 'the', 'de', 'sitter', 'manifold', '... | [-0.14872333104722202, 0.15778888876411656, -0.1675257244729437, 0.13568727429956198, -0.09087259410880506, -0.0939064466394484, -0.03993967946153134, 0.3020372884348035, -0.2092071384366136, -0.2677126180380583, 0.03962270449701464, -0.26773053890792653, -0.11968703510356135, 0.19742782312241616, -0.05838884098557173,... |
710.0316 | Hamiltonian approach to Coulomb gauge Yang-Mills Theory | The vacuum wave functional of Coulomb gauge Yang-Mills theory is determined
within the variational principle and used to calculate various Green functions
and observables. The results show that heavy quarks are confined by a linearly
rising potential and gluons cannot propagate over large distances. The 't Hooft
loop... | hep-th hep-lat hep-ph | the vacuum wave functional of coulomb gauge yangmills theory is determined within the variational principle and used to calculate various green functions and observables the results show that heavy quarks are confined by a linearly rising potential and gluons cannot propagate over large distances the t hooft loop shows... | [['the', 'vacuum', 'wave', 'functional', 'of', 'coulomb', 'gauge', 'yangmills', 'theory', 'is', 'determined', 'within', 'the', 'variational', 'principle', 'and', 'used', 'to', 'calculate', 'various', 'green', 'functions', 'and', 'observables', 'the', 'results', 'show', 'that', 'heavy', 'quarks', 'are', 'confined', 'by'... | [-0.1079575231957153, 0.2913859180608315, -0.10722622021647363, 0.1357698795277272, -0.022160673325335414, -0.11444277830967872, 0.034857887877071086, 0.36520636682238045, -0.22304525871857486, -0.2412574354896386, -0.0008365231855162259, -0.2758773710450222, -0.10188944518951507, 0.12880637541670223, 0.013662979436299... |
710.0317 | A General Strategy for Physics-Based Model Validation Illustrated with
Earthquake Phenomenology, Atmospheric Radiative Transfer, and Computational
Fluid Dynamics | Validation is often defined as the process of determining the degree to which
a model is an accurate representation of the real world from the perspective of
its intended uses. Validation is crucial as industries and governments depend
increasingly on predictions by computer models to justify their decisions. In
this... | physics.comp-ph astro-ph.EP cond-mat.mtrl-sci physics.ao-ph physics.data-an physics.flu-dyn physics.geo-ph quant-ph | validation is often defined as the process of determining the degree to which a model is an accurate representation of the real world from the perspective of its intended uses validation is crucial as industries and governments depend increasingly on predictions by computer models to justify their decisions in this art... | [['validation', 'is', 'often', 'defined', 'as', 'the', 'process', 'of', 'determining', 'the', 'degree', 'to', 'which', 'a', 'model', 'is', 'an', 'accurate', 'representation', 'of', 'the', 'real', 'world', 'from', 'the', 'perspective', 'of', 'its', 'intended', 'uses', 'validation', 'is', 'crucial', 'as', 'industries', '... | [-0.030998447883586563, 0.043355150716995604, -0.08252952630613364, 0.05029284537683684, -0.08677227361830792, -0.08801867406011797, 0.05486272790094874, 0.31396727683205233, -0.2472769479933834, -0.34652923041333755, 0.08085887376127728, -0.2586907602335308, -0.19719460386207657, 0.2004724818679011, -0.113906021814282... |
710.0318 | Fast minimum-weight double-tree shortcutting for Metric TSP: Is the best
one good enough? | The Metric Traveling Salesman Problem (TSP) is a classical NP-hard
optimization problem. The double-tree shortcutting method for Metric TSP yields
an exponentially-sized space of TSP tours, each of which approximates the
optimal solution within at most a factor of 2. We consider the problem of
finding among these tou... | cs.DS cs.CC | the metric traveling salesman problem tsp is a classical nphard optimization problem the doubletree shortcutting method for metric tsp yields an exponentiallysized space of tsp tours each of which approximates the optimal solution within at most a factor of 2 we consider the problem of finding among these tours the one... | [['the', 'metric', 'traveling', 'salesman', 'problem', 'tsp', 'is', 'a', 'classical', 'nphard', 'optimization', 'problem', 'the', 'doubletree', 'shortcutting', 'method', 'for', 'metric', 'tsp', 'yields', 'an', 'exponentiallysized', 'space', 'of', 'tsp', 'tours', 'each', 'of', 'which', 'approximates', 'the', 'optimal', ... | [-0.14378181805916349, 0.014514797129284048, -0.035397122553214914, 0.058421218989940446, -0.08373631599657481, -0.17160358919695118, 0.0849473322954735, 0.34061160163034754, -0.264213056051708, -0.3865720511785422, 0.06489887504626882, -0.2891237009758947, -0.17010316200359585, 0.17137522380677314, -0.0772163415201361... |
710.0319 | Young and Massive Binary Progenitors of Type Ia Supernovae and Their
Circumstellar Matter | We present new evolutionary models for Type Ia supernova (SN Ia) progenitors,
introducing mass-stripping effect on a main-sequence (MS) or slightly evolved
companion star by winds from a mass-accreting white dwarf (WD). The
mass-stripping attenuates the rate of mass transfer from the companion to the
WD. As a result,... | astro-ph | we present new evolutionary models for type ia supernova sn ia progenitors introducing massstripping effect on a mainsequence ms or slightly evolved companion star by winds from a massaccreting white dwarf wd the massstripping attenuates the rate of mass transfer from the companion to the wd as a result quite a massive... | [['we', 'present', 'new', 'evolutionary', 'models', 'for', 'type', 'ia', 'supernova', 'sn', 'ia', 'progenitors', 'introducing', 'massstripping', 'effect', 'on', 'a', 'mainsequence', 'ms', 'or', 'slightly', 'evolved', 'companion', 'star', 'by', 'winds', 'from', 'a', 'massaccreting', 'white', 'dwarf', 'wd', 'the', 'masss... | [-0.07714367233163956, 0.09770282720978919, -0.025610759887921133, 0.15079853657786688, -0.1784763017827741, -0.1153684292785516, 0.13431761355364946, 0.37346811047227113, -0.14531748187872245, -0.29335549796845034, 0.029989366413012492, -0.2749328779959187, -0.00015839055473388164, 0.20495222196626217, -0.093964136403... |
710.032 | Manipulation with Andreev states in spin active mesoscopic Josephson
junctions | We investigate manipulation with Andreev bound states in Josephson quantum
point contacts with magnetic scattering. Rabi oscillations in the two-level
Andreev subsystems are excited by resonant driving the direction of magnetic
moment of the scatterer, and by modulating the superconducting phase difference
across the... | cond-mat.supr-con | we investigate manipulation with andreev bound states in josephson quantum point contacts with magnetic scattering rabi oscillations in the twolevel andreev subsystems are excited by resonant driving the direction of magnetic moment of the scatterer and by modulating the superconducting phase difference across the cont... | [['we', 'investigate', 'manipulation', 'with', 'andreev', 'bound', 'states', 'in', 'josephson', 'quantum', 'point', 'contacts', 'with', 'magnetic', 'scattering', 'rabi', 'oscillations', 'in', 'the', 'twolevel', 'andreev', 'subsystems', 'are', 'excited', 'by', 'resonant', 'driving', 'the', 'direction', 'of', 'magnetic',... | [-0.2769639810385264, 0.28101795312908034, -0.008913202211260796, 0.04133685860155231, -0.023963883308612783, -0.15804651122054328, 0.14920820920252362, 0.34433684795285047, -0.23368608975863975, -0.3112397862421146, -0.04742779280362732, -0.30016715903968916, -0.1029948193984835, 0.20435106843386008, 0.055277735903687... |
710.0321 | Wobbling excitations at high spins in A~160 | We found that in 156Dy and 162Yb the lowest odd spin gamma-vibrational states
transform to the wobbling excitations after the backbending, associated with
the transition from axially-symmetric to nonaxial shapes. The analysis of
quadrupole electric transitions determines uniquely the sign of the
gamma-deformation in ... | nucl-th nucl-ex | we found that in 156dy and 162yb the lowest odd spin gammavibrational states transform to the wobbling excitations after the backbending associated with the transition from axiallysymmetric to nonaxial shapes the analysis of quadrupole electric transitions determines uniquely the sign of the gammadeformation in both nu... | [['we', 'found', 'that', 'in', '156dy', 'and', '162yb', 'the', 'lowest', 'odd', 'spin', 'gammavibrational', 'states', 'transform', 'to', 'the', 'wobbling', 'excitations', 'after', 'the', 'backbending', 'associated', 'with', 'the', 'transition', 'from', 'axiallysymmetric', 'to', 'nonaxial', 'shapes', 'the', 'analysis', ... | [-0.12140294577926397, 0.23736804248765112, -0.056675720177590844, 0.08934149162843824, 0.01579815357690677, -0.08222561158239841, 0.03248966131359339, 0.3564449567347765, -0.2063706736639142, -0.24940760761499406, -0.014595972201786935, -0.31464313570410013, -0.11251755243167282, 0.08092759821563959, 0.074536560773849... |
710.0322 | Identification of the Isotherm Function in Chromatography Using CMA-ES | This paper deals with the identification of the flux for a system of
conservation laws in the specific example of analytic chromatography. The
fundamental equations of chromatographic process are highly non linear. The
state-of-the-art Evolution Strategy, CMA-ES (the Covariance Matrix Adaptation
Evolution Strategy), ... | math.OC math.NA | this paper deals with the identification of the flux for a system of conservation laws in the specific example of analytic chromatography the fundamental equations of chromatographic process are highly non linear the stateoftheart evolution strategy cmaes the covariance matrix adaptation evolution strategy is used to i... | [['this', 'paper', 'deals', 'with', 'the', 'identification', 'of', 'the', 'flux', 'for', 'a', 'system', 'of', 'conservation', 'laws', 'in', 'the', 'specific', 'example', 'of', 'analytic', 'chromatography', 'the', 'fundamental', 'equations', 'of', 'chromatographic', 'process', 'are', 'highly', 'non', 'linear', 'the', 's... | [-0.08405420935334085, 0.02921735045274945, -0.10394328418328519, 0.046164496755199465, -0.05006986607766741, -0.13927458450300517, 0.006286278857010325, 0.3613528086097686, -0.2583586283406795, -0.3092817412689328, 0.14769404888495927, -0.2694473806922171, -0.14188867165952676, 0.2045491743029433, -0.02750268479256512... |
710.0323 | A Dual Algorithm for Non-abelian Yang-Mills coupled to Dynamical
Fermions | We extend the dual algorithm recently described for pure, non-abelian
Yang-Mills on the lattice to the case of lattice fermions coupled to
Yang-Mills, by constructing an ergodic Metropolis algorithm for dynamic
fermions that is local, exact, and built from gauge-invariant boson-fermion
coupled configurations. For con... | hep-lat | we extend the dual algorithm recently described for pure nonabelian yangmills on the lattice to the case of lattice fermions coupled to yangmills by constructing an ergodic metropolis algorithm for dynamic fermions that is local exact and built from gaugeinvariant bosonfermion coupled configurations for concreteness we... | [['we', 'extend', 'the', 'dual', 'algorithm', 'recently', 'described', 'for', 'pure', 'nonabelian', 'yangmills', 'on', 'the', 'lattice', 'to', 'the', 'case', 'of', 'lattice', 'fermions', 'coupled', 'to', 'yangmills', 'by', 'constructing', 'an', 'ergodic', 'metropolis', 'algorithm', 'for', 'dynamic', 'fermions', 'that',... | [-0.09577049834638082, 0.18637026816387875, -0.05632350059077457, 0.043113603301643696, -0.06578034227087844, -0.1551517058093445, 0.03205806530910317, 0.3729738209146161, -0.15820710307785443, -0.2438328845129043, 0.09324617397544921, -0.24414694755330307, -0.16196619531926268, 0.1421223787293464, -0.01541617184000856... |
710.0324 | The emission line spectrum of the UV deficient quasar Ton 34: evidence
of shock excitation? | Emission lines in quasars are believed to originate from a photoionized
plasma. There are, however, some emission features which appear to be
collisionally excited, such as the FeII multiplet bands. Shortward of Ly_alpha,
there also are a few permitted lines of species from low to intermediate
ionization. Ton 34 (z=1... | astro-ph | emission lines in quasars are believed to originate from a photoionized plasma there are however some emission features which appear to be collisionally excited such as the feii multiplet bands shortward of ly_alpha there also are a few permitted lines of species from low to intermediate ionization ton 34 z1928 exhibit... | [['emission', 'lines', 'in', 'quasars', 'are', 'believed', 'to', 'originate', 'from', 'a', 'photoionized', 'plasma', 'there', 'are', 'however', 'some', 'emission', 'features', 'which', 'appear', 'to', 'be', 'collisionally', 'excited', 'such', 'as', 'the', 'feii', 'multiplet', 'bands', 'shortward', 'of', 'ly_alpha', 'th... | [-0.020223908022435455, 0.1125828581684569, 0.0034348512447233926, 0.09200625359948914, -0.04336875252094183, -0.17769274636471677, 0.04546044413579133, 0.5024926953943772, -0.1541924328427488, -0.3438201252687433, 0.007093184886074041, -0.33825535483600433, 0.02374869623723128, 0.16660929705137334, 0.0196468458842423,... |
710.0325 | Structure of Mass Gap between Two Spin Multiplets | Studying our semirelativistic potential model and the numerical results,
which succeeds in predicting and reproducing recently discovered higher
resonances of $D$, $D_s$, $B$, and $B_s$, we find a simple expression for the
mass gap between two spin multiplets of heavy-light mesons, $(0^-,1^-)$ and
$(0^+,1^+)$. The ma... | hep-ph | studying our semirelativistic potential model and the numerical results which succeeds in predicting and reproducing recently discovered higher resonances of d d_s b and b_s we find a simple expression for the mass gap between two spin multiplets of heavylight mesons 01 and 01 the mass gap between chiral partners defin... | [['studying', 'our', 'semirelativistic', 'potential', 'model', 'and', 'the', 'numerical', 'results', 'which', 'succeeds', 'in', 'predicting', 'and', 'reproducing', 'recently', 'discovered', 'higher', 'resonances', 'of', 'd', 'd_s', 'b', 'and', 'b_s', 'we', 'find', 'a', 'simple', 'expression', 'for', 'the', 'mass', 'gap... | [-0.09526236498242487, 0.28329991438102137, -0.04085644408250633, 0.13642994133330397, 0.005809531007316369, -0.1755826816165253, 0.09841742097683574, 0.3040787423758403, -0.14634493054093226, -0.29119702214780063, -0.06257155510272992, -0.33981019493354403, -0.008976545719348866, 0.0962783394806573, 0.0809879463570921... |
710.0326 | On Orbits of the Ring $Z_n^m$ under the Action of the Group $SL(m,Z_n)$ | We consider the action of the finite matrix group $SL(m,Z_n)$ on the ring
$Z_n^m$. We determine orbits of this action for n arbitrary natural number. It
is a generalization of the task which was studied by A.A. Kirillov for $m=2$
and $n$ prime number.
| math.GR math-ph math.MP | we consider the action of the finite matrix group slmz_n on the ring z_nm we determine orbits of this action for n arbitrary natural number it is a generalization of the task which was studied by aa kirillov for m2 and n prime number | [['we', 'consider', 'the', 'action', 'of', 'the', 'finite', 'matrix', 'group', 'slmz_n', 'on', 'the', 'ring', 'z_nm', 'we', 'determine', 'orbits', 'of', 'this', 'action', 'for', 'n', 'arbitrary', 'natural', 'number', 'it', 'is', 'a', 'generalization', 'of', 'the', 'task', 'which', 'was', 'studied', 'by', 'aa', 'kirillo... | [-0.21368555356423521, 0.13577121329428846, -0.029130886590411496, 0.0364058647131504, -0.03709044903083596, -0.1227651048386686, -0.020706441946500957, 0.33235664626713407, -0.22866555013109086, -0.3142413702728443, 0.06780450226235485, -0.22899057438900305, -0.127064180820314, 0.1689355947553765, -0.08520741624281157... |
710.0327 | Similar final states from different initial states using new exact
solutions of relativistic hydrodynamics | We present exact, analytic and simple solutions of relativistic perfect fluid
hydrodynamics. The solutions allow us to calculate the rapidity distribution of
the particles produced at the freeze-out, and fit them to the measured rapidity
distribution data. We also give an advanced estimation of the energy density
rea... | nucl-th | we present exact analytic and simple solutions of relativistic perfect fluid hydrodynamics the solutions allow us to calculate the rapidity distribution of the particles produced at the freezeout and fit them to the measured rapidity distribution data we also give an advanced estimation of the energy density reached in... | [['we', 'present', 'exact', 'analytic', 'and', 'simple', 'solutions', 'of', 'relativistic', 'perfect', 'fluid', 'hydrodynamics', 'the', 'solutions', 'allow', 'us', 'to', 'calculate', 'the', 'rapidity', 'distribution', 'of', 'the', 'particles', 'produced', 'at', 'the', 'freezeout', 'and', 'fit', 'them', 'to', 'the', 'me... | [-0.07305920673834701, 0.12454162437080091, -0.19289636830170262, 0.11369328461812749, 0.012479252076797908, -0.09135078125813555, -0.01858545823638598, 0.31628241618314096, -0.2241758207580255, -0.320627681880949, -0.00998958441496436, -0.3096781784308053, 0.08367637209519144, 0.11114651670739535, 0.016897200877147335... |
710.0328 | Hyperplane Arrangements with Large Average Diameter | The largest possible average diameter of a bounded cell of a simple
hyperplane arrangement is conjectured to be not greater than the dimension. We
prove that this conjecture holds in dimension 2, and is asymptotically tight in
fixed dimension. We give the exact value of the largest possible average
diameter for all s... | math.MG | the largest possible average diameter of a bounded cell of a simple hyperplane arrangement is conjectured to be not greater than the dimension we prove that this conjecture holds in dimension 2 and is asymptotically tight in fixed dimension we give the exact value of the largest possible average diameter for all simple... | [['the', 'largest', 'possible', 'average', 'diameter', 'of', 'a', 'bounded', 'cell', 'of', 'a', 'simple', 'hyperplane', 'arrangement', 'is', 'conjectured', 'to', 'be', 'not', 'greater', 'than', 'the', 'dimension', 'we', 'prove', 'that', 'this', 'conjecture', 'holds', 'in', 'dimension', '2', 'and', 'is', 'asymptotically... | [-0.15290496716656352, 0.13722440657476265, 0.009424428705887129, 0.05057124060363338, -0.014456471105316473, -0.19688452138335152, 0.013116395446441827, 0.33299013067998234, -0.17424322648339413, -0.2706207787838354, 0.11263745473772888, -0.2865410001863355, -0.10973297888713499, 0.17348669902972316, -0.06376384883638... |
710.0329 | Light quark masses and pseudoscalar decay constants from Nf=2 twisted
mass QCD | We present the results of the lattice QCD calculation of the average up-down
and strange quark masses and of the light meson pseudoscalar decay constants,
recently performed with Nf=2 dynamical fermions by the ETM Collaboration. The
simulation is carried out at a single value of the lattice spacing with the
twisted m... | hep-lat hep-ph | we present the results of the lattice qcd calculation of the average updown and strange quark masses and of the light meson pseudoscalar decay constants recently performed with nf2 dynamical fermions by the etm collaboration the simulation is carried out at a single value of the lattice spacing with the twisted mass fe... | [['we', 'present', 'the', 'results', 'of', 'the', 'lattice', 'qcd', 'calculation', 'of', 'the', 'average', 'updown', 'and', 'strange', 'quark', 'masses', 'and', 'of', 'the', 'light', 'meson', 'pseudoscalar', 'decay', 'constants', 'recently', 'performed', 'with', 'nf2', 'dynamical', 'fermions', 'by', 'the', 'etm', 'coll... | [-0.07782741893577028, 0.299131696782436, -0.07497332851421468, 0.06305597836253088, 0.0021820138479807876, -0.10444333695182513, 0.15388239406328014, 0.32183269061604325, -0.14515111457277724, -0.29258029384627227, 0.013963650027448374, -0.34293033695798747, 0.0317708041754925, 0.12011336851674988, 0.09398490657959035... |
710.033 | Singular cohomology of the analytic Milnor fiber, and mixed Hodge
structure on the nearby cohomology | We constructed the analytic Milnor fiber is a non-archimedean model of the
classical topological Milnor fibration. In the present paper, we describe the
homotopy type of the analytic Milnor fiber in terms of a strictly semi-stable
model, and we show that its singular cohomology coincides with the weight zero
part of ... | math.AG | we constructed the analytic milnor fiber is a nonarchimedean model of the classical topological milnor fibration in the present paper we describe the homotopy type of the analytic milnor fiber in terms of a strictly semistable model and we show that its singular cohomology coincides with the weight zero part of the mix... | [['we', 'constructed', 'the', 'analytic', 'milnor', 'fiber', 'is', 'a', 'nonarchimedean', 'model', 'of', 'the', 'classical', 'topological', 'milnor', 'fibration', 'in', 'the', 'present', 'paper', 'we', 'describe', 'the', 'homotopy', 'type', 'of', 'the', 'analytic', 'milnor', 'fiber', 'in', 'terms', 'of', 'a', 'strictly... | [-0.2756924697030813, -0.023679328891329277, -0.16969822896405673, 0.07871540321353585, -0.08117946681494896, -0.1355421518942771, -0.01608305979812613, 0.2617499052714079, -0.31174162452897203, -0.12646599362293878, 0.06317467178898649, -0.19591634835188204, -0.2323150746524334, 0.17710138350211752, -0.213559645204207... |
710.0331 | The strength of crystalline color superconductors | We present a study of the shear modulus of the crystalline color
superconducting phase of quark matter, showing that this phase of dense, but
not asymptotically dense, quark matter responds to shear stress as a very rigid
solid. This phase is characterized by a gap parameter $\Delta$ that is
periodically modulated in... | hep-ph astro-ph cond-mat.supr-con gr-qc nucl-th | we present a study of the shear modulus of the crystalline color superconducting phase of quark matter showing that this phase of dense but not asymptotically dense quark matter responds to shear stress as a very rigid solid this phase is characterized by a gap parameter delta that is periodically modulated in space an... | [['we', 'present', 'a', 'study', 'of', 'the', 'shear', 'modulus', 'of', 'the', 'crystalline', 'color', 'superconducting', 'phase', 'of', 'quark', 'matter', 'showing', 'that', 'this', 'phase', 'of', 'dense', 'but', 'not', 'asymptotically', 'dense', 'quark', 'matter', 'responds', 'to', 'shear', 'stress', 'as', 'a', 'very... | [-0.15859155501778327, 0.2820405139262909, -0.1125588220995351, 0.049036368051554355, -0.08797891484310398, -0.058804928719744846, 0.06448385777414939, 0.3582520709073139, -0.25000373392870995, -0.28505785386525306, 0.05563839497426156, -0.23680715832206825, -0.09967221301785634, 0.1494956140361705, -0.0026324062902838... |
710.0332 | (3+1)-Dimensional Hydrodynamic Expansion with a Critical Point from
Realistic Initial Conditions | We investigate a (3+1)-dimensional hydrodynamic expansion of the hot and
dense system created in head-on collisions of Pb+Pb/Au+Au at beam energies from
$5-200A$ GeV. An equation of state that incorporates a critical end point (CEP)
in line with the lattice data is used. The necessary initial conditions for the
hydro... | nucl-th | we investigate a 31dimensional hydrodynamic expansion of the hot and dense system created in headon collisions of pbpbauau at beam energies from 5200a gev an equation of state that incorporates a critical end point cep in line with the lattice data is used the necessary initial conditions for the hydrodynamic evolution... | [['we', 'investigate', 'a', '31dimensional', 'hydrodynamic', 'expansion', 'of', 'the', 'hot', 'and', 'dense', 'system', 'created', 'in', 'headon', 'collisions', 'of', 'pbpbauau', 'at', 'beam', 'energies', 'from', '5200a', 'gev', 'an', 'equation', 'of', 'state', 'that', 'incorporates', 'a', 'critical', 'end', 'point', '... | [-0.12990320949948259, 0.14025398577255796, -0.15305259768185872, 0.057460438051660144, -0.0019616182853600807, -0.08326761616660015, 0.03420601483101823, 0.3384253301604518, -0.23695721151041133, -0.2578313845821789, 0.062135269033190395, -0.2964284541138581, -0.03780063119983035, 0.16266397650486655, 0.04691614001856... |
710.0333 | Symmetry Breaking Patterns for the Little Higgs from Strong Dynamics | We show how the symmetry breaking pattern of the simplest little Higgs model,
and that of the smallest moose model that incorporates an approximate custodial
SU(2), can be realized through the condensation of strongly coupled fermions.
In each case a custodial SU(2) symmetry of the new strong dynamics limits the
size... | hep-ph | we show how the symmetry breaking pattern of the simplest little higgs model and that of the smallest moose model that incorporates an approximate custodial su2 can be realized through the condensation of strongly coupled fermions in each case a custodial su2 symmetry of the new strong dynamics limits the sizes of corr... | [['we', 'show', 'how', 'the', 'symmetry', 'breaking', 'pattern', 'of', 'the', 'simplest', 'little', 'higgs', 'model', 'and', 'that', 'of', 'the', 'smallest', 'moose', 'model', 'that', 'incorporates', 'an', 'approximate', 'custodial', 'su2', 'can', 'be', 'realized', 'through', 'the', 'condensation', 'of', 'strongly', 'c... | [-0.11746776992894285, 0.22163855405623753, -0.03562170528329727, 0.12366915718326724, -0.07709905674787072, -0.1790608949959278, -0.00015307166679891023, 0.3133175084670264, -0.22607641303306067, -0.2803738284250343, 0.060705452056684935, -0.2593000559363423, -0.10102093947589458, 0.09474429534748197, 0.02301323338131... |
710.0334 | Holographic vector mesons from spectral functions at finite baryon or
isospin density | We consider gauge/gravity duality with flavor for the finite-temperature
field theory dual of the AdS-Schwarzschild black hole background with embedded
D7-brane probes. In particular, we investigate spectral functions at finite
baryon density in the black hole phase. We determine the resonance frequencies
correspondi... | hep-th hep-ph nucl-th | we consider gaugegravity duality with flavor for the finitetemperature field theory dual of the adsschwarzschild black hole background with embedded d7brane probes in particular we investigate spectral functions at finite baryon density in the black hole phase we determine the resonance frequencies corresponding to mes... | [['we', 'consider', 'gaugegravity', 'duality', 'with', 'flavor', 'for', 'the', 'finitetemperature', 'field', 'theory', 'dual', 'of', 'the', 'adsschwarzschild', 'black', 'hole', 'background', 'with', 'embedded', 'd7brane', 'probes', 'in', 'particular', 'we', 'investigate', 'spectral', 'functions', 'at', 'finite', 'baryo... | [-0.10029862397322817, 0.22377672815702637, -0.0817109513338986, 0.10728068469221753, -0.024852657012817775, -0.11244708214219681, 0.07360739398888208, 0.3588348559789999, -0.18168768409078875, -0.25112775490569644, 0.0083032911602055, -0.29298066990394916, -0.021430091976373078, 0.09825320597242057, 0.0535788817238028... |
710.0335 | Long term monitoring of the BHC 1E 1740.7-2942 | The microquasar 1E 1740.7-2942 is one of the most appealing source of the
Galactic Centre region. The high energy feature detected once by SIGMA has been
searched in the last years by INTEGRAL, but never confirmed. Classified as a
persistent source, on 2004 it showed a quiescent-like state. In fact for few
month 1E 1... | astro-ph | the microquasar 1e 174072942 is one of the most appealing source of the galactic centre region the high energy feature detected once by sigma has been searched in the last years by integral but never confirmed classified as a persistent source on 2004 it showed a quiescentlike state in fact for few month 1e 174072942 w... | [['the', 'microquasar', '1e', '174072942', 'is', 'one', 'of', 'the', 'most', 'appealing', 'source', 'of', 'the', 'galactic', 'centre', 'region', 'the', 'high', 'energy', 'feature', 'detected', 'once', 'by', 'sigma', 'has', 'been', 'searched', 'in', 'the', 'last', 'years', 'by', 'integral', 'but', 'never', 'confirmed', ... | [-0.09603197405654514, 0.058404029352294114, -0.07299461321037432, 0.11964206535512031, -0.08191691383465448, -0.1294644733742726, 0.05784183025984517, 0.41626000484790315, -0.19708819250412157, -0.37540476424345054, 0.17348426285025198, -0.30309681518172676, -0.06458659510297532, 0.23155616580730898, -0.03964413757818... |
710.0336 | Flavor Symmetry and Charm Decays | A wealth of new data in charmed particle physics allows the testing of flavor
symmetry and the extraction of key amplitudes. Information on relative strong
phases is obtained.
| hep-ph | a wealth of new data in charmed particle physics allows the testing of flavor symmetry and the extraction of key amplitudes information on relative strong phases is obtained | [['a', 'wealth', 'of', 'new', 'data', 'in', 'charmed', 'particle', 'physics', 'allows', 'the', 'testing', 'of', 'flavor', 'symmetry', 'and', 'the', 'extraction', 'of', 'key', 'amplitudes', 'information', 'on', 'relative', 'strong', 'phases', 'is', 'obtained']] | [-0.1142550192640296, 0.18387764266559056, -0.11723029134528977, 0.11516766149101645, -0.07994955202697643, -0.139490404249435, 0.08564255133803401, 0.25893242763621466, -0.24240262327449663, -0.3027896599045822, 0.03638186440054726, -0.2760080668631417, -0.00026903022080659866, 0.16271441212406249, 0.00772945406580609... |
710.0337 | Graphs on Surfaces and the Partition Function of String Theory | Graphs on surfaces is an active topic of pure mathematics belonging to graph
theory. It has also been applied to physics and relates discrete and continuous
mathematics. In this paper we present a formal mathematical description of the
relation between graph theory and the mathematical physics of discrete string
theo... | math-ph hep-th math.CO math.MP | graphs on surfaces is an active topic of pure mathematics belonging to graph theory it has also been applied to physics and relates discrete and continuous mathematics in this paper we present a formal mathematical description of the relation between graph theory and the mathematical physics of discrete string theory i... | [['graphs', 'on', 'surfaces', 'is', 'an', 'active', 'topic', 'of', 'pure', 'mathematics', 'belonging', 'to', 'graph', 'theory', 'it', 'has', 'also', 'been', 'applied', 'to', 'physics', 'and', 'relates', 'discrete', 'and', 'continuous', 'mathematics', 'in', 'this', 'paper', 'we', 'present', 'a', 'formal', 'mathematical'... | [-0.10470523083566037, 0.06713579891748424, -0.12235791767963859, 0.11205732260379463, -0.10596908441001954, -0.08970534512479543, 0.039789739798391816, 0.3384561611182856, -0.26968683777425945, -0.306016686092238, 0.073708649959613, -0.2475722547892514, -0.21186603706503138, 0.19580561260433157, -0.09684951545475401, ... |
710.0338 | High-temperature expansions through order 24 for the two-dimensional
classical XY model on the square lattice | The high-temperature expansion of the spin-spin correlation function of the
two-dimensional classical XY (planar rotator) model on the square lattice is
extended by three terms, from order 21 through order 24, and analyzed to
improve the estimates of the critical parameters.
| hep-lat cond-mat.stat-mech | the hightemperature expansion of the spinspin correlation function of the twodimensional classical xy planar rotator model on the square lattice is extended by three terms from order 21 through order 24 and analyzed to improve the estimates of the critical parameters | [['the', 'hightemperature', 'expansion', 'of', 'the', 'spinspin', 'correlation', 'function', 'of', 'the', 'twodimensional', 'classical', 'xy', 'planar', 'rotator', 'model', 'on', 'the', 'square', 'lattice', 'is', 'extended', 'by', 'three', 'terms', 'from', 'order', '21', 'through', 'order', '24', 'and', 'analyzed', 'to... | [-0.0978719902383845, 0.13480382008341754, 0.0036345597174836366, 0.04934960396153989, -0.007921068134104333, -0.057538267951913, 0.024227838236384275, 0.3197719467940127, -0.23503046975720945, -0.27887961704556535, 0.1468336324508461, -0.3177532210219197, -0.13730910543079783, 0.16810194266074133, 0.10620058946476159,... |
710.0339 | VLA Limits for Intermediate Mass Black Holes in Three Globular Clusters | The observational evidence for central black holes in globular clusters has
been argued extensively, and their existence has important consequences for
both the formation and evolution of the cluster. Most of the evidence comes
from dynamical arguments, but the interpretation is difficult, given the short
relaxation ... | astro-ph | the observational evidence for central black holes in globular clusters has been argued extensively and their existence has important consequences for both the formation and evolution of the cluster most of the evidence comes from dynamical arguments but the interpretation is difficult given the short relaxation times ... | [['the', 'observational', 'evidence', 'for', 'central', 'black', 'holes', 'in', 'globular', 'clusters', 'has', 'been', 'argued', 'extensively', 'and', 'their', 'existence', 'has', 'important', 'consequences', 'for', 'both', 'the', 'formation', 'and', 'evolution', 'of', 'the', 'cluster', 'most', 'of', 'the', 'evidence',... | [-0.09632293571455709, 0.06429364140195823, -0.08517987696403587, 0.15559141359817413, -0.06008318261985944, -0.06654752860226468, 0.07815053050226935, 0.3782893625981602, -0.14240058000684036, -0.35751979331158706, 0.1259978195680683, -0.2970072662755155, -0.0397605770519255, 0.2065062120893492, 0.0006013500071177888,... |
710.034 | Di-photon Higgs decay in the MSSM with explicit CP violation | The Minimal Supersymmetric Standard Model (MSSM) with explicit CP violation
is studied with the help of the di-photon decay channel of the lightest neutral
Higgs boson. Effects of CP violation, entering via the scalar/pseudo-scalar
mixing at higher order as well as through the Higgs-sfermion-sfermion couplings
at tre... | hep-ph | the minimal supersymmetric standard model mssm with explicit cp violation is studied with the help of the diphoton decay channel of the lightest neutral higgs boson effects of cp violation entering via the scalarpseudoscalar mixing at higher order as well as through the higgssfermionsfermion couplings at treelevel are ... | [['the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'with', 'explicit', 'cp', 'violation', 'is', 'studied', 'with', 'the', 'help', 'of', 'the', 'diphoton', 'decay', 'channel', 'of', 'the', 'lightest', 'neutral', 'higgs', 'boson', 'effects', 'of', 'cp', 'violation', 'entering', 'via', 'the', 'scalarpseudo... | [-0.08509734634814474, 0.31749941875112425, 0.009007830573082493, 0.15399751953508825, -0.09878640953990582, -0.21720774313680044, 0.1117739255556412, 0.32171355780794103, -0.211667740737954, -0.29182927401965125, 0.05926369571151506, -0.27680268877169545, 0.0007363646332043828, 0.12531254455046892, 0.06700447851203774... |
710.0341 | An iterative method to compute the overlap Dirac operator at nonzero
chemical potential | The overlap Dirac operator at nonzero quark chemical potential involves the
computation of the sign function of a non-Hermitian matrix. In this talk we
present an iterative method, first proposed by us in Ref. [1], which allows for
an efficient computation of the operator, even on large lattices. The starting
point i... | hep-lat | the overlap dirac operator at nonzero quark chemical potential involves the computation of the sign function of a nonhermitian matrix in this talk we present an iterative method first proposed by us in ref 1 which allows for an efficient computation of the operator even on large lattices the starting point is a krylov ... | [['the', 'overlap', 'dirac', 'operator', 'at', 'nonzero', 'quark', 'chemical', 'potential', 'involves', 'the', 'computation', 'of', 'the', 'sign', 'function', 'of', 'a', 'nonhermitian', 'matrix', 'in', 'this', 'talk', 'we', 'present', 'an', 'iterative', 'method', 'first', 'proposed', 'by', 'us', 'in', 'ref', '1', 'whic... | [-0.12173065660784069, 0.07037337959422402, -0.09272408418249913, 0.025524930135221578, -0.05574178846421628, -0.1182939383896808, 0.05331592503129146, 0.35354637999971134, -0.2754245448069504, -0.24744319401753062, 0.08767381758885816, -0.2624422645216654, -0.18494047280938292, 0.14381796969339633, -0.0211695682623823... |
710.0342 | A Generalization of A Leibniz Geometrical Theorem | In this article we present a generalization of a Leibniz's geometrical
theorem and an application of it.
| math.GM | in this article we present a generalization of a leibnizs geometrical theorem and an application of it | [['in', 'this', 'article', 'we', 'present', 'a', 'generalization', 'of', 'a', 'leibnizs', 'geometrical', 'theorem', 'and', 'an', 'application', 'of', 'it']] | [-0.09626036783789887, -0.029473696964594315, -0.17991866682217839, 0.05939109028344426, -0.09726692670408417, -0.012526503983227646, 0.0866977921276189, 0.2703762050060665, -0.2616012302391669, -0.2643612630884437, 0.10926298873142942, -0.20191068552872715, -0.2842460835681242, 0.20044772315989523, -0.2084095721845241... |
710.0343 | Spin asymmetry at large x_F and k_T | We suggest that the large single spin asymmetries observed at high momentum
fractions x_F and transverse momenta k_T of the pion in p^\uparrow p ->
\pi(x_F,k_T)+X arise from the coherence of the soft interactions with the hard
parton scattering process. Such coherence can be maintained if x_F -> 1 as k_T
-> \infty, w... | hep-ph | we suggest that the large single spin asymmetries observed at high momentum fractions x_f and transverse momenta k_t of the pion in puparrow p pix_fk_tx arise from the coherence of the soft interactions with the hard parton scattering process such coherence can be maintained if x_f 1 as k_t infty while k_t21x_f lambda_... | [['we', 'suggest', 'that', 'the', 'large', 'single', 'spin', 'asymmetries', 'observed', 'at', 'high', 'momentum', 'fractions', 'x_f', 'and', 'transverse', 'momenta', 'k_t', 'of', 'the', 'pion', 'in', 'puparrow', 'p', 'pix_fk_tx', 'arise', 'from', 'the', 'coherence', 'of', 'the', 'soft', 'interactions', 'with', 'the', '... | [-0.13893491780677, 0.343418805041548, -0.14027751620089862, 0.14079386641223934, 0.0007456522787723577, -0.09413325859967506, 0.007253860532673019, 0.4067542922748911, -0.2784152261423643, -0.21401619984100412, -0.04507731485787327, -0.31157355800722586, 0.024846314255035286, 0.09947724415534975, 0.05428125866397162, ... |
710.0344 | SU(2) meets SU(3) in lattice-Landau-gauge gluon and ghost propagators | A comparative study of the lattice Landau gauge gluon and ghost propagators
for SU(2) and SU(3) pure Yang-Mills theories is carried out. The data were
specially produced with equivalent lattice parameters to allow for a careful
comparison of the two cases. We find very good agreement between the two
theories. Our res... | hep-lat | a comparative study of the lattice landau gauge gluon and ghost propagators for su2 and su3 pure yangmills theories is carried out the data were specially produced with equivalent lattice parameters to allow for a careful comparison of the two cases we find very good agreement between the two theories our results seem ... | [['a', 'comparative', 'study', 'of', 'the', 'lattice', 'landau', 'gauge', 'gluon', 'and', 'ghost', 'propagators', 'for', 'su2', 'and', 'su3', 'pure', 'yangmills', 'theories', 'is', 'carried', 'out', 'the', 'data', 'were', 'specially', 'produced', 'with', 'equivalent', 'lattice', 'parameters', 'to', 'allow', 'for', 'a',... | [-0.10642323009669781, 0.1795549670966076, -0.14574117693056385, 0.11019558593314806, -0.06398582376672753, -0.11537376283667981, 0.04272439189787422, 0.3967112787550182, -0.10397756903964495, -0.2502501411829144, 0.06584825762547553, -0.2890331705499973, -0.10764016968065075, 0.13715113426359105, 0.04037744167393872, ... |
710.0345 | Polar kicks and the spin period - eccentricity relation in double
neutron stars | We present results of a population synthesis study aimed at examining the
role of spin-kick alignment in producing a correlation between the spin period
of the first-born neutron star and the orbital eccentricity of observed double
neutron star binaries in the Galactic disk. We find spin-kick alignment to be
compatib... | astro-ph | we present results of a population synthesis study aimed at examining the role of spinkick alignment in producing a correlation between the spin period of the firstborn neutron star and the orbital eccentricity of observed double neutron star binaries in the galactic disk we find spinkick alignment to be compatible wit... | [['we', 'present', 'results', 'of', 'a', 'population', 'synthesis', 'study', 'aimed', 'at', 'examining', 'the', 'role', 'of', 'spinkick', 'alignment', 'in', 'producing', 'a', 'correlation', 'between', 'the', 'spin', 'period', 'of', 'the', 'firstborn', 'neutron', 'star', 'and', 'the', 'orbital', 'eccentricity', 'of', 'o... | [-0.15353530268117355, 0.1586649468222606, -0.06783897492130274, 0.08676379606586651, -0.09658799799955517, -0.04709582543000579, 0.07737151171697432, 0.35727531526683143, -0.19588395481443274, -0.34298460223320604, 0.04613183357287198, -0.24168988317926077, -0.06470038895191543, 0.19794341444840952, -0.017142713913505... |
710.0346 | Infrared structure of e+e- --> 3 jets at NNLO | We describe the calculation of the next-to-next-to-leading order (NNLO) QCD
corrections to three-jet production and related event shape observables in
electron-positron annihilation. Infrared singularities due to double real
radiation at tree level and single real radiation at one loop are subtracted
from the full QC... | hep-ph | we describe the calculation of the nexttonexttoleading order nnlo qcd corrections to threejet production and related event shape observables in electronpositron annihilation infrared singularities due to double real radiation at tree level and single real radiation at one loop are subtracted from the full qcd matrix el... | [['we', 'describe', 'the', 'calculation', 'of', 'the', 'nexttonexttoleading', 'order', 'nnlo', 'qcd', 'corrections', 'to', 'threejet', 'production', 'and', 'related', 'event', 'shape', 'observables', 'in', 'electronpositron', 'annihilation', 'infrared', 'singularities', 'due', 'to', 'double', 'real', 'radiation', 'at',... | [-0.06396411178175802, 0.11494466076495019, -0.11779185180094535, 0.14547544983669453, -0.05503097060925753, -0.06113591895565012, 0.0016599447186247018, 0.3865746694411767, -0.18609962055175486, -0.23122028006493286, 0.02715828129497576, -0.35032897403017793, -0.06845982173868155, 0.145239529140704, 0.0600342862981359... |
710.0347 | Staggered Diquarks for the Singly Heavy Baryons | In the staggered fermion formulation of lattice QCD, we construct diquark
operators to be embedded in singly heavy baryons. The group theoretical
connections between the continuum and lattice staggered diquark representations
are established.
| hep-lat | in the staggered fermion formulation of lattice qcd we construct diquark operators to be embedded in singly heavy baryons the group theoretical connections between the continuum and lattice staggered diquark representations are established | [['in', 'the', 'staggered', 'fermion', 'formulation', 'of', 'lattice', 'qcd', 'we', 'construct', 'diquark', 'operators', 'to', 'be', 'embedded', 'in', 'singly', 'heavy', 'baryons', 'the', 'group', 'theoretical', 'connections', 'between', 'the', 'continuum', 'and', 'lattice', 'staggered', 'diquark', 'representations', '... | [-0.11741577368229628, 0.3148351346961025, -0.08160908288802161, 0.13523817039800412, -0.07442411510132704, -0.14186686943426277, 0.08630430489552743, 0.4692059318450364, -0.1865400695947535, -0.17467094066016603, -0.02582227353317042, -0.3178692219609564, -0.0360971208040913, -0.07124242235934644, 0.08265324320757028,... |
710.0348 | Finite-temperature Bell test for quasiparticle entanglement in the Fermi
sea | We demonstrate that the Bell test cannot be realized at finite temperatures
in the vast majority of electronic setups proposed previously for quantum
entanglement generation. This fundamental difficulty is shown to originate in a
finite probability of quasiparticle emission from Fermi-sea detectors. In order
to overc... | cond-mat.mes-hall | we demonstrate that the bell test cannot be realized at finite temperatures in the vast majority of electronic setups proposed previously for quantum entanglement generation this fundamental difficulty is shown to originate in a finite probability of quasiparticle emission from fermisea detectors in order to overcome t... | [['we', 'demonstrate', 'that', 'the', 'bell', 'test', 'can', 'not', 'be', 'realized', 'at', 'finite', 'temperatures', 'in', 'the', 'vast', 'majority', 'of', 'electronic', 'setups', 'proposed', 'previously', 'for', 'quantum', 'entanglement', 'generation', 'this', 'fundamental', 'difficulty', 'is', 'shown', 'to', 'origin... | [-0.1099660102455263, 0.1628121889027005, -0.07943466707878212, 0.05772066069237718, -0.047554884063587946, -0.16312235217033463, 0.08391668718435209, 0.33580009880031203, -0.23216246237726326, -0.27592393526257103, 0.004747898238499395, -0.2639543480366807, -0.06916721385840158, 0.21554857452230697, -0.041757426790850... |
710.0349 | An operational calculus for the Mould operad | The operad of moulds is realized in terms of an operational calculus of
formal integrals (continuous formal power series). This leads to many
simplifications and to the discovery of various suboperads. In particular, we
prove a conjecture of the first author about the inverse image of non-crossing
trees in the dendri... | math.QA math.CO | the operad of moulds is realized in terms of an operational calculus of formal integrals continuous formal power series this leads to many simplifications and to the discovery of various suboperads in particular we prove a conjecture of the first author about the inverse image of noncrossing trees in the dendriform ope... | [['the', 'operad', 'of', 'moulds', 'is', 'realized', 'in', 'terms', 'of', 'an', 'operational', 'calculus', 'of', 'formal', 'integrals', 'continuous', 'formal', 'power', 'series', 'this', 'leads', 'to', 'many', 'simplifications', 'and', 'to', 'the', 'discovery', 'of', 'various', 'suboperads', 'in', 'particular', 'we', '... | [-0.16879711563524324, 0.015464855818436263, -0.10399648114253068, 0.09171792879351415, -0.12790132319787517, -0.04042660344566684, 0.0031981256306607975, 0.3481226157746278, -0.371034283132758, -0.25668526644585654, 0.07357466450957872, -0.2203222104544693, -0.20311319938628003, 0.1704750777425943, -0.1774031744171225... |
710.035 | Berry Phases, Quantum Phase Transitions and Chern Numbers | We study the relation between Chern numbers and Quantum Phase Transitions
(QPT) in the XY spin-chain model. By coupling the spin chain to a single spin,
it is possible to study topological invariants associated to the coupling
Hamiltonian. These invariants contain global information, in addition to the
usual one (obt... | cond-mat.str-el cond-mat.stat-mech | we study the relation between chern numbers and quantum phase transitions qpt in the xy spinchain model by coupling the spin chain to a single spin it is possible to study topological invariants associated to the coupling hamiltonian these invariants contain global information in addition to the usual one obtained by i... | [['we', 'study', 'the', 'relation', 'between', 'chern', 'numbers', 'and', 'quantum', 'phase', 'transitions', 'qpt', 'in', 'the', 'xy', 'spinchain', 'model', 'by', 'coupling', 'the', 'spin', 'chain', 'to', 'a', 'single', 'spin', 'it', 'is', 'possible', 'to', 'study', 'topological', 'invariants', 'associated', 'to', 'the... | [-0.24840096917680718, 0.21300647588081614, -0.04460237430281599, 0.0984258551894031, -0.07466554252790626, -0.17383007747544485, 0.06595512612627565, 0.3536198537966067, -0.3059059141246094, -0.3017339594027197, 0.039700906635103325, -0.28759801759257575, -0.1885387818064456, 0.13765980149037205, -0.0076019202824682, ... |
710.0351 | Transition radiation in turbulent astrophysical medium. Application to
solar radio bursts | Modern observations and models of various astrophysical objects suggest that
many of their physical parameters fluctuate substantially at different spatial
scales. The rich variety of the emission processes, including Transition
Radiation but not limited to it, arising in such turbulent media constitutes
the scope of... | astro-ph | modern observations and models of various astrophysical objects suggest that many of their physical parameters fluctuate substantially at different spatial scales the rich variety of the emission processes including transition radiation but not limited to it arising in such turbulent media constitutes the scope of stoc... | [['modern', 'observations', 'and', 'models', 'of', 'various', 'astrophysical', 'objects', 'suggest', 'that', 'many', 'of', 'their', 'physical', 'parameters', 'fluctuate', 'substantially', 'at', 'different', 'spatial', 'scales', 'the', 'rich', 'variety', 'of', 'the', 'emission', 'processes', 'including', 'transition', '... | [-0.047692153625705815, 0.16467134171398357, -0.045164519301449345, 0.11686813934544002, -0.07259983508265577, -0.09555868773687896, -0.011143785060474849, 0.36174178497666226, -0.2605840599613397, -0.33827446112575543, 0.07396614639375391, -0.25195672897306004, -0.10014203204108137, 0.2395132310588711, 0.0092486196455... |
710.0352 | Small x QCD and Multigluon States: a Color Toy Model | We introduce and study a toy model with a finite number of degrees of freedom
whose Hamiltonian presents the same color structure of the BKP system appearing
in the studies of QCD in the Regge limit. We address within this toy model the
question of the importance of finite number of color corrections with respect
to ... | hep-th | we introduce and study a toy model with a finite number of degrees of freedom whose hamiltonian presents the same color structure of the bkp system appearing in the studies of qcd in the regge limit we address within this toy model the question of the importance of finite number of color corrections with respect to the... | [['we', 'introduce', 'and', 'study', 'a', 'toy', 'model', 'with', 'a', 'finite', 'number', 'of', 'degrees', 'of', 'freedom', 'whose', 'hamiltonian', 'presents', 'the', 'same', 'color', 'structure', 'of', 'the', 'bkp', 'system', 'appearing', 'in', 'the', 'studies', 'of', 'qcd', 'in', 'the', 'regge', 'limit', 'we', 'addr... | [-0.14204696831293404, 0.13301485502161087, -0.08381306181351343, 0.02762528607272543, -0.01794570442289114, -0.06651184406752388, 0.03652908856165595, 0.3014073790051043, -0.22495257502111296, -0.3057335720057987, 0.047234365945526706, -0.2764745108472804, -0.11645969034483035, 0.0762122223386541, -0.06415939263145749... |
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